2023 Conference on Lasers and Electro-Optics Europe& European Quantum Electronics Conference

Advance Programme
Munich ICM
International Congress
Centre Munich, Germany

26 - 30 June 2023
www.cleoeurope.org
Sponsored by• European Physical Society / Quantum Electronics and Optics Division• IEEE Photonics Society• Optica

26th International Congress on Photonics in Europe
Collocated with Laser World of Photonics Industry Days

https://world-of-photonics.com/en/Table of contents

TABLE OF CONTENTS
Welcome and Foreword
Days at a Glance
Sessions at a Glance
How to Read the Session Codes?
How to Find the Room?
TopicsCommittees
General Information
Technical Programme

01

02
04
14
15
17
21
25
30
40

Welcome and foreword

GENERAL INFORMATION

2023 Conference on Lasers and ElectroOptics Europe & European Quantum
Electronics Conference

CLEO®/Europe - EQEC 2023
Munich, International
Congress Centre (ICM),
Germany, 26 - 30 June 2023
www.cleoeurope.org
Organised and Sponsored by• European Physical Society / Quantum
Electronics and Optics Division• IEEE Photonics Society• Optica

Also sponsored by• World of Photonics Congress• EPS Young Minds

Welcome to the 2023 Conferenceon Lasers and Electro-Optics
Europe & European Quantum
Electronics Conference (hereafter
CLEO®/Europe-EQEC) at the Worldof Photonics Congress 2023

CLEO®/Europe will showcase the latest
developments in a wide range of laser andphotonics areas including solid-state lasers,
semiconductor lasers, terahertz sources andapplications, applications of nonlinear optics,
optical materials, optical fabrication and characterization, ultrafast optical technologies,
high-field laser and attosecond science, optical sensing and microscopy, optical technologies for communications and data storage,
fibre and guided wave lasers and amplifiers,
micro- and nanophotonics, photonic applications in biology and medicine, and material processing.
EQEC will feature the fundamentals ofquantum optics and ultracold quantum matter, quantum information, quantum communication and sensing, topological states of light,
precision metrology, ultrafast optical science,
nonlinear phenomena, solitons, and self-organization, plasmonics and metamaterials, two-dimensional and novel materials, and theoreticaland computational photonics modelling.
CLEO®/Europe-EQEC creates a uniqueforum where participants can obtain informative overviews and discuss recent advances
on a wide range of topics, from fundamental
light-matter interaction and new sources ofcoherent light to technology development,
system engineering and various applicationsof photonics.
Over five days CLEO®/Europe-EQEC 2023
will showcase around 1759 technical contributions in the form of oral presentations inparallel sessions and posters from university,
research organisations and industry, drawn
from all countries around the world, and will
provide an unparalleled opportunity to bring
together scientists, engineers and users oflaser and photonics technologies under thesame roof.

Following on from the very successful previous
conferences held in Amsterdam (1994), Hamburg (1996), Glasgow (1998), Nice (2000) and
Munich (2003, 2005, 2007, 2009, 2011, 2013,2015, 2017, 2019), and the 2021 virtual conference, the General and Programme Chairs
warmly welcome you to the 2023 CLEO®/
Europe-EQEC conference, which is being
held in Munich from June 26 - 30. CLEO®/
Europe-EQEC targets university and industry
scientists and researchers as well as students
and graduates. We extend a special welcome toattending young researchers, postgraduate and
PhD students, and we wish them every success,especially if this is their first participation in a
major scientific conference.
The CLEO®/Europe-EQEC conference series
has established a strong tradition as the largest,
most comprehensive and prestigious gathering of optics and photonics researchers andengineers in Europe. With technical co-sponsorship provided by the European PhysicalSociety (EPS), the Institute of Electrical andElectronics Engineers (IEEE) Photonics Society, and Optica (formerly OSA), CLEO®/Europe
and EQEC have a strong international presencein the complementary research areas of laser
science, photonics and quantum electronics.
More specifically, CLEO®/Europe emphasizes
applied physics, optical engineering and applications of photonics and laser technology, whereas
EQEC addresses more basic research in laser
physics, nonlinear optics and quantum optics.

02

Particular highlights of the 2023 programme
will be a series of symposia:• JSI - Free electron lasers• JSII - Infrared integrated photonics for astronomical applications• JSIII - Photonics for artificial intelligence• JSIV - Photonics for sustainability• JSV - Diversity in Photonics• JSVI - Nanophoxonics and nanoscaleheat transfer
This year a particular highlight devoted todiversity in photonics will be featured. Several events managed by our conference orother collocated conferences will take place.
See “Special events” in this programme or the
separate leaflet detailing the programme. This
program will span five days and include a rangeof activities, such as workshops, panel discussions, keynote speeches, career and networking
events. These activities will cover a variety of
topics, including:• The importance of diversity, equity, and inclusion in the photonics industry• Support for early-stage researchers• DiversiWiki session• Workshop exploring the concept of privilege.
The programme will be open to all attendees of Laser World of Photonics 2023 and will
be run in collaboration with several organizations, including the European Optical Society(EOS), the European Physical Society (EPS),
Wissenschaftliche Gesellschaft Lasertechnik
und Photonik e.V. (WLT), Optica, IEEE Photonics Society, and the International Society
for Optics and Photonics (SPIE).
Overall, this diversity, equity, and inclusion
programme aims to raise awareness of the importance of diversity and inclusivity within thephotonics community and provide attendees
with the tools and strategies they need to createa more welcoming and inclusive industry forall. See https://www.photonics-congress.com/
en/about/conferences/diversity-program/This year in collaboration with the CLEO/
Europe-EQEC 2023 co-organizers (European
Physical Society, Optica, IEEE Photonics Society), the European Optical Society will chair two
Early-Stage Researcher (ESR) sessions, offering
an opportunity for PhDs and Post-docs to holda 3-minute oral presentation (pitch) to draw
attention to their upcoming poster presentation. Thirteen presentations were selected per
session. Each registered participant is cordiallyinvited to attend on Monday 26 and Wednesday 28 June, 12:00-13:00, Room 4a ICM.
Additionally, one joint session LiMCLEO®/Europe will take place on lightmatter interaction.
As usual a series of prestigious EPS-QEOD
prizes and awards will be remitted during a
special plenary and award ceremony to takeplace on Tuesday 27 June 2023 from 10:30 to12:30, room 1. For further information, see theseparate booklet.
All conferences together form the World of
Photonics Congress bundling various topicalconferences under one roof and under the organisation of Messe München International. It
is a strategic and operative umbrella for various
individual conferences held by leading associations and organisations. The other co-locatedconferences include:• ECBO - European Conferences on Biomedical
Optics organised by SPIE in cooperation with
Optica (Formerly OSA).
• LiM 2023 - Lasers in Manufacturing organisedby the German Scientific Laser Society (WLT).
• Digital Optical Technologies organised by
SPIE Europe.
• Optical Metrology organised by SPIE Europe.
All co-located conferences will share registration and allow delegates to attend sessions.

As in former years, the meeting will be complemented by the LASER 2023 World of Photonics,
the world’s largest tradeshow of laser and opticaltechnology, which will provide researchers withthe opportunity to see the latest developments
in a very wide range of laser sources, optical andphotonics products, and components.

settled to anticipate and capture emerging fields
in optics by giving emphasis to fast developing,well defined topics.
CLEO®/Europe-EQEC 2023 will also present
ten Short Courses covering a wide range of
topics in photonics and laser technology. All
courses will be open to attendees of the Worldof Photonics Congress and Laser World of Photonics subject to payment of the course fee. All
Short Courses will be 2 × 1.5 hour long (with ½
an hour coffee break in-between). The courses
will take place from Monday 26 June to Friday
30 June 2023 as. A few courses are running inparallel. See details at https://www.cleoeurope.
org/short-courses/
The conference will also feature two postdeadline sessions on Thursday evening, 29 June
2023 (from 17:45 to 19:15). Their purpose is
to give the audience the chance to listen to
the latest breaking news in optics. This makes
them particularly attractive events that certainly contribute to the great atmosphere thatmakes the CLEO®/Europe-EQEC conferencea unique meeting.
In addition to the technical sessions involving oral presentations, all scientific areas ofboth CLEO®/Europe and EQEC will be coveredin poster sessions, which will provide an interactive and less formal way for researchers to
discuss their work, interact and exchange ideas.
CLEO®/Europe-EQEC is now establishedas the largest and most comprehensive gathering of optics and photonics researchers andengineers in Europe, spanning classical andquantum optical science, laser technology andphotonics applications.
The conference programme could not havebeen elaborated without the vital support andeffort of 273 scientists, forming 13 CLEO®/Europe, 10 EQEC, 6 Joint Symposia and 1 Joint
Session sub-committees, who have assembled

Conference Structure
and Technical Sessions
CLEO®/Europe-EQEC consists of a large number of technical presentations in a number ofdifferent formats:
Plenary talks are broad-scope, 60-minutelong talks given by these world-leading scientists, and are accessible to a general technical audience including conference attendees,
exhibitors, and exhibit visitors. Plenary talks
are not held in parallel with other sessions,allowing maximum possible attendance. The
2023 plenary talks will be presented by Donna
Strickland (CLEO®/Europe), Claudio Conti(EQEC), and Constantin L. Haefner andTammy Ma (World of Photonics).
Tutorials (60-minute talks) and Keynote
presentations (45-minute talks) are also given by the world leaders in particular technicalareas. They are generally directed at a more specific audience, and are thus delivered in parallelwith other sessions. Keynotes provide a surveyof exciting recent developments, and Tutorials
are particularly valuable for those unfamiliar
with a particular field.
Additionally to these talks the conference
will feature invited talks, orals and poster presentations.
Other very much appreciated CLEO®/EuropeEQEC meetings are the special Symposia

03

an excellent series of talks and posters covering
a wide range of fields in optics and quantum
electronics. The technical programme featuring 1759 presentations including 3 plenary
talks, 7 tutorial talks, 10 keynote talks, 77
invited talks, 17 talks upgraded to invited,1109 oral presentations, 10 short courses anda poster programme including 526 posters
to be presented in five poster sessions (among
them 26 selections for poster pitches). 17 oralpresentations will also be featured in the two
post-deadline sessions to take place on Thursday evening.
The Conference Chairs would like to extend their sincere thanks to the technicalprogramme committee members for all their
hard and fruitful work. A conference as large
as CLEO®/Europe-EQEC requires two years ofplanning and organisation. Here, we also thankthe staff of the European Physical Society, andthe local conference chair in Munich for invaluable profes sional assistance during thisperiod. We thank Messe München GmbH, theWorld of Photonics Congress steering committee, the CLEO/Europe-EQEC steering committee and all the Sponsoring Societies for theirguidance, support, and their invaluable advice,
which ensures that this event not only remains
at the core of optics and photonics research formany nations, but will also be a major event
in Europe.
Let us finally thank our attendees. The real
success of CLEO®/Europe-EQEC 2023 indeed
rests on the effort and commitment of theseresearchers and students, who all contributeto the tremendous evolution of our research
field and to the high quality of the papers thatwill be presented.
We wish you all a lively, fruitful, and enjoyable conference, and we are looking forward tosee you in Munich!

GENERAL INFORMATION

Welcome and foreword

Monday at a glance
ICM - ROOM 1

08:30

GENERAL INFORMATION

09:00
09:30

ICM - ROOM 4A

ICM - ROOM 4B

ICM - ROOM 13A

ICM - ROOM 13B

ICM - ROOM 14A

ICM - ROOM 14B

CM-1

EJ-1

EG-1

CA-1

CB-1

CD-1

CH-1

Laser additive
manufacturing I

Simulating multi-mode andnon-hermitian systems

Nanoantennas andnanoconfinement

Mid-infrared lasers

Photonic crystal lasers

Frequency conversion I

Imaging through scattering
media

10:00
10:30
11:00
11:30

COFFEE BREAK
CM-2

EJ-2

EG-2

CA-2

CD-2

CH-2

Laser semiconductor
processing

Computational photonics at
the light-matter interface

Metasurfaces

Ultrafast lasers at 2 μm
and beyond

Frequency conversion II

AI for optical sensing

12:00

PP-1

12:30

LUNCH BREAK

Early-stage researcher (ESR)
session - Poster pitches I

13:00
13:30
14:00
14:30
15:00

CA, CB, CM, ED, EJ AND JSII POSTER SESSIONS - HALL B0
CM-3

CK-1

EG-3

CA-3

CB-2

CD-3

Temporal and spatial
beam shaping for laser
processing I

Lithium niobate and silica
systems

Optoelectronics and lightelectron interactions

Novel laser materials

Surface-emitting lasers

Integrated nonlinear
photonics

15:30
COFFEE BREAK

16:00
16:30

PL-1
CLEO/Europe 2023 Plenary

17:00
17:30
18:00
18:30

PL-C
Career event with Donna
Strickland

19:00
19:30

HAPPY HOUR KINDLY SPONSORED BY THE QUANTUM ELECTRONICS OPTICS DIVISION (QEOD)
OF THE EUROPEAN PHYSICAL SOCIETY - ICM FOYER, HALL B0, GROUND FLOOR (END 21:00)

20:00

04

Monday at a glance

08:30
09:00

HALL B1 (B11) - ROOM 1

HALL B1 (B12) - ROOM 2HALL B3 (B32) - ROOM 6HALL A1 (A11) - ROOM 7

HALL A1 (A12) - ROOM 8

JSII-1

CF-1

SH-3

ED-1

CE-1

EB-1

The photonic yield in astronomy

Advances in attosecond
technology and high orderharmonic generation I

Short course: Laser beam
analysis, propagation, and spatial
Shaping techniques

Precision spectroscopy
for fundamental science

Specialty optical fibres

Optomechanical and otherquantum oscillators

09:30
10:00
10:30
11:00
11:30

COFFEE BREAK
JSII-2

CF-2

SH-3

ED-2

CE-2

EB-2

Manipulating astronomicalsignals with photonics and futurechallenges I

Advances in attosecond
technology and high orderharmonic generation II

Short course: Laser beam
analysis, propagation, and spatial
Shaping techniques

Direct comb spectroscopy

Hollow core optical fibres

Quantum interferometry

12:00
12:30

LUNCH BREAK

13:00
13:30
14:00
14:30
15:00

CA, CB, CM, ED, EJ AND JSII POSTER SESSIONS - HALL B0
JSII-3

CF-3

CL-1

ED-3

CE-3

EB-3

Manipulating astronomicalsignals with photonics and futurechallenges II

Complex pulses and theircharacterization

Brain imaging

Frequency references
and transfer

Optical materials: Structures

Quantum optics I

15:30
16:00

COFFEE BREAK

16:30
17:00
17:30
18:00
18:30
19:00
19:30

HAPPY HOUR KINDLY SPONSORED BY THE QUANTUM ELECTRONICS OPTICS DIVISION (QEOD)
OF THE EUROPEAN PHYSICAL SOCIETY - ICM FOYER, HALL B0, GROUND FLOOR (END 21:00)

20:00

05

GENERAL INFORMATION

ICM - ROOM OSTERSEEN

Tuesday at a glance
ICM - ROOM 1

08:30

GENERAL INFORMATION

09:00
09:30

ICM - ROOM 4A

ICM - ROOM 4B

ICM - ROOM 13A

ICM - ROOM 13B

ICM - ROOM 14A

ICM - ROOM 14B

CM-4

CK-2

EG-4

CA-4

CB-3

CD-4

CH-3

Temporal and spatial
beam shaping for laser
processing II

Plasmonic structures andcomponents

Ultrastrong light matterinteractions and nonlinear
opticsPolarization effects andstructured laser beams

Novel semiconductor laser
concepts

Specialty fibers

On-chip optical sensing

10:00
10:30
11:00
11:30
12:00

COFFEE BREAK
PL-2a
EQEC 2023 Plenary talkPL-2bAward ceremony

12:30

LUNCH BREAK

13:00
13:30
14:00
14:30

CD, CF, CK AND EG POSTER SESSIONS - HALL B0
PL-3

CM-5

CB-4

CD-5

World of Photonics Plenary

Modelling of laser-induced
processes

Photonic integration I

Supercontinuum
generation

15:00
15:30
16:00
16:30
17:00

COFFEE BREAK
CM-6

CK-3

EG-5

CA-5

CB-5

CD-6

CD-4

Laser volume processing

Resonant structures andcavities

Single emitters

Diamond lasers andfrequency converters

Photonic integration II

Mid-IR applications

Field applications

17:30
18:00
18:30
19:00

"BIER & BREZEL" GET TOGETHER KINDLY SPONSORED BY SPIE - ICM FOYER, HALL B0, GROUND FLOOR

19:30
20:00

06

Tuesday at a glance
ICM - ROOM OSTERSEEN

09:00
09:30

HALL B1 (B12) - ROOM 2HALL B3 (B32) - ROOM 6HALL A1 (A11) - ROOM 7

HALL A1 (A12) - ROOM 8

JSVI-1

CF-4

ED-4

CG-1

EA-1

EB-4

NanophoXonics, optomechanicalsystems and thermal transport

Complex pulse shaping
and characterization

Cavity-enhanced precision
spectroscopy

Ultrafast magnetic fields
and anisotropy

Fundamental quantum optics

Quantum computation I

GENERAL INFORMATION

08:30

HALL B1 (B11) - ROOM 1

10:00
COFFEE BREAK

10:30
11:00
11:30
12:00
12:30

LUNCH BREAK

13:00
13:30

CD, CF, CK AND EG POSTER SESSIONS - HALL B0

14:00
14:30
15:00
15:30
16:00
16:30
17:00

COFFEE BREAK
JSVI-2

CF-5

CE-4

CG-2

CJ-1

EB-5

Radiative heat transfer,thermoelectrics& thermochromics, SPP

Carrier-envelope phasemetrology and applications

Emission materials

Ultrafast physics
in condensed matter

Transverse mode instability
in fiber lasers and amplifiers

Quantum key distribution

17:30
18:00
18:30
19:00

"BIER & BREZEL" GET TOGETHER KINDLY SPONSORED BY SPIE - ICM FOYER, HALL B0, GROUND FLOOR

19:30
20:00

07

Wednesday at a glance
ICM - ROOM 1

08:30

GENERAL INFORMATION

09:00
09:30

ICM - ROOM 4A

ICM - ROOM 4B

ICM - ROOM 13A

ICM - ROOM 13B

ICM - ROOM 14A

ICM - ROOM 14B

CM-7

CK-4

EG-6

CA-6

JSI-1

CD-7

CH-5

Laser written waveguides
and gratings

Active components

Nanomanipulation,nano-organizationand correlation

Visible and UV lasers

Nonlinear X-ray
wave-mixing

Spectroscopy applications

Optical frequency combs

10:00
COFFEE BREAK

10:30
11:00
11:30
12:00

CK-5

JSIV-1

CA-8

JSI-2

CD-8

CH-6

Silicon nitride systems
and devices

Photo(electro)chemistry
and desalination

High-power lasers
and facilities

X-ray source developments

Nonlinear dynamics I

Imaging at the nanoscale

PP-2

12:30

LUNCH BREAK

Early-stage researcher (ESR)
session - Poster pitches I

13:00
13:30
14:00
14:30
15:00

CH, EE, EF, JSI AND JSIV POSTER SESSIONS - HALL B0
JSI-3

CK-6

JSIV-2

CA-7

CB-6

CD-9

CH-7

Imaging geometricand electronic structures

Integrated optical devices I

Thermal radiationand photovoltaics

Power scaling

Integrated photonics
and frequency combs

Nonlinear dynamics II

Instrumentation for opticalsensing and microscopy

15:30
16:00
16:30
17:00

COFFEE BREAK
JSI-4

CK-7

EH-1

CA-9

CB-7

CD-10

CH-8

Nonlinear and ultrafast
X-ray spectroscopy

Integrated optical devices II

Temporal and topologicalmetamaterials

Waveguide lasers

Diode laser
frequency combs

Resonant structures

Methods in optical sensing
and microscopy

17:30
18:00
18:30
19:00
19:30

CLEO®/EUROPE-EQEC CONFERENCE DINNER, LÖWENBRÄUKELLER - MUNICH (END 23:00)

20:00

08

08:30
09:00
09:30

ICM - ROOM OSTERSEEN

HALL B1 (B11) - ROOM 1

HALL B1 (B12) - ROOM 2HALL B2 (B22) - ROOM 5

HALL B3 (B32) - ROOM 6HALL A1 (A11) - ROOM 7

HALL A1 (A12) - ROOM 8

EE-1

CF-6

SH-1

SH-9

CI-1

CJ-2

EB-6

Ultrafast spectroscopy
of solids

New trends inpost-compression I

Short course: High-power
fiber lasers

Short course: Silicon
photonics

Fibers fortelecommunications

Beam combination of fiber
lasers and amplifiers

Integrated quantum optics

10:00
10:30
11:00

COFFEE BREAK
CM-LIM

CF-7

SH-1

SH-9

CI-2

CJ-3

EB-7

Lightmatter interaction

Ultrafast laser technology I

Short course: High-power
fiber lasers

Short course: Silicon
photonics

Frequency combs

Mode-locked fiber lasers

Quantum sensing

11:30
12:00
12:30

LUNCH BREAK

13:00
13:30
14:00
14:30

CH, EE, EF, JSI AND JSIV POSTER SESSIONS - HALL B0
EF-1

CF-8

SH-7

SH-8

CI-3

CJ-4

EB-8

Complex fiber dynamics I

Ultrafast laser technology II

Short course: Nonlinear
crystal optics

Frequency combs principles
and applications

Ultrafast
telecommunications

Specialty fiber
characterisation techniquesand components

Quantum imaging

15:00
15:30
16:00
16:30
17:00

COFFEE BREAK
EF-2

CF-9

SH-7

SH-8

CI-4

CJ-5

EB-9

Kerr solitons and frequency
combs I

Ultrafast spectroscopy

Short course: Nonlinear
crystal optics

Frequency combs principles
and applications

Fibers fortelecommunications
and THz

Novel fiber lasers

Quantum communication

17:30
18:00
18:30
19:00
19:30

CLEO®/EUROPE-EQEC CONFERENCE DINNER, LÖWENBRÄUKELLER - MUNICH (END 23:00)

20:00

09

GENERAL INFORMATION

Wednesday at a glanceThursday at a glance
ICM - ROOM 1

08:30

GENERAL INFORMATION

09:00

ICM - ROOM 4A

ICM - ROOM 4B

ICM - ROOM 13A

ICM - ROOM 13B

ICM - ROOM 14A

ICM - ROOM 14B

EA-2

CK-8

EH-2

CA-10

CB-8

EF-3

CH-9

Nonlinear quantum optics

Advanced design methods

Quantum plasmonics

Ytterbium lasers

Quantum cascade laser
frequency combs

Kerr solitons and frequency
combs II

Quantum andsingle-photon sensing

09:30
10:00
10:30
11:00
11:30
12:00
12:30
13:00

COFFEE BREAK
EA-3

CK-9

EH-3

CA-11

CB-9

EF-4

CH-10

Photonic quantum
technology

Micro optical combs

Nonlinear and active
metastructures

New laser designs

Quantum cascade lasers
and frequency combs

Spatiotemporal effects
in optical systems

Fiber sensors I

CLS-1 - FOYER 1st FLOORLUNCH BREAK

Career and diversity lunchfor early postdocs

13:30
14:00
14:30

CE, CG, EA, EB AND EH POSTER SESSIONS - HALL B0
EA-4

CK-10

EH-4

JSIII-1

CB-10

EF-5

CH-11

Quantum light sources I

Metasurface technologies
and applications

Tunable and holographic
metasurfaces

Photonic reservoir
computing, extreme
learning and isingmachines I

Single mode and narrow
linewidth semiconductor
lasers

Dissipative solitonsand mode-locking I

Fiber sensors II

15:00
15:30
16:00
16:30
17:00
17:30
18:00
18:30

COFFEE BREAK
EA-5

CK-11

EH-5

JSIII-2

CB-11

EF-6

CH-12

Quantum light sources II

Photonic crystals andperiodic structures

Concepts and applications
in plasmonics andmetastructures

Photonic reservoir
computing, extreme
learning and isingmachines II

High-performance
diode lasers

Dissipative solitonsand mode-locking II

Super-resolution imaging

PD-1

PD-2

Postdeadline session I

Postdeadline session II

19:00
19:30
20:00

10

08:30
09:00
09:30

ICM - ROOM OSTERSEEN

HALL B1 (B11) - ROOM 1

HALL B1 (B12) - ROOM 2HALL B2 (B22) - ROOM 5

HALL B3 (B32) - ROOM 6HALL A1 (A11) - ROOM 7

HALL A1 (A12) - ROOM 8

JSI-5

CF-10

SH-2

SH-4

CG-3

CJ-6

EB-10

Ultrafast molecular
dynamics

New trends inpost-compression I

Short course: Opticalparametric oscillators

Short course: Practicalquantum optics

Taylored targets and fields

Specialty fiber and devices

Quantum memories

10:00
10:30
11:00
11:30

COFFEE BREAK
CL-2

CC-1

SH-2

SH-4

CG-4

CE-5

EB-11

Flow cytometry
and ultrasoundNonlinear THz phenomena

Short course: Opticalparametric oscillators

Short course: Practicalquantum optics

Few-cycle drivers
and harmonic sources

Sensor materials
and structures

Single photon sourcesand detectors

12:00
12:30

LUNCH BREAK

13:00
13:30
14:00
14:30

CE, CG, EA, EB AND EH POSTER SESSIONS - HALL B0
CL-3

CC-2

SH-5

SH-6

CG-5

CE-6

EB-12

Lightmatter interaction

High power THz sources

Short course: Mid-infrared
semiconductor lasers

Short course:
THz measurements
and their applications

Ultrafast quantum physics
and correlated systems

Optical materials:
Measurements

Quantum optics II

15:00
15:30
16:00
16:30
17:00

COFFEE BREAK
CL-4

CC-3

SH-5

SH-6

CG-6

CE-7

EB-13

Photonic technology forbiomedical applications

Novel approach THz sources

Short course: Mid-infrared
semiconductor lasers

Short course:
THz measurements
and their applications

Attosecond methods
and fundamentals

Nonlinear optical materials

Quantum simulationand computation

17:30
18:00
18:30
19:00
19:30
20:00

11

GENERAL INFORMATION

Thursday at a glanceFriday at a glance
ICM - ROOM 1

08:30

GENERAL INFORMATION

09:00
09:30

ICM - ROOM 2

ICM - ROOM 3

ICM - ROOM 4A

11:00
11:30
12:00
12:30
13:00

14:30
15:00

ICM - ROOM 11

ICM - ROOM 12A

EA-6

CK-12

EI-1

CC-4

CI-5

CE-8

ED-5

Laser-based surfacefunctionalizationand sensors

Mid-IR fiber sources

Quantum optics inimaging

Photonic crystals

2D van der
Waals materials:
fundamentals andapplications

THz QCL

Quantum andfree-spacecommunications

Photonic integrated
circuits

Precision metrology

COFFEE BREAK
CM-9

CJ-8

EA-7

CK-13

EI-2

CC-5

CI-6

CE-9

ED-6

Laser-induced
periodic surface
structures

Pulsed fiber sources

Atomic systems

Advanced photonic
devicesNonlinear andquantum optics
with van der Waals
layered materials

THz spectroscopy
and techniques

Modulation anddemodulation

Lithium niobate
platform

Frequency combs:
Sources andcharacterization

CLS-2 - FOYER 1st FLOORLUNCH BREAK

Career and diversity
lunch for PhD candidates

CC, CI, CJ, CL, EC, EI AND JSIII POSTER SESSIONS - HALL B0
CM-10

CJ-9

EA-8

CK-14

EI-3

CC-6

CI-7

CE-10

SH-10

Dynamics of laserinduced processes

Novel fibers

Nonclassical statesof light

Recent advancesin laser technology

Novel lowdimensional andfunctional materials

THz devices

Satellite and radio

Doped opticalmaterials

Short course:
Finite element
modelling methods
for photonics

15:30
16:00
16:30
17:00

ICM - ROOM 12B

CJ-7

13:30
14:00

ICM - ROOM 5

CM-8

10:00
10:30

ICM - ROOM 4B

COFFEE BREAK
CM-11

CJ-10

EA-9

CK-15

EI-4

CC-7

CI-8

CE-11

SH-10

Laser additive
manufacturing II

2-micron fiber
sources

Optomechanicalsystems

Micro- and nanooptical cavities

Ultrafast dynamics
in layered materials

THz applications

Frequency combs
and microwave
photonics

Fabrication methods

Short course:
Finite element
modelling methods
for photonics

17:30
18:00
18:30
19:00
19:30
20:00

12

Friday at a glance

08:30
09:00

ICM - ROOM 13B

ICM - ROOM 14A

ICM - ROOM 14B

ICM - ROOM 14C

ICM - ROOM OSTERSEENICM - ROOM 21

ICM - ROOM 22A

JSIII-3

CD-11

EF-7

CH-13

EE-2

CL-5

EJ-3

EC-1

Photonic accelerators I

Nonlinear metasurfaces

Complex fiber
dynamics II

IR & Raman sensing

Ultrafast processes inionised media

Spectroscopy

Nonlinear optics
modeling & artificial
intelligence

Non-linear andnon-hermitian
topological photonics

09:30
10:00
10:30
11:00

COFFEE BREAK
JSIII-4

CD-12

EF-8

CH-14

EE-3

CL-6

EJ-4

EC-2

Photonic accelerators II

Stimulated Brillouinscattering

Symmetry breaking
in coupled resonators

Photothermal andphotoacoustic sensing

Ultrafast XUV and soft
X-ray spectroscopy

Advanced microscopy I

Tailored light andoptical design

Photonic band topology

11:30
12:00
12:30

LUNCH BREAK

13:00
13:30
14:00
14:30
15:00

CC, CI, CJ, CL, EC, EI AND JSIII POSTER SESSIONS - HALL B0
JSIII-5

CD-13

EF-9

CH-15

EE-4

CL-7

CF-11

EC-3

Brain-inspired
photonic devices
and computing I

Nonlinear imaging
and microscopy

Topological andnonlinear effects

Bio-sensing

Ultrafast nonlinear
optics in gases

Advanced microscopy II

Parametric ultrafast
sources

Emerging trends
and singular photonic
topology

15:30
16:00
16:30
17:00

COFFEE BREAK
JSIII-6

CD-14

EF-10

CH-16

EE-5

CL-8

CF-12

Brain-inspired
photonic devices
and computing II

Quantum applications

Extreme events andforecasting techniques

Environmental
optical sensing

Ultrafast manipulationand control

Novel laser sources

Mid-IR sources

17:30
18:00
18:30
19:00
19:30
20:00

13

GENERAL INFORMATION

ICM - ROOM 13A

Sessions at a Glance
PLENARY SESSIONSAWARD CEREMONY

GENERAL INFORMATION

PL-1

PL-2a

PL-2b

PL-3

CLEO®/Europe 2023 Plenary talkMonday, 16:00 - 17:30, Room 1 ICM
EQEC 2023 Plenary talkTuesday, 10:30 - 11:30, Room 1 ICM
Award ceremony
Tuesday, 11:30 - 12:30, Room 1 ICM
World of Photonics Plenary talkTuesday, 14:00 - 15:30, Room 1 ICM

SPECIAL EVENTSDIVERSITY IN PHOTONICS
PP-1	Early-stage Researcher (ESR)
session - Poster pitches I
Monday, 12:00 - 13:00,
Room 4a ICM
PL-C

Career event with Donna Strickland
Monday, 17:30 - 18:30,
Room 4a ICM

PP-2	Early-stage Researcher (ESR)
session - Poster pitches II
Wednesday, 12:00 - 13:00,
Room 4a ICM
CLS-1	Career and diversity lunchfor early postdocs
Thursday, 12:00 - 13:00,
Foyer, 1st floor ICM
CLS-2	Career and diversity lunch
for PhD candidates
Friday, 12:00 - 13:00,
Foyer, 1st floor ICM

POSTDEADLINE

CA-9

Waveguide lasers
Wednesday, 16:00 - 17:30, Room 13a ICM

PD-1	Postdeadline session I: Beam andpulse control and quantum physics
Thursday, 17:45 - 19:15, Room 13a ICM

CA-10

Ytterbium lasers
Thursday, 8:30 - 10:00, Room 13a ICM

CA-11

PD-2	Postdeadline session II: Nonlinear
effects and electron physics
Thursday, 17:45 - 19:15, Room 13b ICM

New laser designs
Thursday, 10:30 - 12:00, Room 13a ICM

CB – SEMICONDUCTOR LASERS

CLEO®/EUROPE 2022 SESSIONS

CB-1

Photonic crystal lasers
Monday, 8:30 - 10:00, Room 13b ICM

CA – SOLID-STATE LASERS

CB-10	Single mode and narrow linewidth
semiconductor lasers
Thursday, 14:00 - 15:30, Room 13b ICM
CB-11

High-performance diode lasers
Thursday, 16:00 - 17:30, Room 13b ICM

CC – TERAHERTZ SOURCES
AND APPLICATIONS
CC-1

Nonlinear THz phenomena
Thursday, 10:30 - 12:00, Room 1 Hall
B1 (B11)

CC-2

High power THz sources
Thursday, 14:00 - 15:30, Room 1 Hall
B1 (B11)CA-1

Mid-infrared lasers
Monday, 8:30 - 10:00, Room 13a ICM

CB-P

CB Poster session
Monday, 13:00 - 14:00, Hall B0

CA-2

Ultrafast lasers at 2 μm and beyond
Monday, 10:30 - 12:00, Room 13a ICM

CB-2

Surface-emitting lasers
Monday, 14:00 - 15:30, Room 13b ICM

CC-3

Novel approach THz sources
Thursday, 16:00 - 17:30, Room 1 Hall B1 (B11)

CA Poster session
Monday, 13:00 - 14:00, Hall B0

CB-3

Novel semiconductor laser concepts
Tuesday, 8:30 - 10:00, Room 13b ICM

CC-4

THz QCL
Friday, 8:30 - 10:00, Room 5 ICM

Novel laser materials
Monday, 14:00 - 15:30, Room 13a ICM

CB-4

Photonic integration I
Tuesday, 14:00 - 15:30, Room 13b ICM

CC-5

THz spectroscopy and techniques
Friday, 10:30 - 12:00, Room 5 ICM

CA-4	Polarization effects andstructured laser beams
Tuesday, 8:30 - 10:00, Room 13a ICM

CB-5

Photonic integration II
Tuesday, 16:00 - 17:30, Room 13b ICM

CC-P

CC Poster session
Friday, 13:00 - 14:00, Hall B0

CC-6

THz devices
Friday June 30, 14:00 - 15:30 Room 5 ICM

CC-7

THz applications
Friday June 30, 16:00 - 17:30 Room 5 ICM

CA-P

CA-3

CB-6	Integrated photonics and frequency combs
Wednesday, 14:00 - 15:30, Room 13b ICM

CA-5	Diamond lasers and frequency converters
Tuesday, 16:00 - 17:30, Room 13a ICM

CB-7
CA-6

Visible and UV lasers
Wednesday, 8:30 - 10:00, Room 13a ICM

CA-8

High-power lasers and facilities
Wednesday, 10:30 - 12:00, Room 13a ICM

CA-7

Power scaling
Wednesday, 14:00 - 15:30, Room 13a ICM

Diode laser frequency combs
Wednesday, 16:00 - 17:30, Room 13b ICM

CB-8	Quantum cascade laser frequency combs
Thursday, 8:30 - 10:00, Room 13b ICM
CB-9	Quantum cascade lasers
and frequency combs
Thursday, 10:30 - 12:00, Room 13b ICM

14

CD – APPLICATIONS OFNONLINEAR OPTICS
CD-1

Frequency conversion I
Monday, 8:30 - 10:00, Room 14a ICM

Sessions at a Glance

CD-3

CD-4

Frequency conversion II
Monday, 10:30 - 12:00, Room 14a ICM
Integrated nonlinear photonics
Monday, 14:00 - 15:30, Room 14a ICM

CE – OPTICAL MATERIALS,FABRICATIONAND CHARACTERISATION
CE-1

Specialty fibers
Tuesday, 8:30 - 10:00, Room 14a ICM
CE-2

CD-P

CD Poster session
Tuesday, 13:00 - 14:00, Hall B0

How to read the session codes?
The following pages contain the abstracts of the papers presented at the 2023 CLEO®/Europe-EQEC.

Specialty optical fibres
Monday, 8:30 - 10:00, Room 7 Hall
A1 (A11)

All CLEO®/Europe sessions are on a white background and have a code beginning with a C.
All EQEC sessions are on a shaded backgroundand have a code that begins with an E.

Hollow core optical fibres
Monday, 10:30 - 11:45, Room 7 Hall
A1 (A11)

CD-5

Supercontinuum generation
Tuesday, 14:00 - 15:30, Room 14a ICM

CE-3

Optical materials: Structures
Monday, 14:00 - 15:30, Room 7 Hall A1 (A11)

CD-6

Mid-IR applications
Tuesday, 16:00 - 17:30, Room 14a ICM

CE-4

Emission materials
Tuesday, 16:00 - 17:30, Room 2 Hall B1 (B12)CD-7Spectroscopy applications
Wednesday, 8:30 - 10:00, Room 14a ICM

CE-5

Sensor materials and structures
Thursday, 10:30 - 12:00, Room 7 Hall A1 (A11)CD-8

Nonlinear dynamics I
Wednesday, 10:30 - 12:00, Room 14a ICM

CE-P

CE Poster session
Thursday, 13:00 - 14:00, Hall B0

CD-9

Nonlinear dynamics II
Wednesday, 14:00 - 15:30, Room 14a ICM

CE-6

Optical materials: Measurements
Thursday, 14:00 - 15:30, Room 7 Hall A1 (A11)CD-10

Resonant structures
Wednesday, 16:00 - 17:30, Room 14a ICM

CE-7

Nonlinear optical materials
Thursday, 16:00 - 17:30, Room 7 Hall A1 (A11)CD-11Nonlinear metasurfaces
Friday, 8:30 - 10:00, Room 13b ICM

CE-8

Photonic integrated circuits
Friday, 8:30 - 10:00, Room 12a ICM

CD-12

Stimulated Brillouin scattering
Friday, 10:30 - 12:00, Room 13b ICM

CE-9

Lithium niobate platform
Friday, 10:30 - 12:00, Room 12a ICM

CD-13

Nonlinear imaging and microscopy
Friday, 14:00 - 15:30, Room 13b ICM

CE-10

Doped optical materials
Friday, 14:00 - 15:30, Room 12a ICM

CD-14

Quantum applications
Friday, 16:00 - 17:30, Room 13b ICM

CE-11

Fabrication methods
Friday, 16:00 - 17:30, Room 12a ICM

Both post-deadline sessions including CLEO®/
Europe and EQEC presentations are on a whitebackground and have a code beginning with PD.
Exceptions mentioned below are on a dark
background:• Short courses referenced with SH• Plenary talks, Award ceremony referenced
with PL• Career event with Donna Strickland referenced
with PL-C• Career and diversity lunches for early postdocs/ for PhD candidates referenced with CLS• CLEO®/Europe-EQEC joint symposia referenced with JS.
• CLEO®/Europe-LiM joint session referenced
with CM-LiM• Early-stage researcher (ESR) sessions - Poster
pitches referenced with PP.

Oral Presentations

Oral presentations have a code made up of twoparts, e.g.
CD-8.1 WED (Invited)

10:30

The first part (CD-8.1) indicates the Conference,
the topic title, the session title and the placementof the presentation within the session, e.g.
CD-8.1 = CLEO®/Europe (Conference)CD-8.1 =	Applications of nonlinear optics (Topic)

15

CD-8.1 =	Nonlinear dynamics I (Session title
and 8th position in the session)
CD-8.1 =	First paper presented in the " Nonlinear dynamics I" session of the
CD topic.
The second part indicates the day when the presentation takes place.
MON
TUE
WED
THU
FRI

= Monday= Tuesday= Wednesday= Thursday= Friday

The figures on the right specify at what time thetalk begins (10:30 am).
Plenary, Tutorial, Keynote and Invited Talks
are marked between brackets. Other talks haveno marking.

Posters

The first part indicates the Conference, the topic title, the poster destination, and the order ofpresentation within the topic, e.g.
EG-P.2 = EQEC
EG-P.2 =	
L ight-matter interactions at
the nanoscale
EG-P.2 = Poster
EG-P.2 =	Second poster in the "Light-matterinteractions at the nanoscale" topic
of the EQEC conference.
The second part indicates the day when theposter presentation takes place with the same
abbreviations as for the oral presentations. All
posters are displayed per topic according to theirreference numbers over the conference days (see“days at a glance”).

GENERAL INFORMATION

CD-2

Sessions at a Glance

GENERAL INFORMATION

CF – ULTRAFAST
OPTICAL TECHNOLOGIES
CF-1	Advances in attosecond	technology and high orderharmonic generation I
Monday, 8:30 - 10:00, Room 1 Hall
B1 (B11)CF-8

Ultrafast laser technology II
Wednesday, 14:00 - 15:30, Room 1 Hall
B1 (B11)CF-9

Ultrafast spectroscopy
Wednesday, 16:00 - 17:30, Room 1 Hall
B1 (B11)

CF-3	Complex pulses andtheir characterization
Monday, 14:00 - 15:30, Room 1 Hall
B1 (B11)
CF-4	Complex pulse shaping
and characterization
Tuesday, 8:30 - 10:00, Room 1 Hall
B1 (B11)

CF-11

CF-12

CG-2
CF-P

CF Poster session
Tuesday, 13:00 - 14:00, Hall B0
CG-3

CF-5	Carrier-envelope phasemetrology and applications
Tuesday, 16:00 - 17:30, Room 1 Hall
B1 (B11)
CF-6

CF-7

New trends
in post-compression I
Wednesday, 8:30 - 10:00, Room 1 Hall
B1 (B11)Ultrafast laser technology I
Wednesday, 10:30 - 12:00, Room 1 Hall
B1 (B11)

CH-2

AI for optical sensing
Monday, 10:30 - 12:00, Room 14b ICM

Parametric ultrafast sources
Friday, 14:00 - 15:30, Room 21 ICM

CH-3On-chip optical sensing
Tuesday, 8:30 - 10:00, Room 14b ICM

Mid-IR sources
Friday, 16:00 - 17:30, Room 21 ICM

CH-4

Field applications
Tuesday, 16:00 - 17:30, Room 14b ICM

CH-5

Optical frequency combs
Wednesday, 8:30 - 10:00, Room 14b ICM

Ultrafast magnetic fields and anisotropy
Tuesday, 8:30 - 10:00, Room 6 Hall B3 (B32)

CH-6

Imaging at the nanoscale
Wednesday, 10:30 - 12:00, Room 14b ICM

Ultrafast physics in condensed matter
Tuesday, 16:00 - 17:30, Room 6 Hall B3 (B32)

CH-P

CG-4

CG-P

Taylored targets and fields
Thursday, 8:30 - 10:00, Room 6 Hall B3 (B32)
Few-cycle drivers and harmonic sources
Thursday, 10:30 - 12:00, Room 6 Hall
B3 (B32)
CG Poster session
Thursday, 13:00 - 14:00, Hall B0

CG-5	Ultrafast quantum physics
and correlated systems
Thursday, 14:00 - 15:30, Room 6 Hall
B3 (B32)

16

CH-11

Fiber sensors II
Thursday, 14:00 - 15:30, Room 14b ICM

CH-12

Super-resolution imaging
Thursday, 16:00 - 17:30, Room 14b ICM

CH-13

IR & Raman sensing
Friday, 8:30 - 10:00, Room 14b ICM

Imaging through scattering media
Monday, 8:30 - 10:00, Room 14b ICM

New trends in post-compression II
Thursday, 8:30 - 10:00, Room 1 Hall
B1 (B11)

CG – HIGH-FIELD LASER
AND ATTOSECOND SCIENCE
CG-1

Attosecond methods and fundamentals
Thursday, 16:00 - 17:30, Room 6 Hall
B3 (B32)

CH – OPTICAL SENSING
AND MICROSCOPY
CH-1

CF-10
CF-2	Advances in attosecond	technology and high orderharmonic generation II
Monday, 10:30 - 12:00, Room 1 Hall
B1 (B11)

CG-6

CH-14	Photothermal and photoacoustic sensing
Friday, 10:30 - 12:00, Room 14b ICM
CH-15

Bio-sensing
Friday, 14:00 - 15:30, Room 14b ICM

CH-16

Environmental optical sensing
Friday, 16:00 - 17:30, Room 14b ICM

CI – OPTICAL TECHNOLOGIESFOR COMMUNICATIONSAND DATA STORAGE
CI-1

Fibers for telecommunications
Wednesday, 8:30 - 10:00, Room 6 Hall
B3 (B32)

CH Poster session
Wednesday, 13:00 - 14:00, Hall B0

CI-2

CH-7	Instrumentation for opticalsensing and microscopy
Wednesday, 14:00 - 15:30, Room 14b ICM

Frequency combs
Wednesday, 10:30 - 12:00, Room 6 Hall
B3 (B32)

CI-3

CH-8	Methods in optical sensing
and microscopy
Wednesday, 16:00 - 17:30, Room 14b ICM

Ultrafast telecommunications
Wednesday, 14:00 - 15:30, Room 6 Hall
B3 (B32)

CI-4

Fibers for telecommunications and THz
Wednesday, 16:00 - 17:30, Room 6 Hall
B3 (B32)

CH-9

Quantum and single-photon sensing
Thursday, 8:30 - 10:00, Room 14b ICM

CH-10

Fiber sensors I
Thursday, 10:30 - 12:00, Room 14b ICM

CI-5	Quantum and freespace communications
Friday, 8:30 - 10:00, Room 11 ICM

Sessions at a Glance
Modulation and demodulation
Friday, 10:30 - 12:00, Room 11 ICM

CJ-7

Mid-IR fiber sources
Friday, 8:30 - 10:00, Room 2 ICM

CI-P

CI Poster session
Friday, 13:00 - 14:00, Hall B0

CJ-8

Pulsed fiber sources
Friday, 10:30 - 12:00, Room 2 ICM

CI-7

Satellite and radio
Friday, 14:00 - 15:30, Room 11 ICM

CJ-PCJ Poster session
Friday, 13:00 - 14:00, Hall B0

CI-8	Frequency combs and microwave photonics
Friday, 16:00 - 17:30, Room 11 ICM

CJ-9Novel fibers
Friday, 14:00 - 15:30, Room 2 ICM

CJ – FIBRE AND GUIDED WAVELASERS AND AMPLIFIERS

CJ-10

2-micron fiber sources
Friday, 16:00 - 17:30, Room 2 ICM

CJ-1	Transverse mode instability
in fiber lasers and amplifiers
Tuesday, 16:00 - 17:30, Room 7 Hall
A1 (A11)

CK – MICRO- AND NANO-PHOTONICS

CJ-2	Beam combination of fiber
lasers and amplifiers
Wednesday, 8:30 - 10:00, Room 7 Hall
A1 (A11)
CJ-3

Mode-locked fiber lasers
Wednesday, 10:30 - 12:00, Room 7 Hall
A1 (A11)

CJ-4	Specialty fiber characterisation
techniques and components
Wednesday, 14:00 - 15:30, Room 7 Hall
A1 (A11)
CJ-5

CJ-6

Novel fiber lasers
Wednesday, 16:00 - 17:30, Room 7 Hall
A1 (A11)Specialty fiber and devices
Thursday, 8:30 - 10:00, Room 7 Hall
A1 (A11)

CK-1

Lithium niobate and silica systems
Monday, 14:00 - 15:30, Room 4a ICM

CK-2

Plasmonic structuresand components
Tuesday, 8:30 - 10:00, Room 4a ICM

CK-P

CK Poster session
Tuesday, 13:00 - 14:00, Hall B0

CK-3

Resonant structures and cavities
Tuesday, 16:00 - 17:30, Room 4a ICM

CK-4

Active components
Wednesday, 8:30 - 10:00, Room 4a ICM

CK-5

Silicon nitride systems and devices
Wednesday, 10:30 - 12:00, Room 4a ICM

CK-6

Integrated optical devices I
Wednesday, 14:00 - 15:30, Room 4a ICM

CK-7

Integrated optical devices II
Wednesday, 16:00 - 17:30, Room 4a ICM

How to find the room?
A map locating all the rooms can be found in the
inner cover of the advance programme.
Talks and courses: CLEO®/Europe-EQEC
talks and courses take place in the congress centre, so called ICM, on your left when entering themain entrance West of Neue Messe Munich orin the exhibition hall B1 or in the exhibition hall
A1 located on your right. The rooms in the halls
are numbered and named according to famous
physicists. A few talks take place in the Osterseen
room: Follow your way to the ICM and then on
your right take the stairs or the elevator to go to
the second floor and reach this room at the endof the corridor.
To save space in the layout of the parallel sessions,
all locations are abbreviated to the strict minimum such as "Room 1 ICM" instead of "Room1, Ground Floor / First Floor, Congress Centre".
Below you will find the detailed locations of all
CLEO®/Europe-EQEC rooms:
Rooms located in the ICM:
Room 1, Ground Floor / First Floor, Congress Centre
Room 2, Ground Floor, Congress Centre
Room 3, Ground Floor, Congress Centre
Room 4a, Ground Floor, Congress Centre
Room 4b, Ground Floor, Congress Centre
Room 5, Ground Floor, Congress Centre
Room 11, First Floor, Congress Centre
Room 12a, First Floor, Congress Centre
Room 12b, First Floor, Congress Centre
Room 13a, First Floor, Congress Centre

17

Room 13b, First Floor, Congress Centre
Room 14a, First Floor, Congress Centre
Room 14b, First Floor, Congress Centre
Room 14c, First Floor, Congress Centre
Room 21, Second Floor, Congress Centre
Room 22a, Second Floor, Congress Centre
Room 22b, Second Floor, Congress Centre
Room Osterseen, Second Floor, Congress Centre
Foyer balcony, First Floor, Congress Centre (opposite Room 14)
Rooms located at the fairground:
Room 1 "Albert Einstein" B11, First Floor, Exhibition Hall B1
Room 2 "Emmy Noether" B12, First Floor, Exhibition Hall B1
Room 3 "Wilhelm Röntgen" B13, First Floor,
Exhibition Hall B1
Room 4 "Theodore Maiman" B21, First Floor,
Exhibition Hall B2
Room 5 "Thomas Edison" B22, First Floor, Exhibition Hall B2
Room 6 "Emmett Leith" B32, First Floor, Exhibition Hall B3
Room 7 "Charles Townes" A11, First Floor, Exhibition hall A1
Room 8 "Gustav Hertz" A12, First Floor, Exhibition hall A1
Note: Be aware that a few minutes are required
to walk from the ICM to the rooms located in
the exhibition hall A1.
Posters: All poster sessions take place in theHall B0, Ground Floor, Congress Centre.

GENERAL INFORMATION

CI-6

GENERAL INFORMATION

Sessions at a Glance
CK-8

Advanced design methods
Thursday, 8:30 - 10:00, Room 4a ICM

CL-5

Spectroscopy
Friday, 8:30 - 10:00, Room Osterseen ICM

CM-7

CK-9

Micro optical combs
Thursday, 10:30 - 12:00, Room 4a ICM

CL-6

Advanced microscopy I
Friday, 10:30 - 12:00, Room Osterseen ICM

CM-LIM Lightmatter interaction
Wednesday, 10:30 - 12:00, Room
Osterseen ICM

CL-P

CL Poster session
Friday, 13:00 - 14:00, Hall B0

CM-8	Laser-based surfacefunctionalization and sensors
Friday, 8:30 - 10:00, Room 1 ICM

CK-10	Metasurface technologies
and applications
Thursday, 14:00 - 15:30, Room 4a ICM
CK-11P hotonic crystals andperiodic structures
Thursday, 16:00 - 17:30, Room 4a ICM

CL-7

CL-8
CK-12

CK-13

Photonic crystals
Friday, 8:30 - 10:00, Room 4a ICM
Advanced photonic devices
Friday, 10:30 - 12:00, Room 4a ICM

CK-14

Recent advances in laser technology
Friday, 14:00 - 15:30, Room 4a ICM

CK-15

Micro- and nano-optical cavities
Friday, 16:00 - 17:30, Room 4a ICM

CL – PHOTONIC APPLICATIONSIN BIOLOGY AND MEDICINE
CL-1

CL-2

CL-3

Brain imaging
Monday, 14:00 - 15:30, Room 2 Hall B1 (B12)
Flow cytometry and ultrasoundThursday, 10:30 - 12:00, Room Osterseen ICM
Lightmatter interaction
Thursday, 14:00 - 15:30, Room Osterseen ICM

CL-4	Photonic technology forbiomedical applications
Thursday, 16:00 - 17:30, Room Osterseen ICM

Advanced microscopy II
Friday, 14:00 - 15:30, Room Osterseen ICM

CM-9	Laser-induced periodic
surface structures
Friday, 10:30 - 12:00, Room 1 ICM

Novel laser sources
Friday, 16:00 - 17:30, Room Osterseen ICM

CM – MATERIALS PROCESSINGWITH LASERS
CM-1

Laser additive manufacturing I
Monday, 8:30 - 10:00, Room 1 ICM

CM-2

Laser semiconductor processing
Monday, 10:30 - 12:00, Room 1 ICM

CM-P

CM Poster session
Monday, 13:00 - 14:00, Hall B0

Laser written waveguides and gratings
Wednesday, 8:30 - 10:00, Room 1 ICM

EA-6Quantum optics in imaging
Friday, 8:30 - 10:00, Room 3 ICM

EA-7

Atomic systems
Friday, 10:30 - 12:00, Room 3 ICM

EA-8

Nonclassical states of light
Friday, 14:00 - 15:30, Room 3 ICM

EA-9

Optomechanical systems
Friday, 16:00 - 17:30, Room 3 ICM

Dynamics of laser-induced processes
Friday, 14:00 - 15:30, Room 1 ICM

EB – QUANTUM INFORMATION,
COMMUNICATION, AND SENSING

CM-11

Laser additive manufacturing II
Friday, 16:00 - 17:30, Room 1 ICM

EB-1	Optomechanical and otherquantum oscillators
Monday, 8:30 - 10:00, Room 8 Hall A1 (A12)

EQEC 2023 SESSIONS

EB-2

Quantum interferometry
Monday, 10:30 - 12:00, Room 8 Hall A1 (A12)EB-3

Quantum optics I
Monday, 14:00 - 15:30, Room 8 Hall A1 (A12)

Fundamental quantum optics
Tuesday, 8:30 - 10:00, Room 7 Hall A1 (A11)

EB-4

Quantum computation I
Tuesday, 8:30 - 10:00, Room 8 Hall A1 (A12)

Nonlinear quantum optics
Thursday, 8:30 - 10:00, Room 1 ICM

EB-5Quantum key distribution
Tuesday, 16:00 - 17:30, Room 8 Hall A1 (A12)

Photonic quantum technology
Thursday, 10:30 - 12:00, Room 1 ICM

EB-6

Integrated quantum optics
Wednesday, 8:30 - 10:00, Room 8 Hall
A1 (A12)

EB-7

Quantum sensing
Wednesday, 10:30 - 12:00, Room 8 Hall
A1 (A12)

EA-1

EA-2

CM-4	Temporal and spatial beam shaping
for laser processing II
Tuesday, 8:30 - 10:00, Room 1 ICM

EA-3

CM-5

Modelling of laser-induced processes
Tuesday, 14:00 - 15:30, Room 13a ICM

EA-P

EA Poster session
Thursday, 13:00 - 14:00, Hall B0

CM-6

Laser volume processing
Tuesday, 16:00 - 17:30, Room 1 ICM

EA-4Quantum light sources I
Thursday, 14:00 - 15:30, Room 1 ICM

18Quantum light sources II
Thursday, 16:00 - 17:30, Room 1 ICM

CM-10

EA – QUANTUM OPTICS ANDULTRACOLD QUANTUM MATTER

CM-3	Temporal and spatial beam
shaping for laser processing I
Monday, 14:00 - 15:30, Room 1 ICM

EA-5

Sessions at a Glance
Quantum imaging
Wednesday, 14:00 - 15:30, Room 8 Hall
A1 (A12)EB-9

Quantum communication
Wednesday, 16:00 - 17:30, Room 8 Hall
A1 (A12)

EB-10

EB-11

ED – PRECISION METROLOGYAND FREQUENCY COMBS

EE-3	Ultrafast XUV and soft X-ray spectroscopy
Friday, 10:30 - 12:00, Room 14c ICM

ED-1	Precision spectroscopy for
fundamental science
Monday, 8:30 - 10:00, Room 6 Hall
B3 (B32)

EE-4

Quantum memories
Thursday, 8:30 - 10:00, Room 8 Hall
A1 (A12)

ED-2

Single photon sources and detectors
Thursday, 10:30 - 12:00, Room 8 Hall
A1 (A12)

ED-P

ED-3
EB-P

EB Poster session
Thursday, 13:00 - 14:00, Hall B0

EB-12

Quantum optics IIThursday, 14:00 - 15:30, Room 8 Hall A1 (A12)

EB-13

Quantum simulation and computation
Thursday, 16:00 - 17:30, Room 8 Hall
A1 (A12)EC – TOPOLOGICAL STATES OF LIGHT
EC-1	Non-linear and non-hermitian
topological photonics
Friday, 8:30 - 10:00, Room 22a ICM
EC-2

EC-P

Photonic band topology
Friday, 10:30 - 12:00, Room 22a ICM
EC Poster session
Friday, 13:00 - 14:00, Hall B0

EC-3	Emerging trends and singular
photonic topology
Friday, 14:00 - 15:30, Room 22a ICM

EE-5

Direct comb spectroscopy
Monday, 10:30 - 12:00, Room 6 Hall
B3 (B32)

Ultrafast manipulation and control
Friday, 16:00 - 17:30, Room 14c ICM

EF – NONLINEAR PHENOMENA,SOLITONS AND SELF-ORGANIZATIONED Poster session
Monday, 13:00 - 14:00, Hall B0

EF-1

Frequency references and transfer
Monday, 14:00 - 15:30, Room 6 Hall B3 (B32)

ED-4	Cavity-enhanced
precision spectroscopy
Tuesday, 8:30 - 10:00, Room 2 Hall
B1 (B12)ED-5

Ultrafast nonlinear optics in gases
Friday, 14:00 - 15:30, Room 14c ICM

Precision metrology
Friday, 8:30 - 10:00, Room 12b ICM

EF-P

EF Poster session
Wednesday, 13:00 - 14:00, Hall B0

EF-2

Kerr solitons and frequency combs I
Wednesday, 16:00 - 17:30, Room Osterseen ICM

EF-3

Kerr solitons and frequency combs II
Thursday, 8:30 - 10:00, Room 14a ICM

EF-5

EG – LIGHT-MATTER INTERACTIONSAT THE NANOSCALE
EG-1

Nanoantennas 		and nanoconfinement
Monday, 8:30 - 10:00, Room 4b ICM

EG-2

Metasurfaces
Monday, 10:30 - 12:00, Room 4b ICM

Complex fiber dynamics I
Wednesday, 14:00 - 15:30, Room Osterseen ICM

EF-4	Spatiotemporal effects in optical systems
Thursday, 10:30 - 12:00, Room 14a ICM

ED-6	Frequency combs: Sources
and characterization
Friday, 10:30 - 12:00, Room 12b ICM

EF-10	Extreme events andforecasting techniques
Friday, 16:00 - 17:15, Room 14a ICM

Dissipative solitons and mode-locking I
Thursday, 14:00 - 15:30, Room 14a ICM

EG-3	Optoelectronics and 		light-electron interactions
Monday, 14:00 - 15:30, Room 4b ICM
EG-4	Ultrastrong light matter interactions
and nonlinear optics
Tuesday, 8:30 - 10:00, Room 4b ICM
EG-P

EG Poster session
Tuesday, 13:00 - 14:00, Hall B0

EG-5

Single emitters
Tuesday, 16:00 - 17:30, Room 4b ICM

EG-6	Nanomanipulation, 		
nano-organization and correlation
Wednesday, 8:30 - 10:00, Room 4b ICM

EF-6

Dissipative solitons and mode-locking II
Thursday, 16:00 - 17:30, Room 14a ICM

Ultrafast spectroscopy of solids
Wednesday, 8:30 - 10:00, Room Osterseen ICM

EF-7

Complex fiber dynamics II
Friday, 8:30 - 10:00, Room 14a ICM

EE-P

EE Poster session
Wednesday, 13:00 - 14:00, Hall B0

EF-8	Symmetry breaking in coupled resonators
Friday, 10:30 - 12:00, Room 14a ICM

EH-1	Temporal andtopological metamaterials
Wednesday, 16:00 - 17:30, Room 4b ICM

EE-2

Ultrafast processes in ionised media
Friday, 8:30 - 10:00, Room 14c ICM

EF-9

EH-2

EE – ULTRAFAST OPTICAL SCIENCE
EE-1

19

Topological and nonlinear effects
Friday, 14:00 - 15:30, Room 14a ICM

EH – PLASMONICS
AND METAMATERIALS

Quantum plasmonics
Thursday, 8:30 - 10:00, Room 4b ICM

GENERAL INFORMATION

EB-8

GENERAL INFORMATION

Sessions at a Glance
EH-3

Nonlinear and active metastructures
Thursday, 10:30 - 12:00, Room 4b ICM

EH-P

EH Poster session
Thursday, 13:00 - 14:00, Hall B0

EH-4

Tunable and holographic metasurfaces
Thursday, 14:00 - 15:30, Room 4b ICM

EH-5	Concepts and applications inplasmonics and metastructures
Thursday, 16:00 - 17:30, Room 4b ICM

EJ-2	Computational photonics
at the light-matter interface
Monday, 10:30 - 12:00, Room 4a ICM
EJ-P

JSII – INFRARED INTEGRATED
PHOTONICS FORASTRONOMICAL APPLICATIONSEJ Poster session
Monday, 13:00 - 14:00, Hall B0

JSII-1

EJ-3	Nonlinear optics modeling& artificial intelligence
Friday, 8:30 - 10:00, Room 21 ICM
EJ-4

JSII-2	Manipulating astronomicalsignals with photonics
and future challenges I
Monday, 10:30 - 12:00, 			
Room Osterseen ICM

Tailored light and optical design
Friday, 10:30 - 12:00, Room 21 ICM

EI – TWO-DIMENSIONALAND NOVEL MATERIALSJSII-P

EI-1	2D van der Waals materials:
fundamentals and applications
Friday, 8:30 - 10:00, Room 4b ICM

CLEO®/EUROPE-EQEC 2023
JOINT SYMPOSIA SESSIONS

JSI-1

EI-P

JSI-2

EI poster session
Friday, 13:00 - 14:00, Hall B0

EI-3	Novel low-dimensional andfunctional materials
Friday, 14:00 - 16:30, Room 4b ICM
EI-4

Ultrafast dynamics in layered materials
Friday, 16:00 - 17:30, Room 4b ICM

JSI-P

Nonlinear X-ray wave-mixing
Wednesday, 8:30 - 10:00, Room 13b ICM

JSIII – PHOTONICS FORARTIFICIAL INTELLIGENCE

X-ray source developments
Wednesday, 10:30 - 12:00, Room 13b ICM

JSIII-1	Photonic reservoir computing,extreme learning andising machines I
Thursday, 14:00 - 15:30, Room 13a ICM

JSI Poster session
Wednesday, 13:00 - 14:00, Hall B0

JSI-3	Imaging geometric andelectronic structures
Wednesday, 14:00 - 15:30, Room 1 ICM

EJ – THEORETICAL
AND COMPUTATIONAL
PHOTONICS MODELLING

JSI-4	Nonlinear and ultrafast
X-ray spectroscopy
Wednesday, 16:00 - 17:30, Room 1 ICM

EJ-1	Simulating multi-mode andnon-hermitian systems
Monday, 8:30 - 10:00, Room 4a ICM

JSI-5

JSII Poster session
Monday, 13:00 - 14:00, Hall B0

JSII-3	Manipulating astronomicalsignals with photonics
and future challenges II
Monday, 14:00 - 15:30, 			
Room Osterseen ICM

JSI – FREE ELECTRON LASERS

EI-2	Nonlinear and quantum optics withvan der Waals layered materials
Friday, 10:30 - 12:00, Room 4b ICM

The photonic yield in astronomy
Monday, 8:30 - 10:00, 		Room Osterseen ICM

JSIII-2 	Photonic reservoir computing,extreme learning andising machines II
Thursday, 16:00 - 17:30, Room 13a ICM
JSIII-3 Photonic accelerators I
Friday, 8:30 - 10:00, Room 13a ICM

Ultrafast molecular dynamics
Thursday, 8:30 - 10:00, 		Room Osterseen ICM

JSIII-4 Photonic accelerators II
Friday, 10:30 - 12:00, Room 13a ICM

20

JSIII-P JSIII Poster session
Friday, 13:00 - 14:00, Hall B0
JSIII-5		Brain-inspired photonic
devices and computing I
Friday, 14:00 - 15:30, Room 13a ICM
JSIII-6		Brain-inspired photonic
devices and computing II
Friday, 16:00 - 17:30, Room 13a ICM

JSIV – PHOTONICS
FOR SUSTAINABILITY
JSIV-1	Photo(electro)chemistry
and desalination
Wednesday, 10:30 - 12:00, 		Room 4b ICM
JSIV-P JSIV Poster session
Wednesday, 13:00 - 14:00, Hall B0
JSIV-2 Thermal radiation and photovoltaics
Wednesday, 14:00 - 15:30, Room 4b ICM

JSV – DIVERSITY IN PHOTONICS
See SPECIAL EVENTSNANOPHOXONICS AND
NANOSCALE HEAT TRANSFER
JSVI-1	NanophoXonics, optomechanicalsystems and thermal transport
Tuesday, 8:30 - 10:00, 		Room Osterseen ICM
JSVI-2	Radiative heat transfer, thermoelectrics& thermochromics, SPP
Tuesday, 16:00 - 17:30, 		Room Osterseen ICM

CLEO®/Europe 2023 Topics
CA – Solid-state Lasers
Advances in solid-state lasers: novel solid-state lasers and amplifiers; high-power and high-energy
lasers; power-scalable laser architectures; lasers
for large-scale facilities; solid-state micro-chiplasers; crystalline waveguide lasers; short-wavelength lasers; up-conversion lasers; mid-infraredlasers; wavelength tuning techniques and tunable
lasers; intracavity wavelength conversion; laser
resonator design; techniques for thermal management and beam quality control; novel pumpsources and pumping configurations; ns-pulse
generation; amplitude and frequency stability;
advanced laser crystals and ceramics, and glasses;
spectroscopic characterization of solid-state gain
media; laser characterization and modelling.
CHAIR: Pavel Loiko, CIMAP, Université de Caen,
Normandie, Caen, France

CB – Semiconductor Lasers
New technology, devices and applications; UV
lasers, visible lasers, near-infrared lasers; mid
to far-infrared semiconductor lasers including
W-lasers, quantum cascade and inter-subband
lasers; quantum well, wire, dot and dash lasers;
high power and high brightness lasers; vertical(extended) cavity surface emitting lasers; optically-pumped semiconductor lasers; photonic crystal semiconductor lasers, micro-cavity
lasers, nanolasers, plasmonic lasers, polariton
lasers; semiconductor ring lasers; short-pulse
generation, mode locking; semiconductor optical amplifiers; new semiconductor laser materials, silicon-based lasers, novel characterization
techniques; functional applications, including but
not limited to: switching, clock recovery, signal
processing; semiconductor lasers in integrated
photonic circuits; laser dynamics, synchronization, chaos.

CHAIR: Mikhail Belkin, Walter Schottky
Institute, Munich, Germany

CHAIR: Mikko J Huttunen, Tampere Universityof Technology, Tampere, Finland

CC – Terahertz Sources and Applications
Sources for generating terahertz (far-infrared)
radiation in the range from 200 GHz to 100 THz,based on various physical principles including
ultrafast time-domain systems, direct generation
using terahertz lasers, and sources based on nonlinear optical mixing and laser-created plasmas;
applications using terahertz radiation for spectroscopy, nonlinear THz phenomena, sensing,and imaging; advances in terahertz communications; new terahertz measurement techniques
and instrumentation, including advances in terahertz imaging, detector technologies, near-fieldmicroscopy, terahertz devices and environmental monitoring.

CE – Optical Materials, Fabrication
and Characterisation
Fabrication of optical materials; new crystalline
and glass laser materials in bulk, fiber and waveguide geometry; micro- and nano-fabricationand -engineering techniques; heterogeneous integration techniques; optical characterisation oflaser and nonlinear materials, micro-structured
fibre and photonic crystal waveguides, micro- andnano-crystalline materials, single defect centres,
quantum wells, quantum wires and quantum
dots, nano-tubes and nano-needles, innovative
organic materials.
CHAIR: Stavros Pissadakis, Instituteof Electronic Structure and Laser (IESL),
Heraklion, Greece

CHAIR: Juliette Mangeney, École Normale
Supérieure, Laboratoire Pierre Aigrain,
Paris, France

CF – Ultrafast Optical Technologies
Femtosecond and picosecond pulse generation from solid state, fiber and waveguidesources; mode-locked lasers; few-cycle optical pulses; pulse compression, carrier-envelope
phase stabilization and pulse characterization;light waveform synthesis metrology; ultrashort-pulse semiconductor lasers and devices;
ultrafast parametric amplifiers and parametricchirped pulse amplifiers; ultrashort-pulse midIR generation; supercontinuum generation;
dispersion management; ultrafast electro-optics; pulse-shaping; carrier-envelope effects;
ultrafast characterization methods and measurement techniques, ultrafast optoelectronicsystems and devices; applications of ultrafast
technology, technological aspects of ultrafast
spectroscopy; ultrafast microscopic techniques;
electro-optic sampling.

CD – Applications of Nonlinear Optics
Novel applications of nonlinear optical phenomena and new devices; nonlinear frequency
conversion for the UV, visible and IR; telecommunications applications and all-optical switching;all-optical delay lines and slow light; optical parametric devices such as optical parametric amplifiers and oscillators; nonlinear optics in waveguides
and fibres, including photonic crystal structuresand microstructured optical fibres; quasi-phasematched materials and devices; novel nonlinear
materials; metamaterials and nanostructures;
stimulated scattering processes and devices; applications of optical solitons and photorefractives;electro-optic and Kerr devices in crystals andsemiconductors; Raman based devices including
amplifiers and lasers; nonlinear probing of surfaces; multi-photon imaging and coherent Raman
microscopy; quantum oriented applications.

CHAIR: Caterina Vozzi, Politecnico di Milano,
Milano, Italy21

CG – High-Field Laser and Attosecond Science
Strong-field and attosecond phenomena; attosecond pulse generation; strong-field ionization andionization dynamics; novel technologies for highfield physics and attosecond science; probing of
ultrafast dynamics with intense free-electron
laser pulses; control of high-field and attosecond phenomena; laser-driven rescattering andrecollision phenomena; high-harmonic generation; time-resolved XUV/soft x-ray spectroscopy,
interferometry and microscopy; attosecond andfemtosecond diffraction imaging with electronsor photons; molecular dynamics driven by strong
fields or probed by high-field/attosecond methods; attosecond or strong-field driven electron
dynamics in the condensed phase, bulk media,
nanostructures, quantum-confined structures orat surfaces/interfaces; ultra-high-intensity laser
physics and technology; laser-plasma interaction
and particle acceleration; relativistic nonlinear
optical phenomena.
CHAIR: Adrian Pfeiffer, Friedrich-SchillerUniversität Jena, Jena, Germany

CH – Optical Sensing and Microscopy
Inspection of a wide range of objects, from themacroscopic to the nanometric scale; recent
progress in all aspects of optical sensing andmetrology, particularly in new photonic sensor
technologies and applications; plasmonic sensors;
metamaterial sensors; biosensors; terahertz sensors; new trends in optical remote sensing; fibre
sensors using conventional and photonic crystal
fibres; active multispectral and hyperspectral imaging; sensor multiplexing; novel spectroscopic
techniques, nanospectroscopy; applications andsystems; novel measurement methods and devices based on interferometry; holography; diffractometry or scatterometry; critical dimension
metrology; multiscale surface metrology; UV
and DUV microscopy; resolution enhancement

GENERAL INFORMATION

TopicsTopics
techniques in microscopy; superresolution microscopy inverse problems; active optics; adaptive
optics; phase retrieval.

fibre and waveguide laser devices; novel waveguide and fibre sources, and beam delivery fibre
for industrial applications; nanomaterials andtheir applications in fibre and guided wave lasers.

reversal; optics in biological media: scattering;coherence; polarization; symmetry and invariance. Advanced light sources and geometries for
microscopy, phototherapy, surgery, biomedicine.

CHAIR: Jayanta Kumar Sahu, University ofSouthampton, Southampton, United Kingdom

CHAIR: Kenneth K. Y. Wong, The University ofHong Kong, Hong Kong, China

CI – Optical Technologies for Communications
and Data Storage
Fibre devices including nonlinear fibre, propagation and polarisation effects, fibre gratings.
Semiconductor devices for generation, processing and detection of optical signals. Digital signal
processing, forward error correction, nonlinear
Fourier transform. Submarine, core and metropolitan transport networks, communication andaccess networks, datacentre networks. Multi-core,multi-mode fibre for transmission, optical amplification and functions; multi-band optical amplification and transmission. Optical sub-systems
including clock recovery, packet/burst switching,advanced modulation formats, radio-over-fibre
and microwave photonic technologies, opticalregeneration and buffering; holographic and3D optical data storage, near-field recording
and super-resolution.

CK – Micro- and Nano-Photonics
Nanostructured materials and fabrication techniques for photonic applications; novel phenomena occurring when light is created, transported
and detected in environments where either dimensionality or size are reduced and, in particular, when light-matter interaction occurs inregions smaller than or similar to the wavelengthof light (nanophotonics). Periodic or quasi-periodic nanostructures (photonic crystals); issues
related to order/disorder in nanostructured materials; photonic integrated circuits and applications
advancing the integration of photonic devices forbiology, lighting, communication, sensing andenergy efficiency; optical MEMS; WGM opticalresonators; hybrid and 2D nanomaterials including in-/organic nano-layers/wires, nanocrystals
and single molecules.

CM – Materials Processing with Lasers
Fundamentals of laser-materials interactions:
phase transformation, chemical reactions,diffusion processes, ablation; high-power laser-materials processing: welding, cutting, surface treatment; thin-film growth: PLD, LCVD,
MAPLE; direct write techniques:, 2D and 3D
micro/nano structuring, LIFT, near-field techniques; plasma related processes; laser assisted
nanosynthesis; femtosecond micromachining;ultrafast laser processing: volume modification,index engineering; laser-assisted manufacturing;
additive manufacturing: two-photon polymerization and 3D laser printing.

CHAIR: Alessandro Tonello, Université deLimoges, Limoges, France

CHAIR: Stefano Pelli, CNR-IFAC, Sesto Fiorentino(FI), Italy

CJ – Fibre and Guided Wave Lasers
and Amplifiers
Waveguide and fibre laser oscillators and amplifiers including novel waveguide and fibre geometries; power and energy scaling of waveguideand fibre lasers – including beam combination
techniques (for both pump and signal beams) andnew waveguide coupling approaches; up-conversion lasers; nonlinear frequency conversion andpulse generation and compression; spatio-temporal pulse evolution; advances in fibre waveguidematerials; fabrication techniques for doped waveguide and fibre devices; active microstructured

CL – Photonic Applications in Biology
and Medicine
Emerging concepts in biophotonics: single
particle/molecule detection and tracking; spatio-temporal manipulation of light fields forbiomedicine; enhanced linear and nonlinear excitation and detection; micro-fluidics, optofluidics and micro-optics; new optical probes for local
measurements including organic and inorganic
nanoparticles, electric fields and temperature
measurements; New routes and modalities for optical detection in biophotonics: spectroscopy; holography, adaptive optics, phase conjugation time

GENERAL INFORMATIONCHAIR: Cristian Focsa, University of Lille,
Lille, France

CHAIR: Jan Siegel, Instituto de Optica – Consejo
Superior de Investigaciones Científicas (CSIC),
Madrid, Spain

EQEC 2023 Topics
EA – Quantum Optics and Quantum Matter
Quantum light sources and applications; nonlocality and quantum interference; squeezing andentanglement; quantum correlations, coherence,and measurement; quantum fluid of light; multimode and mesoscopic quantum optics; single
photon emission and absorption; quantum optics
in cavities; slow light and quantum memories;
quantum imaging and quantum lithography;
quantum coherent effects in biology; Developments in few- and many-body phenomena withultracold quantum gases of atoms and molecules; quantum simulation; superfluidity and22

thermodynamics in Bose and Fermi systems;
dipolar physics with atoms and molecules; Efimov physics; atom interferometry; hybrid systems such as cold and trapped ion/atom setups,
optomechanical devices.
CHAIR: Sebastian Blatt, MPQ,
Garching, Germany

EB – Quantum Information, Communication,and Sensing
Quantum computers and quantum communication systems; quantum algorithms and communication protocols, quantum simulations, quantum
key distribution, quantum logic gates, entanglement distribution and distillation, interfaces
between static and flying qubits, quantum memories; integrated quantum devices, quantum nano-mechanics, ion-trap arrays, superconducting
structures, quantum dots, cavity QED systems.
CHAIR: Marco Genovese, INRIM, Turin, Italy

EC – Topological States of Light
Advances in topological photonic lattices, topological edge states, topological pumps, synthetic
dimensions, Dirac and Weyl points, topological lasers, topology and disorder, topology in
non-Hermitian systems, probes of topologicalinvariants, topological aspects of photonic quasicrystals, nonlinear topological effects, Floquet-topological photonics, spin-orbit couplingin photonic materials, non-reciprocity.
CHAIR: Stefan Rotter, Vienna University ofTechnology, Austria

ED – Precision Metrology and
Frequency Combs
Precision interferometry and spectroscopy including frequency combs; quantum metrology;
ultimate limitations of measurement precision
as imposed by the nature of quanta; tests offundamental symmetries; definition of basic

units; measurement of fundamental constants;
applications in different spectral ranges, including mid-infrared.
CHAIR: Marco Marangoni, Politecnico di Milano
and Institute of Photonics and Nanotechnology,
Milano, Italy

EE – Ultrafast Optical Science
Fundamental aspects of ultrafast science in all
spectral regimes; propagation and instabilities ofultrashort pulses in linear and nonlinear media,
supercontinuum generation, ultrafast filamentation and applications, extreme events, rogue
waves and turbulence dynamics; ultrafast spectroscopy of molecules, solids and low dimensional structures; ultrafast phenomena in physics,
chemistry and biology; propagation media: gas,liquid, and solid materials; free-space and waveguided geometries; coherent control using femtosecond pulses.
CHAIR: Jens Biegert, ICFO - The Institute of
Photonic Sciences, Castelldefels, Spain

EF – Nonlinear Phenomena, Solitonsand Self-organization
Nonlinear optical phenomena including dynamics and self-organization; frequency conversion,
wave mixing, parametric processes, conservativeand dissipative solitons, pattern formation, interaction between disorder and nonlinearities,
complex behaviours and statistically heavy-tailed
phenomena. Applications of nonlinear phenomena; nonlinear imaging and manipulation, novel
optical materials, devices and systems. Fundamental aspects of nonlinear dynamics in single orcoupled photonic devices, polariton condensates,
micro and nano lasers, photonic crystals, optomechanical systems.
CO-CHAIRS:
Alessia Pasquazi, Loughborough University,
Loughborough, United Kingdom

waveguides; multi-layered 2D heterostructures;perovskites and perovskite optoelectronics; NV
centres; phase change materials.

Svetlana Gurevich, University of Münster,
Münster, Germany

EG – Light-matter Interactions 		
at the Nanoscale
Fundamental aspects of light-matter interactions
at the nanoscale: nanoantennas and nanophotonic architectures, classical and quantum models,detection, emission and manipulation of lightand/or matter; quantum nano-optics: coherent,
quantum and nonlinear optical effects; ultrafast
and strong-field phenomena at the nanoscale:interactions with electrons/plasma and their applications, ultrafast dynamics; optical imaging
and spectroscopy: nanoscopy, nano-optical forces and tweezers; nano-energy: radiative transfer,
photovoltaics and catalysis.

CHAIR: Nicolo Maccaferri, Umeå University,Umeå, Sweden

EJ – Theoretical and Computational
Photonics Modelling
Predictive theoretical and computational approaches for all fields of optics and photonics:
full and semi-analytical treatments; applied mathematics and numerical analysis of partial differential equations; high-performance computing,massively parallel codes, including utilizationof hardware accelerators. Modelling of singularnonlinear processes, shocks, wave collapse, material processing; first principle calculations of
optical properties in dielectrics, plasmas, semiconductors and plasmonic structures; modellingof artificial optical materials.

CHAIR: Mathieu Mivelle, Sorbonne University,
Paris, France

EH – Plasmonics and Metamaterials
Metal nanophotonics from fundamentals towards
applications and including all spectral regimes:
plasmonic nanostructures, antennas, cavities andwaveguides; metamaterials; hybrid materials;
nonlinear structures and effects; active systems,
systems with gain.

CHAIR: Fabian Maucher, University of Balearic
Islands, Palma de Mallorca, Spain

CLEO®/Europe-EQEC 2023
Joint Symposia Topics
JSI - Free Electron Lasers
Free-electron lasers (FEL) offer unique opportunity for the investigation of light-matter interaction in the extreme ultraviolet and X-ray
spectral ranges. The symposium aims at bringing together the expertise of FEL developers
and the community of users and potential users
interested in taking advantage for their researchof the unprecedented combination of extreme
time resolution (down to the attosecond domain),photon flux and high peak intensities available at
FELs. The presentations will focus on the latest
developments achieved in the operation of FELs
and in selected highlights of user experiments.

CHAIR: Paloma Huidobro, University of Lisbon,
Lisbon, Portugal

EI – Two-dimensional and Novel Materials
Fundamental aspects and applications ofgraphene and other two-dimensional materials
in optics and optoelectronics; light-matter interactions in 2D materials; ultrafast dynamics andnonlinear phenomena in 2D and novel materials,
and mode-locked lasers; light sources, modulators, detectors, and other optoelectronic devices; photovoltaics; smart windows and flexible
displays; terahertz devices; tunable plasmonics
and metamaterials; integration with cavities and23

Topics:Novel seeding concepts; Polarization control of
XUV and X-ray pulses; Multi-color and multi-harmonic operation; Light-matter interaction
under extreme conditions; Pulse characterization; Time-resolved coherent diffractive imaging; Target development for coherent imaging;
High-repetition rate XUV and X-ray sources;
Novel schemes for attosecond pulse generation;
Crystallography; Biological imaging; FEL optimization based on machine learning approaches;
Theoretical modelling of laser-matter interaction;
Multiphoton processes in the XUV and X-ray
range; Imaging of ultrafast electronic and nuclear dynamics.
CO-CHAIRS:
Christoph Bostedt, Paul Scherrer Institute,Villigen PSI, Switzerland
Giuseppe Sansone, University of Freiburg,
Freiburg, Germany

JSII - Infrared Integrated Photonics for
Astronomical Applications
Major discoveries in astrophysics are enabled by
new technologies that respond to the increasing
demand for higher spectral, angular and temporal resolution across a broad wavelength range,
pushing the limits of the existing infrastructures.
In this regard photonics is playing a growing role.
Over the last decades strong ties have been built
up between the astronomical instrumentationand photonics communities, which has resulted in unique synergies for astrophysics in the
1-10μm infrared wavelength range. The strengthof photonics is in the small-size integration of sophisticated optical functions, which once applied
to the field of astronomy contributes to reduce thesize and complexity of deployable instruments,
as well as to increase their functional stability.
Furthermore, while ground-based instruments
have already directly benefitted from the power

GENERAL INFORMATION

Topics

GENERAL INFORMATION

Topicsof astrophotonics, space applications might be
the next frontier. The proposed symposium aims
at inspiring additional technology exchanges between the fields of astronomy and photonics bysharing new innovative results and ideas that willraise the state of the art of astrophotonics. The following areas will be broadly covered, with a focus
on design, manufacturing and performance, as
well as on the benefit of miniaturization in viewof future integration in a ground- or space-based
scientific instrument.
Topics:Active/Passive Integrated Optics for beam combination and phase control; Integrated photonic
spectrographs: FTS and direct detection units;
New photonic functionalities for high-contrast
science in astronomy; Frequency conversion ofphotonic correlation of signals; New micro-structured optical fibers for astronomy; Bridging the
gap between THz and mid-IR technologies; Advances in ultrafast laser writing for astronomy;
Space qualification of photonic devices; Advancesin the lithographic platforms; Photonic calibration sources (e.g., frequency combs, fiber etalons…); Platforms and technologies for spectral
coverage extended in the UV/VIS/MIR; Wavefront control and photonics – Integrating thedetection stage.
CO-CHAIRS:
Lucas Labadie, I-Physics Institute University of
Cologne, Germany
Robert R. Thomson, Institute of Photonics
and Quantum Sciences, Heriot Watt University,
United Kingdom

JSIII - Photonics for Artificial Intelligence
Nowadays, there are clear global challenges associated to the vast amounts of energy we consume in processing Big Data using Artificial
Intelligence (AI) that are putting our industries

and societies at risk. AI operate at high-power
penalty since they rely on intensive data-driven deep learning neural networks running inconventional computers. There is a demand
for new computing paradigms able to run AIs
at extremely low energy per bit budgets. Neuromorphic systems, that can mimic the way thebrain process information, are among the mostpromising technologies. Photonics enables thedesign of energy-efficient computing approaches such as neuromorphic photonic computing,allowing massively distributed power-efficientarchitectures for parallel processing and enabling
new AI applications as required for the Industrial
5.0 Intelligent era revolution. This symposium
covers the status, prospects, and challenges oflight-based computing for AI taking advantageof new materials, devices, architectures, software,algorithms and simulation tools.

from more traditional photovoltaics, to emerging
devices for the water-energy Nexus. This focused
symposium aims at offering a shared platform fordiscussing photonic innovations for such broad
technological applications, fostering interactions
and ideas exchange.
Topics:Photovoltaics/Luminescent solar concentrators;
Photo (electro) chemistry/plasmonic (thermos)
chemistry; Thermal management; Emerging
Technologies for the Water/Energy Nexus (Solar
desalination, Water purification, Hydrovoltaic
Devices); Sustainable photonics materials.
CO-CHAIRS:
Esther Alarcon Llado, AMOLF Amsterdam,
The Netherlands
Giulia Tagliabue, Ecole PolytechniqueFédérale de Lausanne, Joint Center for Artificial
Photosynthesis, Lausanne, Switzerland

Topics:Device, circuit; architecture design; analysis andoptimization for neuromorphic photonic computing systems; Emerging materials for devices ofneuromorphic photonic computing importance;
Hardware photonic accelerators for machine/
deep learning; Photonic reservoir computing;
Novel neuromorphic photonic computing systems; On-chip learning and inference, learningalgorithms and optimizations; Complexity andscalability of neuromorphic photonic computing; Emerging technologies for brain-inspired
nanophotonic computing and communication.

JSV - Diversity in Photonics
Several events managed by CLEO®/Europe-EQEC
or other collocated conferences will take place.
See “Special events” in this programme or the
separate leaflet detailing the programme.
JSVI - Nanophoxonics and Nanoscale
Heat Transfer
The purpose of the “NanoPhoxonics and Nanoscale Heat Transfer” Symposium is to discuss thestate of the art in the Nanoscale Heat Transfer
and management, as well as the recent advancesin the study of self-heating via electron-phonon
interaction, of thermal polaritonics/plasmon andphonon-polariton heat transfer in nano devices,of new nanophoxonic devices with innovative
optical and acoustical properties, and of nearfield radiation, allowing to exchange relevant
information, to promote collaboration among

CO-CHAIRS:
Antonio Hurtado, University of Strathclyde,
Glasgow,United Kingdom
Bruno Romeira, INL Institute, Braga, Portugal

JSIV - Photonics for Sustainability
Photonics plays a critical role in a growing number of sustainable energy technologies, ranging

24

scientists and to provide the scientific basis tothe newcomers.
The symposium will bring together scientists,
technology developers and young researchers
who are interested in the theoretical tools andin the development and investigation of a large
variety of new materials and applications. Participants are encouraged to present their own resultsin the field.
Topics:Extreme-near-field heat transport; Heattransport in 2D materials and metamaterials; Thermal Polaritonics/Plasmon and Phonon-Polariton Heat Transfer; Surface Wave
Thermal Transport, Heat Guiding and Tunneling; Heat transport in molecular junctions;
Micro/Nanoscale Energy Devices and Systems(including bolometers, calorimeters, energy
components); Nanoscale/microscale thermal
metrology; Near-field radiative heat transfer;
Nonequilibrium effects, thermodynamics anddevices; Quantum effects in heat transport andquantum thermodynamics; Thermal interface
resistance. Thermal rectification; Thermoelectricity and thermophotovoltaics; Ultrafast heattransfer; PhoXonic (i.e., Photonic & Phononic)
Crystal Design and Fabrication. Acoustic Metamaterial Design and Fabrication. Applicationsof Phononic Crystals and Acoustic Metamaterials; Temporally modulated Phononic Crystals and Acoustic Metamaterials; Topological
Acoustics and Phononics; Nonlinear Phononic
Crystals and Acoustic Metamaterials. Optomechanics and Phonon Coupling.
CO-CHAIRS:
Roberto Li Voti, Sapienza Università diRoma, Italy
Sebastian Volz, Laboratory for Integrated MicroMechatronic Systems LIMMS/CNRS-IIS(UMI2820)
University of Tokyo, Japan

Committees

Steering Committee

PROGRAMME COMMITTEESDavid Sampson, University of Surrey, Guilford,
United Kingdom
Peter M Smowton, Cardiff University, Cardiff,
United Kingdom

CA - SOLID-STATE LASERS
CHAIR: Pavel Loiko, CIMAP, Université de Caen
Normandie, Caen, France
Weidong Chen, Fujian Institute of Researchon the Structure of Matter, Chinese Academy of
Sciences, Fuzhou, China
Christelle Kieleck, Fraunhofer Institute of
Optronics, System Technologies and Image
Exploitation IOSB, Karlsruhe, Germany
Xavier Mateos, Universitat Rovira i Virgili,
Tarragona, Spain
Richard Paul Mildren, Macquarie University,
Sydney, Australia
Tomas Mocek, HiLASE Center of Excellence Dolní,Břežany, Czech RepublicFederico Pirzio, University of Pavia, Pavia, Italy
Justinas Pupeikis, ETH Zürich, Zürich, Switzerland
Clara Saraceno, Ruhr University Bochum,
Bochum, Germany
Vasili Savitski, Fraunhofer, Centre for Applied
Photonics, Glasgow, United Kingdom
Takunori Taira, Riken Spring-8 Saitama Japan

European Physical Society (EPS):
Members:
Olivier Dulieu, Laboratoire Aimé Cotton, CNRS,
Orsay, France (Chair)
Trevor Benson, University of Nottingham,
Nottingham, United Kingdom
Crina Cojocaru, Universitat Politecnica deCatalunya, Barcelona, Spain
Lukas Gallmann, ETH Zürich, Zürich, Switzerland
Piotr Maslowski, Nicolaus Copernicus University,
Torun, Poland
Concita Sibilia, Sapienza Università di Roma,
Rome, Italy

Staff Member:
Douglas M. Razzano, IEEE Photonics Society,Piscataway, NJ, USA

Optica (formely OSA):
Members:
Daniele Brida, Université du Luxembourg,
Luxembourg
Alfred Leitenstorfer, University of Konstanz,
Germany
Joyce Poon, Max-Planck-Institute forMicrostructure Physics, Halle, Germany

Co-opted Members:
Aleksandra Foltynowicz, Umeå University,Umeå, Sweden
Rachel Grange, ETH Zürich, Zürich, Switzerland
Julien Javaloyes, University of Balearic Islands,
Palma De Mallorca, Spain
Matthias Kling, Stanford University, Stanford, USA
Marian Marciniak, National Institute of
Telecommunications, Warsaw, Poland
Ioachim Pupeza, Max Planck Instituteof Quantum Optics, Garching & LudwigMaximilians-Universität München, Germany

Staff Members:
Kari Apter, Optica, Los Altos, CA, USA

Staff Members:
Patricia Helfenstein, European Physical Society,Mulhouse, France
Anne C. Pawsey, European Physical Society,Mulhouse, France

Programme Chairs:

IEEE Photonics Society:

Local Chair

Members:
Paul Crump, Ferdinand-Braun-Institut (FBH),
Berlin, Germany

Ioachim Pupeza, Ludwig-MaximiliansUniversität, Munich & Max-Planck-Institut für
Quantenoptik, Garching, Germany

2023 CLEO®/Europe
ORGANISING COMMITTEE

CB - SEMICONDUCTOR LASERS
CHAIR: Mikhail Belkin, Walter Schottky
Institute, Munich, Germany
Dmitri L. Boiko, CSEM, Neuchâtel,Neuchâtel, Switzerland
Frédéric Grillot, Institut Polytechnique de Paris,
Paris, France
Qing Gu, North Carolina State University, Raleigh,NC, USA
Sven Höfling, Würzburg University,
Würzburg, Germany
James A. Lott, OptiPulse, Inc., Albuquerque,
NM, USA
Boon Ooi, KAUST, Jeddah, Saudi Arabia
Benedikt Schwarz, TU Wien, Vienna, Austria
Dries Van Thourhout, Ghent University – imec,
Gent, Belgium

General Chairs:
Lukas Gallmann, ETH Zürich, Zurich,
Switzerland
Marian Marciniak, National Institute of
Telecommunications, Warsaw, Poland

Daniele Brida, University of
Luxembourg, Luxembourg
Crina Cojocaru, Universitat Politecnica deCatalunya, Spain

25

Qi Jie Wang, Nanyang Technological University,
Singapore, Singapore
Dan Yanson, SCD Semiconductor Devices,
Haifa, Israel
CC - TERAHERTZ SOURCES
AND APPLICATIONSCHAIR: Juliette Mangeney, Ecole Normale
Supérieure, Laboratoire Pierre Aigrain,
Paris, France
Francois Blanchard, Université du Quebec,
Québec, Canada
Pernille Klarksov Pedersen, Aarhus University,
Aarhus, Denmark
Jean-Francois Lampin, IEMN, Lille, France
Marco Peccianti, University of Sussex, Sussex, UK
Giacomo Scalari, ETH Zurich, Zurich, Switzerland
Harold Schneider, Institute of Ion-Beam Physics
and Materials Research, Dresden, Germany
Masayoshi Tonouchi, Osaka University,
Osaka, Japan
Dmitry Turchinovich, University of Bielefeld,
Bielefeld, Germany
Karl Unterrainer, Technische Universität Wien,
Vienna, Austria
Miriam Vitiello, CNR Istituto Nanoscienze,
Pisa, Italy
CD - APPLICATIONS OF NONLINEAR OPTICSCHAIR: Mikko J Huttunen, Tampere Universityof Technology, Tampere, Finland
Fabio Biancalana, Australian National
University, Australia and Heriot-Watt University,
United Kingdom
Costantino De Angelis, University of Brescia,
Brescia, Italy
Tal Ellenbogen, Tel Aviv University, Tel Aviv, Israel
Francois Leo, Free University of Brussels,
Brussels, Belgium
Christelle Monat, École centrale de Lyon,
Lyon, France

GENERAL INFORMATION

CLEO®/Europe 2013 Commitee

GENERAL INFORMATION

Committees
Kartik Srinivasan, National Institute ofStandards and Technology and Join Quantum
Institute, NIST/UMD, USA
Zhipei Sun, Aalto University, Espoo, Finland
Nathalie Vermeulen, Free University of Brussels,
Brussels, Belgium
Thomas Zentgraf, University of Paderborn,
Paderborn, Germany
Aleksei Zheltikov, Texas A&M University, USA
CE - OPTICAL MATERIALS, FABRICATIONAND CHARACTERISATIONCHAIR: Stavros Pissadakis, Instituteof Electronic Structure and Laser (IESL),
Heraklion, Greece
Nadège Courjal, FEMTO-ST, Université deFranche-Comté, France
Annamaria Cucinotta, University of Parma
Parma Italy
Jakub Dostalek, Austria institute ofTechnology, Austria
Martina Gerken, Kiel University, Kiel, Germany
Sergey Mirov, The University of Alabama at
Birmingham, Birmingham AL, USA
Christope Moser, EPFL, Lausanne, Switzerland
Virginie Nazabal, Institute of Chemical Sciencesof Rennes, Rennes, France
Silvia Vignolini, University of Cambridge,
Cambridge, UK
Natalie Wheeler, University of Southampton,
Southampton, United Kingdom
Max Yan, KTH, Stockholm, Sweden
CF - ULTRAFAST OPTICAL TECHNOLOGIESCHAIR: Caterina Vozzi, Consiglio Nazionaledelle Ricerche, Milano, Italy
Kristina Chang, NIST, Boulder, USA
Ming-Chang Chen, Institute of Photonics,
National Tsing Hua University, Hsinchu, Taiwan
Hanieh Fattahi, MPI for the Science of Light,
Erlangen, Germany

Sophie Brasselet, Fresnel Institute,Marseille, France
Florenta Costache, Fraunhofer Institute for
Photonic Microsystems IPMS, Dresden, Germany
Marco Grande, Polytechnic University of Bari,
Bari, Italy
Christoph Haisch, Technische Universität
München, Munich, Germany
Robert Halir, University of Malaga, Malaga, Spain
Jian-Jang Huang, National Taiwan University,
Taipei, Taiwan
Doina Nicolae, National Institute for
Optoelectronics, Bucarest, Romania
Adrian Podoleanu, University of Kent,
Canterbury, United Kingdom
Meritxell Vilaseca, Universitat Politécnica deCatalunya, Barcelona, Spain

Nicolas Forget, Fastlite, Antibes, France
Takao Fuji, Toyota Technological Institute,
Nagoya, Japan
Michael Krueger, Department of Physics andSolid State Institute Technion City, Haifa, Israel
Matteo Negro, Cambridge Raman Imaging Ltd,
Milano, Italy
Oleg Pronin, Helmut-Schmidt-Universität/ Universität der Bundeswehr Hamburg,
Hamburg, Germany
Haim Suchowski, Tel Aviv University, Tel Aviv, Israel
Amelle Zair, King’s College London, London, UK
CG - HIGH-FIELD LASER AND
ATTOSECOND SCIENCECHAIR: Adrian Pfeiffer, Friedrich-SchillerUniversität Jena, Jena, Germany
Birgitta Bernhardt, TU Graz, Graz, Austria
Carla Figueira de Morisson Faria, University
College London, London, United Kingdom
Mathieu Gisselbrecht, Lund University,
Lund, Sweden
Christoph M. Heyl, Helmholtz-Institut Jena &DESY, Hamburg, Germany
Heide Ibrahim, Institut national de la recherche
scientifique, Varennes, Canada
Matteo Lucchini, Politecnico di Milano,
Milano, Italy
Balázs Major, ELI ALPS University of Szeged,
Szeged, Hungary
Hiroki Mashiko, NTT Advanced Technology
Corporation, Atsugi-shi, Kanagawa-ken, Japan
Luis Roso, University of Salamanca,
Salamanca, Spain
Laszlo Veisz, Umeå University, Umeå, Sweden

CI - OPTICAL TECHNOLOGIES FORCOMMUNICATIONS AND DATA STORAGE
CHAIR: Alessandro Tonello, Université deLimoges, Limoges, France
Cristian Antonelli, University of L’Aquila,
L’Aquila, Italy
Sonia Boscolo, Aston Institute of Photonic
Technologies, Aston University, Birmingham,
United Kingdom
Nicola Calabretta, Dept of Electrical Engineering,
Eindhoven University of Technology, Eindhoven,
The Netherlands
Francesco Da Ros, Technical University ofDenmark, Kgs. Lyngby, Denmark
Peter Horak, University of Southampton,
Optoelectronics Research Centre, Southampton,
United Kingdom
Son Thai Le, Nubis Communications, New
Providence, NJ, USA Rahman Talha, Huawei
Technologies, Munich, Germany
Akihiro Maruta, Osaka University, Osaka, Japan
Armando Nolasco Pinto, Universidade de
Aveiro, Aveiro, Portugal

CH - OPTICAL SENSING AND MICROSCOPYCHAIR: Cristian Focsa, University of Lille,
Lille, France
Paola Borri, Cardiff University, Cardiff,
United Kingdom

26

Erwan Pincemin, Orange Labs Networks,
Lannion, France
Talha Rahman, Huawei Technologies,
Munich, Germany
CJ - FIBRE AND GUIDED WAVE LASERS
AND AMPLIFIERS
CHAIR: Jayanta Kumar Sahu, University ofSouthampton, Southampton, United Kingdom
Laurent Bigot, CNRS – University of Lille, Lille, France
Liang Dong, Clemson University, Clemson, USA
Alexander Fuerbach, Macquarie
University, Australia
Nicoletta Haarlammert, Fraunhofer IOF,
Jena, Germany
Jesper Laegsgaard, Technical University ofDenmark – DTU Fotonik, Lyngby, Denmark
Jörg Neumann, Laser Zentrum Hannover,Hannover, Germany
Bülend Ortaç, UNAM-Bilkent University,
Ankara, Turkey
Pavel Peterka, Institute of Photonics andElectronics, Czech Academy of Sciences, Prague,
Czech RepublicFederica Poli, University of Parma, Parma, Italy
Grzegorz Sobon, Wroclaw University ofTechnology, Wroclaw, Poland
CK - MICRO- AND NANO-PHOTONICSCHAIR: Stefano Pelli, CNR-IFAC, Sesto
Fiorentino, Italy
Nadia Belabas, C2N, CNRS / Université Paris-Sud– Université Paris-Saclay, Palaiseau, France
Giovanna Calò, Politecnico di Bari, Bari, Italy
Stéphane Clemmen, Ghent University, Ghent, Belgium
Mile Ivanda, Institute Ruder Boskovic,
Zagreb, Croatia
Alejandro Ortega Moñux, Universidad de
Málaga, Málaga, Spain
Anna Peacock, Optoelectronics Research Centre,
University of Southampton, United Kingdom

Committees

CL - PHOTONIC APPLICATIONS IN BIOLOGYAND MEDICINECHAIR: Kenneth K. Y. Wong, The University ofHong Kong, Hong Kong, China
Balpreet Ahluwalia, The Arctic University of
Norway, Tromso, Norway
Martin Booth, University of Oxford, Oxford,
United Kingdom
Thomas Huser, University of Bielefeld,
Bielefeld, Germany
Alexander Jesacher, Medizinische Universität
Innsbruck, Innsbruck, Austria
Dario Polli, Politecnico di Milano, Milan, Italy
Daniel Razansky, ETH Zurich,
Zurich, Switzerland
Chiara Stringari, École Polytechnique,
Palaiseau, France
Benjamin Vakoc, Mass General Brigham andHarvard Medical School, Boston, USA
Giuseppe Vicidomini, Istituto Italiano diTecnologia, Genova, Italy
Xiaoming Wei, South China University ofTechnology, Guangzhou, China
CM - MATERIALS PROCESSING WITH LASERS
CHAIR: Jan Siegel, Instituto de Optica – Consejo
Superior de Investigaciones Científicas (CSIC),
Madrid, Spain
Joern Bonse, Bundesanstalt fürMaterialforschung und -Prüfung (BAM),
Berlin, Germany

Nadezhda M. Bulgakova, Institute of Physics
of the Czech Academy of Sciences, Prague,
Czech RepublicFrançois Courvoisier, Université deFranche-Comté, FEMTO-ST Institute, CNRS,
Besançon, France
Nathalie Destouches, Hubert Curien Laboratory,
St. Etienne, France, Saint Etienne, France
Maria Farsari, FORTH, Institute ofElectronic Structure and Laser, Greece,
Heraklion, Grece
Johannes Heitz, Johannes Kepler University,
Linz, Austria
Gert-Willem Roemer, University of Twente,
Twente, The Netherlands
Klaus Sokolowski-Tinten, University ofDuisburg-Essen, Germany
Robert Thomson, Heriot-Watt University,
Edinburgh, Scotland, UK EH14 4AS,
United Kingdom
Vassilia Zorba, Lawrence Berkeley National
Laboratory, Berkeley, CA, USA

PROGRAMME COMMITTEES

2023 EQEC ORGANISING COMMITTEEEB - QUANTUM INFORMATION,
COMMUNICATION, AND SENSINGCHAIR: Marco Genovese, INRIM, Turin, Italy
Maria Chekhova, Max Planck Institute for the
Science of Light, Erlangen, Germany
Hugues de Riedmatten, ICFO – The Institute of
Photonic Sciences, Castelldefels, Spain
Sara Ducci, Université Paris Diderot, Paris, France
Thomas Gerrits, NIST, USA
Ulrik Lund Anderssen, DTU,
Copenhagen, Danmark
Luis Sanchez Soto, Compulense University of
Madrid, Madrid, Spain
Romana Schirhagl, University of Groningen,
Groningen, The Netherlands
Vincenzo Tamma, Univesity of Portsmouth,
Portsmouth, United Kingdom

EA - QUANTUM OPTICS AND
QUANTUM MATTERCHAIR: Sebastian Blatt, MPQ,
Garching, Germany
Ticijana Ban, Institute of Physics, Zagreb, Croatia
Darrick Chang, ICFO – The Institute of Photonic
Sciences, Castelldefels, Spain
Andrew Daley, University Strathclyde,
Glasgow, Scotland
Ofer Firstenberg, Weizman Institute,Rehovot, Israel
Christian Gross, Universität Tübingen,
Tuebingen, Germany
Börge Hemmerling, UC Riverside, Riverside,
CA, USA
Mathilde Hugbart, INPHYNI, Nice, France
Gerhard Kirchmair, University of Innsbruck,
Innsbruck, Austria
Valentina Parigi, LKB, Laboratoire Kastler
Brossel, Paris, France
Magdalena Stobinska, University of Warsaw,
Warsaw, Poland

General Chairs
Rachel Grange, ETH Zürich, Zurich, Switzerland
Piotr Maslowski, Nicolaus Copernicus University,
Torun, Poland

Programme Chairs
Aleksandra Foltynowicz, Umea
University, Sweden
Julien Javaloyes, University of Balearic Islands,
Palma de Mallorca, Spain

Local Chair
Ioachim Pupeza
Ludwig-Maximilians-Universität, Munich& Max-Planck-Institut für Quantenoptik,
Garching, Germany

27

Giuseppe Vallone, Università di Padova,
Padua, Italy
Val Zwiller, KTH, Stockholm, Sweden
EC - TOPOLOGICAL STATES OF LIGHTCHAIR: Stefan Rotter, Vienna University ofTechnology, Vienne, Austria
Alberto Amo, Laboratoire PhLAM, Villeneuve
D’Ascq, France
Iacopo Carusotto, Università di Trento, Povo
(Trento), Italy
Romain Fleury, École Polytechnique Fédérale deLausanne, Lausanne, Switzerland
Flore Kunst, MPI for the Science of Light,
Nürnberg/Erlangen, Germany
Tomoki Ozawa, Tohoku University,
Sendai, Japan
Laura Pilozzi, Institute for Complex Systems,
CNR, Rome, Italy
Alexander N. Poddubny, Weizmann Institute of
Science, Rehovot, Israel
Hannah Price, University of Birmingham,
Birmingham, United Kingdom
Henning Schomerus, Lancaster University,
Lancaster, United Kingdom
Oded Zilberberg, Konstanz University,
Konstanz, Germany
ED - PRECISION METROLOGY AND
FREQUENCY COMBSCHAIR: Marco Marangoni, Politecnico di Milano
and Institute of Photonics and Nanotechnology,
Milano, Italy
Esther Baumann, NIST, Boulder, USA
Pascal Del’Haye, Max Planck Institute for the
Science of Light, Erlangen, Germany
Frans Harren, Radboud University, Nijmegen,
The Netherlands
Feng-Lei Hong, Yokohama National University,
Yokohama, Japan
Yann Le Coq, Université de Paris, Paris, France

GENERAL INFORMATION

Minhao Pu, Technical University of Denmark,Lyngby, Denmark
Isabelle Robert-Philip, CNRS, Université deMontpellier, Laboratoire Charles Coulomb,
Montpellier, France
Jens Schmid, National Research Council Canada,
Ottawa, Canada
Marc Sorel, University of Glasgow, Glasgow,
United Kingdom

GENERAL INFORMATION

Committees
Helen Margolis, National Physical Laboratory,
London, UK
Ekkehard Peik, Physikalisch-Technische
Bundesanstalt, Braunschweig, Germany
Lucile Rutkowski, Université de Rennes,
Rennes, France
Markku Vainio, Univerisity of Helsinki,
Helsinki, Finland
Piotr Wcislo, Nicolaus Copernicus University,
Torun, Poland
EE - ULTRAFAST OPTICAL SCIENCECHAIR: Jens Biegert, ICFO, The Institute of
Photonic Sciences, Castelldefels, Spain
Elisabetta Collini, University of Padova,
Padova, ItalyGoëry Genty, Tampere University of Technology,
Tampere, Finland
Janos Hebling, University of Pecs, Hungary
Michael Hemmer, JILA, Boulder, CO, USA
Anne-Marie Huijser, University of Twente,
The NetherlandsJérôme Kasparian, University of Geneva,
Geneva, Switzerland
Melanie Müller, Fritz Haber Institute,
Berlin, Germany
Valentina Shumakova, Class 5 Photonics
GmbH, Hamburg, Germany
Francesco Tani, MPI for the Science of Light,
Erlangen, Germany
John Travers, Heriot Watt University, Glasgow,
United Kingdom
EF - NONLINEAR PHENOMENA, SOLITONSAND SELF-ORGANIZATION
Co-Chairs:
Alessia Pasquazi, Loughborough University,
Loughborough, United Kingdom
Svetlana Gurevich, University of Münster,
Münster, Germany
Fabio Baronio, Universita di Brescia, Brescia, Italy

Andrea Blanco-Redondo, Nokia Bell Labs,
Crawford, NJ, USA
German de Valcarcel, University of Valencia,
Valencia, Spain
Miro Erkintako, The University of Auckland,
Auckland, New ZealandKatarzyna Krupa, Institute of Physical Chemistry,
Polish Academy of Sciences, Warsaw, Poland
Mathias Marconi, Université Côte d’Azur
CNRS, Institut de Physique de Nice,
Valbonne, FranceFrank Setzpfandt, Friedrich-Schiller-Universität
Jena, Jena, Germany
Alexander Solntsev, University of Technology
Sydney, Ultimo, Australia
Moustapha Tlidi, Université Libre de Bruxelles,
Bruxelles, Belgium

EH - PLASMONICS AND METAMATERIALSCHAIR: Paloma Huidobro, University of Lisbon,
Lisbon, Portugal
Sébastien Bidault, Institut Langevin, ESPCI,Paris, France
Andrea Bragas, Universidad de Buenos Aires,
Buenos Aires, Argentina
Angela Demetriadou, University ofBirmingham, Birmingham, United Kingdom
Vincenzo Galdi, University of Sannio,
Benevento, Italy
Maria Kafesaki, University of Crete andFoundation for Research and Technology Hellas,
Heraklion, Greece
Alexey Krasavin, King’s College London andLondon Centre for Nanotechnology, London,
United Kingdom
Andrei Lavrinenko, Technical University ofDenmark, Copenhagen, DenmarkPaïvi Törmä, Aalto University, Aalto, Finland
Kosmas Tsakmakidis, National andKapodistrian University of Athens, Athens, Greece
Costas Valagiannopoulos, Nazarbayev
University, Nur-Sultan, Kazakchstan

EG - LIGHT-MATTER INTERACTIONSAT THE NANOSCALECHAIR: Mathieu Mivelle, Sorbonne University,
Paris, France
Paolo Biagioni, Politecnico di Milano, Milan, Italy
Alberto Curto, Ghent University, Ghent, Belgium
Hugo Defienne, University of Glasgow,
School of Physics and Astronomy, Glasgow,
United Kingdom
Alison Funston, Monash University,
Melbourne, Australia
Walter Pfeiffer, Universität Bielefeld,
Bielefeld, Germany
Riccardo Sapienza, Imperial College, The
Blackett Laboratory, London, United Kingdom
Matthew Sheldon, Texas A&T University, College
Station, Texas, USA
Giulia Tagliabue, Ecole Polytechnique Fédérale
de Lausanne, Lausanne, Switzerland
Niek Van Hulst, ICFO – The Institute of Photonic
Sciences, Castelldefels, Spain
Peter Zijlstra, Eindhoven University ofTechnology, Eindhoven, The Netherlands

EI - TWO-DIMENSIONAL ANDNOVEL MATERIALSCHAIR: Nicolò Maccaferri, Umeå University,Umea, Sweden
Pablo Alonso Gonzales, University of Oviedo,
Oviedo, Spain
Monica Craciun, University of Exeter, Exeter, UK
Brian Gerardot, Heriot-Watt University,
Edinburgh, United Kingdom
Giulia Grancini, University of Pavia, Pavia, Italy
Deep Jariwala, Pennsylvania University,
Philadelphia, USA
Jose Lado, Aalto University, Aalto, Finland
Ermin Malic, Chalmers University of Technology,
Goteborg, Sweden

28

Paulina Plochocka, CNRS, Toulouse, France
Klaas-Jan Tielrooij, ICN2, Barcelona, Spain
Chiara Trovatello, Columbia University,
New York, USA
EJ - THEORETICAL AND COMPUTATIONAL
PHOTONICS MODELLINGCHAIR: Fabian Maucher, University of Balearic
Islands, Palma de Mallorca, Spain
Viktoriia Babicheva, University of New Mexico,
Albuquerque, USA
Ihar Babushkin, Max Born Institute for
Nonlinear Optics and Short Pulse Spectroscopy,
Berlin, Germany
Fabrice Catoire, University of Bordeaux,Bordeaux, France
Eduardo Cabrera Granado,
Universidad Complutense Madrid,
Madrid, Spain
Jörg Götte, University of Glasgow, Glasgow,
United Kingdom
Kathy Lüdge, University of Ilmenau,
Ilmenau, Germany
Konstantinos Makris, University of Crete,
Heraklion, Greece
Rachel Nuter, University of Bordeaux,Bordeaux, France
Philippe Tassin, Chalmers University,
Goteborg, Sweden

2023 CLEO/Europe-EQEC
JOINT SYMPOSIAPROGRAMME COMMITTEESJSI - FREE ELECTRON LASERS
Co-Chairs:
Christoph Bostedt, Paul Scherrer Institute,Villigen PSI, Switzerland
Giuseppe Sansone, University of Freiburg,
Freiburg, Germany

Committees
NOTES

GENERAL INFORMATIONJSII - INFRARED INTEGRATED PHOTONICS
FOR ASTRONOMICAL APPLICATIONS
Co-Chairs:
Lucas Labadie, I-Physics Institute Universityof Cologne, Germany
Robert R. Thomson, Institute of Photonics
and Quantum Sciences, Heriot Watt University,
United Kingdom
JSIII - PHOTONICS FORARTIFICIAL INTELLIGENCE
Co-Chairs:
Antonio Hurtado, University of Strathclyde,
Glasgow, United Kingdom
Bruno Romeira, INL Institute,
Braga, Portugal
JSIV - PHOTONICS FOR SUSTAINABILITY
Co-Chairs:
Esther Alarcon Llado, AMOLF, Amsterdam,
The Netherlands
Giulia Tagliabue, École PolytechniqueFédérale de Lausanne, Joint Center
for Artificial Photosynthesis,
Lausanne, Switzerland
JSV - DIVERSITY IN PHOTONICS
Several events chaired by CLEO®/EuropeEQEC or other collocated conferences. See“Special events” in this programme or the
separate leaflet.
JSVI - NANOPHOXONICS AND NANOSCALEHEAT TRANSFER
Co-Chairs:
Roberto Li Voti, Sapienza Università di Roma,
Rome, Italy
Sebastian Volz, Laboratory for Integrated
Micro-Mechatronic Systems, University of Tokyo,
Tokyo, Japan

29

General information
GENERAL INFORMATIONGENERAL INFORMATION

Short abstracts of the papers to be presented at
CLEO®/Europe-EQEC 2023 appear in this advance programme.
The CLEO®/Europe-EQEC 2023 technical programme will feature 1759 presentations including
3 plenary talks, 7 tutorial talks, 10 keynote talks,
77 invited talks, 17 talks upgraded to invited, 1109
oral presentations, 10 short courses and 526 posters. Among them 26 poster presentations wereselected to hold a 3-minute oral presentation(pitch). 17 oral presentations will also be featured.
From 11 to 17 parallel sessions will take place daily during the conference. All sessions and shortcourses will be held at the International Congress
Centre in Munich (so called ICM) or the exhibition halls of the trade fair grounds LASER Worldof PHOTONICS 2023. These rooms are named
according to famous physicists.

Conference dates
CLEO®/Europe-EQEC 2023 will be running from
Monday, June 26th, 08:30am to Friday, June 30th,
2023, 05:30pm.

Special events
This year a particular highlight devoted to diversity in photonics will be featured. Several events
managed by our conference or other collocatedconferences will take place.
This program will include a range of activities,
such as workshops, panel discussions, keynote
speeches, career and networking events including:▶ The importance of diversity, equity, and inclusion in the photonics industry▶ Support for early-stage researchers iversiWiki session
DWorkshop exploring the concept of privilege.
The programme will be open to all attendees ofLaser World of Photonics 2023 and will be run
in collaboration with several organizations, including the European Optical Society (EOS), theEuropean Physical Society (EPS), Wissenschaftliche Gesellschaft Lasertechnik und Photonik e.V.
(WLT), Optica, IEEE Photonics Society, and theInternational Society for Optics and Photonics(SPIE). Full programme at https://www.photonics-congress.com/en/about/conferences/diversity-program/ or see the separate leaflet.

at Adolphe Merkle Institute, University of Fribourg, Switzerland
Arti Agrawal, Professor at the University of Technology Sydney, Australia
Florian Emaury, CEO & Co-founder at Menhir
Photonics, Switzerland
Only registered attendees will get a lunch box
until the quota is reached.
Registration: https://www.cleoeurope.org/
career-and-diversity-lunch-for-early-postdocs/▶
▶

Career and diversity lunch for PhD candidates:
Friday 30 June 2023, 12:00-13:00, Foyer, 1st floor
ICM (opposite room 14)
PhD candidates looking for the next steps in theircareer may discuss with their peers and more advanced researchers.
Four panel members will lead the discussion:
Arti Agrawal, Professor at the University of Technology Sydney, Australia
Clara Saraceno, Professor at Ruhr-Universität
Bochum, Germany
Robert Sewell, Tenured Scientist and Head of
Academic Affairs, Institute of Photonics Science(ICFO), Barcelona, Spain
Sergi Vizcaino, Strategy & Outreach Manager,
LuxQuanta Technologies S.L, Spain
Only registered attendees will get a lunch box
until the quota is reached.
Registration: https://www.cleoeurope.org/
career-and-diversity-lunch-for-phd-student/
Space is limited, the number of participants isfixed. To participate to the above-mentioned
DIVERSITY EVENTS, conference registration
is mandatory and additional registration for the
Diversity Events at https://www.cleoeurope.org/
career-and-diversity/ will be required.
The rule first come, first served will be appliedand only attendees who registered for the careerand diversity lunch events will get a lunch box
until the quota is reached.

Diversity programmeat CLEO®/Europe-EQEC 2023
Career events:
Career event with Donna Strickland: Monday
26 June 2023, 17:30-18:30, Room 4a ICM
PhD students are cordially invited to interact
with Donna Strickland, University of Waterloo, Ontario, Canada and co-laureate of Nobel
Prize in Physics in 2018 for her work on chirped
pulse amplification.
Mandatory registration: www.cleoeurope.org/
career-and-diversity-donna-strickland/
Career and diversity lunch for postdocs: Thursday 29 June 2023, 12:00-13:00, Foyer, 1st floor
ICM (opposite room 14)
Postdocs looking for the next steps in their career may discuss with their peers and more advanced researchers.
Four panel members (researchers at different universities in Europe from different CLEO-EQEC
committees) will lead the discussion:
Francesca Calegari, Leading Scientist at
DESY and Professor at the University of Hamburg, Germany
Viola Vogler-Neuling, Postdoctoral Researcher

30

Poster pitches:This year in collaboration with the CLEO/
Europe-EQEC 2023 co-organizers (European
Physical Society, Optica, IEEE Photonics Society), the European Optical Society will chair
two Early-Stage Researcher (ESR) sessions, offering an opportunity for PhDs and Post-docs
to hold a 3-minute oral presentation (pitch)
to draw attention to their upcoming poster
presentation. Thirteen presentations were selected per session. Each registered participant
is cordially invited to attend on Monday 26
and Wednesday 28 June, 12:00-13:00, Room
4a ICM.
Diversity event managed by Optica(Formerly OSA):DiversiWiki: Monday 26 June 2023, 10:00 –15:00, Foyer Room 1, 1st floor, ICM
Wikipedia is the fifth most visited site in theworld. Still, only 18% of the 1.6 million biographies in the English Wikipedia are about women,
and only 16% of those individuals are tagged as
scientists. During this event, you will learn how
to be a Wikipedia editor – or hone your skills if
you already are one – as we edit, update or add
articles on Wikipedia. Trainers will be on handthroughout the day to provide guidance and assistance. To help get you started, Optica will havea list of people and pages we have identified thatyou can use to edit or create.
Join Optica when you can throughout the day
to help:
1. Improve Diversity – Having more editors focused on strengthening existing or creating
new pages for marginalized people in science.
Visit the Wikipedia Cultural Diversity Observatory to learn more about efforts to improvediversity on the site.

2. Translate Pages – Wikipedia pages exist in multiple languages, but not all are equal. By translating existing pages where a page does not exist
or includes less information, we can help the
distribution of information on a global scale.
3. Simple Wiki – This site is designed for children
and adults learning English. By contributing
to these pages, you can open the door to theworld of optics and physics and inspire the next
generation of scientists.
RSVP here for additional information on the program: https://forms.gle/Au2nVT37viBsLVhU72023 World of Photonics Congress
The World of Photonics Congress bundles various topical conferences under one roof under
the organization by Messe München International. Registered attendees will have access toall conferences:▶ CLEO®/Europe-EQEC - Conference on Lasers
and Electro-Optics®/Europe-European Quantum Electronics Conference organised by theEuropean Physical Society (EPS), Optica (Formerly OSA), IEEE Photonics Society.
▶ ECBO - European Conferences on Biomedical
Optics organised by SPIE in cooperation with
Optica (Formerly OSA).
▶ LiM 2023 - Lasers in Manufacturing organisedby the German Scientific Laser Society (WLT).
▶Digital Optical Technologies organised by
SPIE Europe.
▶ Optical Metrology organised by SPIE Europe.
The 2023 World of Photonics Congress covers
the whole spectrum from science to application.
Current fundamental research, the practice-oriented development of photonics solutions, success stories for industrial applications, networking
and knowledge-sharing – the World of Photonics

Congress has been bridging the gap between science and industry since 1973.

innovations that made this achievement possible,
including advances in photonics.

Opening and Plenary Talk of the World of Photonics Congress, LASER World of PHOTONICS and World of QUANTUM:

Prizes and awards
A series of Prize and Award ceremonies will takeplace during the EQEC Plenary session scheduled
Tuesday 27 June from 10:30 to 12:30, room 1.

Tuesday 27 June 2023, Room 1, Ground
Floor, ICM

During this session Claudio Conti, Sapienza
Università di Roma, Italy will present a plenary
talk on “Photonic Machines for Large-scale Applications and Fundamental Physics”.

14:00 – 14:10 Opening of Congress and Trade
Fairs / 50 years of LASER World of PHOTONICS
Welcome Note by Reinhard Pfeiffer, Managing
Director | CEO, Messe München

Abstract: Which is the simplest way to process
information with light? By spatial modulation,
we demonstrate combinatorial optimization andnatural language processing at the largest scale.
Novel computational paradigms open the roadto new physics and applications with photonics.

14:10 – 14:20 Welcome Note by Peter Loosen, Chair World of Photonics Congress Steering Committee
14:20 – 15:30 World of Photonics Congress
Plenary Talk “Laser-driven inertial confinement fusion, power source of the future?” by
Tammy Ma, PhD, Program Element Leader for
High-Intensity Laser HED Science, Advanced
Photon Technologies, Lead Inertial Fusion Energy (IFE) Institutional Initiative, Lawrence
Livermore National Laboratory LLNL, USA
and Constantin L. Haefner, Director, Fraunhofer-Institute for Laser Technology, Head of theExpert Group on Laser Inertial Fusion Commissary Fusion Research, Fraunhofer Gesellschaft,
German Federal Ministry of Education andResearch, Germany

Speakers’ information

Prizes or Awards of the European Physical Society (EPS) through its Quantum Electronics
and Optics Division:▶ Quantum Electronics Prizes (2021 and 2023).
▶ 2023 Fresnel Prizes.
▶ 2023 PhD Thesis Prizes.
▶ 2023 EPS-QEOD and EPS Young Minds Travel
Grant Student Awards.

Duration of the talks:• Oral presentations are 15 minutes long (12 minutes presentation + 3 minutes for discussion).
• Post-deadline presentations are 10 minutes
long (7 minutes presentation + 3 minutes
for discussion).
• Invited presentations are 30 minutes long (25minutes presentation + 5 minutes for discussion).
• Tutorial presentations are 60 minutes long
(50 minutes presentation + 10 minutes
for discussion).
• Keynote presentations are 45 minutes long (38minutes presentation + 7 minutes for discussion).
• Plenary presentations are 60 minutes long
(50 minutes presentation + 10 minutes
for discussion).
• Short Course presentations are 2 ×1.5 hour andhalf an hour break in-between long.

See separate leaflet.

31

Prize of SPRINGER NATURE:▶
Julius Springer Prize for Applied Physics
The Julius Springer Prize for Applied Physics
recognizes researchers who have made an outstanding and innovative contribution to thefield of applied physics. It has been awarded
annually since 1998 by the editors-in-chief of
the Springer Journals Applied Physics A – Materials Science & Processing and Applied Physics B – Lasers & Optics.

A series of Prizes and Awards will be presented.

Prize, Awards and Honours of the Optica (Formerly OSA):▶ Herbert Walther Award (2021 and 2023).
▶ Bernard J. Couillaud Prize.
▶ Fellow Members.
▶
O ptica Foundation Student Travel
Grant laureates.

Abstract: Fusion ignition has been achieved at
the National Ignition Facility (NIF) at Lawrence
Livermore National Laboratory. This experimental result, decades in the making, is a major
scientific breakthrough for laser-driven inertial
confinement fusion. This talk will present the experimental results and the many technologicalAward of the European Optical Society (EOS):▶ 2023 EOS Early Career Women in Photonics Award
The Early Career Women in Photonics Award ispresented to honour a young female scientist who
has made outstanding contributions to photonics.
Website: https://www.europeanoptics.org/pages/
distinctions/awards/early-career-women.html

GENERAL INFORMATION

General information

General information

GENERAL INFORMATION

Speakers are requested to strictly stick to thesetime lengths, no extra time can be given.
Speakers are asked to check-in with the session
chair in the room of their relevant session ten
minutes before the beginning of the session.
Presentation Management / Speakers‘ Service
Each conference room used for World of Photonics Congress sessions is equipped with the complete presentation equipment: Beamer / screen,
laptop & presenter.
Please note:• Due to time limitations, it is not possible to connect the speaker’s laptop/hardware device for thelecture directly in the conference room.
• It is also not possible to upload presentations directly to the conference room using the installed
presentation laptop.
• For this reason, all presentations must be uploaded in advance to the presentations management system of Neumann & Müller.
Upload Service in advance
All speakers can upload their presentations to aprotected server of Neumann & Müller prior tothe conference. Upload-Link and login details
were announced mid of June. Each speaker got
his/her own account and a link where he/she canupload his/her presentation until one hour before
session starts.
Onsite Service / Opening times Speaker’ Check-In
Onsite at the ICM, speakers can upload theirpresentations at the Speakers’ Check-In.The
Speakers’ Check-In is located in the foyer
on the 1 st floor of the ICM. The Speakers’
Check-In will be open during the following
hours, with technicians available to assist
the attendees:

Sunday, 25 June 2023
Monday, 26 June 2023
Tuesday, 27 June 2023
Wednesday, 28 June 2023
Thursday, 29 June 2023
Friday, 30 June 2023

Session chairs’ information

7:30 a.m. – 6:30 p.m.
7:30 a.m. – 6:30 p.m.
7:30 a.m. – 6:30 p.m.
7:30 a.m. – 6:00 p.m.
7:30 a.m. – 6:00 p.m.
7:30 a.m. – 4:00 p.m.

For each oral session, a nominated session chair
will be responsible for introducing the speakers,
ensuring that they adhere to the allocated time
limits, and facilitating discussion among theparticipants. At the end of the session, a form
will need to be returned to conferences@eps.org
giving feedback on attendance, no-shows,room logistics.

In any case each speaker must be reviewed
and check her/his presentation in the Speakers’ Check-In, when she/he arrives at the ICM,
to certain that the presentation works correct!
It is possible to check or edit the presentation
up to one hour prior to the session timeslot.

Poster sessions - poster
presenters’ information

Guidelines Presentation Formats
We recommend PowerPoint Presentation for all
speakers with a slide ratio 16:9.
It is also possible to use PDF, Word and Excel files
for the presentation.
For video we prefer mp4 file container with a h264
codec. It is also possible to use (.wmv), (.avi) or(.mov), so they will run properly on the computers provided.
There is no Internet available on the presentation computers.

Posters are a major attraction and provide an
intimate interaction between the presenter andthe viewer. To allow participants to see as many
posters as possible, all CLEO®/Europe-EQEC
2023 posters will be displayed in Hall B0 (groundfloor) next to the ICM centre. The conference
will feature 5 poster sessions taking place from
Monday to Friday after lunchtime. There will be
no oral presentations during this time.
Poster day schedules:
MONDAY: CA, CB, CM, ED, EJ and JS-II topics.
TUESDAY: CD, CF, CK and EG topics.
WEDNESDAY: CH, EE, EF, JS-I and JS-IV topics.
THURSDAY: CE, CG, EA, EB and EH topics.
FRIDAY: CC, CI, CJ, CL, EC, EI, JS-III topics.
All take place from 13:00 to 14:00.

On the presentation laptops in the conference
rooms Microsoft Windows 10 with Power Point
2021will be installed.
In case if you have to use another presentation
software, please contact us atmediacheck@neumannmueller.com

Authors are requested to display their poster on
their allocated board in the morning of the dayof their presentation. The poster presentations
can remain on the boards until 4:00pm on the
allocated day.
In order to present their work and answer questions, authors are requested to be present in thevicinity of their poster on the day of their presentation time. There will be no oral presentations

Provided Audiovisual Equipment
The standard AV meeting package available ineach session rooms includes:• HD Video Projector• Screen with ratio 16:9
• Laser pointer• Lectern microphone32

during this time.
Each author is provided with one board on whichto display a summary of the paper. The size of theposter should not exceed 100-105 cm wide x 150
cm high. Fixing material (adhesive tape) will be
provided. The boards will be grouped by topics
and marked with the poster reference numbers.
Authors absolutely need to display their poster on
their allocated board in the morning of the day of
their presentation. In order to present their workand answer questions, authors are requested to bepresent in the vicinity of their poster on the dayof their presentation time. There will be no oralpresentations during this time.
All poster presenters need to be physicallypresent during their assigned poster session on
the assigned day and place. In case of no show,
the poster presentation will be discarded fromthe publications.
Early-stage Researcher (ESR) Session – Poster
Pitches:
In collaboration with the CLEO/Europe-EQEC
2023 co-organizers (European Physical Society,
Optica, IEEE Photonics Society), the European
Optical Society will chair two Early-Stage Researcher (ESR) sessions, offering an opportunity for selected PhDs and Post-docs to hold a3-minute oral presentation (pitch) to introduce
their upcoming poster presentation. Two sessions
with thirteen presentations each will take placeon Monday 26 and Wednesday 28 June, 12:0013:00, Room 4a ICM. As all other oral presentations, presentations will need to be uploadedin advance.

Short courses
Ten short courses at an extra cost will be presented in parallel on Monday, Wednesday, Thursday and Friday. Each course is scheduled in twoparts: Course Part I (1 hour 30 minutes), coffee
break (30 minutes), Course Part II (1 hour 30
minutes). The courses are open to attendees of theWorld of Photonics Congress and Laser World of
Photonics exhibition, subject to payment of thecourse fee. The short course material will only beavailable online.

with the online registration during your conference registration. The dinner can also be added
later on when proceeding with a new registration
including the dinner only. On-site reservations
will not be possible. Only registered individuals with a valid invitation card will be allowed
to attend.

OSA Publishinghttps://www.osa.org/en-us/
publications/
IEEE Photonics Society’s IEEE
Xplore Digital Libraryhttps://ieeexplore.ieee.org/xpl/
conhome/1000412/all-proceedings

Social events
All conference attendants are cordially invited toattend the following parties:

Only papers (either oral or poster) for which theauthor(s) made the presentation at the conference
will be eligible for the publications.

Monday 26 June 2023, from 18:45 to 21:00 – ICM
Foyer and Hall B0, ground floor“Happy Hour” kindly sponsored by the European Physical Society through its Quantum Electronics Optics Division.
Tuesday 27 June 2023, from 17:45 to 19:45 – ICM
Foyer and Hall B0, ground floor“Bier & Brezel” Get together kindly sponsored
by SPIE.

Conference dinner
The “CLEO®/Europe-EQEC Conference Dinner”
will take place on Wednesday 28 June 2023,
from 19:00 at the famous Löwenbräukeller,
Nymphenburger Straße 2, D-80335 München
A delightful selection of authentic Bavarian cuisine will be provided during the buffet dinner.
In case you wish to attend, an exceptional additional cost of 20€ (including buffet + 2 drinks)
will be invoiced per conference participant. For
accompanying person, the cost will be of 35€.
Reservation possible until the quota is reached.
To secure your spot at the dinner, please proceed

Copyright
The CLEO®/Europe-EQEC conference digest
series, containing papers presented as part ofthe conference programme, is registered in
the name of IEEE. To the extent protectable bycopyright law, the 2023 CLEO®/Europe-EQEC
conference digest as a whole shall be copyrighted
by IEEE.

The Löwenbräukeller is located at Stiglmaierplatz in the heart of Munich, offering excellent accessibility:• Public transportation stops directly at Stiglmaierplatz (Metro U1, Tramway 20/21).
• The main station (serving international and regional trains, as well as public transport) is justone metro station away or within an 8-minutewalking distance.

IEEE policy requires that prior to publication
all authors or their employers must transfer tothe IEEE in writing any copyright they hold fortheir individual papers. Transferring copyrightis a necessary requirement for publication, except for material in the public domain or whichis reprinted with permission from a previously
published, copyrighted publication.

Conference publication
The accepted one-page summaries (oral or posters) will be available online during the conference
for those who have registered for the CLEO®/Europe-EQEC conference.

Upon transferring copyright to IEEE, authors
and/or their companies have the right to post
their IEEE-copyrighted material on their own
servers without permission, provided that theserver displays a prominent notice alerting readers to their obligations with respect to copyrighted material and that the posted work includes anIEEE copyright notice.

Post conference publication
After the conference, if approval given during theonline submission and physical presentation doneby the author, the one-page summaries will be
published online by:33

Authors are particularly encouraged to note the“Author Responsibilities” section of the IEEE
Copyright Form, in which portions of IEEE PSPB
Operations Manual, section 8.1.1.B (concerningstatements in work published by IEEE are theexpression of the authors) appear.
Publication with IEEE is subject to the policies
and procedures as described in the IEEE PSPB
Operations Manual. Authors must ensure that
their work meets the requirements as statedin Section 8.2.1 of the IEEE PSPB Operations
Manual, including provisions covering originality, authorship, author responsibilities andauthor misconduct.
IEEE takes the protection of intellectual property seriously. Accordingly, all submissions will
be screened for plagiarism using CrossCheck.
By submitting your work, you agree to allow
IEEE to screen your work. For more information
please visit:
http://www.crossref.org/crosscheck/index.html
IEEE defines plagiarism as the reuse of someone else’s prior ideas, processes, results, orwords without explicitly acknowledging theoriginal author and source. It is important for
all IEEE authors to recognize that plagiarism
in any form, at any level, is unacceptable andis considered a serious breach of professional
conduct, with potentially severe ethical andlegal consequences. To reuse someone else’s
work and make it appear to be your own denies the original author credit for his or her
contributions to the research and to Society.
If you neglect to properly credit the work you
have reused, either by choice or by accident,
you are committing plagiarism.

GENERAL INFORMATION

General information

GENERAL INFORMATION

General information
Note: Part of the process of signing a publicationagreement may include giving permission or not
to IEEE to make and distribute video and audio recordings of their conference presentation.
Granting IEEE this simple permission to record
your presentation will not affect in any way yourrights or your employer’s rights to own and use
your presentations.
An author’s copyright status is determined to alarge extent by the type of employer for whom
the author works. For example, if you are employed by the U.S. Government, and you are thesole author of your paper, then you should select“Employed by United States Government.”
Similarly, if you are the sole author and you areemployed by a Crown Government (or if you andall your co-authors are Crown Government employees), then copyright to your paper will remain
with the Crown Government. You should select“Employed by a Crown Government.”
Optica is the exclusive owner of all rights, titles
and interests throughout the world of the names“Conference on Lasers and Electro-Optics” and“CLEO®” which is a registered trademark CLEO®/.

Anti-harassment policy
and code of conduct
CLEO®/Europe-EQEC is committed to providing
an environment that is conducive to the free androbust exchange of scientific ideas. This environment requires that all participants be treated withequal consideration and respect. While CLEO®/
Europe-EQEC encourages vigorous debate ofideas, personal attacks create an environment
in which people feel threatened or intimidated. This is not productive and does not advancethe cause of science. All participants in CLEO®/

Capture and use of a person's image

Europe-EQEC and CLEO®/Europe-EQEC-managed events and activities are therefore expected to conduct themselves professionallyand respectfully.

By registering at CLEO®/Europe-EQEC, the registrant grants full permission to the management
society to capture, store, use, and/or reproduce
his/her image to be used in future CLEO®//Europe-EQEC marketing materials or the conference website. The registrant also waives any rightto inspect or approve the use of the images orrecordings. They also waive any right to royalties
or other compensation arising from or related tothe use of the images, recordings, or materials.

It is the policy of CLEO®/Europe-EQEC that
all forms of bullying, discrimination, and harassment, sexual or otherwise, are prohibitedin any CLEO®/Europe-EQEC or CLEO®/Europe-EQEC-managed events or activities. This
policy applies to every individual at the event,whether attendee, speaker, exhibitor, award
recipient, staff, contractor or other. It is also a
violation of this policy to retaliate against an individual for reporting bullying, discriminationor harassment or to intentionally file a false report of bullying, discrimination, or harassment.

Persons not wishing to be photographed or videotaped by the management staff or its supplierneed to send their request by email to conferences@eps.org, including their picture to allow for
their identification.

Bullying, discrimination, and harassment of any
sort by someone in a position of power, prestige
or authority is particularly harmful since thoseof lower status or rank may be hesitant to express their objections or discomfort out of fearof retaliation.

By registering at CLEO®//Europe-EQEC, theregistrant also agrees to have Messe MünchenGmbH use their personal particulars (title, first
name, last name, company name, company address, country) for badge printing purposes andto pass on said information to exhibitors in casethe registrant allowed scanning of the badge during online registration.

CLEO®/Europe-EQEC may take any disciplinary
action it deems appropriate if, after thorough investigation, it finds a violation occurred.

Exhibition information

Audio, video, photography,
digital recording policy

From Tuesday to Friday, a major exhibition of laserand electro-optic equipment and services, LASERWorld of PHOTONICS 2023 (See list of exhibitors at https://world-of-photonics.com/en/about/information/exhibitor-list/) and the meeting
place for quantum technology, World of QUANTUM (See https://world-of-photonics.com/en/
about/exhibition-sectors/world-of-quantum/
world-of-quantum-supporting-program.html)
will be held in conjunction with the congress. The
latest technology firsthand will be exhibited. The

Conferences, courses, and poster sessions: For
copyright reasons, photographs or recordings ofany kind are prohibited without the prior writtenconsent of the presenter or instructor.
Exhibition halls: For security and courtesy reasons, recordings of any kind are prohibited unless
one has explicit permission from on-site company representatives.

34

range of products exhibited will cover innovative
optical technologies:• Illumination and energy• Biophotonics and medical engineering• Manufacturing technology for optics• Imaging• Integrated Photonics• Laser systems for industrial productionengineering• Lasers & Optoelectronics• Optics• Optical information and communication• Sensors, test and measurement and opticalmeasurement systems• Security
All conference registrants will have free entrance
to the technical exhibition and World of Quantum. Longer lunch breaks are organized to allow
visits to the exhibition.
This combination of theory and practice, an
extensive program of conferences and related
events, and the presence of all market leaders,
decision-makers, and users make LASER Worldof PHOTONICS unique and, at the same time,the most important international informationand networking platform for the industrial, research, and development sectors.
LASER World of PHOTONICS features around
1,300 exhibitors in 5 halls (A2, A3, B1, B2, B3) andgives a complete overview of all the latest trends
and applications. The exhibition is expected to
attract over 30,000 visitors. World of QUANTUM
will take place in Hall A1.
Further information on the exhibition is available
at https://world-of-photonics.com/en/. Entry is
included in your conference ticket.

General information
will be placed in the corridor between EntranceWest and ICM.
https://www.photonics-congress.
com/en/about/conferences/

Application panels

Wifi

The application panels organized by Messe
München International are now a permanent
part of the World of Photonics congress. The series of lectures held in the forums of the LASERWorld of PHOTONICS 2023 exhibition halls
bridge the gap between science and practicalapplication. Well-known speakers from industry
and research institutes will report on the latest
industrial and medical application findings in
the sector for optical technologies and discusscurrent challenges with attendees. They will provide a comprehensive look at the latest trends
and developments.

All congress attendees with a WiFi-enabled device have free access to the Internet in special
WiFi Lounges at the Foyer of the ICM and in Hall
A1. The Internet in the lounges has an unlimited
bandwidth and download volume.

A series of application panels will be held from
Tuesday to Thursday, broken down into threemain categories:- Forum Lasers and Optics (Hall A2)- Forum Laser Materials Processing (Hall B3)- Forum Biophotonics and Medical Applications(Hall B2)

Catering
All conference attendees are invited to attend
the free coffee breaks as marked in the tables ofthe "Days at a Glance" section (first pages of theadvance program). Lunches are not included in
the conference fee.
Several gastronomy facilities are available onsite. Depending on the weather, the beer garden
outside (located between Halls A1 and B1) will
be open.

How it works:• Switch on the WiFi function on your terminal device.
• Search for wireless networks and connect to themesseWifi network.
• Start your internet browser and enter any internet address.
• The portal page of the free WiFi will appear
on screen.
• Once you have accepted the General Terms andConditions, you may access the internet.
• You only need to register one time during theentire event.

For further information, see https://world-of-photonics.com/en/supporting-program/
information/application-panels/:

In addition, attendees can use Messe München
WiFi at the fairgrounds. Availability is based on
the halls, entrances and atrium areas that are being used for the event in question. Bandwidth is
up to 4 Mbit / sec. and the download volume islimited to 200 MB per user per day.

Admission is free for all trade-fair visitors, exhibitors, and congress participants. All panels will beheld in English.

The reception quality and signal availability depend on structures, exhibits and other sources ofinterference in the halls and cannot be guaranteed.

On-site facilities for attendees

Message board

The entire programme of events at the World of
Photonics Congress is available online at:

A message board will be installed. Participants
should consult it daily for internal messages. It

Following companies offer you ATM/
cash machines:▶ Euronet
East Entrance, North Entrance, 1st floor, expressway next to Hall B4▶ IC Cash Services GmbHWest Entrance, at the Parking Garage next to
the North-West Entrance, North-East Entrance
Note: No currency exchange is available.
Banks can be found at the Riem Arcaden(three-minute walk from the West Entrance), in
the center of Munich or at the main railway station.

Besides two permanent food service operations in
the foyer - the ICM Bistro and the ICM Café - you
can also visit the restaurant Käfer am See which
can be reached directly via the 1st floor.

Taxi service

Snack bars with a large assortment of snacks andbeverages are located on the ground floor in eachhall. The snack bars in the ICM are located on the
ground floor and on the first floor.

Airport shuttle

Full-service restaurants are located on the firstfloors of the East and West entrances and above
the halls. Other self-service restaurants on thefirst floor can also be found in the exhibition
halls, offering international cuisine. Many snackbars located in the exhibition halls offer Alpine,
American, Asian, and Italian cuisine.
Visit the gastronomic guide: https://messemuenchen.de/media/projekt/pdf/service/gastroguide.pdf
Other catering options can be found at the Riem
Arcaden shopping centre located at the exit of the
Messestadt West subway station.

35

Banks

The taxi service is in front of the ICM
main entrance.

An airport shuttle operated is organized in connection with the trade fair (from Monday to
Friday) to and from Munich airport. For further
details, see https://messe-muenchen.de/en/meta/
getting-there/icm/.

First aidFirst-aid stations are located in the West and East
Entrances and on the North side of Hall C4 andare clearly marked.
Bayerisches Rotes Kreuz (BRK)
Perchtinger Straße 581379 München
Tel. +49 89 2373-282
sanitaetsdienst@brk-muenchen.de,www.brk-muenchen.de

GENERAL INFORMATION

Opening hours of the exhibition
The exhibition will be open from Tuesday
through Thursday 09:00 - 17:00 and on Friday
09:00 - 16:00.

GENERAL INFORMATION

General information
Service branch
Messegelände Eingang West, Eingang Ost und
Nordseite Halle C4
81829 München
Tel. +49 89 949-28103
Fax +49 89 949-28106

Dry cleaning

Please visit:

Die Reinigung Laundry dry cleaning is in the
Riem Arcaden shopping center. Opening hours:
Monday through Saturday 10:00-20:00.

http://www.messe-muenchen.de
http://www.icm-muenchen.de

How to reach the ICM centre

Press services

Security service/lost and found office
The Security Headquarters is located in the Administration Building by Gate 1. It is open 24
hours a day and is accessible from the inside (via
the Administration Building) and from the outside. This is also where you can claim lost items orturn in objects found at the Lost & Found office.

Pharmacy
The nearest pharmacy SaniPlus Apotheke is in
the Riem Arcaden shopping center. It is locatedon the ground floor in the right portion of thebuilding. Opening hours: Monday through Saturday 09:00-20:00.

Optician
The optician Fielmann has a retail outlet in the Riem Arcaden (Willy-Brandt-Platz 5) shopping centre. Opening hours: Monday through Saturday 10:00-20:00.

Groceries, information, travel service
They are in the Main Hall of the Entrance Westleading to Halls A1 and B1.

BY CAR
Simply follow the trade fair signs from the outskirts and throughout the city to the ICM. There
you will find parking space.

All members of the press are requested to registerwith Messe Munich. They will receive conferencematerials and badges that will admit them to alltechnical sessions and the exhibition.

BY TRAIN
The ICM is about 20 minutes from Munich central station (Hauptbahnhof) by underground U2,
exit "Messestadt West." The U2 subway runs from
4:04 in the morning to 1:24 after midnight. Further information on the underground is available
at the information counters on the
trade fair grounds or at:

Cloakroom
For congress attendees, a cloakroom is located on
the intermediate level of the ICM. In addition, acloakroom is located on the lower levels of theWest Entrance. As a rule, it opens one hour before
the exhibition begins and closes one hour after
the exhibition ends.

http://www.mvv-muenchen.deNote for smokers

BY U-BAHN FROM THE AIRPORTAt Munich airport, the station for urban railway
lines S1 and S8 is directly below the central area.
Trains in the direction of the city center run at
10-minute intervals. There are two routes fromthe airport to the ICM:

Smoking in the ICM is forbidden. Smoking on the
grounds of the exhibition space is only permitted
in designated smoking areas outside the halls.

All services
https://messe-muenchen.de/en/
services/trade-fair-participation/
trade-fair-services/service-types/
services-for-visitors.php

Post office

Conference venue

Deutsche Post has a branch office in the Riem
Arcaden shopping center (EDEKA Uhlig, WillyBrandt-Platz 5). Opening hours: Monday throughSaturday 10:00-20:00.

CLEO®/Europe-EQEC 2023 will take place at the:New Munich Trade Fair Centreat the ICM International Congress Centre Am Messesee 6,81829 Munich, Germany

▶

▶

36

Route S1/U2:
S 1 from the airport to Feldmoching station or
Munich Central Station (Hauptbahnhof).
Change to underground U2 that takes you directly to the ICM - Messestadt West.
Route S8/U2:
S 8 from the airport to Munich central station (Hauptbahnhof).
Change to underground U2 that takes you directly to the ICM - Messestadt West.

BY TAXI FROM THE AIRPORTThe fixed price for a single taxi journey to theexhibition center is €85. The one-way journey
will take around 35 minutes. Numerous taxis
are available at the airport directly in front of
the terminals
BY RENTAL CAR FROM THE AIRPORTAll the major car rental firms are represented at
Munich airport. The car rental center with its own
parking facilities is in front of module A, to thenorth of car park P6.
Please take the following route:▶ From Munich Airport, follow the signs "Messe/
ICM" on the A92 in the direction of Munich tothe motorway General Information intersection Eching/Neufahrn.
▶ Then take the A9 in the direction of Munich
to the motorway intersection München-Nord.
▶ Continue on the motorway ring road A99 in
the direction of Salzburg to the motorway intersection München-Ost.
▶ Then take the A94 in the direction of Munich to
the exit Feldkirchen-West or München-Riem.
The journey takes about 35 minutes, dependingon the volume of traffic.
TAXI FROM THE ICM CENTRE TO
THE AIRPORT
You will find taxi ranks at all trade fair entrances and in front of the ICM going to the airport(Central Building).
AIRPORT SHUTTLE
An airport shuttle operated by Autobus Oberbayern is organized in connection with thetrade fair (from Monday to Friday) to andfrom Munich airport. The bus departs several times per hour. There is convenient online
ticketing at:

General information

There are two departure points at Munich Airport: Terminal 2 (bus park) and the Central Concourse (MAC). Please follow the signs.
When arriving from Munich Exhibition Centre,
buses stop exclusively at the Central Concourse(MAC), from where both terminals are just a few
minutes' walk away.
At Munich Exhibition Centre, buses arrive at thestop closest to the North, East or West entrance.
Please refer to the timetable for the exact departure and arrival points.
Here you can find all the times of the bus shuttle:
https://www.airport-messe-shutt le.c om/ams/te as er bi lder/
mm23_shuttle_airport-messe_
v2_januar.pdf

European Physical Society
6 rue des Frères Lumière
68200 Mulhouse
FranceApplications for the student rates must include
a copy of an official student identity card, whichmust also be presented on-site when collecting
registration materials.

This program is edited by Patricia Helfenstein andAndré Wobst.

The full week registration fee for the meeting
includes admission to all CLEO®/Europe-EQEC
2023 technical sessions, as well as to those of allconferences co-located with the congress. Coffee
during the coffee breaks (as marked in the days
at a glance) is included. Lunches and tickets for
public transportation are not included in the fees.

Hotel information
The International Congress Centre (ICM) is located about 20 minutes from the Munich Central
Station (Hauptbahnhof) by underground U2, exit
Messestadt West. Whether you are looking for a
hotel, a guesthouse, a private accommodation, ora boarding house, you should be able to find youraccommodation downtown or in the surrounding area of Munich.

One-day registration fees are available for thosewishing to attend one session rather than thewhole conference. Coffee during the coffee breaks(as marked in the days at a glance) is included.
Lunches and tickets for public transportation are
not included in the fees.

The bus runs every 30 minutes. One way journey
costs €11.00, return ticket costs €17.00.

One-day registration tickets are activated on
the day the participant goes through the electronic gates of the congress or the fair and will
only be valid for that day.

Conference registration

Cancellation policy

CONFERENCE REGISTRATION FEES
• EPS, Optica, IEEE Member, Full week registration €750
• Non-Member, Full week registration €900
• Student Member, Full week registration €290
• Student Non-Member, Full week registration€320• One-day registration €370
• Dinner ticket per conference participant €20• Dinner ticket per accompanying guest €35

All requests for refunds must be received in writing by Thursday, 8 June 2023. A € 50.00 service
charge will be assessed for processing refunds. Requests for refunds are to be sent to conferences@
eps.org. All registrations received after Thursday;
8 June 2023 are non-refundable.

Messe Munich has arranged for an online hotel
reservation which can be used for the CLEO/
Europe-EQEC 2023 participants:
https://tradefairs.com/en/
LASER%20World%20of%20
PHOTONICS/2023
The hotel guide of the Munich Trade Fairs offers
you a large variety of accommodation possibilities for a pleasant stay. Whether near the ICM or
centrally located and in the middle of the nightlifeof Munich's trendy neighbourhoods or close to
the mountains with a high recreation value - here
you will find a comprehensive offer of accommodation in and around Munich as well as in thealpine upland - meeting your personal criteria.

Language

Hotels can be directly searched and booked via
the hotel directory. A larger variety of rooms canEnglish is the official language of the conferences.

37

be found using the link of the Tourism office:https://www.muenchen.de/en/
accomodation-hotels
Hotels, pensions, apartments, or youth hostels in
Munich can also be found at:https://www.euro-youth-hotel.
de/enhttps://www.hostelworld.com
Considering the large number of attendants tothe exhibition, running in conjunction with theconference, we recommend making your hotel
reservation as soon as possible.

Transportation in munich
Munich offers very good transportation means(hire cars, trams, metro, and buses).
Participants of the World of Photonics congress
who use local public transportation (MVV) to get
to Neue Messe Munich must buy a travel ticketat their own expense.
The Single Ticket is ideal for spontaneous journeys with the MVV – and it is even cheaper
when bought at a ticket machine by cashless
payment. If you're planning more than 2 trips
in the Munich city area per day, we recommend
purchasing the Day Ticket. It can be used within
the selected area of validity for as many trips as
you like on one day.

GENERAL INFORMATION

https://www.airport-messe-shuttle.com/en

Conference management• Additional cost per Short Course, Student €160
• Additional cost per Short Course, Non-Student €260

General information

GENERAL INFORMATIONThe AirportPLUS-Ticket is a day ticket which
includes the journey to/from the airport and thecity area of Munich (validity zone M - 6). The
AirportPLUS-Ticket is available as a single ticket
or as a group ticket for up to 5 people.
Ticket machines are located at the stops/stations,in trams and on buses within the MVV network.
The machines understand several languages. Just
select your flag. Some ticket machines accept 10€ and 20 € banknotes, and most will give change.
Please have some small coins ready. Online tickets
and mobile tickets can now also be purchased.
Buy your ticket depending on the zones you willcross and the time length you will need to travel:▶ Stripe ticket (Streifenkarte):Stamp two stripes per zone. You are allowed tochange and interrupt your journey. Return andround trips are not permitted.
▶ Single trip ticket:
Valid for one person for one trip. You are allowed
to change and interrupt your journey. Returnand round trips are not permitted. The fare depends on the number of zones passed through.
▶ Single day ticket (Tageskarte):
The most popular day tickets are also available
as excellent value-for-money 3-day tickets. If you
want to stay for 2 days, 4 days, or even longer, simply combine the 1-day ticket and 3-day tickets.
▶ Partner day ticket:
Available for as many trips as you like for up to
five adults together.
Before buying a day ticket you decide which validity it should have. The MVV area is valid for
all ticket offers in tariff zones divided:▶ The M-Zone encompasses the entire city of
Munich and in part extends beyond it▶ The Zones 1 - 6 comprise the interconnecteddistricts belonging to the MVV area▶

 unich Airport is in Zone 5
MMesse Munich is in Zone M▶ On the network plans, each stop is also marked
with the corresponding zone

the nearby Bavarian Alps, fairy-tale castle of Neuschwanstein, or the beautiful Tegernsee.

It can be reached by all S-Bahn trains and U-Bahnlines 3/6 to Marienplatz.

Munich's famous places

ONLY VALID WITH A STAMPYour Single Trip Tickets, Stripe Tickets and Day
Tickets must be stamped prior to the start of yourjourney. These tickets only become valid for travel
once they have been validated in this way at the
ticket machines provided for this purpose.

In June, the weather is likely to be warm with plenty of sunshine, although some rainfall is possible.
Munich boasts an outstanding public transportation system, and the modern Münchner Messe
complex, where CLEO®/Europe-EQEC 2023 andall Laser 2023 events will be held, is easily accessible
from the airport, city center, and various parts ofthe city through U-Bahn and S-Bahn lines.

▶

Munich's churches

VALIDATED AUTOMATICALLY
You can buy most tickets in advance so that you
have a ready supply. However, please note thatsome tickets are already validated at the timeof purchase:▶ Single Trip and Day Tickets bought at ticket
machines in trams, metro buses and city busesin Munich▶ Single Trip and Day Tickets bought from theelectronic ticket printers in MVV regional buses▶ Airport-City Day Tickets

Munich is well-known for its many churches, including:More information can be found at:

Frauenkirche (Church of Our Lady)
Frauenplatz 1, Munich
Opening hours: 07:00-20:00.
It can be reached by all S-Bahn trains and U-Bahnlines 3/6 to Marienplatz.

https://www.mvv-muenchen.de/en/index.html

Munich, Germany

Alter Peter (Church of St. Peter)
Rindermarkt 1, Munich
Climb the 299 steps of this parish church to enjoy
a beautiful view of the Munich city center.
Opening hours: 7:30-19:00.
It can be reached by all S-Bahn trains and U-Bahnlines 3/6 to Marienplatz.

The celebrated capital of Bavaria, located in thefoothills of the Alps, is one of the major cities in
Europe. The city, with its 1.4 million inhabitants, isrenowned for its vibrant science and industry environment. Munich offers fantastic opportunities
for shopping, museums, theaters, art galleries, andsightseeing. Its October beer festival is world-famous. Tourist attractions include the Bavarianbeer and South German cuisine tradition, as wellas numerous half-day or one-day excursions to

Heiliggeistkirche
Prälat-Miller-Weg 1, Munich
Opening hours: 09:00-20:00.

38

Marienplatz
The Marienplatz is named after the columnof the Virgin Mary at its center. The place
is famous for its carillon in the New Town
Hall Tower, the largest carillon in Germany.
It features near-lifesize figures performing
the traditional Coopers' Dance and a jousting
match. The Marienplatz is a central place forthe city's Founding Festival, Fasching (carnival) celebrations, and the popular Christmas
market. Major restaurants, cafes, and shops
are in this area. Please note that shops areclosed on Sundays.
Königsplatz
This Neo-Classical square, commissioned by
Ludwig I, features the Propyläen gateway and the
Glyptothek, a small but enchanting collection of
Greek and Roman sculpture. It hosts an annual
summer outdoor concert series.
Isartor (Isar Gate)
The most easterly of Munich's three remaining
town gates, dating from the 14th century. Careful
restoration has recreated its original dimensions
and appearance. The Isar Gate accommodates the
Valentin Museum.

General information

Sendlinger Tor (Sendlinger Gate)
Remaining towers of southerly fortifications fromthe 14th century.

Beer gardens
Nothing defines Munich more than its beer. You
cannot talk about Munich without mentioning
its beer culture. Today, the Munich breweries dispense 123 million gallons of beer annually, which
is why many beer gardens are located throughout
the city:
Augustiner-Bräustuben, Landsberger Straße 19
A large beer hall and restaurant, Augustiner-Bräustuben is one of those off-the-beatentrack places that’s well worth the detour. Full ofBavarian charm, this beer hall has a warminginterior, with high, amber ceilings and a stylishbar, adorned with copper and dark wood. Bestof all is its jovial atmosphere, and the air is often
bustling with loud German conversations, thehoppy smell of locally brewed Augustiner and, if
you’re lucky, an eruption of traditional singing.
Löwenbräukeller, Nymphenburger Strasse 2
The CLEO®/Europe-EQEC conference dinner
will take place here on Wednesday, 28 June 2023.
Home to another locally brewed beer, Löwenbräu,
the Löwenbräukeller is a beloved beer hall, restaurant and beer garden. Known for its regular
Bavarian music performances and traditional
dances and events, it’s a popular watering holeand restaurant. The large building also includes
roof terraces, ideal for overlooking the nearby,

https://www.muenchen.de/en/
events/theater-dance-operas/
find-english-speaking-theatres-munich-here
Munich is very famous for its theaters, but also
for its Olympic Park, located at Spiridon-Louis-Ring 21.
Getting there: U-Bahn line 3 to
Olympiazentrum. see:lively beer garden, which is popular during thewarmer months.
Hirschgarten, Hirschgarten 1
Located in the park that bears the same name,
Hirschgarten beer garden and restaurant is where
the locals and in-the-know visitors flock to during warmer months. With an impressive 8,000
seats, it’s the largest beer garden in Bavaria andsurrounded by greenery and lush lawns. Offeringa menu of international and Bavarian treats, aswell as huge, cold beers and a lively atmosphere,
it’s a great spot to enjoy traditional treats.

https://www.olympiapark.de/en
Munich is blessed with beautiful parks and serene
lakes, offering tranquil escapes within the bustlingcity. The English Garden, one of the largest urban
parks in the world, invites relaxation and leisurely
strolls. The shimmering waters of Lake Starnberg
and Lake Ammersee beckon visitors with their
picturesque landscapes and recreational activities.

Munich's museums

Augustiner Keller, Arnulfstraße 52
Augustiner Keller is a central, popular beer hall,
complete with a large, traditional interior and alively garden. The restaurant-pub boasts an impressive wooden ceiling, finely polished tables,
hand-crafted timber chairs and a large stage areaadorned with rows of curious hunting trophies.
The menu features fantastic baked pretzels, perfectly roasted ribs, and high-quality, local Augustiner brews.

Munich boasts a diverse array of museums, fromthe historic Bayerisches Nationalmuseum to themodern BMW Museum. Explore art, history,
and science:• Bayerisches Nationalmuseum• BMW Museum• Deutsches Museum• Deutsches Museum Flugwerft Schleißheim
• Glyptothek• Münchner Stadtmuseum

Munich’s theaters and parks
Munich's vibrant theater scene captivates audiences with its world-class performances. From the
grandeur of the National Theatre to the experimental productions at the Residenztheater, there's
something for every taste. Immerse yourself inthe city's rich cultural heritage and indulge in
unforgettable theatrical experiences in Munich:• Neue Pinakothek• Villa Stuck
And many others, see:https://www.muenchen.de/en/sights/museums

Hop on-hop off buses
In the double-decker buses of City Sightseeing, visitors to Munich can enjoy the open roof. During
the hour-long city round trips, participants havea view of the best attractions that Munich offers.
Explanations are given in eight different languages. Highlights and stops include the historic city
center, the Main Station, Odeonsplatz, the Opera,
Maximilian Street, the Food Market, Stachu, thePinakotheken, Nymphenburg Castle, Neuhausen,
Olympia Park, Schwabing, the English Garden,and Haidhausen.
Three tours are available that can be combined:• City-Tour• Nymphenburg-Olympia-Tour• Schwabing-TourThe tickets can also be used flexibly. They canbe purchased online in advance (with a pricereduction) or in the bus and are valid for one
or even two days. The departures of all the tours
start at the 'Bahnhofsplatz outside Elisenhof near
the main railway station Munich. For further information, see:https://www.citysightseeing-munich.com
Further information on Munich(available in 6 languages) is available at:
http://www.muenchen.de

39

GENERAL INFORMATION

Karlstor (Charles' Gate)
A westerly town gate from the 14th century. It wasincorporated into the square known as "Stachus"(officially Karlsplatz) at the end of the 19th century. Today, it marks one end of Munich's primarypedestrian zone.

Technical Programme

GENERAL INFORMATIONSHORT COURSES
CLEO®/Europe EQEC 2023 will present ten
short courses at an extra cost to be presented inparallel on Monday, Wednesday, Thursday andFriday. Each course is scheduled in two parts:
Course Part I (1 hour 30 minutes), coffee break(30 minutes), Course Part II (1 hour 30 minutes). The courses are open to attendees of theWorld of Photonics Congress and Laser Worldof Photonics exhibition, subject to payment of
the course fee. The short course material will
only be available online.

Wednesday Morning, June 28, 2023,
Room 2, Hall B1 (B12), 8:30 - 12:00

Thursday Afternoon, June 29, 2023,
Room 2, HALL B1 (B12), 14:00 - 17:30▶

▶

SH-1 Short course: High-power fiber lasers

SH-5 Short course: Mid-infrared
semiconductor lasers

Andy Clarkson, University of Southampton,
United Kingdom

Jérôme Faist, ETH Zurich, Switzerland

Wednesday Morning, June 28, 2023,
Room 5, Hall B2 (B22), 8:30 - 12:00

Thursday Afternoon, June 29, 2023,
Room 5, HALL B2 (B22), 14:00 - 17:30▶

▶

SH-9 Short course: Silicon photonics

SH-6 Short course: THz measurements
and their applications

Dries Van Thourhout, Ghent University, Belgium

Daniel Mittleman, Brown University,
Providence, Rhode Island, USA

Wednesday Afternoon, June 28, 2023,
Room 2, HALL B1 (B12), 14:00 - 17:30▶

The courses are designed for engineers, scientists, and graduate students with a basic understanding of optics and photonics, aiming
to enhance their knowledge in specific technical domains.
The 2023 Short course topics include:
High-Power Fiber Lasers, Optical Parametric
Oscillators, Laser Beam Analysis, Propagation and Spatial Shaping Techniques, Practical
Quantum Optics, Mid-infrared semiconductor lasers, Terahertz Measurements and their
Applications, Nonlinear Crystal optics, Frequency Combs and Applications, Silicon Photonics and Finite Element Modelling Methods
for Photonics.

Friday Afternoon, June 30, 2023,
Room 12b, ICM, 14:00 - 17:30▶

SH-7 Short course: Nonlinear crystal opticsBenoît Boulanger, Institute Néel-CNRS,
Grenoble, France

SH-10 Short course: Finite element modelling
methods for photonics

Wednesday Afternoon, June 28, 2023,
Room 5, HALL B2 (B22), 14:00 - 17:30

Arti Agrawal, University of Technology
Sydney, Australia▶

SH-8 Short course: Frequency combs principles
and applications

Further Short Course information, see:https://www.cleoeurope.org/short-courses/

Thomas Udem, Max Planck Institute of
Quantum Optics, Garching, Germany

Thursday Morning, June 29, 2023,
Room 2, HALL B1 (B12), 8:30 - 12:00▶

SH-2 Short course: Optical parametric oscillators

Short Course Schedule

Majid Ebrahim-Zadeh, ICFO,
Castelldefels, Spain

Monday Morning, June 26, 2023,
Room 2, Hall B1 (B12), 8:30 - 12:00▶

SH-3 Short course: Laser beam analysis,
propagation, and spatial Shaping techniques

SH-4 Short course: Practical quantum optics

James Leger, University of Minnesota,
Minneapolis, USA

Gerd Leuchs, Max Planck Institute for the
Science of Light, Erlangen, Germany▶

Thursday Morning, June 29, 2023,
Room 5, HALL B2 (B22), 8:30 - 12:00

40

NOTES

Technical Programme

CLEO®/Europe 2023 Plenary Speaker▶

Monday, 16:00 - 17:30
Location: Room 1 ICM

PL-1

MON 16:00

From nonlinear optics to high-intensity
laser physics
Donna Strickland,
University of Waterloo,
Ontario, Canada
Co-laureate of Nobel
Prize in Physics in 2018
for the work on chirped
pulse amplification
Biography
Donna Strickland is a professor in the Department of Physics and Astronomy at the
University of Waterloo and is one of the recipients of the Nobel Prize in Physics 2018
for developing chirped pulse amplification
with Gérard Mourou, her PhD supervisor at
the time. They published this Nobel-winningresearch in 1985 when Strickland was a PhD
student at the University of Rochester.
Strickland earned a B.Eng. from McMaster
University and a PhD in optics from the University of Rochester. Strickland was a research
associate at the National Research Council
Canada, a physicist at Lawrence Livermore
National Laboratory and a member of technical staff at Princeton University. In 1997,
she joined the University of Waterloo, where
her ultrafast laser group develops high-intensity laser systems for nonlinear optics

investigations. She was named a 2021 Hagler
Fellow of Texas A&M University and sits on
the Growth Technology Advisory Board ofApplied Materials.
Strickland served as the president of the Optica (formerly OSA) in 2013 and is a fellow
of Optica, SPIE, the Royal Society of Canada
and the Royal Society. She is an honorary fellow of the Canadian Academy of Engineeringand the Institute of Physics, an international
member of the US National Academy of Science and member of the Pontifical Academy of
Science. Strickland was named a Companionof the Order of Canada.

PL-2a

Photonic machines for large-scale
applications and fundamental physics

Claudio Conti,
Department of Physics,
University Sapienza, Italy
Biography
Claudio Conti is an associate professor at the
Department of Physics of the University Sapienza
in Rome. He was the director of the Institute ofComplex Systems of the Italian National ResearchCouncil (ISC-CNR). Previously, he received the
New Talent Grant from the Research Center Enrico Fermi and held a Humboldt fellowship at
the Max Planck Institute for the Science of Light.
Claudio Conti was the Principal Investigator of
the European Research Council Grant "Light andComplexity" and the Principal Investigator of the
Templeton Foundation Grant "Generalized Uncertainty Principle and the Photon."
Claudio Conti is a prolific author with over 250
articles published in renowned journals; hecontributed to many events, delivering over 50
invited talks. His research interests encompass
complex systems, machine learning, photonics,
and nonlinear optics, leading to applications suchas Ising machines and fundamental tests of quantum mechanics.

Abstract
The laser increased the intensity of lightthat can be generated by orders of magnitude and thus brought about nonlinear optical interactions with matter. Chirped pulse
amplification, also known as CPA, changed
the intensity level by a few more orders ofmagnitude and helped usher in a new typeof laser-matter interaction that is referred toas high-intensity laser physics. In this talk, I
will discuss the differences between nonlinear optics and high-intensity laser physics.
The development of CPA and why short, intense laser pulses can cut transparent material will also be included. I will also discuss
future applications.
The plenary talk will be followed by a career
event with Donna Strickland (Monday, 17:30- 18:30, Room 4a ICM).

EQEC 2023 Plenary SpeakerC

TUE 10:30

Abstract
Which is the simplest way to process information
with light? If we use integrated optics, we needhighly optimized fabrication steps for devices with

Tuesday, 10:30 - 11:30
Location: Room 1 ICM

41

many channels. If we use wavelength multiplexing,
we need sophisticated modulators and expensive
filters. But optics deals with beams of light, andthere is no potential limit to the information density we can store in a beam of light. So, we canuse holograms to exploit the three-dimensional
information and demonstrate demanding computational tasks as natural language processing.
The EQEC plenary talk will be followed by
the Award ceremony (Tuesday, 11:30 - 12:30,
Room 1 ICM).

Opening and World of
Photonics Plenary Session
C

Tuesday, 14:00 - 15:30
Location: Room 1 ICM

PL-3

TUE 14:00

Laser-driven inertial confinement fusion,
power source of the future?

Tammy Ma,
Lawrence Livermore
National Laboratory,
Livermore, CA, USA

Constantin
L. Haefner, Institutefor Laser Technology,
Aachen, Germany

TECHNICAL PROGRAMMEPLENARY TALKSTechnical Programme
Abstract
Fusion ignition has been achieved at the National Ignition Facility (NIF) at Lawrence Livermore National Laboratory. This experimental
result, decades in the making, is a major scientific breakthrough for laser-driven inertial
confinement fusion. This talk will present theexperimental results and the many technological innovations that made this achievement
possible, including advances in photonics. It
will also place this achievement in the broader
context of its significance to the scientific community. The implications of this achievement
for future research in laser inertial confinement
fusion as a sustainable and safe source of clean
energy will also be discussed.

CH-5

WED 08:30

Microcombs for Optical Communications

TUE 16:00

Tuesday, 16:00 - 17:30
Location: Room 6 Hall B3 (B32)

Claus Ropers,
Max Planck Institutefor Multidisciplinary
Sciences, Göttingen,Germany

CA-7

WED 14:00

Power scaling▶

Wednesday, 14:00 - 15:30
Location: Room 13a ICM

CH-5.1
Optical frequency comb
applications beyond frequency
metrology using versatile control
of optical waves

Andreas Tuennermann,
Fraunhofer Institutefor Applied Optics andPrecision Engineering
IOF, Jena, Germany

Optical frequency comb provides powerful tools in broad area using its versatilephase controllability. In this tutorial, ourrecent works on various metrology applications such as highly functional spectroscopy, quantum optics, and imaging arepresented.
CI-2

CG-2.1Frequency combs

Quantum-coherent Electron-LightInteractions in Electron Microscopy▶

Monday, 14:00 - 15:30

Location: Room 8 Hall A1 (A12)This tutorial will give an overview of the enabling
characteristics of microcombs in wavelength division multiplexing and coherent communication systems.

Kaoru Minoshima,
The University ofElectro-Communications,
Chofu, Japan

Ultrafast physics in condensed matter

TECHNICAL PROGRAMME▶

Victor Torres Company,
Chalmers University ofTechnology, Gothenburg

Wednesday, 8:30 - 10:00
Location: Room 14b ICM▶

MON 14:00

Quantum optics I

CI-2.1

CLEO®/Europe Tutorial Talks

▶

EB-3

Optical frequency combs

TUTORIAL TALKS

CG-2

EQEC Tutorial Talks

This tutorial will introduce principles andapplications of electron-light scattering inelectron microscopy. An emphasis will beplaced on quantum-coherent processes andrecent studies of spontaneous and stimulated interactions of free-electron beams withphotonic cavities.

Maciej Lewenstein,
Instituto deCiencias Fotónicas,
Castelldefels, Spain
EB-3.3
Attosecond Sciences, Quantum Optics
and Quantum Information
In my tutorial I will discuss recent developments of attosecond science on the border between ultrafast laser science, quantum optics
and quantum information.
ED-4

TUE 08:30

Cavity-Enhanced Precision Spectroscopy▶

Tuesday, 8:30 - 10:00
Location: Room 2 Hall B1 (B12)CA-7.1
Prospects in power scaling of fiber lasers
and amplifiers
The state of the art of science and technology infiber lasers and amplifiers is reviewed. The prospects for future developments using advanced
fiber designs in combination with modern laser
and amplifier architectures are discussed.

WED 10:30

Wednesday, 10:30 - 12:00
Location: Room 6 Hall B3 (B32)

42

Shui-Ming Hu,
University of Science andTechnology of China,
Hefei, China

Technical Programmefrequency combs, frequency agile
lasers to Erbium amplifiers on chip

Cavity-Enhanced Precision
Spectroscopy of Molecules

CLEO®/Europe Keynote Talks

Cavity-enhanced spectroscopy methods induce km-long molecule-light interaction path
lengths and provide kW-power laser fields,
which allow for high-precision spectroscopy
of molecules, with broad applications in fundamental physics and beyond.
EF-1

CF-1

WED 08:30

Advances in attosecond
technology and high orderharmonic generation I▶

Anatoly Zayats, King's
College London, London,
United Kingdom

Monday, 8:30 - 10:00
Location: Room 1 Hall B1 (B11)

CC-2

WED 14:00

Complex fiber dynamics I▶

Wednesday, 14:00 - 15:30
Location: Room Osterseen ICM

EF-1.1
Nonlinear Multimode Fiber Optics
This tutorial will present an overview of recent research progress in the field of nonlinear
multimode fiber optics. Phenomena such as
multimode solitons, geometric parametric instability and beam self-cleaning lead to newtechnological applications.

High power THz sources

Nonlinear Optics with Nanoparticles
and Metamaterials▶

Thursday, 14:00 - 15:30

Location: Room 1 Hall B1 (B11)

Clara Saraceno, Samira
Mansourzadeh, Tim
Vogel, Celia Millon,
Mohsen Khalili, Ruhr
University Bochum,
Bochum, Germany

CF-1.1
CB-6

Ultrafast attosecond and few-fs
sources for control of molecular
reactivity at the electron
time scale▶

Wednesday, 14:00 - 15:30
Location: Room 13b ICM

CC-2.1High power ultrafast moves
into the Terahertz domain
We discuss latest advances in high average
power laser driven THz sources, discuss limitations and present future applications.

Tobias J. Kippenberg,
EPFL, Lausanne,
Switzerland

WED 08:30

Plasmonic structures and components▶

WED 14:00

Integrated photonics and frequency combs

Attosecond science offers formidable tools
for investigating electronic processes. An
overview on developments for compact
few-femtosecond UV and attosecond VUVsoft-x ray sources, together with their application for studying charge migration inchiral molecules, is presented.
CK-2

THU 14:00

CK-2.1

Weak nonlinearity of conventional materials
can be enhanced by their nanostructuring. We
will overview recent developments and trends
in engineering spectral and temporal responseof coherent and incoherent optical nonlinearities with dielectric, plasmonic and hybrid nanoparticles, nanostructures and metamaterials.

Francesca Calegari,
CFEL-DESY,
Hamburg, Germany

Stefan Wabnitz,
Sapienza Universityof Rome, Rome

Recent advances allowed to create ultra-lowloss, meter-long waveguides in silicon nitride.
I will review advances of this technology, fromchipscale frequency combs, parametric amplifiers, ultra-narrow linewidth lasers with fiber
laser-coherence, and erbium amplifiers on chip.

CB-6.1

Tuesday, 8:30 - 10:00
Location: Room 4a ICM

Ultra-low loss hybrid silicon nitride
integrated photonics: from chipscale

43

EQEC Keynote Talks
EJ-1
Simulating multi-mode
and non-hermitian systems▶

Monday, 8:30 - 10:00
Location: Room 4a ICM

MON 08:30

TECHNICAL PROGRAMMEKEYNOTE TALKS

ED-4.3

Technical Programme
Max Planck Institute for the Science of Light,
Erlangen, Germany
5
Friedrich-Alexander-Universität,
Erlangen, Germany

A new generation of semiconductor nanolasers with ultralow thresholds and important applications in integrated photonics is
emerging. The talk gives an overview of recent experimental and theoretical progress,
highlighting the interesting physics andnew opportunities.
Kestutis Staliunas,
UPC, Barcelona, Spain

ED-1

Laser transverse patterns control
by nonhermitian actions▶

MON 08:30

TECHNICAL PROGRAMME

Monday, 8:30 - 10:00
Location: Room 4b ICM
Jesper Moerk, Yi Yu,
Evangelos Dimopoulos,
Meng Xiong, Marco
Saldutti, Gaoneng Dong,
Matias BundgaardNielsen, KristianSeegert, Shih Lun Liang,
Elizaveta Semenova,
Kresten Yvind, Technical
University of Denmark,Kgs. Lyngby, Denmark

Semiconductor Nanolasers

MON 08:30
EF-4.1

Physics and Application of Complex Lasers
A complex laser supports many spatio-temporalmodes that interact nonlinearly with the gainmaterial. We have controlled spatio-temporal
dynamics of many-mode lasers and applied themto speckle-free imaging, holography and parallel
ultrafast random number generation.

Vitaly Wirthl, Derya
Taray, Omer Amit, Akira
Ozawa, Fabian Schmid,
Jorge Moreno, Johannes
Weitenberg, Theodor
Hänsch, Thomas Udem,
Max-Planck Instituteof Quantum Optics,
Garching, Germany

Nanoantennas and nanoconfinement

EG-1.1

Hui Cao, Yale University,
New Haven, USA

Monday, 8:30 - 10:00
Location: Room 6 Hall B3 (B32)

The classical spatial pattern formation theory
optical vortices, spatial solitons, optical turbulence in broad area lasers will be revised. New
mechanisms of pattern control, in particular the
turbulence control by nonhermitian background
potentials, will be presented.

▶

EA-6.1

Precision spectroscopy
for fundamental scienceEJ-1.1

EG-1

4

Imaging at the single-photon limit using
homodyne detection
Using homodyne detection, we obtain images
in the short-wave infrared region of the spectrum with an illumination flux of order one
photon per image pixel despite the camera
having a noise floor one to two order of magnitude higher.

Ultrafast processes in ionised media▶

EA-6

FRI 08:30

FRI 08:30

EE-2

Friday, 8:30 - 10:00
Location: Room 14c ICM

Quantum optics in imaging▶

Friday, 8:30 - 10:00
Location: Room 3 ICM

ED-1.3
Laser Spectroscopy as a Probe for Physics
Beyond the Standard Model

Osian Wolley1,
Simon Mekhail1,
Paul-Antonie Moreau2,3,
Thomas Gregory1,
Graham Gibson1,
Gerd Leuchs4,5,
Miles Padgett1

Precision spectroscopy of atomic hydrogen andother simple atomic systems is required for testing
quantum electrodynamics, the determination of
fundamental constants and to probe for physics
beyond the Standard Model.
EF-4

University of Glasgow, Glasgow,
United Kingdom
2
National Cheng Kung University, Tainan
City, Taiwan,
3
Center for Quantum Frontiers of Research andTechnology, Tainan City, Taiwan
1

THU 10:30

Spatiotemporal effects
in optical systems▶

Thursday, 10:30 - 12:00
Location: Room 14a ICM

44

Stefan Skupin,
Université de Lyon,
Villeurbanne, FranceEE-2.1
Air Photonics
Interactions of ionizing ultrashort laser pulses in ambient air are frequently exploited in
nonlinear photonics. We review major applications ranging from femtosecond filamentation and pulse compression to broadband
THz generation and describe challenges
and trends.

Technical Programme

Below you will find the invited speakers’ programme indicating on which day and time theinvited talk will begin. In order to not disturb
the session, attendees wishing to participate arerequested to respect the session times to attend
these talks, as follows: From 08:30 to 10:00, from10:30 to 12:00, from 14:00 to 15:30 or from 16:00
to 17:30.

EB-1.1

Quantum state engineering ofmacroscopic oscillators
Eugene S. Polzik, Copenhagen University,
Copenhagen, Denmark

Monday sessions from 10:30 to 12:00
EJ-2.1

Monday, 10:30, Room 4a ICM

Monday sessions from 08:30 to 10:00

Exploring interacting photons
and quantum states of light withatomic metasurfaces

CA-1.4

Thomas Pohl, Department of Physics andAstronomy, Aarhus, Denmark

Monday, 9:15, Room 13a ICM

Broadband direct frequency downconversion to wavelengths beyond 5 µm
using wide-gap non-oxide crystals
Zsuzsanna Heiner, Humboldt-Universität,
Berlin, Germany
CB-1.1

Monday, 8:30, Room 13b ICM

Recent progress of photonic-crystal
surface-emitting lasers
Susumu Noda, Kyoto University,
Kyoto, Japan

Sánchez -Soto1,6, Joel F. Corney7,
Gerd Leuchs1,3, Alexey V. Andrianov4
1
Max Planck Institute for the Science of Light,
Erlangen, Germany
2
Friedrich-Alexander-Universität,
Erlangen, Germany
3
University of Ottawa, Ottawa, Canada
4
Russian Academy of Sciences, Nizhny
Novgorod, Russia
5
Lobachevsky State University of Nizhny
Novgorod, Nizhny Novgorod, Russia
6
Universidad Complutense, Madrid, Spain
7
University of Queensland, Brisbane, Australia

Monday, 8:30, Room 8 Hall A1 (A12)CA-2.1EG-2.3

Humeyra Caglayan, Rakesh Dhama, Tampere
University, Tampere, Finland

Towards few-optical-cycle generation fromThulium / Holmium mode-locked lasers
Valentin Petrov, Weidong Chen, Li Wang,
Yongguang Zhao, Zhongben Pan, Uwe
Griebner, Max Born Institute, Berlin, Germany

Liquid crystals meet strong-field physics:
first attempts of HHG in soft matter
Luise Becker1, Andrea Annunziata2,3, Patrick
Friebel1, Davide Faccialà3, Caterina Vozzi3,
Laura Cattaneo1
1
Max Planck Institute for Nuclear Physics,
Heidelberg, Germany
2
Politecnico di Milano, Milan, Italy
3
Institute for Photonics and Nanotechnologies,
Milan, Italy

JSII-2.1 Monday, 10:30, Room Osterseen ICM
Fibre transitions for astronomical applications

Yong Zhang, Nanjing University,
Nanjing, China
JSII-1.1 Monday, 8:30, Room Osterseen ICM

EB-2.1 Monday, 10:30, Room 8 Hall A1 (A12)

Why Photonic Technologies are Beneficial
to Astronomical Instrumentation

Applying Kerr Squeezed Light
to InterferometryCA-3.1

Sylvain Veilleux, University of Maryland,College Park, USA

Nikolay Kalinin1,2,4, Thomas Dirmeier1,2, Arseny
A. Sorokin4, Elena A. Anashkina4,5, Luis L.

Low-Phonon-Energy Rare-Earth doped
Laser Gain Materials: Crystals vs. Glasses

Monday, 8:30, Room 14a ICM

Nonlinear optics in 3D χ(2) structures

Monday, 14:00, Room 14a ICM

Nonlinear Photonics with Lithium Niobate
Marko Loncar, Harvard University, Cambridge, USA
JSII-3.1 Monday, 14:00, Room Osterseen ICM
What it takes to observe exoplanetswith optical interferometry
Sylvestre Lacour, Observatoire de Paris,
Meudon, France

CF-2.5 Monday, 11:30, Room 1 Hall B1 (B11)

Kerrianne Harrington1, Thomas Wright1,
Stephanos Yerolatsitis1, Robert Harris2,
Tim Birks1
1
University of Bath, Bath, UK
2
Max-Planck-Institute for Astronomy,
Heidelberg, GermanyCD-1.1CD-3.1

Monday, 11:00, Room 4b ICM

Long-Lived Hot Electron dynamics via
hyperbolic meta-antennas

Monday, 10:30, Room 13a ICM

Ei Ei Brown1, Zackery Fleischman1,
Jason McKay1, Larry Merkle1, Uwe
Hommerich2, Witold Palosz3, Sudhir Trivedi3,Mark Dubinskii1
1
DEVCOM Army Research Laboratory,
Adelphi, USA2
Hampton University, Hampton, USA³ Brimrose Technology Corporation, Sparks
Glencoe, USA

Monday sessions from 14:00 to 15:30

45

Monday, 14:00, Room 13a ICM

CL-1.1 Monday, 14:00, Room 2 Hall B1 (B12)
Reconstructing brain tissue withlight microscopy
Johann G. Danzl, Institute of Science andTechnology Austria, Klosterneuburg, Austria
ED-3.1 Monday, 14:00, Room 6 Hall B3 (B32)
Precise Comb-based Time Transfer OverLong Distance Terrestrial Links
Emily D. Caldwell1,2, Jean-Daniel Deschenes3,
Jennifer Ellis1, William C. Swann1, Benjamin K.
Stuhl4, Hugo Bergeron3, Nathan R. Newbury1,
Laura C. Sinclair1
1
National Institute of Standards and Technology,
Boulder, USA
2
University of Colorado, Boulder, USA
3
Octosig Consulting; Quebec City, Canada

TECHNICAL PROGRAMMEINVITED TALKSTechnical ProgrammeSpace Dynamics Laboratory, North Logan, USA

CF-3.2 Monday, 14:15, Room 1 Hall B1 (B11)

Jiaqi Hu, Nathan Lydick, Kai Sun, Hui Deng,
University of Michigan, Ann Arbor, USA

Sampling Mid-infrared Waveforms in Timeand Space

JSVI-1.1 Tuesday, 8:30, Room Osterseen ICM

4Yangyang Liu , Shima Gholam-Mirzaei ,Dipendra Khatri1, Tran-Chau Truong1, Andre
Staudte2, Paul Corkum2, Michael Chini11
University of Central Florida, Orlando, USA
2
National Research Council of Canada andUniversity of Ottawa, Ottawa, Canada
1CB-2.3

2

Monday, 14:30, Room 13b ICM

The quest for ultraviolet vertical-cavity
surface-emitting lasers

TECHNICAL PROGRAMME

1

2

Tuesday sessions from 08:30 to 10:00
EG-4.1

Tuesday, 8:30, Room 4b ICM

Many-body superradiance and dynamical
symmetry breaking in waveguide QEDAna Asenjo-Garcia, Columbia University, New
York, USACB-3.1

Tuesday, 8:30, Room 13b ICM

Different phases of polariton lasers

Engineering thermal transport in lowdimensional systems
Yashpreet Kaur, Chaitanya Arya, Saeko
Tachikawa, Aswathi K. Sivan, Giulio de Vito,
Rahul Swami, Johannes Trautvetter, Diego deMatteis, Begoña Abad, Ilaria Zardo, Universityof Basel, Basel, Switzerland

Optophononic Engineering Using
Semiconductor Nanostructures
Norberto Daniel Lanzillotti-Kimura, Martin
Esmann, Anne Rodriguez, Priya Priya, Edson R.
Cardozo de Oliveira, Chushuang Xiang, Omar
Ortiz, Martina Morassi, Luc Le Gratiet, Isabelle
Sagnes, Aristide Lemaitre, Université Paris
Saclay – CNRS, Palaiseau, France
CG-1.1

Åsa Haglund , Filip Hjort , Johannes Enslin ,Michael Bergmann1, Munise Cobet2, Giulia
Cardinali2, Nando Prokop2, Lars Persson1,
Estrella Torres1, Sarina Graupeter2, Massimo
Grigoletto2, Martin Guttmann2, Luca Sulmoni2,
Neysha Lobo-Ploch3, Tim Kolbe3, Joachim
Ciers1, Tim Wernicke2, Michael Kneissl2,31
Chalmers University of Technology,
Gothenburg, Sweden
2
Technische Universität Berlin, Berlin, Germany
3
Ferdinand-Braun-Institut, Berlin, Germany
1

JSVI-1.2 Tuesday, 9:00, Room Osterseen ICM

CF-4. 3

Tuesday, 9:00, Room 1 Hall B1 (B11)

Arbitrary CEP Manipulationfor Spatiotemporal Control of Sub-cycle
Optical Vortex

Tuesday, 8:30, Room 6 Hall B3 (B32)

Yu-Chieh Lin, Katsumi Midorikawa, Yasuo
Nabekawa, RIKEN Center for Advanced
Photonics, Wako, Japan

Femto- phono- magnetism
Sangeeta Sharma1, J. K. Dewhurst2
Max Born Institute for Nonlinear Optics andShort Pulse Spectroscopy, Berlin, Germany
2
Max Planck Institute for micro-structure Physics,
Halle, Germany1CH-3.1CB-3.4

Boubacar Kante, UC Berkeley, Berkeley, USA

Trace gas absorption spectroscopy ona chipTuesday sessions from 14:00 to 15:30

Jana Jagerska1, Marek Vlk1, Jehona Salaj1,
Henock D. Yallew1, Sebastian Alberti1, Roman
Zakoldaev1, Jens Høvik2, Astrid Aksnes2
1
UiT The Arctic University of Norway,
Tromsø, Norway
2
Norwegian University of Science and Technology,
Trondheim, Norway
EB-4.1

Tuesday sessions from 16:00 to 17:30
CA-5.1

Tuesday, 16:00, Room 13a ICM

A simple pathway to widely tunable singlefrequency light using monolithic diamond
Raman resonators
Eduardo Granados, CERN, Geneva, Switzerland

Tuesday, 9:30, Room 13b ICM

The Berkeley Surface Emitting Laser(BerkSEL): a scale-invariant laser?

Tuesday, 8:30, Room 14b ICM

Andres Remis1, Michele Paparella1,2, Laura
Monge Bartolomé1, Audrey Gilbert1, Guilhem
Boissier1, Marco Grande2, Alan Blake4, Liam
O'Faolain3,4, Laurent Cerutti1, Jean-Baptiste
Rodriguez1, Eric Tournié1
1
University of Montpellier, Montpellier, France
2
Polytechnic University of Bari, Bari, Italy3
Munster Technological University, Cork, Ireland
4
Tyndall National Institute, Cork, Ireland

CH-4.1

Tuesday, 16:00, Room 14b ICM

Laser-based Sensing for Energy and
Propulsion Sciences
Ronald K Hanson, Stanford University,
Stanford, USA
JSVI-2.1 Tuesday, 16:00, Room Osterseen ICM

CM-5.1

Tuesday, 14:00, Room 13a ICM

Spatially and time resolved maps oftransient nonequilibrium states in pulsed
laser ablation in liquid from large-scaleatomistic modelling
Chaobo Chen, Leonid Zhigilei, University ofVirginia, Charlottesville, USA

Tuesday, 8:30, Room 8 Hall A1 (A12)

Quantum computation and quantum
simulation with strings of trapped Ca+ ionsCB-4.1Rainer Blatt, University of Innsbruck,
Innsbruck, Austria

Monolithic integration of GaSb diode lasers
on a silicon photonic circuit

46

Tuesday, 14:00, Room 13b ICM

Massive search space optimization ofthermal radiation metamaterials
Junichiro Shiomi, The University of Tokyo,
Tokyo, Japan
CF-5.1 Tuesday, 16:00, Room 1 Hall B1 (B11)Single-Shot CEP Change Detection in a
Nanoantenna Network
Felix Ritzkowsky1, Matthew Yeung2, Engjell
Bebeti1, Thomas Gebert3,4, Toru Matsuyama3,
Giulio Rossi1, Roland Mainz1,5, HuseyinTechnical Programme
Wednesday sessions from 08:30 to 10:00

CA-8.1

CK-4.1

Advances in mode scaling and TMI
suppression in high-power fibre lasers
Jeffrey Nicholson, Jose Pincha, Ishu Kansal,
Robert Windeler, Eric Monberg, Vasily Lukonin,
Anand Hariharan, Gregory Williams, Andrea
Rosales-Garcia, Lalitkumar Bansal, David
DiGiovanni, OFS Laboratories, Somerset, USA
CE-4.3 Tuesday, 16:30, Room 2 Hall B1 (B12)
Vibrations and Photophysics in WhiteLight Emitting Two-Dimensional Metal
Halide Perovskites
Roman Krahne1, Balaji Dhanabalan1, Beatriz
Martin-Garcia2, Davide Spirito3, Sergey
Artyukhin1, Miao-Ling Lin4, Yu-Chen Leng4, PingHeng Tan4, Seda Kutkan1, Milena Arciniegas1
1
Istituto Italiano di Tecnologia, Genova, Italy2
CIC nanoGUNE, Donostia-San Sebastian, Spain
3
IHP–Leibniz-Institut für innovative Mikroelektronik, Frankfurt (Oder), Germany
4
Chinese Academy of Sciences, Beijing, China
EG-5.5High-Power Q-switched Near Infrared
Cryogenic Lasers

Wednesday, 8:30, Room 4a ICM

Photophysics of single color centers in silicon

Miftar Ganija, Keiron Boyd, Jesper Munch, The
University of Adelaide, Adelaide, AustraliaAnaïs Dréau, Laboratoire Charles Coulomb,
Montpellier, France

CD-8.1
JSI-1.1

CJ-1.1 Tuesday, 16:00, Room 7 Hall A1 (A11)

Wednesday, 10:30, Room 13a ICM

Wednesday, 8:30, Room 13b ICM

Wednesday, 10:30, Room 14a ICM

Laser-guided lightning using kHz
filamentation at 1030 nm

X-ray Transient Grating experiments at Free
Electron Lasers

Aurélien Houard1, Pierre Walch1, Thomas Produit2,
Victor Moreno2, Benoit Mahieu1, Antonio Sunjerga3,
Clemens Herkommer4, Amirhossein Mostajabi3,
Ugo Andral2, Yves-Bernard André1, Magali Lozano1,
Laurent Bizet1, Malte C. Schroeder2, Guillaume
Schimmel2, Michel Moret2, Olivier Maurice5, Bruno
Esmiller5, Knut Michel4, Walter Haas6, Thomas
Metzger4, Marcos Rubinstein7, Farhad Rachidi3,
Vernon Cooray3, André Mysyrowicz1, Jérôme
Kasparian2,9, Jean-Pierre Wolf2
1
École Polytechnique, Palaiseau, France
2
Université de Genève, Geneva, Switzerland
3
École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland
4
TRUMPF Scientific Lasers GmbH + Co. KG, Unterföhring, Germany
5
ArianeGroup, Les Mureaux, France
6
Swisscom Broadcast AG, Bern, Switzerland
7
University of Applied Sciences and Arts Western
Switzerland, Yverdon-les-Bains, Switzerland
8
Uppsala University, Uppsala, Sweden
9
Université de Genève, Geneva, Switzerland

Cristian Svetina, Instituto Madrileño
de Estudios Avanzados en Nanociencia,
Madrid, Spain
CJ-2.1 Wednesday, 8:30, Room 7 Hall A1 (A11)
Coherently combined high power
multicore fibers
Jens Limpert, University Jena, Jena,
GermanyCI-1.3 Wednesday, 9:00, Room 6 Hall B3 (B32)
Optical Communications: A hollow
future ahead?
Francesco Poletti, Greg Jasion,
Eric Numkam Fokoua, Hesham Sakr,
Ian Davidson, University of Southampton,
Southampton, United Kingdom

Wednesday sessions from 10:30 to 12:00

Wednesday sessions from 14:00 to 15:30

Tuesday, 17:00, Room 4b ICM

Deep Ultraviolet Nanophotonics toenhance the sensitivity of autofluorescence
spectroscopy on label-free proteins

JSIV-1.1

Prithu Roy, Jean Benoit Claude, Jerome
Wenger, Aix Marseille Univ, Marseille, France

Emiliano Cortes, University of Munich (LMU),
Munich, Germany

Wednesday, 10:30, Room 4b ICM
JSI-3.1

Plasmonic bimetallic metasurfaces forlarge-scale solar Hydrogen production

Wednesday, 14:00, Room 1 ICM

Imaging ultrafast electron dynamics inisolated nanoparticles
Björn Senfftleben1, Julian Zimmermann1,2,

47

Alessandro Colombo2, Ehsan Hassanpour Yesaghi2,
Linos Hecht2, Andreas Hoffmann1, Martin
Kretschmar1, Katharina Kolatzki2, Björn Kruse3,
Bruno Langbehn5, Nils Monserud1, Tamas Nagy1,
Mario Sauppe1,2, Rico M. Tanyag1,4, Johannes
Tümmler1, Anatoli Ulmer4, Thomas Möller4, Ingo
Will1, Thomas Fennel3, Marc J.J. Vrakking1, Arnaud
Rouzée1, Bernd Schütte1, Daniela Rupp1
1
Max-Born-Institute Berlin, Berlin, Germany
2
ETH Zürich, Zürich, Switzerland
3
University of Rostock, Rostock, Germany
4
TU Berlin, Berlin, Germany
JSIV-2.1

Wednesday, 14:00, Room 4b ICM

Incandescent Metasurfaces
Jean-Jacques Greffet, Université Paris-Saclay,
Palaiseau, France
CK-6.1

Wednesday, 14:00, Room 4a ICM

Lighting up the brain: Implantableneural probes using wafer-scale
integrated photonics
Joyce Poon, Max Planck Institute ofMicrostructure Physics, Halle (Saale), GermanyCF-8.1Wednesday, 14:00, Room 1 Hall B1 (B11)
Novel ultrafast laser technology for generating
gigawatt-class isolated attosecond pulses
Eiji Takahashi, RIKEN, Wako, Japan
CI-3.1 Wednesday, 14:00, Room 6 Hall B3 (B32)
Graphene Plasmonics – A Beyond 100 GHz
Technology
Juerg Leuthold, Stefan M. Koepfli, Ping Ma,
Xinzhi Zhang, Michael Baumann, Shadi
Nashashibi, Jasmin Smajic, Ueli Koch, Yuriy
Fedoryshyn, ETH Zurich, Zurich, Switzerland

TECHNICAL PROGRAMME

Cankaya1,5, Philip Keathley2, Franz Kärtner1,5
Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany
2
Massachusetts Inst. of Technology, Cambridge, USA
3
Max Planck Institute for the Structure and Dynamics of Matter, Hamburg, Germany
4
WiredSense GmbH, Hamburg, Germany
5
Universität Hamburg, Hamburg, Germany
1Technical Programme
JSIV-2.3

Wednesday, 14:45, Room 4b ICM

Diffused light concentration for enhanced
solar energy yield
Rebecca Saive, Univ. of Twente,
Enschede, Netherlands
EF-1.2 Wednesday, 15:00, Room Osterseen ICM
Guided Brillouin interactions from optical vortex isolators to
extreme thermodynamics
Birgit Stiller, Max Planck Institute for the
Science of Light, Erlangen, Germany

EH-2.1

Ultrafast nanophotonics and optoelectronics: from all-optical switching basedon metamaterial-cavity electrodynamics toplasmon-driven polaritonic chemistryCH-9.1

CK-7.1EH-1.1Engineering optical Schrödinger "cat"and entangled states using intense laseratom interactions
Paraskevas Tzallas, Institute of Electronic
Structure & Laser, Heraklion (Crete), Greece

Wednesday, 16:00, Room 4b ICM

EF-2.1 Wednesday, 16:00, Room Osterseen ICM

Leif Oxenløwe, Technical University ofDenmark, Kgs. Lyngby, Denmark

Thermal Effects in Kerr-Microresonator
Optical Frequency Combs
Tara Drake, Gabriel Colacion, Lala Rukh,
Emilio Perez de Juan, Brandon Stone,
University of New Mexico, Albuquerque, USA

Nirit Dudovich, Weizmann Institute of Science,
Rehovot, Israel

Thursday, 10:30, Room 4a ICM

CC-1.1 Thursday, 10:30, Room 1 Hall B1 (B11)
THz Bandwidth Activation of Anharmonic
Coupling in CdWO4

48

Friday, 8:30, Room 2 ICM

CE-7.1 Thursday, 16:00, Room 7 Hall A1 (A11)

All soft glass fiber components and sources

Post-2000 nonlinear optical materials andtheir characterization: data tables andbest practices

Martin Rochette, McGIll University,
Montreal, Canada

Nathalie Vermeulen1, Daniel Espinosa2,
Adam Ball3, John Ballato4, Philippe Boucaud5,
Georges Boudebs6, Cecilia Campos7, Peter
Dragic8, Anderson Gomes7, Mikko Huttunen9,Nathaniel Kinsey3, Rich Mildren10, Dragomir
Neshev11, Lazaro Padilha12, Minhao Pu13,
Ray Secondo4, Eiji Tokunaga14, Dmitry
Turchinovich15, Jingshi Yan11, Kresten Yvind13,
Ksenia Dolgaleva2, Eric Van Stryland16
1
Vrije Universiteit Brussel, Brussels, Belgium
2
University of Ottawa, Ottawa, Canada
3
Virginia Commonwealth University, Richmond, USA
4
Clemson University, Clemson, USA
5
Université Côte d’Azur, Sophia-Antipolis, France
6
Univ Angers, Angers, France
7
Universidade Federal de Pernambuco, Recife, Brazil
8
Univ. of Illinois at Urbana-Champaign, Urbana, USA
9Tampere University, Tampere, Finland

Thursday sessions from 10:30 to 12:00

Optical Combs for High-Capacity
Transmission and Energy-Optimization ofLong-Haul Fiber Cables

Attosecond InterferometryCJ-7.1

Rebecca Boll, European XFEL, Schenefeld, GermanyJoão Serra, Mário Silveirinha, University of
Lisbon, Lisbon, Portugal

CG-6.3 Thursday, 16:30, Room 6 Hall B3 (B32)

Friday sessions from 08:30 to 10:00

X-ray Induced Coulomb Explosion Imaging
of Complex Molecules

CK-9.1

11

Thursday sessions from 16:00 to 17:30

JSI-5.1 Thursday, 8:30, Room Osterseen ICM

Topological Phases of Spacetime Crystals

Macquarie University, Sydney, Australia
Australian National University, Canberra, Australia
12
Univ. Estadual de Campinas, Sao Paulo, Brazil
13
Technical University of Denmark, Lyngby, Denmark
14Tokyo University of Science, Tokyo, Japan
15
Universität Bielefeld, Bielefeld, Germany
16
University of Central Florida, Orlando, USA
10

CG-5.5 Thursday, 15:00, Room 6 Hall B3 (B32)

Thursday, 8:30, Room 14b ICM

Korenobu Matsuzaki, Tahei Tahara, RIKEN,
Wako, Japan

Francesco Ceccarelli1, Ciro Pentangelo2,1, Niki
Di Giano, Riccardo Arpe2,1, Simone Piacentini2,
Andrea Crespi2,1, Roberto Osellame1
1
Consiglio Nazionale delle Ricerche, Milan, Italy
2
Politecnico di Milano, Milan, Italy

Thursday sessions from 14:00 to 15:30

Nicolò Maccaferri, Umeå University, Umeå,Sweden and University of Luxembourg, Luxembourg

Wednesday sessions from 16:00 to 17:30
Wednesday, 16:00, Room 4a ICM

Megan Nielson, Brittany Knighton, Lauren
Davis, Aldair Alejandro, Claire Rader, JeremyJohnson, Brigham Young University, Provo, USA

Thursday, 8:30, Room 4b ICM

Ultrasensitive Concentration and Chirality
Measurements Realized by Sub-Shot-Noise
Absorption Spectroscopy Using Entangled
Photon Pairs

Femtosecond-Laser Written Universal
Photonic Processors

TECHNICAL PROGRAMME

Thursday sessions from 08:30 to 10:00

EI-1.1

Friday, 8:30, Room 4b ICM

Top-down exfoliation of 2D materials andcreation of their artificial structures
Fang Liu, Stanford University, Stanford, USA
ED-5.1

Friday, 8:30, Room 12b ICM

Entanglement-enhanced frequency
comparison of two optical atomic clocks
B. C. Nichol, R. Srinivas, D. P. Nadlinger,
P. Drmota, D. Main, G. Araneda, C. J. Ballance,
D. M. Lucas, Oxford University, Oxford, UK
JSIII-3.1

Friday, 8:30, Room 13a ICM

Motivation and challenges for applying photonic
neuromorphic computing technologies

Technical Programme

CD-11.1

Friday, 8:30, Room 13b ICM

Localized States in Nonlinear
Topological Photonics
Daria Smirnova, Australian National
University, Canberra, Australia

EE-2.2

JSIII-4.1

Friday, 9:15, Room 14c ICM

Ultrafast physics of Bessel beaminteraction with solid dielectrics: dense
plasma formation, second harmonic and
THz radiation

Friday, 10:30, Room 13a ICM

Photonic tensor core and convolution chipfor machine learning acceleration
Volker Sorger, George Washington University,
Washington, USA

Kazem Ardaneh, Mostafa Hassan, Benoit
Morel, Luca Furfaro, Luc Froehly, Remo Giust,
François Courvoisier, University of FrancheComté and CNRS, Besancon, France

EC-2.1

Friday, 10:30, Room 22a ICM

Three-dimensional topologicallight transport induced bylattice dislocations

Friday sessions from 10:30 to 12:00

José Miguel Pablos-Marín, Javier Serrano,
Carlos Hernández-García, Universidad de
Salamanca, Salamanca, Spain

Maria Chernysheva, Dennis C. Kirsch, Leibniz
Institute of Photonic Technology, Jena, Germany

Julius Beck1, Eran Lustig2, Lukas Maczewsky1,
Tobias Biesenthal1, Matthias Heinrich1, Zhaoju
Yang3, Yonatan Plotnik2, Mordechai Segev2,
Alexander Szameit1
1
University Rostock, Rostock, Germany
2
Technion – Israel Institute of Technology, Haifa,
Israel3
Zhejiang University, Hangzhou, China

EC-1.1CC-5.1

EF-8.1EJ-3.1

Friday, 8:30, Room 21 ICM

Complete computation of macroscopic
high harmonic generation using
artificial intelligence

Friday, 8:30, Room 22a ICM

CJ-8.1

Friday, 10:30, Room 2 ICM

Omitting conventional saturable absorbers
in mode-locked fibre lasers

Friday, 10:30, Room 5 ICM

Topological photonics with cavity polaritons

Miniaturised terahertz photonic chips

Jacqueline Bloch, Center for Nanoscience andNanotechnology, Palaiseau, France

Yazan Lampert1, Francesco Bertot1, Alexa
Herter2, Amirhassan Shams-Ansari3,
Alessandro Tomasino1, Shima Rajabali1, Marko
Loncar3, Ileana-Cristina Benea-Chelmus1
1
École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland
2
Eidgenoessische Technische Hochschule, Zurich, Switzerland
3
Harvard University, Cambridge, USA

CL-5.1

Friday, 8:30, Room Osterseen ICM

Unconventional SERS: from metal/plasmonfree to wearable/flexible SERS
Keisuke Goda, The University of Tokyo, Tokyo, Japan
CI-5.3Symmetry breaking and zero modes inphotonic crystal cavity arrays
Alejandro Martin Yacomotti, Kaiwen
Ji, Melissa Hedir, Bruno Garbin, Juan
Ariel Levenson, Université Paris-Saclay,
Palaiseau, FranceEE-3.1

Thomas Roger, Ravinder Singh, Chithrabhanu
Perumangatt, Davide Marangon, Peter
Raymond Smith, Mirko Sanzaro, Andrew
Shields, Toshiba Europe Ltd, Cambridge, UK

CH-14.1

Friday, 10:30, Room 14b ICM

Subhasis Adhikari, Patrick Spaeth, Michel
Orrit, Leiden University, Leiden, Netherlands

49

Thermal wavefront shaping:
Application in fluorescent microscopy
Hadrien M.L. Robert1, Chang Liu1,
Nadja Rutz2, Giulia Faini1, Anis Aggoun1,
Filippo Del Bene1, Gilles Tessier1,
Romain Quidant2, Pascal Berto1,3
1
Sorbonne Université, Paris, France
2
ETH Zürich, Switzerland
3
Université Paris-cité, Paris, France
Friday, 11:00, Room 3 ICM

Eric Cooper, Philipp Kunkel, Avikar Periwal,
Monika Schleier-Smith, Stanford University,
Stanford, USA

Friday sessions from 14:00 to 15:30

Federico Vismarra , Rocio Borrego-Varillas ,Yingxuan Wu1,2, Daniele Mocci1,2, Francisco
Fernández-Villoria3,7, Lorenzo Colaizzi1,
Maurizio Reduzzi1, Fabian Holzmeier4, Laura
Carlini5, Paola Bolognesi5, Robert Ritcher6,
Lorenzo Avaldi5, Jesús González-Vázquez7,

Imaging Circular Dichroismof Single Nanoparticles Using
Photothermal Microscopy

Friday, 10:45, Room Osterseen ICM

Graph States of Atomic Ensembles
Entangled by Light

Friday, 10:30, Room 14c ICM

1,2

CL-6.2EA-7.3Ultrafast Dynamics in Donor-Acceptor
Prototype Molecules by XUV-IR
Attosecond Spectroscopy

Friday, 9:00, Room 11 ICM

High-rate quantum key distribution overfree-space links

Friday, 10:30, Room 14a ICM

Alicia Palacios7, José Santos3,8, Matteo
Lucchini1,2, Luis Bañares3,8, Nazario Martin3,8,Fernando Martin3,7, Mauro Nisoli1,21Politecnico di Milano, Milan, Italy
2
IFN-CNR, Milan, Italy
3
IMDEA-Nanoscience, Madrid, Spain
4
Imec, Leuven, Belgium
5Istituto di Struttura della Materia-CNR (ISMCNR), Rome, Italy
6
Sincrotrone Trieste, Trieste, Italy
7
Universidad Autónoma de Madrid, Madrid, Spain
8
Universidad Complutense de Madrid, Madrid, Spain2

CM-10.1

Friday, 14:00, Room 1 ICM

The switching cycle of Phase-Change
Materials: Time-resolved diffraction afterlaser excitation

TECHNICAL PROGRAMME

Bert Offrein, Elger Vlieg, Felix Hermann,
Ludovico Carraria Martinotti, Folkert
Horst, IBM Research Europe - Zurich,
Rueschlikon, SwitzerlandTechnical ProgrammePeter Zalden, European XFEL,
Schenefeld, Germany
CJ-9.1

Xidian University, Xi’an, China
Vilnius University, Vilnius, Lithuania
6
Polish Academy of Sciences, Warsaw, Poland
5

Friday, 14:00, Room 2 ICM
CE-10.1

Development of active fibres withnanostructured cores
Ryszard Buczynski , Marcin Franczyk ,Dariusz Pysz1, Jan Aubrecht3, GrzegorzStępniewski1,2, Adam Filipkowski1,2, Michal
Kamrádek3, Ivan Kasik3, Pavel Peterka3
1
Institute of Microelectronics and Photonics, Warsaw, Poland
2
University of Warsaw, Warsaw, Poland
3
Institute of Photonics and Electronics of the Czech
Academy of Sciences, Prague, Czech Republic
1,2

EI-3.1

1

Joanna Wolff, Loïc Moczko, Jérémy Thoraval,
Michelangelo Romeo, Stéphane Berciaud,
Arnaud Gloppe, Université de Strasbourg,
Strasbourg, France

TECHNICAL PROGRAMME

Friday sessions from 16:00 to 17:30

Friday, 14:00, Room 12a ICM

Glass-based materials for (bio)photonic applications

CM-11.1

Laeticia Petit, Tampere University,
Tampere, Finland

Laser Induced Forward transfer: Digital
Additive Manufacturing solution
for electronics

JSIII-5.1

Ioanna Zergioti, National Technical Universityof Athens, Athens, Greece

Friday, 14:00, Room 13a ICM

Photonic neuromorphic computing
Wolfram Pernice, Heidelberg University,
Heidelberg, Germany

EI-4.1

Friday, 14:00, Room 4b ICM

Optomechanics of suspended magnetic vander Waals materials

CC-6.1

Valentin Magro, Julien Vaneecloo, Sebastien Garcia,
Alexei Ourjoumtsev, PSL University, Paris, France

4

Friday, 14:00, Room 5 ICM

Holographic THz Imaging by FourierDomain Detection with Feld-EffectTransistors, and the Quest for Phase
Retrieval by Physics-Informed
Deep Learning
Hui Yuan1, Mingjun Xiang1,2,3,4, Alvydas
Lisauskas1,5,6, Lingxiao Wang2,3, MarkThomson1, Kai Zhou2,3, Hartmut Roskos1
1
Goethe-Universität Frankfurt, Frankfurt am
Main, Germany
2Frankfurt Institute of Advanced Studies, Frankfurt am Main, Germany
3
Xidian-FIAS International Joint Research Center,Frankfurt am Main, Germany

CH-15.1

Friday, 14:00, Room 14b ICM

Optical sensing in the brain with tapered
optical fibers: from photoelectric free
optrodes to implantable neuroplasmonics

Friday, 16:00, Room 1 ICM

Hatam Mahmudlu1, Raktim Haldar1, Robert
Johanning1, Anahita Khodadad Kashi1, Albert
van Rees2, Jörn P. Epping2, Klaus-J. Boller2,
Michael Kues1
1
Leibniz University Hannover, Hannover,Germany
2
University of Twente, Enschede, The Netherlands
CH-16.1

Friday, 16:00, Room 14b ICM

Chemical sensing of trace gases andparticulate matter with optical cavities
Weidong CHEN, Université du Littoral Côted'Opale, Dunkerque, France

Friday, 16:00, Room 4b ICM

Lightshift of exciton and exciton-polarons
in a 2D semiconductor

ONLINE DIGEST

Bertrand Evrard, Takahiro Uto, Martin Kroner,
Atac Imamoglu, ETH Zurich, Zurich, Switzerland

The online digest (one-page summaries) will
be accessible for two weeks beginning fromthe conference.
Download information at:

CE-11.1

Friday, 16:00, Room 12a ICM

Filippo Pisano1, Antonio Balena1, Barbara
Spagnolo1, Samuela Andriani1,2, Marco Bianco1,
Di Zheng1, Liam Collard1, Rui Peixoto3, Marco
Grande4, Manuel Valiente5, Liset M De La
Prida6, Bernardo L Sabatini3, Massimo De
Vittorio1,2, Ferruccio Pisanello1
1Istituto Italiano di Tecnologia, Lecce, Italy
2
Università del Salento, Lecce, Italy
3
Harvard Medical School, Boston, USA
4
Dipartimento di Ingegneria Elettrica e dell’Informazione Politecnico di Bari, Bari, Italy
5
Spanish National Cancer Research Center, Madrid, Spain
6
Instituto Cajal, CSIC, Madrid, Spain

Adria Grabulosa1, Anas Skalli1, Johnny
Moughames1, Xavier Porte2, James Lott2,
Stephan Reitzenstein2, Daniel Brunner11
Université Franche-Comté, Besançon, France
2
University of Strathclyde, Glasgow, United Kingdom

EA-8.2

CD-14.1

Laser based 3D printing of fused silica glass
Michael Fokine, Taras Oriekhov, Chunxin Liu,
Nobula3D AB, Stockholm, Sweden
JSIII-6.1

Friday, 16:00, Room 13a ICM

Scalable and autonomous photonic
neural networks

Friday, 14:15, Room 3 ICM

Quantum engineering of light with an
intracavity Rydberg superatom

Friday, 16:00, Room 13b ICM

Fully On-chip Laser-integrated Quantum
Source of Entangled Photon States

50

https://www.cleoeurope.org/
wp-content/uploads/2023/
06/CEE2023-ONLINE-DIGEST.pdf

ADDENDUM
The coming pages group the technical sessions.
Last minute author/session chair changes can be
downloaded from:https://www.cleoeurope.org/
wp-content/uploads/2023/06/
CEE2023-ADDENDUM2.pdf

Technical Programme
NOTES

51

®

CLEO /Europe-EQEC 2023

2023 Conference of Lasers and Electro-Optics Europe &European Quantum Eletronics Conference
Monday, June 26 to Friday, June 30, 2023

Advance Programme (technical part)(This page is just a stub to begin the following pages at an even number.)

1

CLEO

Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Monday 26 June 2023
Room 13a ICM

Room 13b ICM

Room 14a ICM

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

CM-1: Laser additive manufacturing I

EJ-1: Simulating multi-mode
and non-hermitian systems

EG-1: Nanoantennas andnanoconfinement

CA-1: Mid-infrared lasers

CB-1: Photonic crystal lasers

CD-1: Frequency conversion I

Chair: Maria Farsari, FORTH, Institute of Electronic Structure andLaser, Heraklion, Crete

Chair: Julien Javaloyes, University of
the Balearic Islands, Palma de Mallorca, Spain

Chair: Mathieu Mivelle, CNRS, Sorbonne University, Paris, France

Chair: Pavel Loiko, CIMAP, Université de Caen Normandie, France

Chair: Åsa Haglund, Chalmers University, Gothenburg, Sweden

Chair: Nathalie Vermeulen, Free
university of Brussels, Belgium

CM-1.1 MON

EJ-1.1 MON (Keynote)

EG-1.1 MON (Keynote)CA-1.1 MON

CB-1.1 MON (Invited)CD-1.1 MON (Invited)

8:30

Wavelength independent laser
direct writing 3D nanolithography of non-photosensitized
SZ2080T M hybrid polymer
A. Butkus1 , E. Skliutas1 , D.
Ladika2,3 , D. Samsonas1,4 , V.
Melissinaki2 , M. Vengris1 , M.
Farsari2 , S. Juodkazis5,6 , and ∙M.
Malinauskas1 ; 1 VU LRC, Vilnius,
Lithuania; 2 IESL-FORTH, Heraklion, Greece; 3 UOC, Heraklion,
Greece; 4 Light Conversion, Vilnius,
Lithuania; 5 SUT, Hawthorn, Australia; 6 Tokyo Inst Technol, Tokyo,
Japan
Wavelength independent femtosecond laser direct writing 3D nanolithography of non-photosensitized
SZ2080T M hybrid polymer is experimentally demonstrated. No wavelength or pulse durations are foundto be restricting the photopolymerization, but rather influencing its
dynamic fabrication range.
CM-1.2 MON

8:30

Laser transverse patterns control
by nonhermitian actions∙K. Staliunas; UPC, Barcelona, Spain
The classical spatial pattern formation theory (optical vortices, spatial solitons, optical turbulence) in
broad area lasers will be revised.
New mechanisms of pattern control,in particular the turbulence control
by nonhermitian background potentials, will be presented.

8:30

Semiconductor Nanolasers∙J. Moerk, Y. Yu, E. Dimopoulos,
M. Xiong, M. Saldutti, G. Dong, M.
Bundgaard-Nielsen, K. Seegert, S.L.
Liang, E. Semenova, and K. Yvind;
DTU Electro, Technical University ofDenmark, Kgs. Lyngby, Denmark
A new generation of semiconductor
nanolasers with ultralow thresholds
and important applications in integrated photonics is emerging. The
talk gives an overview of recent experimental and theoretical progress,
highlighting the interesting physics
and new opportunities.

8:30

Roadmap to Femtosecond Pulse
Power/Energy-Scaling in
Mid-Infrared OscillatorAmplifier Laser Systems∙A. Rudenkov1 , V.L. Kalashnikov1,4 ,E. Sorokin2,3 , M. Demesh1 , and I.T.
Sorokina1,3 ; 1 Norwegian Universityof Science and Technology, Trondheim, Norway; 2 Photonics Institute,
Vienna University of Technology,
Vienna, Austria; 3 ATLA Lasers
AS, Trondheim, Norway; 4 Facoltá
di Ingegneria dell’Informazione,
Sapienza Universitá di Roma, Roma,Italy
We suggest the prospective technique opening up a route towards
extremely intense ultra-short pulses
in the chirped-pulse oscillatoramplification mid-infrared systems.
CA-1.2 MON

8:45

Ce3+-Doped Selenide-Glass
Lasers Tunable in the 4.5–5.6 μm
Range∙P. Fjodorow1 , M. Frolov2 , Y.
Korostelin2 , V. Kozlovsky2 , S.
Leonov2 , Y. Skasyrsky2 , C. Schulz1 ,B. Denker3 , B. Galagan3 , S.
Sverchkov3 , V. Koltashev4 , V.
Plotnichenko4 , M. Sukhanov5 , and
A. Velmuzhov5 ; 1 EMPI, Institutefor Energy and Materials Processes– Reactive Fluids, University ofDuisburg-Essen, Duisburg, Germany; 2 P.N. Lebedev PhysicalInstitute of the Russian Academyof Sciences, Moscow, Russia;
3
Prokhorov General Physics Instituteof the Russian Academy of Sciences,
Moscow, Russia; 4 Prokhorov General
Physics Institute of the Russian
Academy of Sciences, Moscow, Russia, Dianov Fiber Optics ResearchCenter, Moscow, Russia; 5 Devyatykh
Institute of Chemistry of High-Purity

8:45

Multiphoton Lithography Enabling a Novel Approach in
Tissue Engineering ThroughMicrofabrication
O.
Kopinski-Grünwald1,2 ,O.
Guillaume1,2 , and ∙A. Ovsianikov1,2 ;1
3D Printing and Biofabrication
Group, Institute of Materials Scienceand Technology, TU Wien, Vienna,
Austria; 2 Austrian Cluster for Tissue
Regeneration (https://www.tissueregeneration.at), Vienna, Austria
Multiphoton lithography (MPL) allows realization of complex 3D
structures with unprecedented precision. In this contribution we
present our recent data on a novel
tissue engineering approach enabledby this technology.

52

8:30

Recent progress of photoniccrystal surface-emitting lasers∙S. Noda; Kyoto University, Kyoto,
Japan
Recent progress of photonic-crystal
surface-emitting lasers are described: The brightness has now
reached up to 1GWcm-2sr-1 evenunder CW condition, and a functionality to emit any beam patterns
including ”The Great Wave” hasbeen achieved.

8:30

Nonlinear optics in 3D χ(2)structures∙Y. Zhang; Nanjing University, Nanjing, China
Benefiting from the developmentsof laser writing techniques, 3D
χ(2) structures have been successfully fabricated, which provides a
promising platform to investigate
nonlinear optical phenomena suchas efficient nonlinear beam shaping
and nonlinear multiplexing holography.

CLEO

Room 14b ICM

Room Osterseen ICM®

/Europe-EQEC 2023

⋅ Monday 26 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

CH-1: Imaging throughscattering media

JSII-1: The photonic yield inastronomy

ED-1: Precision spectroscopy
for fundamental science

CE-1: Specialty optical fibres

EB-1: Optomechanical andother quantum oscillators

Chair: Adrian Podoleanu, Universityof Kent, UK

Chair: Lucas Labadie, University of
Cologne, Köln, Germany

CF-1: Advances in attosecond
technology and high orderharmonic generation I

CH-1.1 MON

JSII-1.1 MON (Invited)

8:30

Deterministic Terahertz Imaging
through Scattering media
V. Kumar1 , ∙V. Cecconi1,2 , L.
Peters1,2 , L. Olivieri1,2 , J.S. Totero
Gongora1,2 , A. Pasquazi1,2 , and M.
Peccianti1,2 ; 1 Emergent Photonics
Lab (EPic), Department of Physics
and Astronomy, University of Sussex,
BN1 9QH, Falmer, UK; 2 Emergent
Photonics Research Centre, Department of Physics, School of Science,
Loughborough University, LE11
3TU, Loughborough, UK
We demonstrate deterministic
broadband terahertz image reconstruction through scattering media
via large area time-resolved fieldimaging and ghost-imaging-like
retrieval of an orthogonal baserepresentation of the scattering interms of input illumination.
CH-1.2 MON

8:30

Why Photonic Technologies are
Beneficial to Astronomical
Instrumentation∙S. Veilleux; University of Maryland,College Park, USA
Photonic technologies allow tominiaturize and improve astronomical instrumentation. Photonic
devices with capabilities exceeding
those of conventional instruments
will be described, followed by adiscussion of promising avenues ofresearch for the next decade.

Chair:
Laura Cattaneo, MaxPlanck-Institut Heidelberg, Germany

Chair: Piotr Wcislo, Nicolaus Copernicus University in Torun, Torum,
PolandCF-1.1 MON (Keynote)

ED-1.1 MON

8:30

Ultrafast attosecond and few-fs
sources for control of molecular
reactivity at the electron timescale
∙F. Calegari; CFEL-DESY, Hamburg,
Germany
Attosecond
scienceoffersformidable tools for investigating electronic processes. An
overview on developments forcompact few-femtosecond UV andattosecond VUV/soft-x ray sources,
together with their application forstudying charge migration in chiralmolecules, is presented.

8:45

8:30

53

CE-1.1 MON

8:30

First Observation of the 1S-2STransition of Singly-IonizedHelium in an Atomic Beam
∙V. Barbé, E. Gründeman, A. Martinez de Velasco, M. Collombon, C.
Roth, and K. Eikema; LaserLaB,
Vrije Universiteit Amsterdam, Amsterdam, Netherlands
We report the first laser excitation,in an atomic beam, of the 1S –2S two-photon transition of singlyionized helium using near-infraredand extreme ultraviolet light, which
is an important step towards precision spectroscopy of He+.

Metal-Free Perovskite Optical
Fibre
H.C.L. Tsui1 , D. Sirbu1 , N. Alsaif1 ,G. Tizzard2 , P. Docampo3 , and ∙N.
Healy1 ; 1 Newcastle University, Newcastle, United Kingdom; 2 Universityof Southampton, Southampton,
United Kingdom; 3 University ofGlasgow, Glasgow, United Kingdom
This paper will present a new fibre platform for nonlinear optics.
A few-mode fibre with a metalfree perovskite core that has a widebandgap of 5 eV and a second-ordernonlinearity.

ED-1.2 MON

CE-1.2 MON

8:45

Comb-calibrated Raman
Spectroscopy of Molecular
Hydrogen∙M. Lamperti1 , L. Rutkowski2 ,D. Ronchetti3 , D. Gatti3 , R.
Gotti4 , G. Cerullo3 , F. Thibault2 ,H. Jóźwiak5 , S. Wójtewicz5 , P.
Masłowski5 , P. Wcisło5 , D. Polli3 ,and M. Marangoni3 ; 1 Departmentof Science and High Technology,
University of Insubria, Como, Italy;
2
Univ Rennes, CNRS, IPR (Institut
de Physique de Rennes), Rennes,
France; 3 Dipartimento di Fisica Politecnico di Milano and IFN-CNR,
Milan, Italy; 4 Department of Electrical, Computer and Biomedical
Engineering, Università degli studi
di Pavia, Pavia, Italy; 5 Instituteof Physics, Faculty of Physics, Astronomy and Informatics, Nicolaus
Copernicus University,
Torun,
PolandWe determine the frequency of the

Delivering Broadband Light Deep
into Diffusive Media∙R. McIntosh1 , N. Bender2 , A.
Yamilov3 , A. Goetschy4 , C.W.
Hsu5 , H. Yilmaz6 , and H. Cao1 ;1Yale University, New Haven, USA;
2
Cornell University, Ithaca, USA;
3
Missouri University of Science andTechnology, Rolla, USA; 4 ESPCIParisTech, PSL Research University,
CNRS, Institut Langevin, Paris,
France; 5 University of Southern
California, Los Angeles, USA;
6
Bilkent University, Ankara, Turkey
We present a single wavefront that
optimizes broadband optical energy
delivery inside multiple-scattering
media in an on-chip experiment byintroducing the broadband deposition matrix and utilizing its maximal eigenvector. Applications include deep-tissue imaging and optogenetics.

Chair: Natalie Wheeler, University ofSouthampton, United Kingdom

8:45

Toward low-loss mid-infrared
Ga2O3-BaO-GeO2 optical fibers:
Solving 30 years of high losses∙T. Guérineau1 , S. Aouji1,2 , S.
Morency1 , J.-l.
Delarosbil1 , F.
Calzavara2 , P. Larochelle1 , P.
Labranche1 ,J. Lapointe1 ,S.
2Danto , T. Cardinal2 , E. Fargin2 ,M. Bernier1 , R. Vallée1 , and Y.
Messaddeq1 ; 1 Center for Optics,
Photonics and Lasers, Québec,Canada; 2 Institut de Chimie de laMatière Condensée de Bordeaux,Bordeaux, France
The development of robust high-Tg
mid-infrared glass fibers made ofgermanium, gallium and barium oxides (BGG) is studied. We report thefirst BGG glass fiber with low losses
down to 200 dB.km-1.

Chair: Gerd Leuchs, Institute for the
Science of Light, Erlangen, GermanyEB-1.1 MON (Invited)

8:30

Quantum state engineering ofmacroscopic oscillators∙E.S. Polzik; Copenhagen University,
Copenhagen, Denmark
Generation of an entangled state of
distant mechanical and atomic oscillators with applications to precision measurements will be presented. Progress towards generationof a Fock state of motion of a macroscopic object will be reported.

CLEO

Room 1 ICM
CM-1.3 MON

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM

Room 13a ICM

9:15

Ultra-thin metasurfaces
fabricated by two-photon
polymerization∙G. Zyla1 , S. Papamakarios2 , O.
Tsilipakos3 , D. Zografopoulos4 ,M. Kafesaki1 , M. Farsari1 , and1
C. Soukoulis1 ;IESL/FORTH,
Institute
Electronic
Structure
Laser/Foundation for Research
and Technology-Hellas, Heraklion,
Greece; 2 University of Crete, Heraklion, Greece; 3 National Hellenic
Research Foundation,
Athens,Greece; 4 Consiglio Nazionale delle
Ricerche, (CNR-IMM), Rome, Italy
This work presents the potential ofusing maskless 3D printing by twophoton polymerization to fabricate
photonic metamaterials with minimum interaction volume on several mm2. The printed metamaterial
can be used for various THz applications.

Room 13b ICM

Substances of the Russian Academyof Sciences, Nizhny Novgorod, Russia
We review our recent achievementswith room-temperature Ce-doped
selenide-glass lasers, including up to
45 mJ of output energy with a slope
efficiency of 25 %, tunability in the
4.5–5.6 μm spectral range, and Qswitched operation.

9:00

Versatile tomographic volumetricadditive manufacturing∙J. Madrid-Wolff, A. Boniface,F. Maitre, and C. Moser; Ecole
Polztechnique Federale de Lausanne,
Lausanne, Switzerland
Tomographic volumetric additive
manufacturing is a novel fabrication
method that allows to produce cmscale devices in seconds. We report
improvements to tomographic patterns calculation to extend the technique to larger objects and scattering photoresins.

CM-1.4 MON⋅ Monday 26 June 2023

CA-1.3 MON

9:00

Comparison of Diode-Pumped
Dy:KPC and Dy:PGS Lasers
Operating above 4.4 μm∙P. Schlosser and V. Savitski; Fraunhofer UK Research Ltd., Glasgow,
United Kingdom
This work compares laser performance of Dy:KPC and Dy:PGS crystals for quasi-cw pumping at 1710
nm emitting near 4.4 to 4.6 μm respectively. Experimental results areused to calculate Q-switched performance and optimized resonator
configurations.
EJ-1.2 MON

9:15

Transient growth in non-Hermitian photonics∙K. Makris; ITCP-Physics Department, University of Crete, Heraklion,
Greece; Institute of Electronic Structure and Laser (IESL)-FORTH, Heraklion, Greece
We study the counter-intuitive phenomenon of optical power growthin non-Hermitian Hatano-Nelson
lattices, that exhibit a decaying
eigenvalue spectrum. Singular value
decomposition and pseudospectra
methods are applied to calculate themagnitude of such transient growth.

EG-1.2 MON

9:15

CA-1.4 MON (Invited)

Performance of gallium
phosphide nanoantennas from
optimized design∙C. Vidal1 , B. Tilmann2 , S. Tiwari3 ,T.V. Raziman1 , S. Maier1,2,4 , J.
Wenger3 , and R. Sapienza1 ; 1 The
Blackett Laboratory, Department of
Physics, Imperial College London,
London, United Kingdom; 2 NanoInstitute Munich,Departmentof Physics, Ludwig-MaximiliansUniversity, Munich, Germany; 3 Aix
Marseille Univ, CNRS, Centrale
Marseille, Institut Fresnel, Marseille,
France; 4 chool of Physics andAstronomy, Monash University,
Clayton, Australia
We fabricated GaP nanoantennas
from an optimized design, measured their brightness enhancement
and compared it with the calculated
enhancement factor. We show thatbeyond design optimization, further
performance improvement requires
tailored fine-tuning.

9:15

Broadband direct frequency
down-conversion to wavelengths
beyond 5 μm using wide-gap
non-oxide crystals∙Z. Heiner; Humboldt-Universität zu
Berlin, Berlin, Germany
We present practical applicationsof novel sulfide nonlinear optical crystals (LiGaS2, BaGa4S7, andCdxHg1-xGa2S4) in the direct frequency down-conversion of 1 μm
pump pulses and the resulting 100kHz, ultrafast infrared OPA’s basedon these materials.

54

CB-1.2 MON

Room 14a ICM
9:00

InAs/GaAs quantum dot based
distributed feedback laser arrays
and photonic crystal lasers∙Y. Yu, Z. Yang, H. Zhong, and S. Yu;
Sun Yat-sen University, Guangzhou,
China
We developed a novel dielectric
grating structure and high performance InAs/GaAs quantum
dot (QD) based laterally coupled
distributed-feedback laser arrays.
Furthermore, we demonstrated
continuous wave operated QD
photonic crystal lasers with lowthresholds using miniaturizedbound states in the continuum
cavities.

CB-1.3 MON

9:15

Dual-mode lasing and beating
oscillations in a microscopic laser
based on electromagneticallyinduced transparency∙K. Seegert1,2 , Y. Yu1,2 , M. Heuck1,2 ,and J. Mørk1,2 ; 1 Department ofElectrical and Photonics Engineering, Technical University of Denmark , DK-2800 Lyngby, Denmark;
2
NanoPhoton - Center for Nanophotonics, DK-2800 Lyngby, Denmark
We propose and analyze a novel microscopic laser, that uses an EITresonance from a highly dispersive
mirror to achieve stable dual-mode
lasing, with a dynamically tunable
beat note frequency.

CD-1.2 MON

9:00

Large-Scale 3D Nonlinear
Woodpile Photonic Crystals from
Sol-Gel Derived Barium Titanate∙V.V. Vogler-Neuling1,2 , Ü.-L. Talts1 ,R. Ferraro1 , H. Weigand1 , G.
Finco1 , J. Winiger3 , P. Benedek4 , J.
Kusch5 , A. Karvounis1 , V. Wood 4 ,J. Leuthold3 , and R. Grange1 ; 1 ETH
Zurich, Department of Physics,
Institute for Quantum Electronics,
OpticalNanomaterialGroup,
Zurich, Switzerland; 2 Université deFribourg, Adolphe Merkle Institute,Soft Matter Physics Group, Fribourg,
Switzerland; 3 ETH Zurich, Department of Information Technology
and Electrical Engineering, Institutefor Electromagnetic Fields, Zurich,
Switzerland; 4 ETH Zurich, Department of Information Technology andElectrical Engineering, Institute forElectronics, Zurich, Switzerland;
5
ETH Zurich, ScopeM, Zurich,
Switzerland
The first bottom-up fabricated 3D
nonlinear photonic crystal with periodicities of 1 μm and large surface areas of 5.3 ⋅ 104 μm2 is demonstrated. The structures are fabricated with sol-gel derived barium titanate and soft-nanoimprint lithography.
CD-1.3 MON

9:15

Coherent difference frequency
generation in nonlinear photonic
crystals∙A. El Hassan, H. Vo Van Qui, and
K. Gallo; KTH, Stockholm, Sweden
We report experimental results on
difference frequency generation in
2D periodically poled lithium tantalate crystals pumped at 532nm andseeded at 1550 nm, yielding coherent DFG output beams around 800
nm with 96% visibility.

CLEO

Room 14b ICM
CH-1.3 MON

Room Osterseen ICM
9:00

10 MHz swept-source for opticalcoherence tomography at 1050 nm∙S. Grelet1,2 , P.B. Montague1 , and A.
Podoleanu2 ; 1 NKT Photonics, Birkerød, Denmark; 2 University of Kent,
Canterbury, United Kingdom
We present a design of a 10 MHz
swept-source for optical coherence
tomography, operating at 1050 nm.
Based on low-noise supercontinuum dynamics and time stretch, thisdesign could improve current speed
and bandwidth limitations.

CH-1.4 MON

9:15

Mid-infrared OCT for nondestructive sub-surface inspection
and in-line production
monitoring∙C. Lapre1 , R.E. Hansen1 , C.R.
Petersen1,2 , N.M. Israelsen1,2 , and
O. Bang1,2,3 ; 1 DTU Electro, Department of Electrical and Photonics Engineering, Technical Universityof Denmark, Kgs. Lyngby, Denmark;
2
NORBLIS ApS, Virum, Denmark;3
NKT Photonics A/S, Birkerød, Denmark
OCT detection is well known inmedical domain and biology research for its non-destructive imaging and spectroscopy measurement.
In this presentation, I will highlight how mid-infrared OCT could
be used in various industrial in-line
detection.

JSII-1.2 MON/Europe-EQEC 2023

Room 1 Hall B1 (B11)

9:15

Creating a monolithic, lowinsertion loss, photonic chip for
the FIRST instrument∙H.-D. Kenchingotn Goldsmith1 , E.
Huby1 , K. Barjot1 , M. Lallement1,2 ,G. Martin2 , S. Lacour1 , D. Rouan1 ,S. Vievard3 , O. Guyon3 , V. Deo3 ,C. Pham4 , C. Cassagnettes4 , and
A. Billat4 ; 1 OBSERVATOIRE DE
PARIS, Meudon, France; 2 Institutde Planétologie et d’Astrophysiquede Grenoble , Grenoble, France;
3
National Astronomical Observatoryof Japan (NAOJ), Hilo, USA; 4 TEEM
photonics, Meylan, France
Photonic chips are improving sensitivity in astronomy instruments.
The FIRST instrument will soon
contain a completely monolithic⋅ Monday 26 June 2023
Room 6 Hall B3 (B32)

Q(1) line of the H2 fundamentalrovibrational band with uncertainty
20 times lower than previous experiments and 3 times lower than stateof-art theoretical calculations.

9:00

PolyOculus: Low-Cost PhotonicsEnabled Telescope Arrays∙S. Eikenberry1,2,3 , C. Moraitis1,2,3 ,R. Amezcua-Correa1 , C. Warner4 ,S. Yerolatsitis1 , D. Wright2 , H.
Reale1 , J. Foran1 , N. Harmon1 , A.
Akers1 , J. Rowe1 , K. Semmen1 , N.
Salem1 , V. Pagliuca1 , T. Thomas1 ,V. Miller1 , M. Bentz5 , A. Gonzalez4 ,J. Harrington3 , N. Law6 , T.
Maccarone7 , and R. Quimby8 ;1
CREOL - University of Central
Florida, Orlando, USA; 2 Physics
Dept - University of Central Florida,
Orlando, USA; 3 Planetary Sciences- University of Central Florida,
Orlando, USA; 4 University of
Florida, Gainesville, USA; 5 Georgia
State University, Atlanta, USA;
6
University of Norht Carolina Chapel Hill, Chapel Hill, USA;
7
Texas Tech University, Lubbock,
USA; 8 San Diego State University,
San Diego, USA
We present an overview of the PolyOculus approach - including photonic lantern couplers - and its potential scientific applications, particularly for time-domain astronomy and extreme precision radial
velocity measurements.
JSII-1.3 MON®

ED-1.3 MON (Keynote) 9:00

Laser Spectroscopy as a Probe forPhysics Beyond the Standard
Model
V. Wirthl, D. Taray, O. Amit, A.
Ozawa, F. Schmid, J. Moreno, J. Weitenberg, T. Hänsch, and ∙T. Udem;
Max-Planck Institute of Quantum
Optics, Garching, Germany
Precision spectroscopy of atomic
hydrogen and other simple atomic
systems is required for testing quantum electrodynamics, the determination of fundamental constants
and to probe for physics beyond theStandard Model.

CF-1.2 MON

9:15

Generation of high-order vortex
harmonics in solids throughspin-orbit interaction of light∙K. Nagai, T. Okamoto, Y. Shinohara, H. Sanada, and K. Oguri;
NTT Basic Research Laboratories,
NTT Corporation, 3-1, MorinosatoWakamiya, Atsugi-shi, Kanagawa
243-0198, JapanWe demonstrated the generationof high-order vortex harmonics ina bulk solid from Gaussian-likeshaped circularly polarized ultrashort laser pulses utilizing spinorbit interaction of light.

Room 7 Hall A1 (A11)
CE-1.3 MON

9:00

EB-1.2 MON

9:00

Optical Properties of ThuliumDoped Glasses in Optical Fibres
M. Leich, S. Unger, A. Schwuchow,
R. Müller, A.C. Pratiwi, J. Kobelke,
A. Lorenz, and ∙M. Jäger; Leibniz Institute of Photonic Technology, Jena,
Germany
Optical properties of Tm-doped
fibres based on two different
host glasses (silica-based andYAG-derived), are compared. As aresult, an energy level scheme withall absorption and emission transitions is obtained with enhanced
fluorescence lifetimes.

Quantum coherent control in
pulsed waveguide optomechanics
for photon-phonon entanglement
via Brillouin scattering∙C. Zhu1,2 , J. Zhang1,3 , C. Wolff4 ,and B. Stiller1,2 ; 1 Max Planck
Institute for the Science of Light,
Erlangen, Germany; 2 University
Erlangen-Nuremberg,
Erlangen,Germany; 3 University of Science andTechnology of China, Hefei, China;
4
University of Southern Denmark,Odense, Denmark
We present a Hamiltonian formalism for the time dynamics of backward Brillouin scattering in waveguides including quantum Langevinnoise. We show its applications
to photon-phonon entanglement via
Brillouin scattering, phonon cooling and coherent information transfer.

CE-1.4 MONEB-1.3 MON

9:15

Optical fibre doped with
YPO4:Pr3+ nanocrystals - glass
powder doping technique for newlaser transitions∙D. Dorosz1 , M. Kochanowicz2 ,R. Valiente3 , A. Diego-Rucabado3 ,N. Siñeriz-Niembro3 , M. Lesniak1 ,J. Posseckardt4 , G.L. Jimenez1 ,R. Müller5 , M. Lorenz5 , A.
Schwuchow5 ,M. Leich5 ,K.
5Wondraczek , and M. Jäger5 ; 1 AGH
University of Science and Technology, Krakow, Poland; 2 Bialystok
University of Technology, Bialystok,
Poland; 3 University of Cantabria,
4
Santander, Spain;
Fraunhofer
Institute for Ceramic Technologies
and Systems IKTS, Dresden, Germany; 5 Leibniz Institute of Photonic
Technology, Jena, Germany
We developed new optical fibre withactive YPO4:Pr3+ nanocrystals using glass powder doping technique.
Luminescence of the nanocrystals in
the fibre core and TEM/EDX analysis confirmed YPO4:Pr3+ survival
during fibre drawing.
55

Room 8 Hall A1 (A12)

9:15Free rotation and optically driven
spinning motion of a levitatednano-dumbbell
J. Zielinska, F. van der Laan, A. Norrman, M. Rimlinger, R. Reimann, L.
Novotny, and ∙M. Frimmer; Photonics Laboratory, ETH Zurich, Zurich,
Switzerland
We control the potential governing
the angular orientation of an optically levitated nanoparticle by controlling the degree of polarization of
the trapping light. This is an important step towards optically levitatedtorque sensors.

CLEO

Room 1 ICM
CM-1.5 MON

Room 4a ICM
9:30

EJ-1.3 MON®

/Europe-EQEC 2023

Room 4b ICM
9:30

EG-1.3 MON

Room 13a ICM

A normal form for frequency
combs and localized states intime-delayed Kerr-Gires-Tournois
interferometers∙T. Seidel1 , J. Javaloyes2 , and S.
Gurevich1 ; 1 Institute for Theoretical
Physics & Center for Nonlinear Science (CeNoS), University of Münster,
Schlossplatz 2, 48149 Münster, Germany; 2 Dpt. de Física, Universitat
de les Illes Balears & IAC-3, Campus UIB, E-07122 Palma de Mallorca, Spain
We elucidate the mechanisms that
underlie the formation of temporal
localized states and frequency
combs in vertical external-cavity
Kerr-Gires-Tournois interferometers by performing a multiple
time-scale analysis in the vicinity ofthe onset of optical bistability.

Advances in Electron-LightInteractions for Probing
Nanomaterials∙P.A.D. Gonçalves1 , F. Iyikanat1 , andF.J. García de Abajo1,2 ; 1 ICFO The Institute of Photonics Sciences,
Barcelona, Spain; 2 ICREA - Catalan Institution for Research and Advanced Studies, Barcelona, Spain
We show that free electrons canbe used to retrieve the quantum
response from nanostructured materials, including quantum nonlocal effects in nanoplasmonics andatomic-scale spectroscopy of defects
in atomically thin materials.

CM-1.6 MON

EJ-1.4 MON

EG-1.4 MON

9:45

9:45

Bayesian statistics for multimodal
problems applied to emission
spectra broadening of a single
core/shell CdSe/CdS nanocrystal.
∙D. Simonot, S. Huppert, M.
Trassinelli, and A. Maître; Institut
des Nanosciences de Paris, Paris,
FranceA model involving numerous unknown parameters is used to describes the spectral broadening of
single core/shell nanocrystal. With aMarkov Chain Monte Carlo Nested
Sampling method we determine theposterior probability distribution ofeach parameter.

Room 13b ICM

9:30

Zeroth-order and vortex Bessel
beams from single-mode fibers
with 3D printed photonic
structures
I. Reddy, A. Bertoncini, and ∙C. Liberale; King Abdullah University of
Science and Technology (KAUST),
Thuwal, Saudi Arabia
We present a 3D printed photonic
structure designed to transform thefundamental mode of single-mode
fibers into zeroth- and higher-order(vortex) Bessel beams, up to large
topological charges.

1530nm fiber laser fabricated via
additive manufacturing of silica
gain fibers
P. Maniewski1,2 , ∙M. Brunzell1 ,C. M. Harvey1 , L. Barrett1 , V.
Pasiskevicius1 , F. Laurell1 , and M.
Fokine1 ; 1 Department of Applied
Physics, KTH Royal Institute ofTechnology, Stockholm, Sweden;
2
Optoelectronic
ReseachCentre, University of Southampton,
Southampton, United Kingdom
In this work, we demonstrate a mirrorless fiber laser operating at 1530
nm, based on a high-performancesilica gain fiber, manufactured using laser-aided Additive Manufacturing.

⋅ Monday 26 June 2023
CB-1.4 MON

9:45

CA-1.5 MON

Ultrafast non-classical lightsources based on single
InAs/GaAs quantum dot
embedded in a hybrid plasmonic
nanopillar cavity
T. Hakkarainen1 , ∙A. Chellu1 , S.
Bej2 , H. Hulkkonen2 , R. Hytönen1 ,H. Rekola3 , T. Uusitalo1 , H. Kahle1 ,P. Karvinen3 , T. Niemi2 , and M.
Guina1 ; 1 Optoelectronics ResearchCentre (ORC), Physics Unit, Tampere University, Tampere, Finland;
2
Nanophotonics group, Physics Unit,
Tampere University, Tampere, Finland; 3 Institute of Photonics, University of Eastern Finland, Joensuu, Finland
We demonstrate an ultrafast
Purcell-enhanced
singlephoton source based on individual
InAs/GaAs quantum dots embedded in a deeply subwavelength
hybrid plasmonic-GaAs nanopillar
cavity.

9:45

Generation of Multicolor Pulse
Bursts for Pumping Long-Wave
Infrared Optical Parametric
Amplifiers∙R. Jutas1 , J. Roman1 , I. Astrauskas1 ,P. Polynkin2 , E. Kaksis1 , T. Floery1 ,J. Kolenda3 , T. Bartulevicius3 , K.
Michailovas3 , A. Michailovas3,4 ,A. Baltuska1,4 , and A. Pugzlys1,4 ;1Photonics Institute, TU Wien,
Wien, Austria; 2 College of Optical
Sciences, The University of Arizona,
Tucson, USA; 3 Ekspla Ltd., Vilnius,
Lithuania; 4 Center for PhysicalSciences & Technology, Vilnius,
Lithuania
Pulse-bursts from Nd:YAG amplifier are converted into angularly
separated multicolour pulses in
KTA-based parametric amplifier.
Energy of all eight generated
2100-nm pulses can be transferred to a single LWIR pulse
in non-collinearly pumped ZGP
OPCPA.

56

Room 14a ICM
9:30

CD-1.4 MON

9:30

Ultrashort pulse generation using
cavity-dumping in a Fano laser∙G. Dong1,2 , J. Mørk1,2 , and Y. Yu1,2 ;1DTU Electro, Technical Universityof Denmark, Kgs. Lyngby, Denmark;
2
NanoPhoton – Center for Nanophotonics, Technical University of Denmark, Kgs. Lyngby, Denmark
Ultrashort pulse (~1 ps) can be generated in a microscopic Fano laser
through cavity-dumping even in thepresence of a long carrier lifetime innanocavity.

High Sensitivity Active Imaging at
2 μm Using Upconversion
Detection∙R. Demur, A. Grisard, E. Lallier,and L. Leviandier; Thales Research &Technology, Palaiseau, France
We present an upconversion active imaging system at 2 μm withoutdoor images acquisition using adouble-pulsed fiber laser architecture. We benefit from the use ofa high sensitivity CMOS camera to
detect infrared images.

CB-1.5 MONCD-1.5 MON

9:45

Operating characteristics ofsurface-emitting quantum cascadelasers using photonic crystals withlow-symmetric pillars∙S. Saito1 , R. Hashimoto1 , K.
Kaneko1 , T. Kakuno1 , S. Okuma1 ,H. Tanimura2 , S. Takagi2 , Y.
Yao3 , N. Ikeda3 , T. Kuroda3 , Y.
Sugimoto3 , T. Mano3 , and K.
Sakoda3 ; 1 Corporate Manufacturing
Engineering Center, Toshiba Corporation, Yokohama, Japan; 2 Schoolof Engineering, Tokyo Universityof Technology, Hachioji, Japan;
3
Research Center for Functional
Materials, National Institute forMaterials Science, Tsukuba, Japan
We fabricated quantum cascadelasers with photonic crystal of
low-symmetric pillars as unit cell.
We have achieved an optical output
of 50mW in single-mode andover 1W in multi-mode in 4μm
wavelength region.

9:45

Infrared upconversion imaging
based on membrane siliconmetasurface∙Z. Zheng1 , L. Huang2,3 , D.
Smirnova4 , K. Zangeneh Kamali4 ,A. Yousefi1 ,F. Deng5 ,R.
Camacho-Morales4 ,C. Ying1 ,A. Miroshnichenko2 , D. Neshev4 ,M. Rahmani1 , and L. Xu1 ;1
Nottingham Trent University,
Nottingham,
United Kingdom;
2
University of New South Wales,
Canberra, Australia; 3 East China
Normal University,
Shanghai,
China; 4 The Australian National
University, Canberra, Australia;
5
Hong Kong University of Scienceand Technology, Hongkong, China
We experimentally converted theinvisible near-infrared images tovisible based on the third-harmonic
generation process by designing asilicon membrane metasurface supporting symmetry-protected boundstates in the continuum.

CLEO

Room 14b ICM
CH-1.5 MON

Room Osterseen ICM
9:30

Label-Free Three-Photon Deep
Imaging with High Power
Femtosecond Yb-Fiber Laser
A. Fernandez, A. Classen, N.K.
Josyula, P. Straight, and ∙A. Verhoef;
Texas A&M University, College Station, USA
We demonstrate simultaneous multicolor two- and three-photon imaging of bacterial filaments using
a single high-power femtosecond
Yb-fiber laser. Our experiments
demonstrate the superior signal-tobackground ratio obtainable withthree-photon imaging deep below
the sample surface.

CH-1.6 MON

9:45

Experimental Characterizing The
Complex Light Scattering
Properties of Finite Objects By
Mutual Scattering∙A. Rates, M.D. Truong, A. Lagendijk, and W.L. Vos; Universityof Twente,Complex Photonic Systems(COPS), MESA + Institute for Nanotechnology, Enschede, Netherlands
We study the light scattering properties of finite objects using Mutual
Scattering. We modulate the phaseand angle of two incident beams andmeasure light extinction. This permits full complex scattering characterization of finite objects.

chip with low loss in the visible spectrum. The selection between highand low index chips is discussed.
JSII-1.4 MON

9:30

A Near-infrared, on-chip
Astrophotonic Spectrograph witha Resolving Power of 40,000∙P. Gatkine1 , N. Jovanovic1 , G.
Sercel2 , J. Jewell3 , J.K. Wallace3 ,and D. Mawet1 ; 1 California Institute of Technology, Pasadena, USA;2
California State University, Los Angeles, USA; 3 Jet Propulsion Laboratory, Pasadena, USA
We present an on-chip astrophotonic spectrograph using thin(200nm) SiN platform. This spectrograph has a peak resolving power of
40,000, size of 2cmx2cm, and operates over a broadband (1250-1650nm).
JSII-1.5 MON

9:45

Demonstration of Photonic
Correlation of GHz Signals for10.6 um Astronomical
Heterodyne Interferometry∙T. ALLAIN1,2 , G. BOURDAROT3 ,C. SIRTORI2 , and J.-P. BERGER1 ;1
Univ. Grenoble Alpes, CNRS, IPAG,
Grenoble, France; 2 Laboratoirede Physique de l’Ecole Normale
Supérieure, ENS, Université PSL,
CNRS, Sorbonne Université, Université de Paris, Paris, France;
3
Max-Planck-Institut für Extraterrestrische Physik (MPE), Garching
bei München, Germany
In the context of mid-infrared astronomical heterodyne interferometry,
we demonstrate the photonic correlation of two GHz signals originating from the heterodyne beating of
a 10.6 um local oscillator and a science channel on two detectors.

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)
CF-1.3 MON

Room 6 Hall B3 (B32)

9:30

Room 7 Hall A1 (A11)
CE-1.5 MON

Isolated Attosecond Pulse
Generation Driven by
Spatio-Temporal Pulse Reshaping
in a Semi-infinite Gas Cell
∙F. Vismarra1,2 , D. Mocci1 , L.
Colaizzi1 , M.F. Galán3 , V.W.
Segundo3 , R. Boyero-García3 , J.
Serrano3 , E. Conejero Jarque3 ,M. Pini1,2 , L. Mai1 , Y. Wu1,2 , M.
Reduzzi1,2 , M. Lucchini1,2 , H.J.
Wörner4 , C.L. Arnold5 , J. San
Román3 , C. Hernández-García3 , M.
Nisoli1,2 , and R. Borrego-Varillas2 ;1
Department of Physics, Politecnicoof Milano, Milano, Italy; 2 IFN-CNR,
3
Milano, Italy;
Departamentode Física Aplicada, University of
Salamanca, Salamanca, Spain;
4
Laboratorium fur Physikalische
Chemie, ETH Zurich,, Zurich,
5
Switzerland;
Department of
Physics, Lund University, Lund,
SwedenIsolated attosecond pulses have been
generated in a semi-infinite cellfilled with noble gases by taking advantage of spatio-temporal reshaping of 3.8-fs driving pulses. Theinterplay between HHG and IR reshaping is investigated with simulations.
CF-1.4 MON⋅ Monday 26 June 2023

ED-1.4 MON

9:45

Enhanced sensitivity to bosonicultralight dark matter fromacetylene transitions between
near-degenerate vibrational
modes∙F.L. Constantin;
Laboratoire
PhLAM, CNRS UMR 8523,
Villeneuve d’Ascq, France
Fourier-transform microwave spectroscopy of a transition of 12 C2 H2with enhanced sensitivity to theproton-electron mass ratio (μ) variation may constrain a fractionalvariation of μ at the 10−12 level in 1 s.

9:45

High repetition rate, high photon
flux VUV source∙A. Omoumi1,2,3 , M. Natile2 , E.
Papalazarou3 , Y. Zaouter2 , M.
Hanna1 , T. Auguste4 , P. Georges1 ,and M. Marsi3 ; 1 Laboratoire Charles
Fabry, Paris, France; 2 Amplitude,
Pessac, France; 3 Laboratoire dePhysique des Solides , Orsay, France;
4
Laboratoire
Interactions
Dynamiques et Lasers, Gif-sur-Yvette,
FranceWe report a vacuum ultraviolet laser
source based on the ninth harmonicof a high-power ytterbium femtosecond laser. An in-depth analysisof phase-matching and efficiency ofthe process will be presented.

57

9:30

Room 8 Hall A1 (A12)EB-1.4 MON

9:30

Multimode Fluoroindate OpticalFiber Coupler∙F. Anelli1 , A. Annunziato1 , V.
Portosi1 , S. Cozic2 , S. Poulain2 ,P. Le Pays Du Teilleul2 , and F.
Prudenzano1 ; 1 Department of Electrical and Information Engineering,
Politecnico di Bari, Bari, Italy; 2 Le
Verre Fluoré, Bruz, France
A 2×2 coupler based on multimodefluoroindate optical fibers is fabricated and characterized for the firsttime. The experimental results show
the possibility to manufacture fused
optical fiber components for use in
the mid-infrared spectrum.

Miniaturized crossed beam
optical dipole trap for compact
atom-based quantum sensors∙M. Christ1,2 , C. Zimmermann1 ,O. Anton2 , and M. Krutzik1,2 ;1Ferdinand-Braun-Institut, Berlin,
Germany; 2 Humboldt-Universität
zu Berlin, Berlin, Germany
We present our development andqualification efforts towards compact and mobile physics packagesof quantum sensors, including a
micro-integrated 1064 nm crossedbeam optical dipole trap, UHVcompatible miniaturized optic systems and prospects of additive manufacturing methods.

CE-1.6 MONEB-1.5 MON

9:45

Highly focused photonic nanojetby molded high curvature fiber
micro-lenses∙T. Hajj1,2 , A. Guessoum3 , G.
Chabrol1,4 , N.-E. Demagh3 , andS. Lecler1,2 ; 1 ICube, Université deStrasbourg, CNRS, 67412 Illkirch,
France; 2 INSA Strasbourg, 67 000
Strasbourg, France; 3 Laboratoired’Optique Appliqu´ee, IOMP, Ferhat
Abbas University, 19 000 Setif,
Algeria; 4 Icam Strasbourg-Europe,
67 300 Schiltigheim, France
Highly focused beams out of single mode fibers are made possibleby high curvature molded microlenses deposited on their cores. The
technique also works for non-silica
and multicore fibers making it a very
promising one.

9:45

In situ optomechanical modetuning engineered using an integrated MEMS varactor for enhancing efficiency of microwaveto-optical quantum transduction∙A. Khurana, P. Jiang, and K.C. Balram; University of Bristol, Bristol,
United Kingdom
We show that the acoustic-optic
modulation in an optomechanicalcavity can be tuned with an integrated MEMS varactor within an
impedance matching network, designed to enhance the efficiency of
microwave-to-optical signal transduction in piezoelectric optomechanical platforms.

CLEO

Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Monday 26 June 2023
Room 13a ICM

Room 14a ICM

Room 14b ICM

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 11:45

CM-2: Laser semiconductor
processing

EJ-2: Computational photonics at the light-matterinterfaceEG-2: Metasurfaces

CA-2: Ultrafast lasers at 2 μm
and beyond

CD-2: Frequency conversion II

CH-2: AI for optical sensing

Chair: Yong Zhang, Nanjing University, China

Chair:
Sivankutty
PhLAM, Lille, France

CD-2.1 MON

CH-2.1 MON

Chair:
Stefan Nolte, Friedrich
Schiller University Jena, GermanyCM-2.1 MON

10:30

Single Femtosecond Laser Pulse
induced Amorphization, Re-crystallization and Native Oxide
Removal at Silicon Wafer Surfaces∙J. Bonse1 , C. Florian1,2 , D. Fischer1 ,K. Freiberg3 , M. Duwe4 , M. Sahre1 ,S. Schneider4 , A. Hertwig1 , J.
Krüger1 , U. Beck1 , and A. Undisz5 ;1
Bundesanstalt
fürMaterialforschung und -prüfung (BAM),
Berlin, Germany; 2 Consejo Superior de Investigaciones Científicas(CSIC), Madrid, Spain; 3 FriedrichSchiller-Universität Jena,
Jena,
Germany; 4 Park Systems GmbH,
Göttingen, Germany; 5 Technische
Universität Chemnitz, Chemnitz,
Germany
Single femtosecond laser pulse
inducedamorphization,
recrystallization and native oxide
layer removal at silicon wafer
surfaces of different crystal orientation is studied via spectroscopic
imaging ellipsometry, atomic force
microscopy, and high-resolution
transmission electron microscopy.
CM-2.2 MON

10:45

Ultra-High Space-Time Localization of Laser Energy for 3D Fabrication inside Semiconductors∙A. Wang1 , P. Salter1 , D. Grojo2 ,and M. Booth1 ; 1 Department of Enineering Science, University of Oxford, Oxford, United Kingdom; 2 AixMarseille Université, CNRS, LP3,
UMR7341, 13288, Marseille, France
By using spatially or temporally
shaped laser pulses, we obtain highlaser energy density at the focal spotthat successfully crosses the damage
threshold, thus opening new possibilities for fabricating 3D embedded
devices inside semiconductors.

Chair: Fabian Maucher, Universityof the Balearic Islands, Palma de
Mallorca, Spain
EJ-2.1 MON (Invited)

10:30

Exploring interacting photons
and quantum states of light withatomic metasurfaces∙T. Pohl; Department of Physics andAstronomy, Aarhus, Denmark
This talk will explore different approaches to realize strong effective
photon-photon interactions via extended regular arrangements of individual quantum emitters. Potential applications of the presented settings will also be discussed.

Chair: Jesper Moerk, Technical University of Denmark, Lyngby, Danemark

EG-2.1 MON

Chair: Weidong Chen, Fujian Institute of Research on the Structureof Matter, Chinese Academy of Sciences, China

10:30

CA-2.1 MON (Invited)

All-optical steering of light upconversion by nonlinear metasurfaces through coherent control
A. Di Francescantonio1 , A. Zilli1 ,D. Rocco2 , F. Conti1 , V. Vinel3 , A.
Borne3 , M. Morassi4 , A. Lemaitre4 ,P. Biagioni1 , L. Duò1 , C. De Angelis2 ,G. Leo3 , M. Finazzi1 , and ∙M.
Celebrano1 ; 1 Physics Department,
Politecnico di Milano, Milano, Italy;
2
Department of Information Engineering, University of Brescia, Brescia, Italy; 3 Laboratoire Matériaux etPhénomènes Quantiques, Universitéde Paris, Paris, France; 4 CNRS Centre de nanosciences et de Nanotechnologie, Université Paris Saclay,
Paris, France
We achieve all-optical switching of
the upconverted light in periodic dielectric metasurfaces through a ω +2ω pump scheme. Exploiting thepump pulse delay as tuning knob,
upconversion is switched between
diffraction orders with an efficiency>90%EG-2.2 MON

10:30

Towards few-optical-cycle
generation from Thulium /Holmium mode-locked lasers∙V. Petrov, W. Chen, L. Wang, Y.
Zhao, Z. Pan, and U. Griebner; Max
Born Institute, Berlin, Germany
Essential requirements and properties of Tm- and Ho-doped laser materials for successful operation in
the sub-100-fs pulse regime near 2
μm are discussed and more recent
mode-locking laser results will besummarized.

10:45

Optical Parametric Metamaterials– Frequency Mixing, Frequency
Combs and Control of Brownian
Motion∙T. Liu1 , J. Li1,2 , V. Raskatla1 ,J.-Y. Ou1 , K. MacDonald1 , andN. Zheludev1,2 ; 1 University ofSouthampton, Southampton, United
Kingdom; 2 Nanyang Technological
University, Singapore, Singapore
Nano-opto-mechanical metamaterials on semiconductor nanomembranes are a perfect platform
for parametric optical devices,
frequency mixing and optical
comb generation, and fundamental

10:30

10:30

Free-Space Quasi-Phase Matching∙N. Kovalenko, V. Hariton, K.
Fritsch, and O. Pronin; Helmut
Schmidt University,
Hamburg,
Germany
The first proof-of-concept experimental
demonstrationofχ(2)-based multipass nonlinear
conversion is presented. The freespace true phase-matching andquasi-phase matching can berealized with nearly all types ofnonlinear materials.

Deep Ensemble Learning andTransfer Learning Methods forClassification of Senescent Cells
in Nonlinear Optical Microscopy
Images∙F. Manetti1 , S. Sorrentino1 , A.
Bresci1 , F. Vernuccio1 , C. Ceconello1 ,S. Ghislanzoni2 , I. Bongarzone2 ,R. Vanna3 , G. Cerullo1,3 , and D.
Polli1,3 ; 1 Department of Physics, Politecnico di Milano, P.zza Leonardo
da Vinci 32, 20133, Milan, Italy;
2
IRCCS Istituto Nazionale dei Tumori Foundation, Via Venezian 1,
20133, Milan, Italy; 3 CNR-Institutefor Photonics and Nanotechnologies (IFN-CNR), P.zza Leonardo Da
Vinci 32, 20133, Milan, Italy
Image classification using Deep
Ensemble Learning and Transfer
Learning is performed on nonlinear
optical microscopy data to differentiate proliferating cancer cells
from senescent ones, a peculiar
phenotype following an anti-cancer
treatment responsible for tumour
relapse.

CD-2.2 MON

CH-2.2 MON

10:45

Multipass Spectral Broadening of
Spatially Chirped Pulses∙A. Imani1 , P.A. Carpeggiani1 ,E. Kaksis1 , D. Popmintchev1 , T.
Popmintchev1,2 , A. Pugzlys1 , and
A. Baltuska1 ; 1 Photonics Institute,
TU Wien, Gußhausstraße 25-29,
Vienna, Austria; 2 University ofCalifornia San Diego, Physics Department, and Center for Advanced
Nanoscience., La Jolla, USA
We propose a method to overcome
the energy handling limit in a fixedgeometry multipass gas-SPM pulse
scheme by a simple modificationof the grating-pair compressor in a58

Siddharth,

10:45

Metrology System Based on Metasurface Implementation of
Artificial Inteligence∙A. Burguete-Lopez, M. Makarenko,
Q. Wang, F. Getman, and A. Fratalocchi; King Abdullah Universityof Science and Technology, Thuwal,
Saudi Arabia
We present a metrology system forthin film measurements that employs artificial intelligence implemented in metasurfaces. We show
initial results on the performanceand fabrication of this system.

CLEO

Room Osterseen ICM®

/Europe-EQEC 2023

⋅ Monday 26 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 11:45

10:30 – 12:00

JSII-2: Manipulating astronomical signals with photonics
and future challenges I

CF-2: Advances in attosecond
technology and high orderharmonic generation II

ED-2: Direct comb spectroscopy

CE-2: Hollow core opticalfibresEB-2: Quantum interferometry

Chair: Robert R. Thomson, Heriot
Watt University, Edinburgh, United
Kingdom

Chair: Caterina Vozzi, Consiglio
Nazionale delle Ricerche, Milan,
Italy

Chair: Markku Vainio, Helsinki University, Helsinki, Finland

Chair: Stavros Pissadakis, FORTH,
Heraklion, Greece

Chair: Maria Chekhova, MPL, Erlangen, Germany

JSII-2.1 MON (Invited) 10:30

CF-2.1 MON

ED-2.1 MON

CE-2.1 MONEB-2.1 MON (Invited)

Fibre transitions for astronomical
applications∙K. Harrington1 , T. Wright1 , S.
Yerolatsitis1 , R. Harris2 , and T.
Birks1 ; 1 University of Bath, Bath,United Kingdom; 2 Max-PlanckInstitute for Astronomy, Heidelberg,
Germany
Using an optical fibre transition, we
present an all-fibre wavefront sensor
for local tip-tilt of a wavefront. It hasapplications within adaptive optics
and we present a validation case toshow its applicability to astronomy.

Bright, high-frequency, circularly
polarized structured attosecond
pulses∙A. de las Heras1 , N.J. Brooks2 , B.
Wang2 , I. Binnie2 , J. San Román1 ,L. Plaja1 , H.C. Kapteyn2 , M.M.
Murnane2 , and C. HernándezGarcía1 ; 1 Universidad de Salamanca, Salamanca, Spain; 2 JILA Department of Physics, University ofColorado and NIST, Boulder, USA
We demonstrate the generation ofbright circularly polarized structured attosecond pulses throughhigh harmonic generation. The implementation of a rotating polarization grating along the azimuthal focal plane allows for high brightness
and extended photon energies towards the soft x-rays.

Dual-comb spectroscopy from the
UV to VUVJ. McCauley1 , Y. Zhang1,2 , R.
Weeks1 , M. Phillips1 , and ∙R.J.
Jones1 ; 1 Wyant College of Optical
Sciences, University of Arizona,
Tucson, USA; 2 Department of
Physics, University of Arizona,
Tucson, USAWe
demonstrate
ultraviolet
dual-comb spectroscopy on laserproduced plasmas using the 4th
harmonic from Yb fiber systems.
We extend this capability towards
the vacuum ultraviolet by utilizing
intra-cavity high harmonic generation to measure atomic absorption
spectra.

Development of Next Generation
UV-Visible, Single-Mode, Hollowcore Optical Fibers∙I. Davidson, G. Jackson, T. Kelly, T.
Varghese, G. Jasion, N. Wheeler, D.
Richardson, and F. Poletti; University of Southampton, Southampton,
United Kingdom
We report on the development of
a new generation of broadband,
UV-Visible guiding, single-mode,
hollow-core optical fibers, via anovel fabrication approach, that offer performance levels comparable to commercial solid-core singlemode fibers.

CF-2.2 MON

ED-2.2 MON

CE-2.2 MON

10:30

10:45

1.7-cycle intense pulse source for
MHz attosecond pulse generation∙T. Okamoto1 , K. Nagai1 , Y.
Kunihashi1 , Y. Shinohara1 , H.
Sanada1 , M.-C. Chen2 , and K.
Oguri1 ; 1 NTT Basic ResearchLaboratories, Kanagawa, Japan;
2
National Tsing Hua University,
Hsinchu, Taiwan
We present MHz operation of 1.7cycle intense pulses (35 μJ) bycompressing 80-W Yb:KGW laser
pulses via the multi-plate continuum method.

10:30

10:45

Near-Ultraviolet Frequency-Agile
Dual-Comb Spectroscopy∙B. Xu1 , T.W. Hänsch1,2 , and N.
Picqué1 ; 1 Max-Planck Institute of
Quantum Optics, Garching, Germany; 2 Ludwig-Maximilian University of Munich, Munich, Germany
Near-ultraviolet dual-comb absorption spectroscopy is reported at 390
nm with photon-counting and shotnoise limited signal-to-noise ratio.
The repetition frequencies and center frequency of the dual-comb system can be changed at will.

10:30

10:45

The stadium fibre: a novelanti-resonant hollow-core fibre∙L.R. Murphy, J.M. Stone, T.A. Birks,
J.C. Knight, and D. Bird; Universityof Bath, Bath, United Kingdom
We report novel anti-resonant
hollow-core fibre with “stadium”
resonators, which are radiallyelongated compared to tubular
resonators.
We simulate thatelongating the resonators reduces
confinement loss by a factor of ten
and fabricate the fibre.

59

10:30

Applying Kerr Squeezed Light toInterferometry
N. Kalinin1,2,4 , T. Dirmeier1,2 , A.A.
Sorokin4 , E.A. Anashkina4,5 , L.L.
Sánchez-Soto1,6 , J.F. Corney7 , ∙G.
Leuchs1,2,3 , and A.V. Andrianov4 ;1
Max Planck Institute for the
Science of Light, Erlangen, Germany;
2
Friedrich-Alexander-Universität, Erlangen, Germany; 3 Nexus for
Quantum Technologies, University ofOttawa, Ottawa, Canada; 4 Instituteof Applied Physics of RAS, Nizhny
Novgorod, Russia; 5 Lobachevsky
State University , Nizhny Novgorod,
Russia; 6 Facultad de Física, Universidad Complutense, Madrid,
Spain; 7 University of Queensland,
Brisbane, Australia
The optical Kerr effect in fibers canbe used for robust squeezed light
generation. Here we demonstrate,
for the first time, interferometer
sensitivity enhancement beyond theshot noise limit using a third ordernonlinearity.

NOTES

CLEO

Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Monday 26 June 2023
Room 13a ICM

Room 14a ICM

studies of coupling between thermal
excitations in metamaterials andtheir optical properties.
CM-2.3 MON

11:00

EJ-2.2 MON

11:00

Through-Silicon Ultrafast Laser
Welding∙M. Chambonneau1 , Q. Li1 , M.
Blothe1 , and S. Nolte1,2 ; 1 Friedrich
Schiller University Jena, Instituteof Applied Physics, Abbe Center of
Photonics, Albert-Einstein-Str. 15,07745 Jena, Germany, Jena, Germany; 2 Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Albert-Einstein-Str. 7, 07745
Jena, Germany, Jena, Germany
We demonstrate through-silicon ultrafast laser welding by determining and precompensating the nonlinear focal shift in the filamentation regime in silicon for optimizing the energy deposition at the interface between metals and silicon.

Modeling Surface Enhanced
Raman Scattering: a Novel Fully
Atomistic QM/Classical Approach∙T. Giovannini, P. Lafiosca, L. Nicoli,
and C. Cappelli; Scuola Normale Superiore, Pisa, Italy
We present a novel fully atomistic approach to model thesurface-enhanced Raman spectraof molecular system, described
quantum-mechanically, adsorbed
on graphene and metal nanoparticles, treated by means of a classicalelectromagnetic method.

CM-2.4 MON

EJ-2.3 MON

11:15

Gap materials drilling with femtosecond laser in GHz-burst mode
∙I. Manek-Hönninger1 , P. Balage1 ,G. Bonamis2 , C. Hönninger2 , and
J. Lopez1 ; 1 Université de BordeauxCNRS-CEA CELIA UMR5107, Talence, France; 2 Amplitude, Pessac,
FranceWe report novel results on topdown percussion drilling with a
GHz-burst mode femtosecond laser
in different gap materials including
glasses, crystals and silicon. We
studied the drilling rates and reachable hole dimensions.

EG-2.3 MON (Invited)

Room 14b ICM

standard CPA. A proof of concept
is demonstrated for 2.5-mJ 1030-nm
pulses.

11:00

CA-2.2 MONLong-Lived Hot Electron dynamics
via hyperbolic meta-antennas∙H. Caglayan and R. Dhama; Tampere University, Tampere, Finland
The tunable absorption band of
hyperbolic meta-antenna control
and modify the lifetime of theplasmon-induced hot electrons
with enhanced excitation efficiency
ins the near-infrared region andalso broadens the utilization of thevisible/NIR spectrum.

11:00

0.5-μJ, 328-fs KLM Ho:YAG
Thin-Disk Oscillator at 2.1 μm∙S. Tomilov, Y. Wang, W. Yao, M.
Hoffmann, and C. Saraceno; RuhrUniversität Bochum, Bochum, Germany
We report on a 2-μm, 328-fs
Kerr-Lens-modelocked
Ho:YAG
thin-disk oscillator with an output
power of 14 W, corresponding to apulse energy of 0.5 μJ, representing
almost two-fold improvement incomparison with state-of-the-art
2-μm KLM results.

11:15

CA-2.3 MON

Simple modeling of weak ultrashort photonic wavepackets using
quantum-classical correspondence principle∙I. Babushkin, S. Bose, P. Rübeling,
O. Melchert, A. Demircan, M. Kues,
and U. Morgner; Leibniz University,
Hannover, Germany
We consider photons, interactingwith refractive index steps createdby strong pulses in waveguides withcomplex dispersion. We show thatevolution equations in such cases
can be determined uniquely via thequantum-classical correspondence
principle.

11:15

Bulk Supercontinuum Generation
for Ultra-CEP-Stable Single-Cycle
Pulses at 2.2 μm∙P. Steinleitner1 , M. Kowalczyk1,2,3 ,N. Nagl1,2 ,N. Karpowicz1 ,2
V. Pervak , A. Głuszek4 , A.
Hudzikowski4 ,J. Sotor4 ,F.
Krausz1,2,3 , K.F. Mak1 , and A.
Weigel1,3 ; 1 Max-Planck-Institut für
Quantenoptik, Garching, Germany;
2
Fakultät für Physik, LudwigMaximilians-Universität München,
Garching, Germany; 3 Center for
Molecular Fingerprinting, Budapest,
Hungary; 4 Laser & Fiber Electronics
Group, Faculty of Electronics,
Photonics
andMicrosystems,
Wrocław University of Science andTechnology, Wrocław, Poland
We present the generation of ultrastable single-cycle pulses at 2.2 μm
from a Kerr-lens-modelocked 22.9MHz Cr:ZnS oscillator by supercontinuum generation in TiO2. The system features carrier-envelope-phasestabilization with a residual phasejitter of 5.9 mrad.
60CD-2.3 MON

11:00

Towards a versatile photonic platform with 2D Materials grown on
Exposed-Core Fibers∙G.Q. Ngo1 , E. Najafidehaghani2 ,S.
Khazaee3 , M.P. Siems1 , A.
George2 , A. Tuniz4 , H. EbendorffHeidepriem5 , A. Turchanin2 , M.
Schmidt6 , and F. Eilenberger7 ;1Institute of Applied Physics,
Friedrich Schiller University Jena ,Albert-Einstein-Str. 15, 07745 Jena
, Germany; 2 Institute of Physical
Chemistry, Friedrich Schiller University Jena, Lessingstrasse 10, 07745
Jena, Germany; 3 Institute of Solid
State Theory and Optics, Friedrich
Schiller University Jena, Max-WienPlatz 1, 07743 Jena, Germany;
4
University of Sydney, School ofPhysics, Physics Road, Camperdown
NSW 2006, Australia; 5 Institute for
Photonics and Advanced Sensing,
University of Adelaide , Adelaide SA
5005, Australia; 6 Leibniz Institutefor Photonic Technology IPHT,
Albert-Einstein-Str. 13, 07745 Jena,
Germany; 7 Fraunhofer-Institute forApplied Optics and Precision Engineering IOF, Albert-Einstein-Str. 7,07745 Jena, Germany
We introduce a versatile photonic
platform, where two-dimensional
semiconductors are conformallygrown on the core of microstructured exposed-core fibers to enablesecond-harmonic
generation,
third-harmonic generation, in-fiber
exciton excitation, photoluminescence collection, and real-time gas
sensing.
CD-2.4 MON

11:15

Novel Coercive Field Engineering
Method for Short Period
KTiOPO4∙L. Barrett, A. Zukauskas, F. Laurell,and C. Canalias; Royal Institute ofTechnology (KTH), Stockholm, Sweden

CH-2.3 MON

11:00

Compressive Sensing Enhancedby Machine Learning
∙W.
Li1 ,
K.
Abrashitova1 ,G.
Osnabrugge1 ,
and
L.V.
1
Amitonova1,2 ;Advanced Research Center for Nanolithography(ARCNL), Amsterdam, Netherlands;
2
LaserLaB, Department of Physics
and Astronomy, Vrije Universiteit Amsterdam,
Amsterdam,
Netherlands
We propose and experimentallydemonstrate fast super-resolution
imagingtechniquebringing
together compressive sensing, multimode fiber imaging & machinelearning. A generative adversarial
network improves image quality
and noise robustness in the fiber
imaging system.
CH-2.4 MON

11:15

Digital Holographic Microscopy
applied to 3D Computer
Microvision by using Deep Neural
Networks∙J.E. Brito Carcaño, S. Cuenat, B. Ahmad, P. Sandoz, R.
Couturier,and M. Jacquot;
UniversitédeFranche-Comté,
SUPMICROTECH-ENSMM, CNRS,
Institut FEMTO-ST, Besançon,FranceWe present new results in 3D reconstruction trajectories at video-ratewith high level range-to-resolution
ratio for microrobotics and automated microscopy applications by
combining digital holography, computer microvision approaches andnew generations of deep neural networks.

CLEO

Room Osterseen ICM

JSII-2.2 MON

11:00

Lithium Niobate-on-Insulator for
Integrated Near-to Mid-infrared
Interferometry∙G. Li1 , G. Finco1 , A. Maeder1 ,D. Pohl1 , F. Kaufmann1 , M.M.
Ballester2 , J. Faist2 , A.M. Glauser3 ,S.P. Quanz3 , and R. Grange1 ; 1 ETH
Zurich, Department of Physics,
Institute for Quantum Electronics,
Optical Nanomaterial Group, 8093
Zürich, Switzerland; 2 ETH Zurich,Department of Physics, Institutefor Quantum Electronics, Quantum Optoelectronics Group, 8093
Zürich, Switzerland; 3 ETH Zurich,Department of Physics, Institute ofParticle Physics and Astrophysics,
8093 Zürich, Switzerland
We successfully demonstrated
an on-chip Fourier transform
infrared spectrometer on lithium
niobate-on-insulator working innear-infrared. We also extended ourdesign of integrated interferometry
to mid-infrared to be potentiallyused in astrophysics.
JSII-2.3 MON

11:15

An arrayed waveguide grating for
astronomical spectroscopy in thenear infrared∙O. Pfuhl, V. Gopinath, S. Lévêque,S. Lewis, and N. Hubin; European Southern Observatory, Garching, Germany
We present the development andverification of an arrayed waveguidegrating chip, working in the astronomical J-band with a spectral resolution of 10,000 for the applicationin astronomical spectrographs.

Room 1 Hall B1 (B11)CF-2.3 MON

11:00

®

/Europe-EQEC 2023

Room 6 Hall B3 (B32)

ED-2.3 MON⋅ Monday 26 June 2023
Room 7 Hall A1 (A11)11:00

CE-2.3 MON

11:00

Room 8 Hall A1 (A12)EB-2.2 MON

11:00

Point-spread function reduction
through high-harmonic generation deactivation∙K. Murzyn1 , L. Guery1 , Z. Nie1 , M.
van der Geest1 , and P.M. Kraus1,2 ;1Advanced Reseach Center for
Nanolithography,
Amsterdam,
Netherlands; 2 LaserLaB, Department of Physics and Astronomy,
Vrije
Universiteit
Amsterdam,
Amsterdam, Netherlands
This work demonstrates theworking principle of a superresolution microscope utilizing
high-harmonic
generationinsolids. This novel experimental
technique can extract the band
structure as well as phase transitions of correlated materials on ananometer-scale.

Cavity-enhanced frequency comb
spectroscopy in a supersonic jet∙R. Dubroeucq1 , Q. Le Mignon1 , N.
Suas-David1 , S. Kassi2 , R. Georges1 ,and L. Rutkowski1 ; 1 Univ. Rennes,
CNRS, IPR (Institut de Physiquede Rennes) - UMR 6251, Rennes,
France; 2 Univ.
Grenoble Alpes,
CNRS, LIPhy, Grenoble, France
We demonstrate Fourier transform
spectroscopy of acetylene in a supersonic jet with an optical frequency
comb. The acquired spectra achieve
high frequency precision limited by
the comb stability and consecutive
measurements could be efficiently
averaged.

Geometrical Deformation Effects
on Loss and Modal Content in
Hollow-Core Tube-Lattice Fibers∙F. Melli1 , E. Soli1 , L. Rosa1 ,K. Vasko2 , F. Benabid2 , and L.
Vincetti1 ; 1 Department of Engineering “Enzo Ferrari”, Universityof Modena and Reggio Emilia,
Modena, Italy; 2 GPPMM Group,
XLIM Institute, CNRS UMR 7252,
University of Limoges, Limoges,
FranceEffects of geometrical deformations
due to the fabrication process on
propagation loss and modal content
in Hollow-Core Tube-Lattice Fibres are numerically investigated byapplying two different approaches:overlap integral at discontinuities
and coupled mode theory

Quantum nonlinear interferometry vs induced coherence
N. Gemmell1 , ∙E. Pearce1 , Y. Ma1 ,J. Florez1 , C. Phillips1 , M. Kim1 , R.
Oulton1 , and A. Clark2 ; 1 Imperial
College London, London, United
Kingdom; 2 Bristol University, Bristol, United Kingdom
Here we provide - for the first time
– a direct comparison between thetwo possible modalities of quantum sensing with undetected photons: induced coherence and nonlinear interferometry, using both anexperimental and theoretical model.

CF-2.4 MON

ED-2.4 MON

CE-2.4 MONEB-2.3 MON

11:15

A simplified method for the characterization of extreme-ultraviolet pulses down to the attosecond
regime∙N. Di Palo1 , G.L. Dolso1 , G.
Inzani1 , B. Moio1 , F. Medeghini1 ,R. Borrego-Varillas2 , M. Nisoli1,2 ,and M. Lucchini1,2 ; 1 Departmentof Physics, Politecnico di Milano,
Milano, Italy; 2 Institute of Photonics
and Nanotechnologies, IFN-CNR,
Milano, Italy
We present STRIPE, a novel method
for the reconstruction of ultrashortextreme-ultraviolet pulses down
to the attosecond regime basedon two-colour photoemission
measurements,
demonstrating
its superior performances withrespect to other established retrieval
algorithms.

11:15

High Accuracy Line Lists of CH4
and H2 CO in the 8 μm Range
from Optical Frequency Comb
Fourier Transform Spectroscopy
M. Germann1 , A. Hjältén1 , V.
Boudon2 , C. Richard2 , J. Tennyson3 ,S. Yurchenko3 , I.E. Gordon4 , C.
Pett5 , I. Silander1 , K. Krzempek6 ,A. Hudzikowski6 , A. Głuszek6 ,G. Soboń6 , and ∙A. Foltynowicz1 ;1Department of Physics, Umeå University, Umeå, Sweden; 2 Laboratoire
ICB, UMR 6303 CNRS/Université
Bourgogne Franche-Comté, Dijon
Cedex, France; 3 Department of
Physics and Astronomy, University
College London, London, United
Kingdom; 4 Center for Astrophysics,
Harvard and Smithsonian, Atomic
and Molecular Physics Division,
Cambridge, USA; 5 Department ofChemistry, Umeå University, Umeå,Sweden; 6 Faculty of Electronics
Photonics
andMicrosystems,
Wroclaw University of Science andTechnology, Wroclaw, Poland
We measure line positions of

11:15

Distributed measurement ofhollow-core fibre gas filling andventing via optical time-domainreflectometry∙E. Elistratova, T.W. Kelly, I.A.
Davidson, H. Sakr, T.D. Bradley, A.
Taranta, F. Poletti, R. Slavik, P. Horak, and N.V. Wheeler; University ofSouthampton, Southampton, United
Kingdom
We present distributed measurements of the gas flow dynamic inside a hollow-core nested antiresonant nodeless fibre via optical timedomain reflectometry and validatethem with a simplified circular capillary gas flow model.

61

11:15

Scanning Quantum Interference
across the Unbroken PT-Symmetric Phase∙F. Klauck, T. Wolterink, M. Heinrich, and A. Szameit; Institute ofPhysics, University of Rostock, Rostock, Germany
Losses in PT-symmetric systems inevitably change the quantum correlations of interfering photons. We
study the impact of increased loss
on the two-photon correlation inlossy couplers and observe the corresponding changes in Hong-OuMandel dip visibility.

NOTES

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Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Monday 26 June 2023
Room 13a ICM

Room 14a ICM

Room 14b ICM

We demonstrate a new, reliable method for short period
QPM structures in KTP, throughcoercive field engineering via
Ba2+/K+ indiffusion. We showthat this method is compatible
with waveguide implementation
without compromising the domain
structure.
CM-2.5 MON

11:30

Nanosecond Laser-Induced
Micro-Modifications in Bulk of
Crystal Silicon∙V. Kadan1,2 , S. Pavlova4 , A. Bek1,3 ,Y. Aydin1 , I. Blonskyi2 , and I.
Pavlov1,2,3 ; 1 Department of Physics,
Middle East Technical University,
Ankara, Turkey; 2 Institute of Physics
of the NAS of Ukraine, Kyiv, Ukraine;
3
Center for Solar Energy Researchand Applications, Middle East Technical University, Ankara, Turkey;
4
FiberLAST Fiber Lazer Sistemleri ve
Teknolojileri A.Ş., Ankara, Turkey
Local micro-modification producedby 1550 nm-wavelength ns-laser inc-Si in a wide range of energies, durations, repetition rates, and writing
speeds is studied. We found dependency of the refractive index change
on pulse duration.

EJ-2.4 MON

11:30

Quantum optics tensor networks
in time for the design of nonlinear
photonic devices∙Q.M.B. Palmer1 , J.C. Adcock1 ,W.J. Munro2 , and J.W. Silverstone1 ;1
University of Bristol, Quantum
Engineering Technology Labs, Bristol, United Kingdom; 2 NTT Basic
Research Laboratories & ResearchCenter for Theoretical Quantum
Physics, Kanagawa, JapanWe employ time evolving block decimation to simulate nonlinear quantum optics in time. From this we canextract photon spatial, temporal andspectral information of the underlying quantum state with applications
in single photon sources.

EG-2.4 MON

EG-2.5 MON

CM-2.6 MON

11:45

Inscription and Characterizationof Transversely Written Waveguides in Silicon with Picosecond
Laser Pulses∙M. Blothe1 , M. Chambonneau1 , A.
Alberucci1 , N. Alasgarzade1 , and S.
Nolte1,2 ; 1 Friedrich Schiller University Jena, Institute of Applied Physics,
Abbe Center of Photonics, Jena, Germany; 2 Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Center of Excellence in Photonics, Jena, Germany
We demonstrate the transverse in-

EJ-2.5 MON

11:45

Quantum phases of bosonic chiralmolecules in helicity lattice
F. Isaule, R. Bennett, and ∙J.B.
Götte; School of Physics and Astronomy, University of Glasgow, Glasgow,
United Kingdom
We reveal the existence of polarizing quantum phases for the enantiomers of cold, interacting chiralmolecules in an optical helicity lattice by means of an extended BoseHubbard model.

11:30

CA-2.4 MON

Light-to-sound conversion insilicon nanodrums∙V. Kornienko, T. Koskinen, and I.
Tittonen; Aalto University, Helsinki,
Finland
We investigate opto-acoustic conversion in tailored periodic nanostructures on silicon with an optical pump-probe set-up. We demonstrate the impact of the optical andacoustic resonances on the properties of the excited acoustic pulse.

11:45

Dynamic Dielectric Metasurfaces
Based on Lattice Resonances:
Tuning and Switching Effects via
Superstrate-to-Substrate
Dielectric Contrast∙I. Allayarov1,2,3 , A. Evlyukhin3,4 ,D.J. Roth5 , B. Chichkov3,4 , A.
Zayats5 , and A. Cala Lesina1,2,3 ;1Institute of Transport and Automation Technology, Leibniz University
Hannover, Garbsen, Germany;
2
Hannover Centre for Optical
Technologies, Leibniz University
Hannover, Hannover, Germany;3
Cluster of Excellence PhoenixD,
Leibniz
University
Hannover,Hannover, Germany; 4 Institute of
Quantum Optics, Leibniz University
Hannover, Hannover, Germany;

11:30

11:30

Spontaneous Parametric Down
Conversion in Orientation-Patterned Gallium Phosphide Waveguides at Telecom Wavelength∙A. Marceau1,2 , S. Colmbrié1 , I.
Ghorbel1 , I. Sagnes2 , A. De Rossi1 ,K. Panzas2 , and A. Grisard1 ; 1 Thales
Research & Technology, Palaiseau,
France; 2 Centre de Nanosciences
et de Nanotechnologies, Palaiseau,
FranceSpontaneous parametric down
conversion is presented in a newpromising platform : OrientationPatterned
Gallium
Phosphide(OP-GaP). Spectral measurementson the generated pairs in thetelecom range is performed inaddition to coincidence between
polarization correlated pairs.

CA-2.5 MON

CD-2.6 MON

11:45

Single-cavity Dual-comb 2.36-μm
Cr:ZnS Laser∙A. Barh, A. Nussbaum-Lapping, M.
Gaulke, M. Golling, C.R. Phillips,
and U. Keller; ETH Zürich, Zürich,
Switzerland
The first single-cavity SESAMmodelocked dual-comb Cr:ZnS
laser operating at 2.36 μm ispresented. At 242 MHz, an average
power over 200 mW per comb anda pulse duration close to 200 fs isachieved.

62

CD-2.5 MON

1.2-ps SESAM mode-locked
Tm:LiYF4 laser at 2.31 μm
A. Tyazhev1 , M. Gaulke2 , ∙P.
Loiko3 , J. Heidrich2 , M. Golling2 , L.
Guillemot3 , T. Godin1 , P. Camy3 , U.
Keller2 , and A. Hideur1 ; 1 CORIA
UMR6614, CNRS-INSA-Universitéde Rouen, Normandie Université,Saint Etienne du Rouvray, France;
2
ETH Zurich, Department of
Physics, Institute for Quantum
Electronics, Zurich , Switzerland;
3
Centre de Recherche sur les Ions,
les Matériaux et la Photonique(CIMAP), UMR 6252 CEA-CNRSENSICAEN, Université de Caen
Normandie, Caen, France
A Tm:LiYF4 laser upconversionpumped by 1043-nm Yb-fiber laser
is mode-locked by a GaSb-based
SESAM. It delivers 1.2-ps pulses at
2308 nm with an output power of
252 mW at a repetition rate of 114.5
MHz.

11:45

Wavelength Conversion of
32GBaud 16QAM Signal Without
Preamplifiers Using Ultra-lowloss Compact Integrated Silicon
Nitride Nonlinear Photonic Waveguides∙P. ZHAO, Z. He, V. Shekhawat,
M. Karlsson, and P.A. Andrekson;
Chalmers University of Technology,
GOTHENBURG, Sweden
We present the wavelength conversion of single-polarization coherent
signal beyond 100 Gbps using acompact integrated Si3N4 nonlinear

CH-2.5 MON

11:30

Towards whispering-gallery-resonance photonic learning machine∙D. D’Ambrosio1 , M. Capezzuto1 ,S. Avino1 , A. Giorgini1 , P. Malara1 ,D. Pierangeli2 , C. Conti2 , and G.
Gagliardi1 ; 1 Consiglio Nazionaledelle Ricerche, Istituto Nazionale
di Ottica (INO), Pozzuoli, Italy;
2Consiglio Nazionale delle Ricerche,
Institute for Complex Systems(ISC-CNR), Roma, Italy
A novel neuromorphic photonic
scheme based on a spatial light
modulator and a whispering-gallery
mode resonator is demonstrated.
The proposed setup is both feasible for automatic alignment applications and for machine learning classification tasks

CLEO

Room Osterseen ICM

Room 1 Hall B1 (B11)®

/Europe-EQEC 2023

Room 6 Hall B3 (B32)⋅ Monday 26 June 2023
Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)methane and formaldehyde with
sub-MHz accuracy using Fouriertransform spectroscopy based on acompact 8 μm comb source and use
them to refine theoretical models ofthese molecules.

JSII-2.4 MON

11:30

18 GHz Ultraviolet Astrocomb via
Chip-Integrated Harmonic
Generation∙M. Ludwig1 , F. Ayhan2 , T.
Voumard1 ,T. Wildi1 ,M.A.
1Gaafar , D. Grassani3 , E. Obrzud3 ,T. Schmidt4 , F. Bouchy4 , L.G.
Villanueva2 , V. Brasch5 , and T.
1
Herr1,6 ;Deutsches ElektronSynchrotron
DESY,
Hamburg,
Germany; 2 Ecole PolytechniqueFédérale de Lausanne (EPFL), Lausanne, Switzerland; 3 Centre Suissed’Electronique et Microtechnique
SA (CSEM, Neuchâtel, Switzerland; 4 Department of Astronomy,
University of Geneva, Chemin desMaillettes 51, Versoix, Switzerland;
5
Q.ant GmbH, Stuttgart, Germany;
6
Physics Department, Universität
Hamburg, Hamburg, Germany
We present an electro-optic astrocomb at 18 GHz repetition rate centered at 390 nm via on-chip cascaded harmonic generation covering more than 8000 lines spanning
across 150 THz.
JSII-2.5 MON

11:45

Mid-IR SWIFTS : a miniature
integrated spectrometer in the
L-band∙M. Bonduelle1 , G. Martin1 , A.
Morand2 , N. Courjal3 , R. Salut3 ,and L. Robert3 ; 1 IPAG , Grenoble, France; 2 IMEP-LAHC, Grenoble, France; 3 FEMTO-ST, Besançon,FranceWe are presenting a new miniature
spectrometer in the Mid-InfraRed(L-band) using the SWIFTS (Stationary Wave Integrated Fourier
Transform Spectrometer) Gabor

CF-2.5 MON (Invited)

11:30

Liquid crystals meet strong-field
physics: first attempts of HHG in
soft matter
L. Becker1 , A. Annunziata2,3 , P.
Friebel1 , D. Facciala’3 , C. Vozzi3 ,and ∙L. Cattaneo1 ; 1 Max Planck
Institute for Nuclear Physics, Heidelberg, Germany; 2 Physics Department, Politecnico di Milano, Milano,
Italy; 3 National Research Council(CNR), Institute for Photonics andNanotechnologies, Milano, Italy
We present preliminary results of
HHG spectroscopy in 8CB smectic A liquid crystal under different
geometries and temperature, using
a single colour pumping scheme in
the mid-IR wavelength with subsequent detection in the NIR-visible
range.

ED-2.5 MON

11:30

CE-2.5 MON

Mid-IR optical frequency comb
Fourier transform spectroscopyusing an antiresonant hollow-core
fiber
∙D.
Tomaszewska-Rolla1 ,P.
Jaworski1 , D. Wu2,3 , F. Yu2,3 , A.
Foltynowicz4 , G. Soboń1 , and K.
Krzempek1 ; 1 Laser & Fiber Electronics Group, Wroclaw Universityof Science and Technology, Wroclaw,
Poland; 2 Hangzhou Institute for Advanced Study, University of Chinese
Academy of Sciences, Hangzhou ,China; 3 Key Laboratory of Materials
for High Power Laser, Shanghai
Institute of Optics and Fine Mechanics, Chinese Academy of Sciences,
Shanghai, China; 4 Department of
Physics, Umeå University, Umeå,SwedenWe show the first demonstration ofgas detector based on an opticalfrequency comb using an antiresonant hollow-core fiber gas absorption cell, which is capable of measuring molecules with transition lines
in the mid-infrared region.
ED-2.6 MON

11:30

Enhancing the Optical Properties
of Hollow Core Fibre Gas Cells bySelective Core Pressurisation∙S. Pradhan, T.W. Kelly, I.A.
Davidson, P. Horak, and N.V.
Wheeler; Optoelectronics ResearchCentre, University of Southampton, Southampton SO17 1BJ,
Southampton, United Kingdom
We fabricate a hermetically-sealed
hollow-core fibre-based gas cell,
where the core is filled with a higher
gas pressure than the cladding to enhance optical performance. Measurements over time indicate no
degradation due to gas permeation.

EB-2.4 MONEB-2.5 MON

11:45

11:30

Post-Selection Free Franson
Interference of Hyperentangled
Quantum States∙K. Lozano-Mendez1 , S. Sharma1 ,and F. Steinlechner1,2 ; 1 Fraunhofer
Institute for Applied Optics andPrecision Engineering IOF, Jena,
Germany; 2 Abbe Center of Photonics, Friedrich-Schiller-University
Jena, Jena, Germany
A post-selection free scheme formeasuring time-energy entanglement based on optical interference
and photon pairs simultaneously
entangled in polarization and timeenergy was implemented, yielding
high visibility values of 96.6% .

11:45

Self-stabilized optical phase sensor based on nonlinear interferometer∙R. Dalidet, A. Martin, G. Sauder,S. Tanzilli, and L. Labonté; Université Côte d’Azur, CNRS, Institut
de physique de Nice, France, Nice,
FranceWe report an optical phase sensor, enaling to perform a highprecision measurement in a selfstabilized way. We highlight the performance of our system by measuring the second and the third order ofdispersion.

Dual-comb spectroscopy in thewater-transparent 8-12 μm region∙L. Moretti1 , M. Walsh2 , D. Gatti1 ,M. Lamperti3 , J. Genest2 , A.
Farooq4 , and M. Marangoni1 ;1Dipartimento di Fisica - Politecnico
di Milano and IFN-CNR, Lecco,
Italy; 2 Centre d’optique, photoniqueet laser, Université Laval, Québec
City, Québec, Canada; 3 Departmentof Science and High Technology,
University of Insubria, Como, Italy;
4King Abdullah University for
Science and Technology (KAUST),
63

NOTES

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Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Monday 26 June 2023
Room 13a ICM

Department of Physics and London
Centre for Nanotechnology, King’s
College London, London, United
Kingdom
We present a new practical strategy for dynamic manipulation of
optical metasurfaces response via
the superstrate-to-substrate dielectric contrast.
5

scription of optical waveguides inthe bulk of silicon using picosecond
laser pulses

Room 14a ICM

Room 14b ICM

photonic waveguide, without additional optical amplification of thesignal and idler waves for the firsttime.

Room 4a ICM
12:00 – 12:52
PP-1: Early-stage researcher (ESR) session Poster pitches I
Chair: Emiliano Descrovi, European Optical Society,
Palaiseau, France
PP-1.1 MON (Poster pitch of CA-P.6)

12:00

Alexandrite Lasers Operating with High-power
Blue-diode-pumping∙H. Xiao, X. Jiang, and M. Damzen; Imperial College London, London, United Kingdom
We have demonstrated a blue-diode pumped Alexandrite laser with the highest power to date and performed
a full characterisation and analysis of laser performanceand prospects of blue as an alternative to red diodepumping.
PP-1.2 MON (Poster pitch of CA-P.21) 12:04

High average power amplification of femtosecond
pulses based on Yb: CaYAlO4 crystal∙C. Bai1 , W. Tian1 , G. Wang1 , L. Zheng1 , X. Tian1 , Y.
Yu1 , X. Xu3 , Z. Wei2 , and J. Zhu1 ; 1 Xidian University,
Xi’an 710071, China; 2 Chinese Academy of Sciences, Beijing 100190, China; 3 Jiangsu Normal University, Xuzhou
221116, China
In this report, we demonstrated the direct amplification
with the Yb:CALYO crystal for the first time. The amplifier delivered amplified pulses with the average powersof 55.4 W and pulse duration of 166 fs.
PP-1.3 MON (Poster pitch of CB-P.1)

12:08

Dual-wavelength DFB Laser Based on Four Phaseshifts Sections and Equivalent Chirp Technology for
Millimeter-wave Generation∙B. Yuan1 , Y. Fan1 , S. Zhu1 , Y. Zhang2 , J. Marsh1 , andL. Hou1 ; 1 University of Glasgow, Glasgow, United Kingdom; 2 Nanjing University of Posts and Telecommuinications, Nanjing, China
A monolithic dual-wavelength DFB laser based on fourphase-shifts sections and equivalent chirp is demon-tre & Centre for Photonic Metamaterials, University ofSouthampton, Southampton, United Kingdom; 2 Centre
for Disruptive Photonic Technologies, Nanyang Technological University, Singapore, Singapore
We demonstrate optical metrology for two-dimensional
sub-wavelength objects with resolution beyond λ/50 via
deep learning-enabled analysis of light scattering fromtarget objects illuminated by the phase singularity of superoscillatory structured light.

strated. A 61.2 GHz RF signal is observed by beating thetwo optical signals in a photodetector.
PP-1.4 MON (Poster pitch of CB-P.2)

12:12

Analysis of ultra-low frequency noise external cavity
diode laser-systems for optical ion clocks∙N. Kolodzie1,2 , I. Mirgorodskiy1 , C. Nölleke1 , and P.O.
Schmidt2,3 ; 1 TOPTICA Photonics AG, Gräfelfing, Germany; 2 Physikalisch-Technische Bundesanstalt, Braunschweig, Germany; 3 Institut für Quantenoptik, Leibniz
Universität Hannover, Hannover, Germany
We investigate the characteristics of two different diodebased ultra-low noise lasers for quantum applications.
Differences in operation are analysed both experimentally and theoretically, and advantages and disadvantagesof each system-type are discussed.
PP-1.5 MON (Poster pitch of CD-P.2)

PP-1.7 MON (Poster pitch of CH-P.8)

12:16

Efficient Generation of Vacuum-Ultraviolet Light inan Ultracompact Setup for Applications in Molecular
and Nuclear Spectroscopy∙M. Seitz1 , J. Al-Nuwaider2 , F. Belli3 , L. Silletti1 , V.
Wanie1 , F. Calegari1,4 , and A. Trabattoni1,2 ; 1 Center
for Free-Electron Laser Science, Deutsches ElektronenSynchrotron DESY, Hamburg, Germany; 2 Institute of
Quantum Optics, Hannover, Germany; 3 Heriot-Watt
University, School of Engineering and Physical Sciences,
Edinburgh, United Kingdom; 4 Physics Department, Universität Hamburg, Hamburg, Germany
This contribution presents an innovative and efficientvacuum ultraviolet light source, employing consecutive
nonlinear frequency conversion in nonlinear crystals
and up-conversion in a hollow core fiber via four-wave
mixing.
PP-1.6 MON (Poster pitch of CH-P.4)

12:24

Optical Localization of Nanoparticles in SubRayleigh Clusters∙B. Wang1 , Y. Li2 , E.A. Chan1 , G. Adamo1 , B. An2 ,Z. Shen1 , and N.I. Zheludev1,3 ; 1 Centre for Disruptive
Photonic Technologies, The Photonics Institute, School ofPhysical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore; 2 Artificial Intelligence Research Institute, School of Computer Science and Engineering, Nanyang Technological University,
Singapore, Singapore; 3 Optoelectronics Research Centre
and Centre for Photonic Metamaterials, University ofSouthampton, Southampton, United Kingdom
By deep learning analysis of diffraction patterns oflight scattered on sub-wavelength nano-holes clustered
within Rayleigh distance, we retrieve their positions withhigh accuracy breaking the diffraction limit of opticalresolution.
PP-1.8 MON (Poster pitch of CM-P.4)

12:28

Tailoring the optical response of 3D-printed photonic
crystals using Aluminum Zinc Oxide∙D. Ladika1,2 , A. Theodosi1 , O. Tsilipakos3 , A. Klini1 , P.
Loukakos1 , M. Kafesaki1,2 , M. Farsari1 , and D. Gray1 ;1
IESL-FORTH,Nik. Plastira 100, 70013 , Heraklion,Crete,
Greece; 2 Department of Materials Science and Technology, 70013, University of Crete, Heraklion,Crete, Greece;3
National Hellenic Research Foundation (N.H.R.F.), 48
Vassileos Constantinou Avenue, 11635, Athens, Greece
The extraordinary optical properties of the Epsilon Near
Zero material, Aluminum Zinc Oxide will be studied in

12:20

Deeply Sub-wavelength 2D Optical Metrology with
Superoscillatory Light∙Y. Wang1 , J.-K. So2 , E.A. Chen2 , C. Rendón-Barraza2 ,B. Wang2 , G. Adamo2 , E. Plum1 , K. MacDonald1 , J.-Y.
Ou1 , and N. Zheludev1,2 ; 1 Optoelectronics Research Cen64

three dimensions, by deposing it on 3D photonic crystals, which are responsive in the Telecommunication
Spectrum.
PP-1.9 MON (Poster pitch of CM-P.5)

12:32

In-depth jet dynamics investigations of femtosecond
laser bioprinting∙B. Kreidl1 , J. Zhang2 , S. Niehren2 , H. ClausenSchaumann1 , S. Sudhop1 , and H.P. Huber1 ; 1 Lasercenter,
Department of Applied Sciences and Mechatronics, Munich University of Applied Sciences HM, Lothstrasse 34,80335, München, Germany; 2 Molecular Machines & Industries, Breslauer Strasse 2, 85386, Eching, Germany
In-depth investigations of jet dynamics in previously
developed femtosecond laser bioprinting allow precise
control over the transfer process, enabling printing resolutions of <42±3 μm and single cell deposition accuracyof <15 μm.
PP-1.10 MON (Poster pitch of EF-P.4)

12:36

Programmable THz-range comb multiplication using
a feedback-controlled multi-wavelength laser∙S. Abdollahi, P. Marin-Palomo, M. Ladouce, and M.
Virte; Brussels Photonics Team (B-PHOT), Vrije Universiteit Brussel, Brussels, Belgium
We demonstrate all-optical THz-range comb multiplication based on a feedback-controlled on-chip multiwavelength laser. Varying the phase of the signal fed
back to the laser we clone the injected comb to offset frequencies up to 1.3THz.
PP-1.11 MON (Poster pitch of EJ-P.1)

12:40

Squeezed light source on lithium niobate on
insulator for GKP generation without periodic poling∙T.N. Arge, R.R. Domeneguetti, J.S. Neergaard-Nielsen,
T. Gehring, and U.L. Andersen; Center for Macroscopic
Quantum States (bigQ) Department of Physics, Technical
University of Denmark, Kgs. Lyngby, Denmark
In this work we present simulations and novel ideas forgenerating squeezed light on a Lithium Niobate on Insulator platform for continous variable quantum computa-

CLEO

Room Osterseen ICM

Room 1 Hall B1 (B11)technology. The chosen material
is Lithium Niobate, thus allowing for integrated active beamcombination.

®

/Europe-EQEC 2023

Room 6 Hall B3 (B32)⋅ Monday 26 June 2023
Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)

NOTES

Physical Science and Engineering
Division, Thuwal, Saudi Arabia
We demonstrate fast dual-comb
spectroscopy in the mid-IR region
with a figure of merit in excess of
107 Hz0.5 as a tool for investigationofnon-repetitive
phenomena
related to the chemical kinetics in
combustion processes.

Room 4a ICM
tion. We focus on purity and indistinguishability of thesource.
PP-1.12 MON (Poster pitch of JSII-P.2) 12:44

OPA! The Original PolyOculus Array for Mt. Laguna
Observatory∙C. Moraitis1,5 , S. Eikenberry1,5 , R. Amezcua-Correa1 ,S. Yerolatsitis1 , C. Warner3 , D. Wright2 , H. Reale1 , J.
Foran1 , A. Akers1 , J. Rowe1 , K. Semmen1 , V. Pagliuca1 ,T. Thomas1 , N. Salem1 , V. Miller1 , N. Harmon1 , M.
Bentz4 , A. Gonzalez3 , J. Harrington5 , N. Law6 , T.

Maccarone7 , and R. Quimby8 ; 1 College of Optics andPhotonics (CREOL), University of Central Florida, Orlando, FL, USA; 2 Department of Physics, University ofCentral Florida, Orlando, FL, USA; 3 Department of Astronomy, University of Florida, Gainesville, FL, USA;
4
Georgia State University, Atlanta, GA, USA; 5 Planetary
Sciences Group, Department of Physics, University of Central Florida, Orlando, FL, USA; 6 University of North Carolina - Chapel Hill, Chapel Hill, NC, USA; 7 Texas Tech
University, Lubbock, TX, USA; 8 San Diego State University, San Diego, CA, USA

The OPA project, the Original PolyOculus Array, isa seven-pack telescope array that uses the PolyOculus
technology to create a large-area-equivalent telescope forspectroscopy by combining the light of each small telescope via photonic lantern
PP-1.13 MON (Poster pitch of JSIV-P.2) 12:48

Photo-Electrochemical Imaging of Ultrathin
Single-Crystalline Gold Micro-Flakes∙M. Sabzehparvar, P. Feurstein, F. Kiani, and G. Tagliabue; École Polytechnique Fédérale de Lausanne, Lau-

NOTES

65

sanne, Switzerland
We study photo-induced activity of gold micro-flakes ofdifferent thicknesses using light-assisted scanning electrochemical microscopy. Our work aims to reveal dependencies on thickness and wavelength for photocatalytic activity and stability, and the possible edge effects.

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Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Monday 26 June 2023
Room 13a ICM

Room 13b ICM

Room 14a ICM

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

CM-3: Temporal and spatial
beam shaping for laser
processing I

CK-1: Lithium niobate andsilica systems

EG-3: Optoelectronics andlight-electron interactions

CA-3: Novel laser materials

CB-2: Surface-emitting lasers

Chair: Mathieu Mivelle,CNRS, Sorbonne university, Paris, France

Chair: Susumu Noda, Kyoto University, Japan

CD-3: Integrated nonlinear
photonics

Chair: Stéphane Clemmen, Ghent
University, Belgium

Chair: Federico Pirzio, University ofPavia, Italy

CK-1.1 MON

EG-3.1 MON

CA-3.1 MON (Invited)

CB-2.1 MON

Chair: Alexandre Mermillod-Blondin,
Max-Born-Institute Berlin, GermanyCM-3.1 MON

14:00

Microexplosions in bulk sapphire
driven by simultaneously spatiallyand temporally focused femtosecond laser beams
W. Cheng1 , Z. Wang2 , X. Liu3 ,A. Rudenko1 , Y. Cheng2,4 , and ∙P.
Polynkin1 ; 1 College of Optical Sciences, University of Arizona, Tucson, USA; 2 State Key Laboratory ofHigh Field Laser Physics, Shanghai
Institute of Optics and Fine Mechanics (SIOM), Chinese Academy of Sciences, Shanghai, China; 3 Aerospace
Information Research Institute, Chinese Academy of Sciences, Beijing,
China; 4 School of Physics and Electronic Sciences, East China Normal
University, Shanghai, China
We show by simulations thatpeak pressures inside ultrafastlaser-driven microexplosions insapphire are limited by ~250GPa,
two orders of magnitude below
earlier estimates. We use SSTF
focusing as a potential route toward
overcoming this limitation.
CM-3.2 MON

14:15

Taming Laser Wavefronts for
Advanced Multiphoton Polymerization∙M. Manousidaki1 , A. Kyriakakis2 ,K. Misdanitis2 , D.G. Papazoglou1,2 ,M. Farsari1 , and S. Tzortzakis1,2,3 ;1
IESL-FORTH, Heraklion, Greece;
2
Materials Science and Technology
Department, University of Crete,
Heraklion, Greece; 3 Art & Science,
Texas A&M University at Qatar,
Doha, Qatar
Taming Laser Wavefronts can surpass the limitations of the conventional single point-by-point andtime-consuming 3D printing. Advanced light shaping accelerates the
fabrication by Multi-photon Poly-

14:00

High Extinction Ratio Thermooptic Switch On Thin Film Lithium Niobate With Fast Rise Times∙A. Maeder, F. Kaufmann, G. Finco,
J. Kellner, R.J. Chapman, and R.
Grange;Optical NanomaterialGroup, Institute for Quantum
Electronics, Department of Physics,
ETH Zurich, Zurich, Switzerland
We present a thermo-opticallycontrolled switch on the lithium
niobate-on-insulator platform. We
measured extinction ratios up to 36
dB, power consumptions below 50
mW and fast rise times of 1.7 μs
using overdrive voltage signals.

EG-3.2 MON

CK-1.2 MON

14:15

Wavelength meter on thin filmlithium niobate based on superconducting single photon
detectors∙A. Prencipe, S. Gyger, M.A. Baghban, J. Zichi, K.D. Zeuner, T. Lettner,
L. Schweickert, S. Steinhauer, A.W.
Elshaari, K. Gallo, and V. Zwiller;
KTH Royal Institute of Technology,
Stockholm, Sweden
We demonstrate a waveguideintegrated wavelength-meter basedon superconducting single photon
detectors on thin film lithium
niobate waveguides. The device
exhibits a sensitivity of -5e-3
counts/nm for wavelengths around1550 nm.

14:00

Ultrastrong light matter interaction at the single element level∙E. Jöchl1 , M. Barra Burrillo2 , S.
Rajabali1 , M. Beck1 , J. Faist1 , and
G. Scalari1 ; 1 ETH Zürich, Zürich,
Switzerland; 2 CIC NanoGUNE,
Donostia-San Sebastian, Spain
To potentially uncover new states ofmatter we investigate the light matter interaction of single metamaterial cavities ultrastrongly coupled
to different systems. These include
electrically depleted quantum wells
and high quality monolayer hBNgraphene stacks.

14:00

Low-Phonon-Energy Rare-Earth
doped Laser Gain Materials:
Crystals vs. Glasses∙E.E. Brown1 , Z. Fleischman1 ,J. McKay1 , L. Merkle1 , U.
Hommerich2 , W. Palosz3 , andS. Trivedi3 ; 1 DEVCOM Army
Research Laboratory,
Adelphi,USA; 2 Hampton University, Hampton, USA; 3 Brimrose Technology
Corporation, Sparks Glencoe, USA
We present a comparative spectroscopic study of RE3+ (Dy3+,
Ho3+, Er3+) doped low-phonon
fluoride (BaF2, NaYF4) and chloride (CsCdCl3, CsPbCl3) single
crystals, as well as Ga-Ge based
chalcogenide (S, Se) glasses, withthe emphasis on their respective
mid-IR transitions.

14:15

Photocurrent nanoimaging ofstructural and spin-momentum
locking chiralities in topologicalinsulators∙A. Dubrovkin1,2 , G. Adamo1,2 ,L. Wang3 , Q.J. Wang1,2,4 , N.
Zheludev1,2,5 , and C. Soci1,2,4 ;1
Centre for Disruptive Photonic
Technologies, TPI, Nanyang Technological University, 637371 Singapore,
Singapore, Singapore; 2 School ofPhysical and Mathematical Sciences,
Nanyang Technological University,
637371
Singapore,
Singapore,
3
Singapore;
RMIT University,
Department of Physics, Schoolof Applied Sciences, Melbourne,
VIC 3000, Australia, Melbourne,
Australia; 4 School of Electrical andElectronic Engineering, Nanyang
Technological University, 639798
Singapore, Singapore, Singapore;
5
Optoelectronics Research Centre
and Centre for Photonic Metamaterials, University of Southampton,
SO17 1BJ, UK, Southampton, UK

14:00

2.04-μm single and dual-comb
modelocked InGaSb-MIXSEL∙M. Gaulke1 , J. Heidrich1 , N.
Huwyler1 , M. Schuchter1,2 , M.
Golling1 , A. Barh1 , and U. Keller1 ;1Department of Physics, Institutefor Quantum Electronics, ETH
Zürich,Zürich,Switzerland;
2
Optoelectronics Research Centre,
Physics Unit, Faculty of Engineeringand Natural Sciences, Tampere
University, Tampere, Finland
We present an InGaSb-MIXSEL operating at 2035 nm in single anddual-comb operation. In singlecomb operation we obtained 1.5-ps
pulses with an average output powerof 27 mW at 3.9 GHz repetition rate.

CB-2.2 MON

14:15

Recent developments on
MECSELs: Multi-type quantum
well gain structures for widely
tunable continuous wave
operation and a non-resonant
sub-cavity design∙H. Kahle1,2 , P. Rajala2 , P.
Tatar-Mathes2 , and M. Guina2 ;1Institute for Photonic Quantum
Systems (PhoQS), Center for
Optoelectronics
andPhotonics
Paderborn, and Department of
Physics,
Paderborn University,
Warburger Straße 100, Paderborn,
Germany; 2 Optoelectronics ResearchCentre (ORC), Physics Unit / Photonics, Faculty of Engineering andNatural Science, Tampere University,
66

Chair: Nathalie Vermeulen,Vrije
Universiteit Brussel, Belgium
CD-3.1 MON (Invited)

14:00

Nonlinear Photonics with
Lithium Niobate∙M. Loncar; Harvard University,
Cambridge, USAI will discuss recent progress withthin film lithium niobate photonic
platform, focusing on applications
in nonlinear photonics.

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/Europe-EQEC 2023

⋅ Monday 26 June 2023

Room 1 Hall B1 (B11)

Room 2 Hall B1 (B12)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

JSII-3: Manipulating astronomical signals with photonics
and future challenges II

CF-3: Complex pulses andtheir characterization

CL-1: Brain imaging

ED-3: Frequency references
and transfer

CE-3: Optical materials:
Structures

EB-3: Quantum optics I

Chair: Piotr Maslowski, Nicolaus
Copernicus University in Torun, Torum, Poland

Chair: Argyro Klini, IESL, FORTH,
Heraklion, Greece

ED-3.1 MON (Invited)CE-3.1 MON

Chair: Lucas Labadie, University of
Cologne, Köln, Germany

Chair: Haim Suchowski, Tel Aviv
University, Israel

JSII-3.1 MON (Invited) 14:00

CF-3.1 MON

What it takes to observe exoplanets with optical interferometry∙S. Lacour; Observatoire de Paris,
Meudon, France
I will present the lessons learned
from the GRAVITY interferometer,
focusing on the science case of exoplanet detection. I will show how
photonics were crucial to enable
this.

Electro-Optic Sampling of
Femtosecond Electric-Field
Transients Generated in a
Synchronously-Pumped OpticalParametric Oscillator∙H. Kempf1 , F. Breuning1 , A.
Muraviev2 , K. Vodopyanov2 , and
1
A. Leitenstorfer1 ;Departmentof Physics and Center for Applied
Photonics, University of Konstanz,
2
Konstanz, Germany;
CREOL,
College of Optics and Photonics,
University of Central Florida,
Orlando, USA
We generate intense and phaselocked mid-infrared waveforms
pumping a divide-by-two opticalparametric oscillator with a passively phase-stable Er:fiber source.
Few-femtosecond
near-infrared
probes sensitively resolve theoctave-wide electric-field traces ofthese transients in electro-optic
sampling.

CF-3.2 MON (Invited)

14:00

Chair: Kenneth K. Y. Wong, The University of Hong Kong, China

CL-1.1 MON (Invited)

14:00

Reconstructing brain tissue withlight microscopy∙J.G. Danzl; Institute of Science andTechnology Austria, Klosterneuburg,
Austria
Brain tissue constitutes an extremelycomplex and dense arrangement ofneurons, forming the informationprocessing network underlying all
brain function.
I will present
our developments of optical superresolution technologies to decode
brain tissue architecture and dynamics.

14:00

Precise Comb-based Time
Transfer Over Long Distance
Terrestrial Links
E.D. Caldwell1,2 , J.-D. Deschenes3 ,J. Ellis1 , W.C. Swann1 , B.K. Stuhl4 ,H. Bergeron3 , N.R. Newbury1 , and∙L.C. Sinclair1 ; 1 National Instituteof Standards and Technology, Boulder, USA; 2 Department of Electrical, Energy and Computer Engineering, University of Colorado, Boulder, USA; 3 Octosig Consulting, Quebec City, Canada; 4 Space Dynamics
Laboratory, North Logan, USA
We present a quantum-limited approach to frequency comb-based
optical time transfer. Operating
at nearly the quantum-limit, wedemonstrate femtosecond synchronization of 300-km distant opticaltimescales with received powers of
only a few hundred femtowatts.

14:15

Sampling Mid-infrared Waveforms in Time and Space
Y. Liu1 , ∙S. Gholam-Mirzaei2 , D.
Khatri1 , T.-C. Truong1 , A. Staudte2 ,P. Corkum2 , and M. Chini1 ;1University of Central Florida,
Orlando, USA; 2 National ResearchCouncil of Canada and University ofOttawa, Ottawa, Canada
We demonstrate that multiphoton
excitation in a CMOS image sensor
can be used as a sub-cycle temporal gate, allowing the measurementof the full space, time, and polarization state of structured mid-infraredlaser waveforms.

14:00

EB-3.1 MON

14:00

Covalent Organic Frameworkwith Polarization Dependence for
Ultrafast Pulse generation∙H.-S. Wang1 , A.F.M.E. Mahdy2 , S.W. Kuo2 , G.-R. Lin3 , and C.-K. Lee1 ;1Department of Photonics, National
Sun Yat-sen University, Kaohsiung,Taiwan; 2 Department of Materials
and Optoelectronic Science, National
Sun Yat-Sen University, Kaohsiung,Taiwan; 3 Graduate Institute of Photonics and Optoelectronics and Department of Electrical Engineering,
National Taiwan University, Taipei,
TaiwanWe successfully generate modelocked pulses at 1.5μm using aunique covalent–organic framework (COF)-based SA withpolarization dependence, showcasing the potential of COFs as
a promising platform in ultrafast
photonics applications.

Generation and parallel
manipulation of frequency
entangled qubits from a 21 GHz
Silicon-On-Insulator
micro-resonator∙A. Henry1,2 , D. Fioretto2 , L.
Proccopio3 , S. Montfray4 , F. Boeuf4 ,L. Vivien2 , E. Cassan2 , C. Ramos2 ,K. Bencheikh2 , I. Zaquine1 , and1
N. Belabas2 ;Telecom Paris,
2
PALAISEAU,France;C2N,
3
PALAISEAU, France; Weizmann
Institute of Science, Tel Aviv, Israel;
4
STMicro-electronics,
Crolles,FranceWe leverage on 21-GHz free spectral range microring resonators forbroadband generation of frequencybin entangled photons. We use
electro-optics devices to manipulate
the generated states. We demonstrate an application of this systemfor quantum communication.

CE-3.2 MONEB-3.2 MON

14:15

High-Precision Measurement of
Birefringent Mode Splitting in an
Ultrastable High-Finesse Optical
Cavity with Crystalline Mirrors∙M. Prinz1 , M. Bober2 , D.
Charczun2 , P. Morzyński2 , M.
Narożnik2 , L.W. Perner1 , G.-W.
Truong3 , G.D. Cole3 , O.H. Heckl1 ,and P. Masłowski2 ; 1 Christian
Doppler Laboratory for Mid-IR
Spectroscopy and Semiconductor
Optics, Faculty Center for Nano
Structure Research, Faculty ofPhysics, University of Vienna, Vienna, Austria; 2 Institute of Physics,
Faculty of Physics, Astronomy
and Informatics, Nicolaus Copernicus University, Toruń, Poland;
67

Chair: Eugene S. Polzik, Niels Bohr
Institute, København, Danemark

14:15

A Franson interferometer forbroadband frequency-entangled
photon pairs∙L. Matheis, S. Gstir, G. Weihs, and
R. Keil; Universität Innsbruck, Innsbruck, Austria
We realised a Franson interferometer for narrow- (4.2 nm) and broadband (100 nm) frequency-entangled
photon pairs. In the broadband
case, dispersion altered the shapeof the interference pattern, whicharises from two distinct types of dispersive influences.

CLEO

Room 1 ICM

Room 4a ICM

14:30/Europe-EQEC 2023

Room 4b ICM

merization, of complex, high-resolution, and large-scale microstructures for versatile applications.

CM-3.3 MON®

Room 13a ICM

Understandingthenanoscalebehavior of helicity-dependent
photocurrents is important tounderstand light-matter interaction
in structured topological materials.
Here we report direct nanoimagingof the distribution of circular polarization dependent surface currents
on nanostructured topologicalinsulators.
CK-1.3 MON

14:30

EG-3.3 MON

Engineered dispersion measurements in LiNbO3 nanophotonic
wires∙H.R. Fergestad1 , W. Hänsel2 ,A. Kordts2 , A. Prencipe1 , R.
Holzwarth2 , and K. Gallo1 ; 1 KTH
Royal Institute of Technology,
Stockholm, Sweden; 2 Menlo Systems
GmbH, Martinsried, Germany
We engineer and measure group velocity dispersion (GVD) in lithium
niobate nanophotonic waveguides.
Using dual comb spectroscopy, wemeasure GVD at telecom wavelength for both TE00 and TM00
guided modes showing good agreement with simulations.

Coulomb-correlated multi-electron states generated by nanotip
photoemission∙R. Haindl1,2 , A. Feist1,2 , T.
Domröse1,2 , M. Möller1,2 , J.H.
Gaida 1,2 , S.V. Yalunin1,2 , and C.
Ropers1,2 ; 1 Max Planck Institutefor
Multidisciplinary
Sciences,
Göttingen, Germany; 2 4th PhysicalInstitute - Solids and Nanostructures,Georg-August-Universität
Göttingen, Göttingen, Germany
Femtosecond photoemission froma nanoscale field emitter generates few-electron pulses characterized by event-based spectroscopy.
The Coulomb-mediated final twoelectron state exhibits a pair energy of about 2 eV, facilitating
nanoscale electron probing with
sub-Poissonian beam statistics.

CM-3.4 MON

CK-1.4 MON

EG-3.4 MON

14:45

14:45

Low-loss compact lithium niobate
photonic integrated circuits∙Y. Gao, F. Lei, M. Girardi, R.
Van Laer, V. Torres-Company,
and J. Schröder; Department ofMicrotechnology and Nanoscience(MC2), Chalmers University ofTechnology, Gothenburg, Sweden
We demonstrated a compact fullyetched lithium niobate platform
with mean propagation losses down
to 8.4 dB/m. The highest Q/Vmicro-ring resonator and highest
repetition rate soliton microcomb
in LN have been demonstrated.

CA-3.2 MON

Room 13b ICM

14:30

Tm:CALGO: Spectroscopy andLaser Operation at 2.32 μm∙H. Dupont1 , P. Loiko2 , Z. Pan3 ,H. Chu3 , D. Li3 , L. Giordano4 , B.
Viana4 , A. Hideur5 , L. Guillemot2 ,A. Braud2 , P. Camy2 , P. Georges1 ,and F. Druon1 ; 1 Université ParisSaclay, Institut d’Optique Graduate
School, CNRS, Laboratoire Charles
Fabry, Palaiseau, France; 2 CIMAP,UMR 6252 CEA-CNRS-ENSICAEN,
Université de Caen, 6 Boulevard
Maréchal Juin, Caen, France;
3
School of Information Science andEngineering, Shandong University,
Qingdao, China; 4 Chimie ParisTech,PSL University, CNRS, Institut deRecherche de Chimie Paris, 11 rue
Pierre et Marie Curie, Paris, France;
5
CORIA UMR6614, CNRS-INSAUniversité de Rouen, Normandie
Université, Avenue de l’université,Saint Etienne du Rouvray, France
We achieved laser emission at 2.3
μm using a Tm:CALGO crystal. To
have a deeper understanding of theprocess, we have performed spectroscopic measurements and examined different pumping methods,
including direct and upconversion
pumping.

14:30

Volumetric modification ofshaped and dual wavelength ultrashort laser pulses in fused silica∙M. Zukerstein1 , V. Zhukov1,2,3 , and
N. Bulgakova1 ; 1 HiLASE Centre,
Institute of Physics ASCR, Dolni
Brezany, Czech Republic; 2 Federal
Research Center for Information
and Computational Technologies,
Novosibirsk, Russia; 3 Novosibirsk
State Technical University, Novosibirsk, Russia
In this experimental and theoretical work, we show the effect of different wavelengths and pulse shapes
on volumetric modification in fusedsilica. The results can be important
for the purposes of laser writing processes.

Laser machining of sub-micrometric-pitch structures with atruncated ultrafast Bessel beam in
the bulk of fused silica∙S. Datta, R. Clady, O. Utéza, and N.
Sanner; LP3, Marseille, France
We demonstrate in-volume laserfabrication of dense periodic structures in bulk fused silica in femtosecond ablation regime. Using alength-controlled Bessel beam, regular arrangements of nanochannels
stacked with a pitch down to 0.7 μm
are demonstrated.

⋅ Monday 26 June 2023

14:45

CA-3.3 MON

Atomic Fluctuations and Light
Emission in Electrically Excited
Plasmonic Nanojunction∙S.P. Amirtharaj, X. Zhiyuan, and
C. Galland; École polytechnique
fédérale de Lausanne, Lausanne,
Switzerland
We demonstrate overbias light emission from electrically driven selfassembled molecular junctions. We
further investigate atomic fluctuations in the metal-molecule interface via simultaneous light emission
spectroscopy and conductance measurements.

14:45

Tm,Ho:(Y,Sc)2O3 ceramic laser at~2.1 μm∙K. Eremeev1 , P. Loiko1 , R.
Maksimov2,3 , V. Shitov2 , V. Osipov2 ,P. Camy1 , and A. Braud1 ; 1 Centre deRecherche sur les Ions, les Matériaux
et la Photonique (CIMAP), UMR
6252 CEA-CNRS-ENSICAEN, Université de Caen Normandie, Caen,
France; 2 Institute of Electrophysics,
Ural Branch of the Russian Academyof Sciences, Ekaterinburg, Russia;
3
Ural Federal University named
after the first President of Russia B.
N. Yeltsin, Ekaterinburg, Russia
Tm3+,Ho3+-codoped
yttria68

Room 14a ICM

Kor-keakoulunkatu 3, Tampere,
Finland
MECSELs have experienced rapid
progress during the last years. The
most important recent progress, like
continuous wave broadband tuning(Δλ > 86 nm around λ0 = 985 nm)
and anti-resonant gain membrane
design will be discussed.

CB-2.3 MON (Invited)

14:30

The quest for ultraviolet verticalcavity surface-emitting lasers∙Å. Haglund1 , F. Hjort1 , J. Enslin2 ,M. Bergmann1 , M. Cobet2 , G.
Cardinali2 , N. Prokop2 , L. Persson1 ,E. Torres1 , S. Graupeter2 , M.
Grigoletto2 , M. Guttmann2 , L.
Sulmoni2 , N. Lobo-Ploch3 , T.
Kolbe3 , J. Ciers1 , T. Wernicke2 , and
M. Kneissl2,3 ; 1 Chalmers Universityof Technology, Gothenburg, Sweden;
2
Technische Universität Berlin,
3
Berlin, Germany;
FerdinandBraun-Institut, Berlin, Germany
We will summarize state-of-the-art
results and focus on our method
to simultaneously achieve highreflectivity mirrors and cavity
length control by electrochemical etching and show the firststeps towards an electricallydriven ultraviolet vertical-cavity
surface-emitting laser.

CD-3.2 MON

14:30

High-Efficiency Second Harmonic
Generation in HeterogeneouslyIntegrated Periodically-Poled
Lithium Niobate on Silicon
Nitride∙T.
Vandekerckhove1,2 ,T.
Vanackere1,2 , J. De Witte1 , I.
Luntadila Lufungula1 , E. Vissers1 ,G. Roelkens1 , S. Clemmen1,2 , andB. Kuyken1 ; 1 Ghent University,
Ghent, Belgium; 2 Universite Libre deBruxelles, Brussels, Belgium
CMOS-compatible photonic platforms such as silicon nitride lacka χ (2) nonlinearity. We heterogeneously integrate periodically-poledlithium niobate on silicon nitride
through a back-end micro-transfer
printing process and achieve second harmonic generation with 2500%/Wcm2 efficiency.

CD-3.3 MON

14:45

Terahertz physics with thin-filmlithium niobate - custom-tailoredgeneration and sensitive detection
on-chip∙A. Herter1 , A. Shams-Ansari2 ,F.F. Settembrini1 , H.K. Warner2 ,J. Faist1 , M. Loncar2 , and I.-C.
Benea-Chelmus3 ; 1 ETH Zürich,Institue of Quantum Electronics,
Zurich, Switzerland; 2 Harvard John
A. Paulson School of Engineeringand Applied Sciences, Harvard
University, Cambridge, MA, USA;
3
EPF Lausanne, Hybrid Photonics
Laboratory, Lausanne, Switzerland
We present integraded nonlinear

CLEO

Room Osterseen ICM

Room 1 Hall B1 (B11)®

/Europe-EQEC 2023

Room 2 Hall B1 (B12)⋅ Monday 26 June 2023
Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)Thorlabs Crystalline Solutions,
Santa Barbara, CA, USA
We report temperature-resolved
high-precision measurements ofbirefringent cavity mode shifts ofan ultrastable high-finesse opticalcavity with substrate-transferredcrystalline supermirrors in thenear-infrared wavelength range, by
mapping the cavity modes with an
optical frequency comb.
3

JSII-3.2 MON

14:30

CL-1.2 MON

Towards the development of theself-calibrating nulling interferometry beam combiner for the
VLTI visitor instrument ASGARD
to detect exoplanets∙S. Ahmed1,2 , S. Gross2 , M.
Withford2 , D. Defrère3 , and L.
Labadie1 ; 1 University of Cologne,
Köln, Germany; 2 Macquarie University, Sydney, Australia; 3 KU Leuven,
Leuven, Belgium
Using 3D ultrafast laser inscription, an achromatic behaviouralbeam combining device is being
developed for the NOTT of ASGARD/VLTI visiting instrument
using self-calibrating 4-telescopenulling interferometry technique
for the high-contrast exoplanet
detection in the mid-infrared(3.5-4.0~μm).

JSII-3.3 MON

14:45

Ultrafast Laser Inscription of
Achromatic Phase Shifters∙G. Douglass1,2 , T. Klinner-Teo3 , E.
Arcadi2 , M.J. Withford2 , B. Norris3 ,P. Tuthill3 , M.-A. Martinod3 , O.
Guyon4 , and S. Gross1,2 ; 1 School ofEngineering, Macquarie University,
Sydney, Australia; 2 School of Mathematics, Macquarie University, Sydney, Australia; 3 Sydney Institute for
Astronomy, School of Physics, University of Sydney, Sydney, Australia;
4
National Astronomical Observatoryof Japan, Subaru Telescope, Hawaii,
USA
Using ultrafast laser inscription a

CF-3.3 MON

14:45

Temporal Characterization of
Sub-3-fs, μJ-level Deep UV Pulses
Generated by Resonant Dispersive
Wave Emission∙M. Pini1,2 , F. Cappenberg1 , L.
Colaizzi1 , F. Vismarra1,2 , M.
Lucchini1,2 , A. Crego2 , C. Brahms3 ,J. Travers3 , R. Borrego Varillas2 ,M. Reduzzi1 , and M. Nisoli1,2 ;1Department of Physics, Politecnico
di Milano, Milan, Italy; 2 Institutefor Photonics and Nanotechnologies,
IFN-CNR, Milan , Italy; 3 School ofEngineering and Physical Sciences,
Heriot-Watt University, Edinburgh,
United Kingdom

14:30

EB-3.3 MON (Tutorial) 14:30

Implantable Nanophotonic
Neural Probes with 3D-Printed
Microfluidics∙X. Mu1,2 , F.-D. Chen1,2 , K.M.
Dang1 , M.G.K. Brunk1 , J. Li1 ,H. Wahn1 , A. Stalmashonak1 , P.
Ding1,2 , X. Luo3 , G.-Q. Lo3 , J.K.S.
Poon1,2 , and W.D. Sacher1 ; 1 Max
Planck Institute of Microstructure
Physics, Halle (Saale), Germany;
2
Department of Electrical andComputer Engineering, Universityof Toronto, Toronto, Canada;
3
Advanced Micro Foundry Pte. Ltd.,Singapore, Singapore
We present implantable nanophotonic neural probes with integrated
silicon nitride photonic waveguidegrating emitters and 3D-printed microfluidic channels. Simultaneouslight and fluid delivery from theneural probes is demonstrated.

14:30

ED-3.2 MON

Fully-digital implementation of a
Doppler cancellation techniquefor local ultra-stable frequency
dissemination∙M. Matusko, I. Ryger, G. GoavecMerou, J. Millo, C. Lacroûte, É.
Carry, J.-M. Friedt, and M. Delehaye; FEMTO-ST, Besancon, France
We demonstrate a fully-digital setup
for local frequency dissemination
over optical fiber with instabilities
in the 1E-18 range and implement a
novel characterization method that
does not require access to the remote fiber end.

Nanostructured optical coatings
for spatial filtering and polarization control∙L. Grineviciute1 , J. Nikitina1 , C.
Babayigit3 , D. Gailevičius2 , and
K. Staliunas4 ; 1 Center for Physical Sciences and Technology, Vilnius, Lithuania; 2 Vilnius University, Vilnius, Lithuania; 3 Universityof California, Irvine, USA; 4 ICREA,
Barcelona, Spain
Proposed 1D and 2D photonic
structures, based on dielectric
single- and multi-layers, can beconsidered as a promising component for intracavity spatial filteringand polarization control even inhigh power microlasers

Attosecond Sciences, Quantum
Optics and Quantum Information∙M. Lewenstein; Instituto de Ciencias Fotónicas, Castelldefels, Spain;
ICREA, Barcelona, Spain
I my tutorial i will discuss recent
developments of attosecond scienceon the border between ultrafast laser
science, quantum optics and quantum information

CL-1.3 MON

ED-3.3 MON

CE-3.4 MON

14:45

Out-of-Plane Focusing Grating on
Implantable Neural Probes for
Spatially Targeted Optogenetic
Stimulation∙T. Xue1,2 , A. Stalmashonak1 , P.
Ding1,2 , W. Sacher1 , and J. Poon1,2 ;1Max Planck Institute of Microstructure Physics, Halle, Germany;
2
Department of Electrical andComputer Engineering, University ofToronto, Toronto, Canada
We demonstrate an implantableneural probe with gratings forout-of-plane focusing in fixed
brain tissue for spatially precise
optogenetic experiments. A mini-

14:30

14:45

Hertz Level Dual Polarization
Brillouin Fiber Laser∙J. Lampen1 , P. Li1 , J. Jiang1 , A.
Rolland2 , and M. Fermann1 ; 1 Imra
America Inc., Ann Arbor, USA;
2
Boulder Research Labs, Imra America Inc., Longmont, USA
We demonstrate a dual polarization
Brillouin fiber laser with approximately 1 Hz intrinsic linewidth,suitable for self-referenced temperature sensing at the 20 nK level for
operation with record short- andlong-term frequency stability.

69

CE-3.3 MON

14:45

First demonstration of Type-A
femtosecond-written Volume
Bragg Gratings using a
Gaussian-Bessel laser beam
∙J. Harb1 , L. Talbot 2 , Y. Petit1,3 ,M. Bernier2 , and L. Canioni1 ;1University of Bordeaux, CNRS,
CEA, CELIA, UMR 5107, 351
Cours de la Libération,
33405
Talence, Cedex, France; 2 Centre
d’Optique, Photonique et Laser(COPL), Université Laval, Québec
City, Québec G1V0A6, Canada;
3
University of Bordeaux, CNRS,ICMCB, UMR 5026, 87 avenue duDr. A. Schweitzer, 33608 Pessac,

CLEO

Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Monday 26 June 2023
Room 13a ICM

Room 13b ICM

Room 14a ICM

scandia transparent ceramic wasprepared by solid-state vacuum
sintering at 1750 ∘ C. The ceramic
laser generated 291 mW at 2.09 μm
with 54.3% slope efficiency. The
laser wavelength was tuned over
1937.6–2128.0 nm.

CM-3.5 MON

15:00

Writing chiral nanostructuresinside silica with polarizationengineered Bessel beams∙M. Hassan1 , J. Lu2 , B. Poumellec2 ,M. Lancry2 , and F. Courvoisier1 ;1
FEMTO-ST
Institute,
Univ.
Franche-Comte and CNRS, Besan2con, France; Institut de Chimie
Moléculaire et des Matériaux
d’Orsay, Université Paris Saclay,
Orsay, France
We exploit space varying birefringent waveplates in combination with
Bessel beam to shape the polarization of a femtosecond laser along theoptical path. This allows us inscribing nanostructures in silica with chiral optical properties.

CK-1.5 MON

15:00

Tailoring guided-wave Fano
resonances in LiNbO3
nanophotonic wires∙T. Li, A. Prencipe, and K. Gallo;
KTH Royal Institute of Technology,
Stockholm, Sweden
We demonstrate with theory and experiment, Bragg grating nanowires
in thin film lithium niobate thatgive rise to engineerable Fano resonances at telecom C-band, enabledby the TE-TM mode coupling via
their longitudinal field components.

EG-3.5 MON

15:00

CA-3.4 MON

Efficient and Continuous CarrierEnvelope Phase Control for Terahertz Lightwave-Driven Scanning
Probe Microscopy∙J. Allerbeck1 , J. Kuttruff2 , L.
Bobzien1 , L. Huberich1 , M. Tsarev2 ,and B. Schuler1 ; 1 Empa - Swiss
Federal Laboratories for Materials
Science and Technology, Dübendorf, Switzerland; 2 University ofKonstanz, Konstanz, Germany
Frustrated internal reflection enables precise and efficient THz phase
control for ultrafast scanning tunneling microscopy, allowing stateselective investigation of quantum
dynamics with picosecond time andatomic spatial resolution at multiMHz repetition rate.

15:00

Power Limits of Compact
Ho3+ :YAG Laser Resonators With
Homogeneously Doped andSegmented Crystals∙K. Goth1,2 , M. Griesbeck1 , M.
Rupp1,2 , M. Eitner1 , M. Eichhorn1,2 ,and C. Kieleck1 ; 1 Fraunhofer IOSB(Institute of Optronics, System Technologies and Image Exploitation), Ettlingen, Germany; 2 Institute of Control Systems, Karlsruhe Institute ofTechnology, Karlsruhe, Germany
We present Ho3+ :YAG laser resonators with a homogeneously
doped and a segmented crystal andinvestigate them concerning theirpower limitation while maintaining
an excellent beam quality.
Amaximum output power of 57.6 W
is reached with the homogeneous
crystal.

70

THz generation and detecton on
thin-film lithium niobate. The arrangement of THz antennas andwaveguide design allow control overthe generated THz waveform, while
the on-chip confinement enhances
the interaction of the mixing fields.

CB-2.4 MON

15:00

VCSELs with integrated surface
gratings for polarization
dynamics above 65 GHz∙N.
Manrique-Nieto1 ,M.
Lindemann1 , N. Jung1 , T. Pusch2 , R.
Michalzik2 , M.R. Hofmann1 , andN.C. Gerhardt1 ; 1 Photonics and Terahertz Technology, Ruhr-Universitat
Bochum, Bochum, Germany; 2 Inst.
of Functional Nanosystems, Ulm
University, Ulm, Germany
Polarization dynamics above 65
GHz were observed in currentdriven VCSELs with birefringent
surface gratings after optical spin
injection. The results demonstrate
the potential of surface grating
spin-VCSELs for high-bandwidthpolarization-based optical datacom.

CD-3.4 MON

15:00

Generation and engineering ofpolarization entangled photons
from a lithium niobate nonlinear
metasurface∙J. Ma, J. Zhang, Y. Jiang, T. Fan,
M. Parry, D. N. Neshev, and A.
A. Sukhorukov; The Australian National University, Canberra, Australia
We reveal that an ultrathin lithium
niobate metasurface with multiplexed metagratings featuring different orientations allows the engineering of bi-photon polarization states and optically controllable
generation of arbitrary polarization
qutrits, overcoming the limitationsof current sources.

CLEO

Room Osterseen ICM≈2 mm long 180∘ differential achromatic phase shifter was fabricatedin borosilicate glass, that exhibits ameasured phase shift of 171 ± 6∘ between 1440-1640 nm.

JSII-3.4 MON

15:00

Development of a Fiber
Connectorized Ultrafast Laser
Inscribed 2 Telescope Beam
Combiner for the CHARA
Telescope array∙A. Benoit1 , J. Siliprandi1 , D.G.
MacLachlan1 , C.A. Ross1 , T.K.
Sharma2 , L. Labadie2 , K. Madhav3 ,A.S. Nayak3 , A.N. Dinkelaker3 ,M.M. Roth3 , E. Pedretti4 , T.A. ten
Brummelaar5 , N.J. Scott5 , V. Coudé
du Foresto6 , and R.R. Thomson1 ;1SUPA, Institute of Photonics andQuantum Sciences, Heriot-Watt
University,
Edinburgh,
UnitedKingdom; 2 I. Physikalisches Institut
der Universität zu Köln, Zülpicher
Strasse 77, Cologne, Germany;
3
Leibniz-Institut für Astrophysik
Potsdam, An der Sternwarte 16,
Postdam, Germany; 4 UKRI STFC
Rutherford Appleton Laboratory,
Chilton, United Kingdom; 5 Centerfor High Angular Resolution Astronomy, Georgia State University,
Atlanta, USA; 6 LESIA of Paris
Observatory/CNRS/UPMC/Univ.
Paris Diderot, Paris, France
We report on the complete design and fabrication of an efficient
fiber-connectorized 2-telescope Kband integrated-optics beam combiner manufactured using ultrafast laser inscription in combination
with selective chemical etching to
produce high contrast interferometric visibility.

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)

Room 2 Hall B1 (B12)

We demonstrate the generation of
sub-3 fs UV pulses obtained by
Resonant Dispersive Wave emission
in gas-filled Hollow Core Fibers,
tuneable between 230 and 430 nm
and characterized using an allin-vacuum Self-Diffraction FROG
technique.

mum beam waist of 4.3μm×5.2μm(FWHM) at a wavelength of 488nm
was achieved.

CF-3.4 MON

CL-1.4 MON

15:00

An in-situ method for thereconstruction of ultrashort andultrabroadband synthesized lighttransients∙M. Kubullek1,2 , F. Scheiba1,2 , M.A.
Silva-Toledo1,2 ,R.E. Mainz1,2 ,G.M. Rossi1,2 , and F.X. Kärtner1,2 ;1Center for Free-Electron Laser
Science CFEL, Deutsches Elektronen Syncrotron DESY, Hamburg,
Germany; 2 Physics Department and
The Hamburg Centre for Ultrafast
Imaging (CUI), Hamburg, Germany
We present a method for full insitu characterization of the electric field waveform from a parametric waveform synthesizer by thirdorder cross-correlation of the underlying few-cycle pulses in a noble
gas target.

⋅ Monday 26 June 2023
Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)
Cedex, France
To our knowledge, we report thefirst Type-A Volume Bragg grating
inscribed in silver-containing phosphate glasses using Gaussian-Besselbeam. Diffraction efficiency of 95%
at 632.8 nm was achieved indicating a strong refractive-index modulation of 1.78x10^-3.

15:00

ED-3.4 MON

Biophotonic platform for detection of hallmarks of Alzheimer’s
disease via combined microfluidics and nanofunctionalized
fiber sensors
D. Santano Rivero1 , L. Zu2 ,J. Xie2 , P. Liu2 , X. Zhang2 , L.
Shi2 , A.B. Socorro Leránoz1 , I.R.
Matias1 , A. Giannetti3 , F. Baldini3 ,E. Santamaría4 , J. FernándezIrigoyen4 , K. Li5 , W. Bi6 , D. van den
Hove7 , I. Del Villar1 , T. Guo2 , and∙F. Chiavaioli3 ; 1 Public Universityof Navarra, Electrical and Electronic
Engineering Dept. and Instituteof Smart Cities (ISC), Pamplona,
Spain; 2 Jinan University, Institute of
Photonics Technology, Guangzhou,
China; 3 National Research Councilof Italy (CNR), Institute of Applied
Physics “Nello Carrara”, Sesto
Fiorentino, Italy; 4 Public Universityof Navarra, Navarrabiomed, Hospital Universitario de Navarra (HUN),
Pamplona, Spain; 5 Jilin University,
Key Laboratory of Bionic Engineering of Ministry of Education, Jilin,
China; 6 The First Affiliated Hospitalof Jinan University, Departmentof Neurology, Guangzhou, China;
7
Maastricht University, Departmentof Psychiatrie & Neuropsychologie,
Maastricht, Netherlands
The
combinationofnanomaterials,
microfluidics
andsuitably-functionalized optical fiber
sensors enables the detection of
Alzheimer’s disease hallmarks incomplex biofluids with detection
limit below 10-12 M, hereby having
potential in early diagnosis andpersonalized medicine.

15:00

Ultrastable Femtosecond
Frequency Combs for Precision
Measurements in the Time andFrequency Domain∙S.R. Hutter1 , A. Seer2 , T. Koenig1 ,R. Herda2 , D. Hertzsch1 , H. Kempf1 ,R. Wilk2 , and A. Leitenstorfer1 ;1Department of Physics and Center for Applied Photonics, Konstanz,
Germany; 2 Toptica Photonics AG,
Gräfelfing, Germany
We study the noise properties ofmodelocked fiber lasers systematically varying pump power and intracavity dispersion. Our insights leadto tailor-designed femtosecond frequency combs featuring quantumlimited optical linewidths below 1
kHz over ultrabroadband spectral
ranges.

71

CE-3.5 MON

15:00

Polarization-dependent
photoluminescence in
ZnO-ZnWO4 eutectic∙E. Petronijevic1 , M. Tomczyk2,3 ,A. Belardini1 , P. Osewski4 , P.
Piotrowski2,3 ,M.
Centini1 ,G. Leahu1 , R. Li Voti1 , D.A.
Pawlak2,3,4 , C. Sibilia1 , and M.C.
Larciprete1 ; 1 Univesità di Roma
La Sapienza, SBAI Department,
Rome, Italy; 2 Centre of Excellence
ENSEMBLE3, Warsaw, Poland;
3
Department of Chemistry, University of Warsaw, Warsaw, Poland;4Łukasiewicz Research Network –Institute of Microelectronics andPhotonics, Warsaw, Poland
We investigate emission propertiesof self-organized ZnO-ZnWO4 eutectic, made of ZnO lamellae in biaxial ZnWO4 matrix. The refractive
index matching in the microstructured composite leads to strong polarization dependence in both excitation and generated photoluminescence.

Room 8 Hall A1 (A12)CLEO

Room 1 ICM
CM-3.6 MON®

Room 4a ICM
15:15

Bessel beam dielectric cuttingwith femtosecond laser in
GHz-burst mode
∙P. Balage1 , J. Lopez1 , G. Bonamis2 ,C. Hönninger2 , and I. Manek1
Hönninger1 ;UniversitédeBordeaux-CNRS-CEA,
CELIA
UMR 5107, Bordeaux, France;
2
Amplitude, Pessac, France
We report, for the first time up
to our knowledge, on the use of
a Bessel beam with a femtosecond
laser operating in GHz-burst modefor cutting of glasses and sapphire.

CK-1.6 MON/Europe-EQEC 2023

⋅ Monday 26 June 2023

Room 4b ICM
15:15

Far-field petahertz sampling ofplasmonic fields∙K.-F. Wong1,2 , W. Li3,4 , Z. Wang3,4 ,V. Wanie2 , E. Månsson2 , D. Höing1,5 ,J. Blöchl3,4 , T. Nubbemeyer3,4 , A.
Trabattoni2,6 , H. Lange1,5 , F.
Calegari1,2 , and M.F. Kling3,4,7 ;1
The Hamburg Centre for Ultrafast
Imaging,
Hamburg,
Germany;
2Center for Free-Electron Laser
Science, Hamburg, Germany; 3 Max
Planck Institute of Quantum Optics, Munich, Germany; 4 LudwigMaximilians-Universität München,
Munich, Germany; 5 Institute ofPhysical Chemistry Universität
Hamburg, Hamburg, Germany;
6
Institute of Quantum Optics
Leibniz Universität Hannover, Hannover, Germany; 7 SLAC National
Accelerator Laboratory Stanford
University, Menlo Park, USA
We demonstrate the realtime observation of linear plasmonic fields by
optical field sampling. Our findings
also demonstrate the ability to manipulate the spectral properties ofultrashort laser pulses by plasmonic
samples.

EG-3.6 MON

Room 13a ICM
15:15

CA-3.5 MON

Effect of the Gouy-phase on
field-induced transport across ananojunction∙A. Rossetti1 , M. Ludwig2,3 , A.
Leitenstorfer2 , and D. Brida1 ;1
University of Luxembourg, Luxembourg, Luxembourg; 2 Universityof Konstanz, Konstanz, Germany;3
Deutsches Elektronen-Synchrotron
DESY, Hamburg, Germany
Carrier-envelope-phasestablesingle-cycle laser pulses are
employed to coherently control
field-induced current across ananojunction. Scanning the sample
position along the focus, the effectof the Gouy phase on the transport
process is investigatedRoom 13b ICM
15:15

Growth and efficient 1 μm laser
operation of Yb-doped mixed
sesquioxides∙A. Uvarova, P. Eckhof, L. Hülshoff,
P. Wegener, S. Kalusniak, and C.
Kränkel; Leibniz-Institut für Kristallzüchtung (IKZ), Berlin, Germany
We report on the Czochralskiand micro-pulling-down growthand laser operation of Yb3+ -doped(Scx Y1−x )2 O3 single-crystals. The
crystals were characterized spectroscopically. In laser experiments, we
obtained 1.2 W of output power at
89% of slope efficiency.

CB-2.5 MON

Room 14a ICM
15:15

Single-frequency 2 μm
GaSb-based VECSEL for
quantum-frequency-converter
pumping∙S. Adler, P. Holl, E. Diwo-Emmer,
A. Bächle, and M. Rattunde; Fraunhofer Institute for Applied Solid State
Physics IAF, Freiburg, Germany
Design and improvements of narrow linewidth VECSEL modules
based on the (AlGaIn)(AsSb) material system with 2 μm emission
wavelength for quantum frequency
conversation are shown

CD-3.5 MON

15:15

Towards
two-photon-absorption-freehybrid silicon nitride waveguides
reaching silicon Kerr nonlinearity∙M. Dyatlov1,2 , K. Stoll3 , P. Delaye4 ,J. Hu3 , S. Serna3,5 , L. Vivien2 ,and N. Dubreuil1 ; 1 LP2N, Institutd’Optique Graduate School, Université de Bordeaux, CNRS, Talence,France; 2 Centre de Nanosciences
et de Nanotechnologies, Université
Paris-Saclay, CNRS, Palaiseau,
France; 3 Materials Science and Engineering Department, Massachusetts
Institute of Technology , 77 Massachusetts Avenue, Cambridge, MA,
USA; 4 Laboratoire Charles Fabry,
Institut d’Optique Graduate School,
Université Paris-Saclay,
CNRS,
Palaiseau, France; 5 Bridgewater
State University, Physics andPhotonics and Optical Engineering
Department, Bridgewater, MA, USA
A highly-nonlinear hybrid silicon
nitride waveguide with GeSbS
cladding showing no TPA isreported, enriching possibilities
for the integrated optical circuits
development. We demonstrate suchan increase in nonlinear index witha highly-accurate method.

Room 1 ICM
16:00 – 17:30

PL-1.1 MON (Plenary)

PL-1: CLEO/Europe 2023 Plenary

From Nonlinear Optics to High-Intensity Laser
Physics∙D. Strickland; University of Waterloo, Waterloo, Canada
In this talk, I will discuss the differences between non-

Chair: Rachel Grange, ETH Zurich, Switzerland andCrina Cojocaru, Universitat Politecnica de Catalunya,
Barcelona, Spain

16:00

linear optics and high-intensity laser physics. The development of CPA and why short, intense laser pulses cancut transparent material will also be included.

Room 4a ICM
17:30 – 18:30

PL-C.break1 MON

PL-C: Career event with Donna Strickland

PhD students wanting to interact with Donna
Strickland about career are cordially invited.
Registration mandatory.
∙D. Strickland; University of Waterloo, Waterloo, Canada

Chair: Marian Marciniak, National Institute of Telecommunications, Warsaw, Poland ; Crina Cojocaru, Universitat Politecnica de Catalunya, Barcelona, Spain

17:30

72

Move to Room 4a to meet with Donna Strickland (Career event for PhD students)

CLEO

Room Osterseen ICM
JSII-3.5 MON

15:15

A Metasurface-based Scalar
Vortex Phase Mask Design∙L. König1 , O. Absil1 , N. Desai2 ,D. Mawet2 , S. Palatnick3 , and M.
Millar-Blanchaer3 ; 1 STAR Institute,
University of Liège, Liège, Belgium;
2
California Institute of Technology,
Pasadena, USA; 3 University of California at Santa Barbara, Santa Barbara, USA
We propose a metasurface-based
implementation of the scalar vortex phase mask for high contrast
imaging using square nanoposts andshow that it is a promising approachto the challenge of achromatizing
the scalar vortex coronagraph.

Room 1 Hall B1 (B11)
CF-3.5 MON

15:15

Ultrashort laser vector pulses
characterization with amplitude
swing∙C. Barbero, B. Alonso, and Í.J. Sola;
Grupo de investigación en Aplicaciones del Láser y Fotónica, Salamanca, Spain
Ultrashort laser vector pulses, i.e.,
those exhibiting time-varying polarization, are interesting in many
scientific fields. We completely reconstruct those pulses using theamplitude swing technique, which
has a simple, robust, and versatile
scheme.

®

/Europe-EQEC 2023

Room 2 Hall B1 (B12)CL-1.5 MON⋅ Monday 26 June 2023
Room 6 Hall B3 (B32)

15:15

ED-3.5 MON

Transcranial diffuse correlation
imaging of cerebral blood flow
microcirculation in rodent
models
∙E. Zherebtsov1 , M. Kaakinen2 , A.
Sdobnov1 , O. Sieryi1 , T. Myllylä1,3 ,A. Bykov1 , and I. Meglinski1,4 ;1Optoelectronics and Measurement
Techniques Unit, University of Oulu,
Oulu, Finland; 2 Centre for CellMatrix Research, University of Oulu,
Oulu, Finland; 3 Health Sciences
and Technology Unit, University ofOulu, Oulu, Finland; 4 College ofEngineering and Physical Sciences,
Aston University, Birmingham,
United Kingdom
We present a transcranial visualization of cerebral blood flow using diffuse correlation spectroscopy
and laser speckle contrast imaging,which was validated in phantom
studies and in vivo in murine models.

15:15

Thin Cell Spectroscopy at
Telecommunication Wavelengths:
Towards Acetylene based
Compact Frequency References
G. Garcia Arellano, ∙H. Mouhanna,
F. DuBurck, B. Darquié, D. Bloch, I.
Maurin, and A. Laliotis; Laboratoirede Physique des Lasers, Villetaneuse,FranceWe probe rovibrations of acetylene,
confined inside a thin-cell of micrometric thickness, at telecommunication wavelengths. Molecularconfinement at the wavelength scale
allows for linear, high-resolution
spectroscopy making thin-cells attractive platforms for compact frequency referencing applications.

NOTES

73

Room 7 Hall A1 (A11)
CE-3.6 MON

15:15

Core-Shell Halide Perovskite
Nanocubes for Low-threshold
Lasing Applications∙S. Khan1,2 , M. Mohammadi1 ,S.B. Anantharaman1 , and M.C.
1
Lemme1,2 ;AMO GmbH,OttoBlumenthal Straße 25, 52074
Aachen, Germany, Aachen, Germany; 2 RWTH Aachen University,
Templergraben 55, 52062 , Aachen,
Germany
Here, in-situ formation of perovskite nanocubes during spin
coating from different halide
compositionsisinvestigated.
The core-shell heterojunctions in
CsPbBr3/CsPbBr3–xClx nanocubes
will be presented alongside their
optical properties, which open
new routes for low threshold lasing
applications.

Room 8 Hall A1 (A12)

CLEO

®

/Europe-EQEC 2023

⋅ Monday 26 June 2023

Hall B0
13:00 – 14:00
CA-P: CA Poster session
CA-P.1 MON

Difference Frequency Generation in BaGa4 Se7 ,LiGaSe2 , and LiGaS2 Tunable in a 5 - 13 μm Range
with Output Energy up to 100 μJ Pumped by 1.03
μm, 1.8 ps Laser∙M. Jelínek1 , M. Frank1 , V. Kubeček1 , O. Novák2 , J.
Huynh2 , M. Cimrman1,2 , M. Chyla2 , M. Smrž2 , and T.
Mocek2 ; 1 Czech Technical University in Prague, Faculty of
Nuclear Sciences and Physical Engineering, Prague, Czech
Republic; 2 HiLASE Centre, FZU - Institute of Physics of
the Czech Academy of Sciences, Prague, Czech Republic
We present difference frequency generation in
BaGa4 Se7 , LiGaSe2 , and LiGaS2 tunable in a spectral range from 5 to 13 μm pumped by a picosecond
1μm-laser
CA-P.2 MON

Instability study of a high-power, high repetition rate
fs-OPCPA driven tunable femtosecond UV source for
FEL seeding.
∙T. Lang, M. Kazemi, J. Zheng, S. Hartwell, N.-P. Hoang,
E. Ferrari, L. Schaper, and I. Hartl; Deutsches Elektronen
Synchrotron DESY, Hamburg, Germany
We present a start-to-end simulation of our highlyefficient, broadly-tunable, OPCPA-based UV laser system for FEL seeding, predicting the system performance
regarding tunability, beam-quality, stability and pointing based on measured CPA-pump laser and white-lightseeder fluctuations.
CA-P.3 MON

MW-peak and Watt-average Power LED-Pumped
Nd:YAG Laser
X.-L. Ho, M.-H. Wu, and ∙Y.-C. Huang; Institute of
Photonics Technologies, National TsingHua University,
Hsinchu, Taiwan
We report the generation of 3.5-MW peak power and
4.5-W average power in Q-switched and quasi-CW operation modes respectively, from a LED-pumped Nd:YAG
laser.
CA-P.4 MON

Buried Depressed-Cladding Waveguides Fabricatedin RE3+:CLNGG Laser Crystals using Direct Laser
Writing Technique∙G. Croitoru1 , I. Anghel2 , F.-M. Voicu1 , M. Greculeasa1 ,A. Broasca1 , L.-M. Gheorghe1 , and N. Pavel1 ; 1 National
Institute for Laser, Plasma and Radiation Physics, SolidState Quantum Electronics Laboratory, Magurele, Romania; 2 National Institute for Laser, Plasma and Radiation Physics, Nonlinear Optics and Photonics Laboratory,

Magurele, Romania
Depressed-cladding waveguides were inscribed in 0.7at.% Nd:Ca3Li0.275Nb1.775Ga2.95O12 (Nd:CLNGG)
and 4.3-at.% Yb:CLNGG crystals using direct-writing
technique with a femtosecond-laser beam. Laser emission at 1.06 and 1.03 μm was obtained, under the pumpwith fiber-coupled diode lasers.

The shortest generated pulses have 76 ns and pulse energy 56 μJ with corresponding peak power 0.72 kW.
CA-P.9 MON

Comparison of Ho:YLF and Ho:CaF2 for Single Pass
Amplification of 2 ps Pulses at 2065 nm∙M. Jelínek1 , M. Frank1 , V. Kubeček1 , Z. Zhonghan2 , D.
Jiang2 , and L. Su2 ; 1 Czech Technical University in Prague,
Faculty of Nuclear Sciences and Physical Engineering,
Prague, Czech Republic; 2 Key Laboratory of Transparent
and Opto-functional Inorganic Materials, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai,
China
Single pass amplification in an amplifier based on
Ho:YLF or Ho:CaF2 crystal operating at wavelength of
2065 nm seeded by 2ps pulses is presented.

CA-P.5 MON

Comparison of Self-Seeded Perfluorooctane SBSCompressor Configurations for Obtaining HighEnergy 90 ps Pulses
A. Černeckytė, ∙P. Mackonis, and A.M. Rodin; Center for
Physical Sciences and Technology, Vilnius, Lithuania
Self-seeding configurations of a perfluorooctane SBScompressor with a double-pass phase-conjugated
Nd:YAG amplifier provide up to 50 mJ, 94 ps output pulses from 2 mJ, 1.1 ns input. These pulses are
suitable for dermatology and interference patterning.

CA-P.10 MON

Spectral and laser properties of cryogenically cooled
Tm,Gd:SrF2 crystal∙K. Veselský1 , M. Jelínek1 , V. Kubeček1 , J. Šulc1 , H.
Jelínková1 , Y. Wang2,3 , Z. Zhang2 , and L. Su2,3 ; 1 Facultyof Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic; 2 StateKey Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics,
Chinese Academy of Sciences, Shanghai, China; 3 Center ofMaterials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
Temperature dependence (300 – 78 K) of spectral andlaser properties of a novel Tm,Gd:SrF2 crystal was investigated. A broad absorption spectrum and very long
lifetime was observed. Laser slope efficiency of 69 % wasachieved at 1868 nm.

CA-P.6 MON

Alexandrite Lasers Operating with High-power
Blue-diode-pumping∙H. Xiao, X. Jiang, and M. Damzen; Imperial College London, London, United Kingdom
We have demonstrated a blue-diode pumped Alexandrite laser with the highest power to date and performed
a full characterisation and analysis of laser performanceand prospects of blue as an alternative to red diodepumping.
CA-P.7 MON

μ-PD-grown Tm,Ho-doped Multicomponent Garnets
for Diode-pumped 2.1 μm Lasers∙J. Šulc1 , M. Němec1 , J. Pejchal2 , J. Havlíček2,3 , H.
Jelínková1 , M. Nikl2 , and K. Nejezchleb3 ; 1 Czech Technical University in Prague, FNSPE, Prague, Czech Republic;2
Institute of Physics AS CR, Division of Solid State Physics,
Prague, Czech Republic; 3 Crytur, Ltd. Turnov, Turnov,
Czech Republic
Set of new multicomponent garnets doped by Tm3+
and Ho3+ was grown using μ-PD method. In case ofTm,Ho:GLAG, Tm,Ho:GSAG, and Tm,Ho:LSAG lasing
at 2.1 μm under 0.8 μm diode pumping was successfully
demonstrated.

CA-P.11 MON

Gain-Switched Ti:Sapphire Microchip Laser:
Spectroscopic and Laser Characteristics within 5-300
K temperature range∙M. Fibrich1,2 , J. Šulc1 , and H. Jelínková1 ; 1 Czech Technical University in Prague, Faculty of Nuclear Sciences andPhysical Engineering , Prague, Czech Republic; 2 Extreme
Light Infrastructure ERIC, ELI Beamlines Facility, DolníBřežany, Czech Republic
Temperature influence on spectroscopic as well as lasing
properties of the gain-switched Ti:Sapphire microchip
laser are described in detail within 5-300 K crystal temperature range.

CA-P.8 MON

Electro-optically Q-switched Er:YLF laser at 2.8 μm∙R. Svejkar, D. Popelova, J. Sulc, D. Vyhlidal, M. Nemec,
and H. Jelinkova; Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague,
Prague, Czech Republic
Pockels cell electro-optically Q-switched Er:YLF laser
emitting at 2.8 μm was tested with 10 kHz repetition rate.

CA-P.12 MON

Amplification of a Pulsed Laser Source with aCompact Wedged Thin-Disk Amplifier∙R.-A. Lorbeer, B. Ewers, C. Santek, M. Augsburger, D.
Keil, J. Speiser, and T. Dekorsy; German Aerospace Center74(DLR), Institute of Technical Physics, Stuttgart, Germany
Solid state lasers as e.g. thin-disk lasers allow to achieve
high average power and high pulse energies for short andultra-short pulses. Here we investigate the amplificationof short laser-pulses with our compact wedged-thin-disk
amplifier.
CA-P.13 MON

5 kHz, 6.5 mJ Yb:CaYAlO4 dual-crystal regenerative
amplifier∙g. wang1 , w. tian1 , c. bai1 , y. yu1 , x. xu3 , z. wei2 ,and j. zhu1 ; 1 Xidian University, Xi’an, China; 2 Instituteof Physics, Chinese Academy of Sciences, Beijing, China;
3
Jiangsu Normal University, Xuzhou, China
This paper reports on a dual-crystal Yb:CALYO regenerative amplifier that delivering laser outputs with a pulse
energy of 5.3 mJ, a compressed pulse duration of 187 fs,
and a repetition rate of 5 kHz.
CA-P.14 MON

Versatile Ultrashort Pulse Laser Tunable up to
Nanosecond Range∙T. Bartulevičius1 , M. Lipnickas1 , K. Madeikis1 , R.
Burokas1,2 , and A. Michailovas1,2 ; 1 Ekspla, Vilnius,
Lithuania; 2 Center for Physical Sciences and Technology,
Vilnius, Lithuania
A versatile active fiber loop technology enabled GHz
burst operation mode and pulse duration tuning froma few hundred femtoseconds even up to the nanosecond
range in the single industrial-grade 30 W-level average
power femtosecond laser.
CA-P.15 MON

Experimental and numerical analysis of thermal
aberrations in Nd:YVO4 laser amplifiers∙M. Schneewind1,2 , P. Booker1,2 , S. Spiekermann1 , P.
Weßels1,2 , J. Neumann1,2 , and D. Kracht1,2 ; 1 Laser Zentrum Hannover e.V., Hanover, Germany; 2 Cluster of Excellence QuantumFrontiers, Hanover, Germany
The power-dependent wavefront distortions in
Nd:YVO4 amplifiers were analyzed with a ShackHartman sensor and a Zernike-polynomial decomposition. The experimental analysis was complemented
by numerical simulations based on split-step Fourier
propagation with excellent agreement.
CA-P.16 MON

Iterative 3D modeling of pulse generation in
end-pumped Ho3+:YAG laser resonators utilizing
active Q-switching∙M. Rupp1,2 , K. Goth1,2 , M. Eichhorn1,2 , and C. Kieleck1 ;1Fraunhofer Institute of Optronics, System Technologies
and Image Exploitation, Ettlingen, Germany; 2 Institute ofControl Systems, Karlsruhe Institute of Technology, Karls-

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Hall B0ruhe, Germany
In this work we present a highly accurate model for simulating Q-switched laser resonators based on a beam
propagation method algorithm. The model is validatedwith an experimental Ho3+:YAG resonator setup andshows excellent agreement.
CA-P.17 MON

Laser Photon Statistics caused by Outcoupling and
Losses∙M. Eichhorn; Fraunhofer IOSB, Ettlingen, Germany;
Karlsruhe Institute of Technology, Karlsruhe, Germany
The effect of a laser output coupler being a beam-splitteris introduced and its implication on photon statistics isinvestigated for the first time, leading to non-Poisson
statistics at low additional losses.
CA-P.18 MON

Polarized mid-infrared emission properties of Er3+
and Ho3+ ions in YAlO3∙S. Normani1 , P. Loiko1 , G. Zin Elabedine2 , R.M. Solé2 ,X. Mateos2 , A. Braud1 , W. Chen3 , V. Petrov3 , D. Sun4 ,P. Zhang5 , and P. Camy1 ; 1 Centre de Recherche sur lesIons, les Matériaux et la Photonique (CIMAP), UMR 6252
CEA-CNRS-ENSICAEN, Université de Caen Normandie,
Caen, France; 2 Universitat Rovira i Virgili (URV), Tarragona, Spain; 3 Max Born Institute for Nonlinear Optics
and Short Pulse Spectroscopy, Berlin, Germany; 4 Anhui
Institute of Optics and Fine Mechanics, Hefei Institutesof Physical Science, Chinese Academy of Sciences, Hefei,
China; 5 Jinan University, Guangzhou, China
Polarized stimulated-emission cross-sections for mid-

13:00 – 14:00
CB-P: CB Poster session
CB-P.1 MON

Dual-wavelength DFB Laser Based on Four Phaseshifts Sections and Equivalent Chirp Technology for
Millimeter-wave Generation∙B. Yuan1 , Y. Fan1 , S. Zhu1 , Y. Zhang2 , J. Marsh1 , andL. Hou1 ; 1 University of Glasgow, Glasgow, United Kingdom; 2 Nanjing University of Posts and Telecommuinications, Nanjing, China
A monolithic dual-wavelength DFB laser based on fourphase-shifts sections and equivalent chirp is demonstrated. A 61.2 GHz RF signal is observed by beating thetwo optical signals in a photodetector.
CB-P.2 MON

Analysis of ultra-low frequency noise external cavity
diode laser-systems for optical ion clocks

Politecnico di Torino and RU INSTM, Turin, Italy;
LINKS Foundation, Turin, Italy; 4 Politecnico di Milano,
Milan, Italy
A high-quality Tm-germanate glass was fabricated withhomogeneous ion distribution. Spectroscopic characterization for pump and laser transitions as well as preliminary results on laser generation at 2 μm are reported.
2

infrared emissions of Er3+(4I11/2→4I13/2) andHo3+(5I6→5I7) in orthorhombic YAlO3 are determined, well matching recent results on ~3-μm laser
operation. The peak σSE is 1.44×10-20 cm2 at 3015 nm(Ho3+) for E||c.

3

CA-P.19 MON

Spectroscopy and Laser Operation of Yb:LuGG
Crystal at Cryogenic temperatures
S. Slimi1 , ∙V. Jambunathan2 , G. Zin Elabedine1 , H.
Yu3 , H. Zhang3 , W. Chen4 , R. Maria Solé1 , M.
Aguiló1 , F. Díaz1 , M. Smrz2 , T. Mocek2 , and X.
Mateos1 ; 1 Universitat Rovira i Virgili (URV), Física i
Cristal⋅lografia de Materials (FiCMA), Marcel⋅lí Domingo
1, E-43007 , Tarragona, Spain; 2 HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, Za Radnicí 828, 252 , Dolní Břežany, Czech Republic; 3 StateKey Laboratory of Crystal Materials, Shandong University, 250100, Jinan, China; 4 Fujian Institute of Researchon the Structure of Matter, Chinese Academy of Sciences,
Fuzhou, 350002 , Fujian, China
We present the spectroscopic and laser characteristics of
Yb: LuGG garnet crystal at cryogenic temperatures. At
80 K, a maximum output power of 15.28 W was achieved
pumped by a VBG stabilized 969 nm diode.

CA-P.21 MONHigh average power amplification of femtosecond
pulses based on Yb: CaYAlO4 crystal∙C. Bai1 , W. Tian1 , G. Wang1 , L. Zheng1 , X. Tian1 , Y.
Yu1 , X. Xu3 , Z. Wei2 , and J. Zhu1 ; 1 Xidian University,
Xi’an 710071, China; 2 Chinese Academy of Sciences, Beijing 100190, China; 3 Jiangsu Normal University, Xuzhou
221116, China
In this report, we demonstrated the direct amplification
with the Yb:CALYO crystal for the first time. The amplifier delivered amplified pulses with the average powersof 55.4 W and pulse duration of 166 fs.
CA-P.22 MON

Temporal Contrast Improvement at ELI-NP∙O. Chalus1 , C. Derycke1 , M. Zhan2 , A. Guggenmos2 , S.
Steinke3 , and I. Dancus4 ; 1 Thales LAS France, Elancourt,
France; 2 UltraFast Innovations GmbH, Garching, Germany; 3 MARVEL FUSION GmbH, Munich, Germany;
4
Extreme Light Infrastructure - Nuclear Physics, IFINHH, Magurele, Romania
Improvements to HPLS led to removal of pre-pulses andsignificant reduction of the pedestal in the contrast. A di-

CA-P.20 MON

Fabrication and spectroscopy of high-quality
Tm3+-doped germanate glass for 2 μm laser emission∙M. Segura1 , D. Pugliese2 , M. Ceballos1 , F. Diaz1 ,M. Aguilo1 , X. Mateos1 , N. Boetti3 , and J. Lousteau4 ;1
Universitat Rovira i Virgili, Tarragona, Spain;∙N. Kolodzie1,2 , I. Mirgorodskiy1 , C. Nölleke1 , and P.O.
Schmidt2,3 ; 1 TOPTICA Photonics AG, Gräfelfing, Germany; 2 Physikalisch-Technische Bundesanstalt, Braunschweig, Germany; 3 Institut für Quantenoptik, Leibniz
Universität Hannover, Hannover, Germany
We investigate the characteristics of two different diodebased ultra-low noise lasers for quantum applications.
Differences in operation are analysed both experimentally and theoretically, and advantages and disadvantagesof each system-type are discussed.

A monolithic optical injection locking DFB laser basedon four phase-shifted sampling gratings is demonstrated.
Precise lasing wavelength control and a higher grating
coupling coefficient can be achieved.
CB-P.4 MON

Controlling transverse modes in Quantum Cascade
Laser Frequency Combs using radio-frequency
injection∙S. Dal Cin1 , F. Pilat1 , A. Konecny1 , N. Opacak1 , G.
Strasser1,2 , and B. Schwarz1 ; 1 Institute for Solid StateElectronics, TU Wien, Vienna, Austria; 2 Zentrum für
Mikro- und Nanostrukturen, TU Wien, Vienna, Austria
We present the observation of controlled lateral modeswitching in a two section, RF-modulation optimized,
12μm broad ridge FP-QCL. The mode switching is induced by strong RF modulation close to the free-running
repetition frequency.

CB-P.3 MON

Monolithic Optical Injection Locking DFB Lasers
Based on Four Phase-Shifts Sampling Sections∙Y. Fan1 , Y. Zhang2 , Y. Sun1 , B. Yuan1 , J. Marsh1 , and L.
Hou1 ; 1 James Watt School of Engineering, University ofGlasgow, Glasgow, United Kingdom; 2 College of OpticalEngineering, Nanjing University of Posts and Telecommunications, Nanjing, China
75

rect measurement of thirteen orders of magnitude contrast performed on a PW laser for the first time.
CA-P.23 MON

Investigation of Fractional Thermal Load in
Cryogenically Operated Yb:YLF and Yb:YAG Lasers∙M. Kilinc1,2 , U. Demirbas1 , J. Thesinga1 , M. Kellert1 ,M. Pergament1 , and F.X. Kärtner1,2,3 ; 1 Center for FreeElectron Laser Science CFEL, Deutsches ElektronenSynchrotron DESY, Notkestr. 85, 22607, Hamburg, Germany; 2 Physics Department, University of Hamburg, Luruper Chaussee 149, 22761, Hamburg, Germany; 3 The
Hamburg Centre for Ultrafast Imaging, Luruper Chaussee
149, 22761, Hamburg, Germany
We have directly measured the pump-induced fractional
thermal load (FTL) in cryogenically operated Yb:YAG
and Yb:YLF lasers to the first time, and found that FTL
is 1.5 and 1.7 times of quantum defect limit, respectively.
CA-P.24 MON

LIDT Evaluation of Bonded Crystals for J-class
Energy System∙A. Kausas1 and T. Taira2 ; 1 Institute for Molecular Science, Okazaki, Japan; 2 RIKEN SPring-8 Center, Sayocho,
Japan
In this work, the laser induced damage threshold
was measured for crystals bonded by surface activatedbonding. By use of sub-ns Nd:YAG/Cr:YAG passively
Q-switched laser at 1064 nm, crystals like sapphire,
Nd:YAG and quartz were evaluated.

CB-P.5 MON

Qualification of Semiconductor Optical Amplifiersfor Space-Borne Laser Modules∙K. Häusler, J. Baumann, A. Bawamia, H. Wenzel, A.
Maaßdorf, J. Fricke, J.E. Boschker, J. Glaab, A. Knigge, A.
Wicht, and G. Tränkle; Ferdinand-Braun-Institut, Berlin,
Germany
Laser modules for wavelength-stabilized narrow
linewidth single-mode emission at 1064nm and 767nm
were manufactured and subjected to qualification forspace applications. For 1064nm modules the reliability
exceeds 99% over 10,000 hours at 500mW optical power.
CB-P.6 MON

Wiener-Filter Enhanced Estimation of the Intrinsic
Laser Linewidth From Delayed Self-Heterodyne Beat
Note Measurements∙M. Kantner and L. Mertenskötter; Weierstrass Institutefor Applied Analysis and Stochastics (WIAS), Berlin, Germany

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Hall B0
We present a novel method to estimate of the intrinsic laser linewidth from self-heterodyne beat note measurements even at strong detector noise. Our method
yields an artifact-free reconstruction of the frequency
noise power spectral density.
CB-P.7 MON

Strahlwerkzeuge, University of Stuttgart, Stuttgart, Germany
The thermally imposed performance limits of traditional
VECSELs can be overcome by introducing a grating
waveguide structure into the design. We report on its
fabrication and characterization for a red-emitting semiconductor laser structure.

waveguides is presented. This includes the effects of thecurvature of the different S-bends on the electro-opticaland spectral behavior.

cal feedback. Performing random parameter space sampling we categorize the range of values leading to switching and contrast them with experimental data.

CB-P.15 MON

CB-P.19 MON

Q-switched semiconductor lasers as sources for
optical frequency comb generation∙P. López-Querol, C. Quevedo-Galán, A. Pérez-Serrano,
J.M. García Tijero, and I. Esquvias; CEMDATIC–E.T.S.I.
Telecomunicación, Universidad Politécnica de Madrid,
Madrid, Spain
In this contribution we study and simulate the behaviourof a four section DBR laser under Q-switching operation, generating broad optical frequency combs (202
GHz within 10 dB) with a low repetition frequency (100MHz).

Abrupt transition to coherent emission in asemiconductor laser with optical feedback∙M. Duque Gijón1 , C. Masoller1 , and J. Tiana-Alsina2 ;1
Departament de Fisica, Universitat Politecnica deCatalunya, Terrassa, Spain; 2 Department de Fisica
Aplicada, Facultat de Fisica, Universitat de Barcelona,
Barcelona, Spain
We use the speckle contrast technique to show experimentally that, in a semiconductor laser with optical feedback, the transition to coherent emission varies fromsmooth to abrupt as the amount of feedback increases.

CB-P.16 MON

CB-P.20 MON

Waveguide width dependence of reliability in
GaAs-based laser diodes∙A.K. Sünnetçioğlu, K. Ebadi, and A. Demir; Bilkent University, UNAM - Institute of Materials Science and Nanotechnology, Ankara, Turkey
Despite much higher heat load densities, low waveguide
width laser diodes demonstrate superior characteristics
in terms of reliability and temperature. We demonstrate
the effect of waveguide width on reliability with experiment and simulation.

From coherence to incoherence in harmonic modelocked lasers∙T. Seidel1 , S. Gurevich1 , and J. Javaloyes2 ; 1 Institutefor Theoretical Physics & Center for Nonlinear Science(CeNoS), University of Münster, Schlossplatz 2, 48149
Münster, Germany; 2 Dpt. de Física, Universitat de les Illes
Balears & IAC-3, Campus UIB, E-07122 Palma de Mallorca, Spain
We demonstrate that the pulses formed in an harmonically mode-locked laser are not necessarily coherent
and that multiple frequency combs shifted in frequency
may coexist. The laser may wander between such states,
thereby impacting coherence.

Fiber-coupled tapered amplifier in a hermetic 14-pin
butterfly package emitting 3 W at 780 nm and morethan 2.5 W at 850 nm∙H. Thiem, D. Brauda, M. Schütz, B. Globisch, and M.
Malach; EAGLEYARD Photonics GmbH, Berlin, Germany
We present miniaturized fiber-coupled tapered amplifiers at 780 nm and 850 nm with high output power andcollimated output for applications in spectroscopy andquantum technology. The SMSR is > 50 dB and the M^2<2.

CB-P.8 MON

CB-P.12 MON

Optical Injection-Induced Timing Jitter Reduction in
Gain-Switched 1550-nm Discrete Mode Semiconductor Laser
M. Duque Gijon1 , A. Quirce2 , J. Tiana-Alsina3 , ∙A.
Valle2 , and C. Masoller1 ; 1 Departament de Fisica, Universitat Politecnica de Catalunya, Barcelona, Spain;
2
Instituto de Fisica de Cantabria (IFCA), Universidad
de Cantabria-CSIC, Santander, Spain; 3 Departament de
Fisica Aplicada, Universitat de Barcelona, Barcelona,
Spain
We have investigated the effect of optical injection on thetiming jitter observed in gain-switched single-mode discrete mode lasers. Jitter reductions larger than 80 % overa 42 GHz detuning range are obtained.

Quantum Cascade Laser active region modification
toward efficient integration with Photonic Integrated
Circuits∙K. Pierściński, D. Pierścińska, G. Sobczak, K. Pieniak, A.
Broda, A. Kużmicz, and P. Gutowski; Łukasiewicz Resorach Network - Institute of Microelectronics and Photonics, Warsaw, Poland
In this work we focus on hybrid horizontal integrationof QCL with passive waveguides fabricated in Ge-on-Si
wafer. Some modifications of laser chips were investigated and will be presented in this work.

Identification of lasing modes of photonic-crystal
surface-emitting lasers by polarization dependence ofthe far-field pattern: an application of the k-p
perturbation theory∙K. Sakoda1 , Y. Yao1,2 , N. Ikeda1 , T. Kuroda1 , Y.
Sugimoto1 , T. Mano1 , H. Koyama1 , R. Hashimoto3 , K.
Kaneko3 , T. Kakuno3 , S. Ookuma3 , R. Togawa3 , H.
Ohno3 , and S. Saito3 ; 1 National Institute for Materials Science, Tsukuba, Japan; 2 University of Tsukuba,
Tsukuba, Japan; 3 Toshiba Corporation, Yokohama, Japan
We formulated a k-p perturbation theory for the polarization dependence of the far-field pattern of thephotonic-crystal surface-emitting lasers, and successfully identified the resonance mode of our quantum cascade lasers with photonic-crystal cavities.

CB-P.13 MON

CB-P.17 MON

Piecewise continuous tuning of an integrated tunable
laser based on an intra-cavity AMZI filter∙M. Skënderas1 , P. Marin-Palomo1 , S.W. Jolly1,2 , and M.
Virte1 ; 1 Brussels Photonics (B-PHOT), Vrije Universiteit
Brussel, Brussels, Belgium; 2 OPERA-Photonique, Universite Libre de Bruxelles, Bruxelles, Belgium
We investigate the tunability of a laser with an
intra-cavity asymmetric Mach-Zehnder interferometer(AMZI). We demonstrate a piece-wise continuous tuning by taking advantage of the coupling between amplitude and phase in the AMZI response.

Bandwidth broadening from vertical strain coupling
effect in chirped stacked InAs/InGaAsP quantum
dash lasers∙G. Chen and X. Zhang; Concordia University, Montreal,
CanadaBy taking advantage of the vertical strain coupling effect,
the output bandwidth of chirped stacked Qdash laser canbe improved by adjusting the stacking sequence which
provides a new strategy for the design of the broadband
devices.

CB-P.14 MON

Modal Gain and Cross-Saturation Effects on the
Switching Capabilities of an Integrated Multi-Wavelength Laser∙M. Ladouce, P. Marin-Palomo, and M. Virte; Brussels Photonics Team (B-PHOT), Vrije Universiteit Brussel,
Brussels, Belgium
We identify key multi-wavelength laser parameters enabling mode switching based on phase-controlled opti-

CB-P.9 MON

Coupled mode-locked VECSEL cavities with a sharedgain medium∙J.V. Moloney, S. Tsouassis, and R.J. Jones; Wyant College
of Optical Sciences, University of Arizona, Tucson, USA
We demonstrate a coupled V-cavity semiconductor disklaser outputting two GHz mode-locked pulse trains
while drawing gain from separated spectral regions.
Cavity angle dictates spectral separation making this apotential candidate for dual-comb GHz spectroscopy
CB-P.10 MON

Towards AlGaInP-VECSELs with a grating waveguide structure
P. Gierss1 , A. Ćutuk1 , M. Leyzner2 , U. Brauch2 , M. Abdou
Ahmed2 , ∙M. Jetter1 , T. Graf2 , and P. Michler1 ; 1 Institut
für Halbleiteroptik und Funktionelle Grenzflächen, University of Stuttgart, Stuttgart, Germany; 2 Institut für

CB-P.11 MON

CB-P.18 MON

Investigation of bent DBR-RW Laser Diodes emitting
at 785 nm∙L.S. Theurer, J.-P. Koester, A. Müller, J. Fricke, M. Maiwald, B. Sumpf, A. Knigge, and G. Tränkle; FerdinandBraun-Institut (FBH), Berlin, Germany
An experimental investigation of the losses in GaAsbased DBR-RW diode lasers containing straight and bent
76

CB-P.21 MON

Integration of QCLs in photonic platforms - thermal
considerations∙D. Pierścińska, K. Pierściński, G. Sobczak, K.
Chmielewski, K. Michalak, A. Kuźmicz, and P. Gutowski; Łukasiewicz Research Network - Institute of Microelectronics and Photonics, Warsaw, Poland
This paper focuses on the thermal aspects of a single
emitter QCLs as well as multi-spectral QCLs integrated
on silicon-based platform. The experimental and numerical investigation of temperature distributions of integrated multi emitter QCLs are presented.
CB-P.22 MON

On-chip multi-wavelength lasers for all-optical THz
signal processing∙P. Marin-Palomo, S. Abdollahi, M. Ladouce, and M.
Virte; Brussels Photonics Team (B-PHOT), Vrije Universiteit Brussel, Brussels, Belgium
Using a multi-wavelenght laser monolithically integrated with an optical feedback control loop, we demonstrate selective filtering and amplification with a gain
above 15 dB of an optical signal comprising two narrowlines separated by 1.3 THz.

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Hall B0
13:00 – 14:00
CM-P: CM Poster session
CM-P.1 MON

Formation Dynamics Of Periodic Surface Patterns In
Ge Induced By UV Nanosecond Laser Pulses
M. Alvarez-Alegria1,2 , C. Ruiz de Galarreta1 , and ∙J.
Siegel1 ; 1 Laser Processing Group, Instituto de Óptica, IOCSIC, Madrid, Spain; 2 Instituto de Física Interdisciplinar
y Sistemas Complejos, IFISC (CSIC-UIB), Palma de Mallorca, Spain
We have employed single interfering excimer laser pulses
to imprint homogenous diffraction gratings in crystalline Germanium. The formation dynamics havebeen investigated with nanosecond time-resolved optical diffraction, yielding the quantitative evolution of thesurface topography.
CM-P.2 MON

3D-printed scaffolds via Multi-photon Polymerization for Peripheral Nervous System Regeneration∙A. Kordas1,2 , P. Manganas1 , M. Farsari1 , and A.
Ranella1 ; 1 IESL/FORTH, N.Plastira 100, 70013, Heraklion, Greece; 2 Department of Materials Science and Technology, University of Crete, Heraklion, Greece
A novel scaffold fabricated with Multi-Photon Polymerization that provided topographical cues for the cultureof two cell lines is reported. Cell behavior was monitored for the system’s possible application to Peripheral
Nervous System Regeneration.
CM-P.3 MON

3D Injectable Mechanical Metamaterials for Tissue
Engineering Applications∙S. Skrepetos1,2 , A. Ranella1 , and M. Farsari1 ;1
IESL/FORTH, Heraklion, Greece; 2 Department ofMaterials Science and Technology, Heraklion, Greece
Extraordinary 3D injectable mechanical metamaterials
are being reported. Fabricated by an organic – inorganic
photosensitive resin through Multiphoton Lithography(MPL) and then characterized via 3D modeling and indentation.
CM-P.4 MON

Tailoring the optical response of 3D-printed photonic
crystals using Aluminum Zinc Oxide∙D. Ladika1,2 , A. Theodosi1 , O. Tsilipakos3 , A. Klini1 , P.
Loukakos1 , M. Kafesaki1,2 , M. Farsari1 , and D. Gray1 ;1
IESL-FORTH,Nik. Plastira 100, 70013 , Heraklion,Crete,
Greece; 2 Department of Materials Science and Technology, 70013, University of Crete, Heraklion,Crete, Greece;3
National Hellenic Research Foundation (N.H.R.F.), 48
Vassileos Constantinou Avenue, 11635, Athens, Greece
The extraordinary optical properties of the Epsilon Near

Zero material, Aluminum Zinc Oxide will be studied inthree dimensions, by deposing it on 3D photonic crystals, which are responsive in the Telecommunication
Spectrum.
CM-P.5 MON

In-depth jet dynamics investigations of femtosecond
laser bioprinting∙B. Kreidl1 , J. Zhang2 , S. Niehren2 , H. ClausenSchaumann1 , S. Sudhop1 , and H.P. Huber1 ; 1 Lasercenter,
Department of Applied Sciences and Mechatronics, Munich University of Applied Sciences HM, Lothstrasse 34,80335, München, Germany; 2 Molecular Machines & Industries, Breslauer Strasse 2, 85386, Eching, Germany
In-depth investigations of jet dynamics in previously
developed femtosecond laser bioprinting allow precise
control over the transfer process, enabling printing resolutions of <42±3 μm and single cell deposition accuracyof <15 μm.

CM-P.8 MON

CM-P.12 MON

Wavelength Dependence of Energy Transfer from
Femtosecond Laser Double Pulse to Silicon∙E. Gushiken, M. Tani, and K.L. Ishikawa; School of Engineering, The University of Tokyo, Tokyo, Japan
With calculations based on the time-dependent density
functional theory, we have found the efficient energy
transfer to Silicon from the femtosecond laser double
pulse which has a short-wavelength first pulse and longwavelength second pulse.

3D microstructures of TiO2 for applications inphotocatalysis
I. Syngelakis1,2 , C. Aivalioti1,2 , E. Aperathitis1 , G.
Kenanakis1 , S. Tzortzakis1,2 , ∙A. Klini1 , and M. Farsari1 ;1
IESL/FORTH, Heraklion, Greece; 2 Department of Materials Science and Technology, University of Crete, Heraklion, Greece
In this study we demonstrate the fabrication of complex three-dimensional (3D) microstructures of TiO2
Nanorods (NRs) and their photocatalytic performance.
The proposed fabrication scheme applies Laser based
techniques (MPL and PLD), as well as pyrolysis and
ACG.

CM-P.9 MON

Nanostructured Back Surface Amorphization of
Silicon with Picosecond Infrared Laser Pulses∙M. Blothe1 , M. Chambonneau1 , and S. Nolte1,2 ;1Friedrich Schiller University Jena, Institute of Applied
Physics, Abbe Center of Photonics, Jena, Germany;
2
Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Center of Excellence in Photonics, Jena,
Germany
We demonstrate back surface silicon amorphization withpicosecond Bessel beams. Ring-like and continuous
modifications are observed by optical and electron microscopy. Raman spectroscopy reveals a full allotropicchange. Regular polarization-dependent nanostructures
are detected.

CM-P.6 MON

Unravelling the transient complex refractive index
change of aluminium after ultrashort pulse laser
irradiation
J. Winter1 , ∙D. Redka1,2 , J. Minár2 , M. Schmidt3 , and H.P.
Huber1 ; 1 Lasercenter, Department of Applied Sciences
and Mechatronics, Munich University of Applied Sciences
HM, Lothstr. 34, Munich, Germany; 2 New TechnologiesResearch Center, University of West Bohemia, Univerzitní 8, Plzen, Czech Republic; 3 Lehrstuhl für Photonische
Technologien, Friedrich-Alexander-Universität ErlangenNürnberg, Konrad-Zuse-Straße 3-5, Erlangen, Germany
Pump-probe ellipsometry and simulations are used to
examine the dynamics of ultrashort pulse laser ablationof aluminum. Our material model predicts transient
temperature and density variations, aiding in the understanding of issues of laser micro-machining.

CM-P.10 MON

Nanolayered Natural Mineral Muscovite - Single fs
Laser Pulse Interaction: A Tool To Uncover Material
Variability∙D.M. Kane1 , S. Awasthi2,3 , A. Fuerbach2 , and D.J.
Little2 ; 1 Australian National University, Canberra,
Australia; 2 Macquarie University, Sydney, Australia;
3
University of Connecticut, Storrs, USA
Single femtosecond laser pulse interaction studies onhigh quality muscovite show the impact of nanolayered
structure, mineral water content, and detailed chemicalcomposition. Micro-shaping outcomes reflect and giveinsight into the mineral and its variation.

CM-P.7 MON

Double-Pulse Laser Modification of Transparent
Materials: Energy Coupling and Plasma Shielding
M. Zukerstein1 , V. Zhukov1,2,3 , and ∙N. Bulgakova1 ;1
HiLASE Centre of the Institute of Physics of the Czech
Academy of Sciences, Dolni Brezany, Czech Republic;2
Federal Research Center for Information and Computational Technologies, Novosibirsk, Russia; 3 Novosibirsk
State Technical University, Novosibirsk, Russia
Volumetric modification of glass by two successive laser
pulses was studied experimentally and numerically. A
weak pre-pulse followed by a more energetic pulse isfavorable for enhanced modification. The role of selftrapped excitons is discussed.

CM-P.11 MON

Spiraling optical vortices in Tornado Waves∙A. Brimis1,3 , K.G. Makris1,3 , and D.G. Papazoglou1,2 ;1Institute of Electronic Structure and Laser, Foundation
for Research and Technology-Hellas (FORTH), Herakleion, Greece; 2 Department of Material Science and Technology, University of Crete, Herakleion, Greece; 3 ITCP,
Department of Physics, University of Crete, Herakleion,
GreeceTornado waves are generated using a discrete numberof optical vortices to modulate the phase of a ring-Airybeam. In this novel generation scheme, vortices andhigh intensity lobes follow a coupled accelerating spiraling trajectory.
77

CM-P.13 MON

The contribution has been withdrawn.
CM-P.14 MON

Femtosecond inscription of Type-A Volume Bragg
Gratings in silver-containing phosphate glasses
J. Harb1 , L. Talbot2 , Y. Petit1,3 , M. Bernier2 , and ∙L.
Canioni1 ; 1 University of Bordeaux, CNRS, CEA, CELIA,
UMR 5107, 351 Cours de la Libération, 33405 Talence,
Cedex, France; 2 Centre d’Optique, Photonique et Laser(COPL), Université Laval, Québec G1V0A6, Canada;
3
University of Bordeaux, CNRS, ICMCB, UMR 5026, 87
avenue du Dr. A. Schweitzer, 33608 Pessac, Cedex, France
Here, we report Type-A Volume Bragg gratings (VBGs)
in silver-containing phosphate glasses using the lightsheet and the phase-mask approaches. Those techniques
open the avenue for the high throughput inscription of
VBGs for industrial applications.
CM-P.15 MON

Ultrafast Laser Surface Functionalization and Routeto Industrial Applications∙X. Sedao, L. Leggio, and T. Fournel; Laboratory Hubert
Curien, UMR 5516 CNRS, Jean Monnet University, University of Lyon, Saint-Étienne, France
Ultrafast laser surface functionalization can be applied
for photonics, wetting and bio-engineering. When large
and freeform surface is in question, an intelligent, precise and lightweight vision system capable of addressing
laser head is essential.
CM-P.16 MON

Laser-Assisted Nanosynthesis of Fluorescent Carbon
Nanocomposites with Variable Plasmonic Properties∙Y.V. Ryabchikov; HiLASE Center, Institute of Physics of
the Czech Academy of Sciences, Prague, Czech RepublicThis research highlights new achievements on ultrafast laser nanosynthesis of multi-modal semiconductor nanocomposites with adaptable plasmonic proper-

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ties due to variable chemical content for their further applications in optical nanothermometry, bioimaging andbiosensing.
CM-P.17 MONStandardized Material Characterization of TwoPhoton Polymerized Materials on the Macroscopic
Scale∙F. Chalupa-Gantner1 , T. Koch2 , J. Puchhammer1 , M.
Lunzer3 , and A. Ovsianikov1 ; 1 3D Printing and Biofabrication Group, Institute of Materials Science and Technology, TU Wien , Vienna, Austria; 2 Research Group for
Structural Polymers, Institute of Materials Science andTechnology, TU Wien, Vienna, Austria; 3 UpNano GmBH,
Vienna, Austria
Substantial improvements in the throughput of 2PP permit to close the gap to other additive manufacturing
technologies in the meso- and macro-range. Those advances demand materials suitable for up-scaled 2PP, andstandardized mechanical material testing.
CM-P.18 MON

Ultrashort Laser-induced Nano/microstructuring ofMetallic Anode Coated by Carbon Nanoparticles for
Li-ion Cells and Supercapacitors∙I. Gnilitskyi1,2,3 , C. Leonardi4 , P. Medaglia4 , R. Pezzilli4 ,G. Prestopino4 , L. Rizzo3,5 , and S. Bellucci3 ; 1 ”NoviNano
Lab” LLC, Lviv, Ukraine; 2 Department of Applied Physics
and Nanoscience, Lviv Polytechnic National University,
Lviv, Ukraine; 3 INFN, Frascati, Italy; 4 Department ofIndustrial Engineering, University of Rome Tor Vergata,Rome, Italy; 5 Università degli studi di Cassino e del Lazio, Rome, Italy
Substrate modification by femtosecond laser-induced
periodic surface structures has improved the cyclic resistance of metallic electrodes, also owing to the enhancement of the adhesion of carbon-based nanoparticles.

tonic Science and Engineering (CPhSE), Skolkovo Instituteof Science and Technology, Moscow, Russia
We present the production of MoS2, WS2, nanoribbons
with extremely high aspect ratio, by direct interferometric patterning of single source precursor films, using visible laser radiation. The patterning process is followed
by a material-synthesis step.
CM-P.21 MON

Bacterial attachment on large area two-photon polymerised scaffolds with different nanostructured
surfaces
Y.M. Somorin1,2 , N. Farid1 , and ∙G.M. O’Connor1 ;1
National Centre for Laser Applications, School of Natural Sciences, University of Galway, Galway, Ireland; 2 Irish
Photonic Integration Centre (IPIC), Tyndall National Institute, Cork, IrelandThis study investigated the interaction of Staphylococcus
aureus and Pseudomonas aeruginosa with two-photon
polymerised scaffolds with different nanostructured surfaces. Smooth-surface scaffolds had fewer bacteria attached and gold-coated scaffolds had 85 – 98% reduction
in bacteria attachment.
Eigenmode-based analysis of the multiple-temperature model∙H. Katow1 and K. Ishikawa1,2 ; 1 Photon Science Center,
Graduate School of Engineering, The University of Tokyo,
Tokyo, Japan; 2 Department of Nuclear Engineering andManagement, Graduate School of Engineering, The University of Tokyo, Tokyo, JapanWe developed an eigenmode-based analysis for the multiple temperature model. We report universal properties
valid for any choice of parameters and system compositions, and a counterintuitive phenomenon where thelattice temperature exceeds electron temperature.
CM-P.23 MON

Simulating Ultrashort-Pulsed Laser Ablation ofDielectrics with Rate-Equation Models and ElectricField Propagation∙P.S. Sneftrup, S.H. Møller, and P. Balling; Aarhus University, Aarhus, Denmark
We present a model of ultrashort-pulse laser ablation ofdielectrics combining a rate-equations model and finitedifference time-domain propagation. We compare thismodel with previous methods of propagation by simulating observables in ablation experiments.

Spiraling polarization structures∙A. Brimis1,3 , K.G. Makris1,3 , and D.G. Papazoglou1,2 ;Institute of Electronic Structure and Laser, Foundation
for Research and Technology-Hellas (FORTH), Herakleion, Greece; 2 Department of Material Science and Technology, University of Crete, Herakleion, Greece; 3 ITCP,
Department of Physics, University of Crete, Herakleion,
GreecePolarization structures can be produced by the suitablesuperposition of polarized states of light that carry orbital angular momentum. Such structures follow a spiraltrajectory, while their transverse profile depends on the
choice of superimposed light.

CM-P.20 MON

Laser-synthesis of 2D TMD nanoribbons∙A. Kalganova, A. Averchenko, O.A. Abbas, I. Salimon, E.
Zharkova, P.G. Lagoudakis, and S. Mailis; Center for Pho-

CM-P.28 MON

Indium Tin Oxide Ultrafast Ablation: From Electron
Dynamics to Fine Crater Structure∙G.E. Hallum1,2 , D. Kürschner2 , S. Vogel2 , W. Schulz2 ,and H.P. Huber1 ; 1 Munich University of Applied Sciences,
Munich, Germany; 2 RWTH Aachen University, Aachen,
Germany
Indium tin oxide ablation is observed with pump-probe
microscopy. Rate equations, fit to the reflectivity, estimate the free electron density and absorptivity. Correlations are drawn between atomic force microscopy, absorbed energy, and observed ablation dynamics.

Improving Adhesive Properties on the Plastic Surface
by Femtosecond Laser Treatment∙A. Zhuravlov1,2 , V. Barvinska1,2 , A. Andrushchak1 ,and I. Gnilitskyi1,2 ; 1 NoviNano Lab LLC, Lviv, Ukraine;2
Department of Applied Physics and Nanomaterials Science, Lviv Polytechnic National University, Lviv, Ukraine
In this paper, we used femtosecond laser to form
anisotropic and isotropic surface modification on Teflon.
Adhesion properties of laser-modified Teflon surface
were studied and discussed.

CM-P.25 MON

Photothermal processing of commercial polymers
under high frequencies femtosecond laser irradiation
A. Pérez1 , ∙D. Puerto1,2 , M.G. Ramirez1,2 , G. Nájar1 ,J. Francés1,2 , S. Gallego1,2 , A. Márquez1,2 , I. Pascual1,3 ,and A. Beléndez1,2 ; 1 I.U. Física Aplicada a las Ciencias
y las Tecnologías, Universidad de Alicante, Sant Vicent
del Raspeig, Spain; 2 Dept. Física, Ingeniería de Sistemasy Teoría de la Señal, Universidad de Alicante, Sant Vicent del Raspeig, Spain; 3 Dept. Óptica, Farmacología
y Anatomía, Universidad de Alicante, Sant Vicent delRaspeig, Spain
We investigate the response of three commercial polymer (PVC, PET, and PP) under irradiation with high frequency (until 1 MHz) femtosecond (450 fs) multi-pulse(N = 30-100) laser at λ=515 and 1030 nm (2.9 J/cm2).

Femtosecond laser writing of a Fabry-Perot cavity in
a Polarizing Maintaining fiber: towards an all-fiberedphotonic cell for future atom cooling applications∙A. Abou Khalil1 , M. Berisset1 , L. Gibert1 , C. Pierre1 ,M.J. Milla1 , T. Billotte2 , F. Amrani3 , M. Popenda3 , F.
Gérôme2 , B. Debord2 , F. Benabid2 , and M. Castaing1 ;1
ALPhANOV, 33400 Talence, France; 2 GPMM Groupe,
XLIM Institute, CNRS UMR 7252, 87060 Limoges,
France; 3 GLOphotonics, 87060 Limoges, France
Femtosecond laser writing of HR FBGs in Polarizing
Maintaining fiber to create a Fabry-Perot cavity in a hollow core fiber as a first step towards an all-fibered photonic cell for future alkali atom cooling applications.

CM-P.22 MON

CM-P.19 MON

CM-P.24 MON

CM-P.26 MON

1Mass Spectrometric Study of the Plasma Plume
Produced by Picosecond Laser Ablation of a
CrFeCoNiMn High Entropy Alloy∙O. Gatsa, M. Flimelova, and A. Bulgakov; HiLASE Centrum, Institute of Physics CAS, Za Radnici 828, 252 41
Dolni Brezany, Czech Republic
The composition and expansion dynamics of plasma
plumes produced by picosecond laser ablation of threedifferent types of CrFeCoNiMn High Entropy Alloy targets in vacuum are investigated by time-of-flight mass
spectrometry.

CM-P.30 MON

CM-P.27 MON

3D micro-optical elements by multiphoton
lithography and nano-imprinted patterns using highlaser induced damage threshold photoresists
E. Kabouraki1 , ∙V. Melissinaki1 , A. Yadav2 , A.
Melninkaitis3,4 , K. Tourlouki5 , T. Tachtsidis5 , N.
Kehagias5,6 , G.D. Barmparis7 , D.G. Papazoglou1,8 ,E. Rafailov2 , and M. Farsari1 ; 1 IESL/FORTH, Heraklion, Greece; 2 Optoelectronics and Biomedical Photonics
Group, AIPT, Aston University, Birmingham, United
Kingdom; 3 Laser Research Center, Vilnius University,
Vilnius, Lithuania; 4 Lidaris Ltd, Vilnius, Lithuania;
5
Nanotypos, Thessaloniki, Greece; 6 NCSR Demokritos,
Institute of Nanoscience and Nanotechnology, Athens,

Nanoscale Control of Surface Machining with a
fs-UV interference approach∙D. Gailevicius, D. Stonytė, A. Butkutė, and D. Paipulas;Vilnius University Laser Research Center, Vilnius, Lithuania
Pulsed femtosecond UV interference patterning ofdifficult-to-process transparent dielectric materials provides pristine and periodic sub-micrometer features, focusing on fused silica, sapphire and YAG.

78

CM-P.29 MON

Surface Structure Modelling for Laser-Assisted
Reduction of SEY∙A. Din, R. Uren, S. Wackerow, and A. Abdolvand; University of Dundee, Dundee, United Kingdom
We propose a model capable of predicting energydependent electron response of surfaces with their geometry after laser irradiation. The model offers insights
into why the structures are effective at reducing secondary electron yield.
CM-P.31 MON

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Greece; Physics Department, University of Crete, Heraklion, Greece; 8 Materials Science and Technology Department, University of Crete, Heraklion, Greece
New organic inorganic hybrid photoresists that exhibit
enhanced laser-induced damage threshold are presented
here. These photoresists were used for the fabricationof micro-optical elements (MOEs) using multiphoton
lithography (MPL) as well as for nano-imprint lithography.

CM-P.32 MON

Laser Powder Bed Fusion thermal monitoring using
optical fiber sensors: in situ measurements andmodelling∙A. Lerner1,2 , Y. Anquetin3 , J. Gaspar3 , Q. Pouille4 , A.
Ladaci4 , Y. Corre5 , G. Bouwmans2 , and G. Laffont1 ;1
Université Paris-Saclay, CEA, List, F-91120, Palaiseau,
France; 2 Univ. Lille, CNRS, UMR 8523 – PhLAM –Physique des Lasers Atomes et Molécules, F-59000, Lille,
France; 3 Aix Marseille Univ, CNRS, IUSTI, Marseille,

France; 4 Université Paris-Saclay, CEA, Service d’Études
Analytiques et de Réactivité des Surfaces, 91191, Gif-surYvette, France; 5 CEA, Institute for Research on Fusion by
Magnetic confinement, 13108 Saint-Paul-Lez-Durance,
FranceWe performed temperature measurements in a partmanufactured by Laser Powder Bed Fusion using opticalfiber sensors. A simplified model of the process was developed, and the experimental measurements are compared to simulated temperature values.

13:00 – 14:00

ED-P.3 MON

ED-P.5 MON

ED-P: ED Poster session
A compact cold atom gravimeter utilizing a grating
magneto optical trap
S. Seo1 , J.H. Lee1 , S.-B. Lee1 , S.E. Park1 , M.H. Seo1 , J.
Park2 , S. Lee1 , H.-G. Hong1 , and ∙T.Y. Kwon1 ; 1 Korea Research Institute of Standards and Science, Daejeon, South
Korea; 2 National NanoFab Center, Daejeon, South Korea
We present a compact atomic gravimeter based on theatom interferometer that uses a gMOT. The grating parameter is optimized by applying a machine learning algorithm to the Monte Carlo simulation of our experimental setup.

Towards a robust and stand-alone ultra-stable laser
system based on a 124 K Si resonator with an
instability of 4 × 10−17∙S. Herbers1 , J. Yu1 , L. Anders1 , J. Kawohl1 , M. Misera1 ,T. Legero1 , K. Hanhijärvi2 , A. Wallin2 , T. Lindvall2 ,T. Fordell2 , and U. Sterr1 ; 1 Physikalisch-Technische
Bundesanstalt, Hannover, Germany; 2 Teknologian
tutkimuskeskus VTT Oy - Mittatekniikan keskus(MIKES), Espoo, Finland
To make a state-of-the art laser system self-contained
and robust for continuous operation, a closed cycle cooling system was designed. The robustness to ambient seismic noise was increased by adding low-frequency feedback and feedforward corrections.

Impurity-Free Gas Recycling System for an XUVFrequency Comb
∙L. Guth1,2 , J.-H. Oelmann1,2 , T. Heldt1,2 , J. Nauta1,3 ,N. Lackmann1 , N. Griesbach1 , T. Pfeifer1 , and J.R. Crespo López-Urrutia1 ; 1 Max-Planck-Institute for Nuclear
Physics, Heidelberg, Germany; 2 Heidelberg Graduate
School for Physics, Heidelberg, Germany; 3 Department of
Physics, Swansea University, Swansea, United Kingdom
We present a gas recycling system for High Harmonic
Generation processes. The system operates in a closedloop, with high purity, at pressures up to 200 bar, andwith a recycling rate of over 95 percent.

ED-P.2 MON

ED-P.4 MON

7

ED-P.1 MON

A Comb-calibrated Raman Spectrometer for Highaccuracy Measurements of Quadrupole Transitions
in Gases∙M. Lamperti1 , L. Rutkowski2 , D. Gatti3 , R. Gotti4 , L.
Moretti3 , D. Polli3 , G. Cerullo3 , and M. Marangoni3 ;1
Department of Science and High Technology, Universityof Insubria, Como, Italy; 2 Univ Rennes, CNRS, IPR (Institut de Physique de Rennes)-UMR 6251, Rennes, France;
3
Dipartimento di Fisica - Politecnico di Milano and IFNCNR, Milan, Italy; 4 Department of Electrical, Computer and Biomedical Engineering, Università degli studi
di Pavia, Pavia, Italy
We present a comb-calibrated coherent Raman spectrometer for the measurement of quadrupole transitionsof hydrogen-like molecules. The spectrometer reaches
an uncertainty lower than 100 kHz on the frequency axis.

Cavity-Enhanced Frequency-Comb-Based OpticalOptical Double-Resonance Spectrometer∙A. Rosina1 , V. Silva de Oliveira1 , I. Silander1 , A.
Hjältén1 , L. Rutkowski2 , G. Soboń3 , K.K. Lehmann4 , andA. Foltynowicz1 ; 1 Department of Physics, Umeå University, Umeå, Sweden; 2 Université de Rennes, CNRS, IPR(Institut de Physique de Rennes), Rennes, France; 3 Facultyof Electronics, Photonics and Microsystems, Wrocław University of Science and Technology, Wrocław , Poland;
4
Departments of Chemistry and Physics, University ofVirginia, Charlottesville, USA
We demonstrate an improved optical-optical doubleresonance spectrometer based on a 3.3 μm CW pump
and a 1.67 μm cavity-enhanced comb probe for detection of sub-Doppler hot-band transitions in the 3󰜈3 ←󰜈3 range of methane.

13:00 – 14:00

EJ-P.1 MON

EJ-P: EJ Poster session

Squeezed light source on lithium niobate on insulator for GKP generation without periodic poling∙T.N. Arge, R.R. Domeneguetti, J.S. Neergaard-Nielsen,
T. Gehring, and U.L. Andersen; Center for Macroscopic
Quantum States (bigQ) Department of Physics, Technical

ED-P.6 MON

A robust low-phase noise frequency comb
∙T. Puppe, C. Tresp, S. Mueller, A. Seer, P. Thoumany, and
R. Wilk; TOPTICA Photonics AG, Munich, Germany
A new locking scheme for a frequency comb basedon difference-frequency generation combines the lowphase noise by locking to an optical reference with longterm stability via a GPS disciplined RF-oscillator.
ED-P.7 MON

Stability improvement of a fiber-based frequency
reference at 1.5 μm using an original detection
technique for interference cancellation∙V. Roncin1 , J. Hrabina2 , L. Pravdova2 , and F.
Du-Burck1 ; 1 Laboratoire de Physique des Lasers,
C.N.R.S./Université Sorbonne Paris Nord, Villetaneuse, France; 2 Institute of Scientific Instruments, Czech
Academy of Sciences, Brno, Czech Republic
The signal is detected at a frequency that does not mod-

University of Denmark, Kgs. Lyngby, Denmark
In this work we present simulations and novel ideas forgenerating squeezed light on a Lithium Niobate on Insulator platform for continous variable quantum computation. We focus on purity and indistinguishability of thesource.
79

CM-P.33 MON

Self-Hydrophobization of Femtosecond
Laser-Textured Patterns on Aluminium Surfaces
O. Myronyuk1 , D. Baklan1 , and ∙A.M. Rodin2 ; 1 Igor Sikorsky Kyiv Polytechnic Institute, Kyiv, Ukraine; 2 Center for
Physical Sciences and Technology, Vilnius, Lithuania
The spontaneous liquid-repellency and its stability havebeen studied as a function of fractal-like nanopatterns
and microgrooves on an aluminum surface textured witha femtosecond laser.

ulate the interference fringes superimposed on the error
signal in order to improve the stability of a fiber-basedfrequency standard at 1.5 μm.
ED-P.8 MON

Attention Mechanisms for Broadband Feature
Prediction for Electromagnetic and Photonic
Applications
M. Soroush1 , ∙E. Simsek1 , G. Moille2,3 , K. Srinivasan2 ,and C.R. Menyuk1 ; 1 University of Maryland Baltimore
County, Baltimore, USA; 2 National Institute of Standards and Technology (NIST), Gaithersburg, USA; 3 Joint
Quantum Institute, NIST/University of Maryland, College
Park, USA
Different neural network architectures are used to predict the coupling quality factor of microring resonators
across broad spectral bandwidths. Attention mechanisms perform the best. Neural networks can significantly reduce the computation time during optimization
studies.
ED-P.9 MON

Tunable Polarization-Multiplexed Single-Cavity
Dual-Comb∙A. Rodriguez Cuevas, H. J. Kbashi, D. Stoliarov, and S.
Sergeyev; Aston Institute of Photonic Technologies, College
of Engineering and Physical Sciences, Aston University, B4
7ET, Birmingham, United Kingdom
A dual-comb laser based on Er-doped fibre laser andmode-locked by carbon nanotubes is stable over 6 hours
and can be separated with an extinction ratio of 19 dB,
potentially being use in polarimetric LIDAR.

EJ-P.2 MON

Temporal localized states and square-waves in semiconductor micro-resonators with strong time-delayed
feedback∙E.R. Koch1 , T.G. Seidel1 , J. Javaloyes2 , and S.V.
Gurevich1,3 ; 1 Institute for Theoretical Physics, University

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of Münster, Münster, Germany; Departament de Física,
Universitat de les Illes Balears & IAC-3, Palma de Mallorca, Spain; 3 Center for Nonlinear Science (CeNoS), University of Münster, Münster, Germany
We investigate dynamics of temporal localized statesin injected micro-resonators containing a quantum-wellnonlinearity. A normal form partial differential equation
is derived to investigate the role of second and third order dispersion on their emergence.
2

EJ-P.3 MON

Fast computation method to characterize the propagation dynamics of Ultrashort Laser Pulses∙E. Franco, J.A. Rodrigo, and Ó. Martínez-Matos; Universidad Complutense de Madrid, Facultad de Ciencias Físicas, Madrid, Spain
We propose a fast numerical GPU-based algorithm todescribe the spatio-temporal propagation of ultrashortlaser pulses in paraxial approximation. The numericalresults for femtosecond Curved-Shaped Laser pulses focused along arbitrary trajectories are analyzed in detail.
EJ-P.4 MON

Modelling of Gaussian and Bessel laser beams sharp
focused into complex tissue-like scattering medium
with the Helmholtz equation approximation
Y. Kistenev1,2 , ∙I. Meglinski3,4 , and A. Bulygin1,2 ; 1 Tomsk
State University, Tomsk, Russia; 2 V.E. Zuev Institute ofAtmospheric Optics of Siberian Branch of the Russian
Academy of Sciences, Tomsk, Russia; 3 University of Oulu,

13:00 – 14:00
JSII-P: JSII Poster session
JSII-P.1 MON

Six-Telescope Ultrafast Laser Inscribed Beam
Combiner for Stellar Interferometry in the J-Band∙A.N. Dinkelaker1 , S. Smarzyk1 , A.S. Nayak1,2 , S.
Piacentini3,4 , G. Corrielli4 , R. Osellame4 , E. Pedretti5 ,M.M. Roth1 , and K. Madhav1 ; 1 Leibniz-Institut für Astrophysik Potsdam (AIP), Potsdam, Germany; 2 Institut
für Angewandte Physik, Friedrich-Schiller-Universität
Jena, Jena, Germany; 3 Dipartimento di Fisica - Politecnico di Milano, Milano, Italy; 4 Istituto di Fotonica e Nanotecnologie (IFN) - CNR, Milano, Italy; 5 UKRI STFC

Oulu, Finland; Aston University, Birmingham, UK
A comparative analysis of the sharp focused Gaussianand Bessel laser beams within the turbid tissue-likescattering medium is performed utilising unidirectional
Helmholtz equation approximation.
4

EJ-P.5 MON

Coexistence of collapsed-snaking-related dark andbright Kerr localized states∙E.K. Akakpo1 , M. Haelterman 1 , F. Leo1 , and P. ParraRivas1,2 ; 1 OPERA-photonics, Universit libre de Bruxelles, Bruxelles, Belgium; 2 Dipartimento di Ingegneria dell’Informazione, Elettronica e Telecomunicazioni,
Sapienza Universitá di Roma, Roma, Italy
We study the formation and stability of dissipative brightand dark localized states emerging in Kerr cavities including second- and fourth-order dispersion. We showthat these states undergo collapsed snaking.

EJ-P.7 MON

EJ-P.9 MON

GPU-Accelerated Full-Field Modelling of Highly
Dispersive Ultrafast Optical Parametric Oscillators∙S.C. Robarts, D.T. Reid, and R.A. McCracken; Scottish Universities Physics Alliance (SUPA), Institute of
Photonics and Quantum Sciences, School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, United Kingdom
We demonstrate GPU-accelerated modelling of ultrafast optical parametric oscillators via the nonlinear envelope equation, with 1071x improvement in execution
time, enabling the exploration of large time-bandwidth
product systems such as highly-dispersive or chirpedpumped cavities.

Laser heating and amorphous Si crystallization incomposites ”amorphous silicon/gold film/quartz
substrate”∙A. Fedotov1 , I. Dadenkov1 , Y. Tsitavets1 , Y. Shafarevich1 ,and O. Fedotova2 ; 1 Belarusian State University, Minsk,
Belarus; 2 Scientific-Practical Materials Research Centre,
NAS Belarus, Minsk, Belarus
We study numerically a process of laser heating of
nanocomposites in configuration “amorphous silicon
film/Au film/quartz substrate” by short pulses and establish that the gold layer may uniformize the distributionof heat increasing the quality of crystallized silicon

EJ-P.8 MON

Plane-wave Expansion based Modelling of Linear and
Non-Linear Response of Resonant Metasurfaces
under Realistic Excitation Conditions∙L.K. A.S., J. Deka, R. Biswas, and V. Raghunathan; Indian Institute of Science, Bangalore, India
We report a unified plane-wave expansion method tomodel linear and nonlinear optical characteristics of resonant metasurfaces considering arbitrary excitation angular profile. Good agreement is obtained between themodel and experimentally obtained sum-frequency generation spectra.

Square-Wave Generation in Vertical External-Cavity
Kerr-Gires-Tournois Interferometers∙E.R. Koch1 , T.G. Seidel1 , S.V. Gurevich1,3 , and J.
Javaloyes2 ; 1 Institute for Theoretical Physics, Universityof Münster, Münster, Germany; 2 Departament de Física,
Universitat de les Illes Balears & IAC-3, Palma de Mallorca, Spain; 3 Center for Nonlinear Science (CeNoS), University of Münster, Münster, Germany
We investigate the mechanisms of square-wave formation in vertical external-cavity Kerr-Gires-Tournois Interferometers. We provide a simple analytical approximation for the plateau values and we demonstrate thatsquare-waves can emerge in a homoclinic snaking scenario.

EJ-P.6 MON

Multiplexed spatially-focused localisation of light inadipose biological tissues∙A. Bykov1 , V. Tuchin2 , and I. Meglinski1,3 ; 1 University ofOulu, Oulu, Finland; 2 Saratov State University, Saratov,
Russia; 3 Aston University, Birmingham, United Kingdom
We report the observation of a new type of natural
spatially-resolved longitudinal multi-spot focusing localisation of light within adipose tissues, where the cascade of individual adipocytes act as an ensemble ofmicro-scale lenses.

Rutherford Appleton Laboratory, Chilton, United Kingdom
We have fabricated a six-telescope near-infrared discrete
beam combiner (DBC) for stellar interferometry in the Jband using ultrafast laser inscription (ULI). For laboratory characterization, we populate the visibility-to-pixelmatrix and identify the complex visibility.

Bentz4 , A. Gonzalez3 , J. Harrington5 , N. Law6 , T.
Maccarone7 , and R. Quimby8 ; 1 College of Optics andPhotonics (CREOL), University of Central Florida, Orlando, FL, USA; 2 Department of Physics, University ofCentral Florida, Orlando, FL, USA; 3 Department of Astronomy, University of Florida, Gainesville, FL, USA;
4
Georgia State University, Atlanta, GA, USA; 5 Planetary
Sciences Group, Department of Physics, University of Central Florida, Orlando, FL, USA; 6 University of North Carolina - Chapel Hill, Chapel Hill, NC, USA; 7 Texas Tech
University, Lubbock, TX, USA; 8 San Diego State University, San Diego, CA, USA
The OPA project, the Original PolyOculus Array, isa seven-pack telescope array that uses the PolyOculus
technology to create a large-area-equivalent telescope for

JSII-P.2 MON

OPA! The Original PolyOculus Array for Mt. Laguna
Observatory∙C. Moraitis1,5 , S. Eikenberry1,5 , R. Amezcua-Correa1 ,S. Yerolatsitis1 , C. Warner3 , D. Wright2 , H. Reale1 , J.
Foran1 , A. Akers1 , J. Rowe1 , K. Semmen1 , V. Pagliuca1 ,T. Thomas1 , N. Salem1 , V. Miller1 , N. Harmon1 , M.

80

EJ-P.10 MON

spectroscopy by combining the light of each small telescope via photonic lantern
JSII-P.3 MON

Study of optimized photonic building blocks andfunctions in electro-optic mid-infrared lithium
niobate waveguides for astrophotonic applications∙G. Martin1 , M. Bonduelle1 , R. Salut2 , L. Robert2 , and
N. Courjal2 ; 1 IPAG, Grenoble, France; 2 FEMTO ST, Besançon, France
In order to develop new photonic based astronomical instruments, optimized mid infrared waveguides
and functions in electro-optical lithium niobate material
have been conceived and fabricated. The characterization results on these samples will be presented.

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⋅ Monday 26 June 2023

CLEO

Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Tuesday 27 June 2023

Room 13a ICM

Room 13b ICM

Room 14a ICM

Room 14b ICM

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

CM-4: Temporal andspatial beam shaping forlaser processing II

CK-2: Plasmonic structures and components

EG-4: Ultrastrong lightmatter interactions andnonlinear optics

CA-4: Polarization
effects and structured
laser beams

CB-3: Novel semiconductor laser concepts

CD-4: Specialty fibers

CH-3: On-chip opticalsensing

Chair:
Mathieu Mivelle,
CNRS, Sorbonne university,
Paris, France

Chair: Ammar Hideur, CORIA, Université de Rouen Normandie, France

Chair: Francois Courvoisier,
Université de Franche-Comté,
FEMTO-ST Institute, CNRS,FranceCM-4.1 TUE

Chair: Humeyra Caglayan,
Tampere University, Finland

Chair: Marco Gaulke, ETH,
Zürich, Switzerland

Chair: Goery Genty,Tampere
University, Finland

Chair:
Florenta Costache,
Fraunhoffer IPMS Dresden,
Germany

8:30

CK-2.1 TUE (Keynote) 8:30

EG-4.1 TUE (Invited) 8:30

CA-4.1 TUE

8:30

CB-3.1 TUE (Invited) 8:30

CD-4.1 TUE

8:30

CH-3.1 TUE (Invited) 8:30

High aspect ratio nanopillars fabricated by a single
pulse of ultrafast Bessel
beam∙V.V. Belloni, M. Hassan, L.
Furfaro, L. Froehly, C. Billet,
R. Giust, and F. Courvoisier;
FEMTO-ST Institute, Besancon, France
Radially and azimuthally polarized Bessel beams present ahollow cylindrical focus. Usedin single femtosecond illumination, they can produce positive structures up to 15 μm
high with a sub-micron diameter by matter ejection.

Nonlinear Optics with
Nanoparticles and Metamaterials∙A. Zayats; King’s College London, London, United Kingdom
Weak nonlinearity of conventional materials can beenhanced by their nanostructuring. We will overview
recent developments andtrends in engineering spectral
and temporal response ofcoherent and incoherent
optical nonlinearities with dielectric, plasmonic and hybrid
nanoparticles, nanostructuresand metamaterials.

Many-body superradianceand dynamical symmetry
breaking in waveguide QED∙A. Asenjo-Garcia; Columbia
University, New York, USAI will discuss the many-bodydecay of extended collectionsof two-level systems, and focus on the situation where
they are all coupled to a onedimensional photonic reservoir.

Radially polarized ceramic
Yb:Lu2O3 thin-disk laser∙D. Didychenko, S. Esser,
F. Beirow, T. Graf, and M.
Abdou Ahmed; Institut fürStrahlwerkzeuge, University of
Stuttgart, Pfaffenwaldring 43,70569 Stuttgart, Germany
We report on generation ofradially polarized beam in aceramic Yb:Lu2O3 thin-disk
oscillator. An output power
and optical efficiency of 175W
and 39.7% were respectively
achieved. A degree of radialpolarization >93% is obtained.

Different Phases of
Polariton Lasers
J. Hu, N. Lydick, K. Sun, and∙H. Deng; University of Michigan, Ann Arbor, USA
We will discuss phase separation in a polariton condensate, between a quasi-BEC
without long-range order anda BKT-like phase with quasilong range order, due to theinterplay of nonlinearity andpumping, thermalization anddecay.

Intra-Modal Phase-Sensitive
Four-Wave Mixing in a
Few-Mode Fiber∙V. Gaudillat1 , M. Barbier1 ,L. Bramerie1 , M. Gay1 , M.
Bigot-Astruc2 , P. Sillard2 , Y.
Dumeige1 , and C. Peucheret1 ;1
Univ Rennes, CNRS, FOTON- UMR 6082, Lannion, France;2
Prysmian Group, Haisnes,
FranceWe
experimentallydemonstrate
intra-modal
signal/idler-degenerate
phase-sensitive
four-wave
mixing in two LP modes(LP01 and LP11) of a 2-km
long step-index 4-mode fiber.

Trace gas absorption
spectroscopy on a chip
∙J. Jagerska1 , M. Vlk1 , J. Salaj1 ,H.D. Yallew1 , S. Alberti1 , R.
Zakoldaev1 , J. Høvik2 , andA. Aksnes2 ; 1 UiT The Arctic
University of Norway, Tromsø,
Norway; 2 NTNU, Trondheim,
NorwayWe report on sensitive tracegas
spectroscopy
using
nanophotonic
waveguides
with extraordinarily large air
confinement factors. Methane
and isotope-specific CO2
detection down to 300 and
30 ppb, respectively, wereachieved with only 1 cm2chips.

CM-4.2 TUE

8:45

Conductive Microelectrode
Generation in Diamond
Using Pulsed Bessel Beams∙A.
Kuriakose1,2 ,A.
Chiappini3 ,B.
Sotillo4 ,A. Britel5 , P. Apra5 , F.
Picollo5 , and O. Jedrkiewicz1 ;1
IFN-CNR, Udr di Como,
Como, Italy; 2 Dipartimento
di Scienza e Alta Tecnologia,
Università
dell’Insubria,
Como, Italy; 3 Istituto di
Fotonica e Nanotecnologie(IFN)-CNR, CSMFO andFBK-CMM, Trento, Italy;
4
Department of Materials
Physics, Faculty of Physics,
Complutense University of

CA-4.2 TUE

8:45

Phase-locked dual polarization frequency combs in
Yb:YAG∙H. Akagla, G. Loas, M. Vallet,
and M. Brunel; Univ Rennes,
CNRS, Institut FOTON–UMR
6082, Rennes, France
An experimental demonstration of a fully phase-locked
dual polarization pulsed passively mode-locked Yb:YAG
solid-state laser was achieved.
Two frequency combs are associated to the two orthogonal polarization resulting inadjustable pulsed polarization
sequences.
82

CD-4.2 TUE

8:45

Low-Threshold GreenPumped Ultraviolet
Resonant Dispersive-Wave
Emission in Small-Core
Anti-Resonant Hollow-Fibre∙M. Sabbah1 , K. Harrington2 ,R. Mears2 , C. Brahms1 ,A.
Alisauskas1 ,L.R.
Murphy1 , S. Yerolatsitis2 ,W.J.
Wadsworth2 ,J.C.
Knight2 , J.M. Stone2 , R.R.
1
2
Thomson , T.A. Birks , andJ.C. Travers1 ; 1 School ofEngineering and Physical Sciences, Heriot-Watt University,
Edinburgh, United Kingdom;2
Centre for Photonics andPhotonic Materials, Depart-

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⋅ Tuesday 27 June 2023

Room Osterseen ICM

Room 1 Hall B1 (B11)

Room 2 Hall B1 (B12)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

JSVI-1: NanophoXonics,
optomechanical systems
and thermal transport

CF-4: Complex pulse
shaping and characterization

ED-4: Cavity-enhanced
precision spectroscopy

CG-1: Ultrafast magnetic fields and anisotropy

EA-1: Fundamental
quantum optics

EB-4: Quantum
computation I

Chair:
Roberto Li Voti,
Sapienza Università di Roma,
Dept SBAI, Roma, Italy

Chair: Matteo Negro, Cambridge raman imaging, Milano, Italy

Chair: Marco Marangoni, Politecnico di Milano, Milano,
Italy

Chair: Cord Arnold, Lund
University, Lund, Sweden

Chair:
Fabian Maucher,
University of the Balearic
Islands,Palma, Spain

JSVI-1.1 TUE (Invited) 8:30

CF-4.1 TUE

ED-4.1 TUE

8:30

CG-1.1 TUE (Invited) 8:30

EA-1.1 TUE

8:30

EB-4.1 TUE (Invited) 8:30

Optophononic Engineering
Using Semiconductor
Nanostructures∙N.D.
Lanzillotti-Kimura,
M. Esmann, A. Rodriguez,
P. Priya, E.R. Cardozo de
Oliveira, C. Xiang, O. Ortiz,
M. Morassi, L. Le Gratiet, I.
Sagnes, and A. Lemaitre; Université Paris Saclay – CNRS
– Centre de Nanosciences etde Nanotechnologies C2N,
Palaiseau, France
We design and experimentally study a series ofnanophononic devices basedon planar and micropillar
resonators, including FabryPerot and topological cavities.
The structures are basedon superlattices designed
to confine light and soundsimultaneously.

Programmable spatiotemporal control of femtosecond laser pulses focusedalong arbitrary trajectories∙E. Franco, Ó. MartínezMatos, and J.A. Rodrigo;
Universidad Complutense de
Madrid, Facultad de Ciencias
Físicas, Madrid, Spain
We present a theoreticalframework and experimental
setup that allows straightforward
engineeringofstructured ultrashort lightpulses with control of its
peak intensity velocity, timedelay, and pulse phase along
arbitrary 3D trajectories.

Measurement and Assignment of Hot-Band MethaneTransitions Using CavityEnhanced Comb-Based
Double-Resonance
Spectroscopy∙V. Silva de Oliveira1 , I.
Silander1 , A. Hjältén1 , A.
Rosina1 ,L. Rutkowski2 ,G. Soboń3 ,O. Axner1 ,4
K.K. Lehmann , and A.
Foltynowicz1 ; 1 Departmentof Physics, Umeå University,Umeå, Sweden; 2 Université deRennes, CNRS, IPR (Institut
de Physique de Rennes),
3
Rennes, France;
Facultyof Electronics,
Photonics
and Microsystems, Wrocław
University of Science andTechnology, Wrocław, Poland;
4
Departments of Chemistry
and Physics, University ofVirginia, Charlottesville, USA
We use optical-optical doubleresonance spectroscopy with acavity-enhanced comb probe
to measure transitions fromhigh excited rotational levelsin the 3󰜈3 ← 󰜈3 rangeof methane and assign themusing combination differences
and intensity ratios.

Femto- phono- magnetism∙S.
Sharma1
andJ.K.
1
Dewhurst2 ;Max Born
Institute for Nonlinear Optics
and Short Pulse Spectroscopy,
Berlin, Germany; 2 Max Planck
Institute for micro-structure
physics, Halle, Germany
Using a parameter freeab-initio approach to treating ultrafast light-matterinteractions I will show that
selective excitation of opticalphonon modes exert a strong
influence on femtosecond
demagnetisation, offering a
new route to light-controlledfemto-magnetism.

High-Efficiency, UltraBroadband, and Low-Noise
Quantum Memory in
Atomic Barium Vapor∙K.
Shinbrough1,2 ,B.D.
1,2Hunt ,
S. Park3 ,K.
Oolman1,2 , T. Loveridge1,2 ,J.G. Eden3 ,and V.O.
Lorenz1,2 ; 1 Department of
Physics, University of Illinois,
Urbana-Champaign,
USA;
2
IQUIST, University of Illinois,
Urbana-Champaign,USA;
3
Department of Electricaland Computer Engineering,
University of Illinois UrbanaChampaign, Urbana, USAWe
demonstraterecordstorage efficiency, bandwidth,
and noise performance simultaneously in a collisionallybroadened barium vapor
quantum memory, operatingin the ultrabroadband (>100
GHz) regime.

Quantum computation andquantum simulation withstrings of trapped Ca+ ions
∙R. Blatt; University of Innsbruck, Institute for Experimental Physics, Innsbruck, Austria; Austrian Academy of Science, Institute for Quantum
Optics and Quantum Information, Innsbruck, Austria
The state-of-the-art of the
Innsbrucktrapped-ion
quantum computer is briefly
reviewed.
We present an
overview on the available
quantum toolbox and discuss
the scalability of the approach.

CF-4.2 TUE

8:30

8:45

Demonstration of kilometer
propagation of space-timewave packets∙L. Hall1 , M. Romer1 , B.
Turo1 , T. Hayward2 , R.
Menon2 , and A. Abouraddy1 ;1
University of Central Florida,
Orlando, USA; 2 University of
Utah, Salt Lake City, USA
For the first time, we observe a propagation invariant
space-time wave packet propagating under turbulent conditions with an initial beam
size of 2 and 8 mm. This result outperforms the equivalent Gaussian beam by 100x.

ED-4.2 TUE

EA-1.2 TUE

8:45

Will a single two-level atom
simultaneously scatter two
photons?
L. Masters, X. Hu, M.
Cordier, G. Maron, L. Pache,A.
Rauschenbeutel,
M.
Schemmer, and ∙J. Volz;
Humboldt-UniversitätzuBerlin, Berlin, Germany
Here
weexperimentallydemonstrate that, by spectrally rejecting the coherently
scatteredcomponentofthe fluorescence of a single
two-level atom, the remaining
light consists of photon pairsthat have been simultaneously
scattered by the atom.

8:45

Sensitive Fourier-transform
cavity ring down spectroscopy based on a near-infrared frequency comb
R. Dubroeucq1 , D. Charczun2 ,P. Masłowski2 , and ∙L.
Rutkowski1 ; 1 Univ Rennes,
CNRS, IPR (Institut dePhysique de Rennes)-UMR
6251,
Rennes,France;
83

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Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Tuesday 27 June 2023

Room 13a ICM

Room 13b ICM

Madrid,Madrid,Spain;
5
Department of Physics and“NIS”
Inter-departmental
Centre, University of Torino,
Torino, Italy
Top-notch quality, in-bulk
conductive graphitic microelectrodes with a very small
resistivity of 0.04 Ω cm are
fabricatedperpendicular
to the surface of a 500 μm
thick monocrystalline CVD
diamond sample using pulsed
Bessel beams.
CM-4.3 TUE

9:00

Ultrafast Laser Writing with
Pulse Temporal Contrast
Control∙H. Wang, Y. Lei, G. Shayeganrad, and P. Kazansky; Optoelectronics Research Centre,
University of Southampton, Southampton, United
Kingdom
Nanostructuring of silica glass
are controlled by temporalcontrast of femtosecond laser
pulses.
Nanopore-based
birefringent
modificationis created with pulse contrast of 107, while stronger
nanograting-based modification is observed with reduced
contrast of 103

Room 14a ICM

Room 14b ICM

ment of Physics, University ofBath, Claverton Down, Bath,United Kingdom
We demonstrate tunabledeep-ultraviolet
pulsespumped with just several tensof nJ at 515 nm through resonant dispersive wave emission
in a 6 μm core-diameter
argon-filled
anti-resonant
hollow-core fibre.

EG-4.2 TUE

9:00

Ultrafast Dynamics ofMolecular Polaritons in
Photoswitch Nanoantennas
J. Kuttruff1 , M. Romanelli2 ,E.
Pedrueza-Villalmanzo3 ,J. Allerbeck4 , J. Fregoni5 ,V. Saavedra-Becerril6 ,J.
Andreasson6 , D. Brida7 , A.
Dmitriev3 , S. Corni2 , and∙N. Maccaferri8 ; 1 Universityof Konstanz, Konstanz, Germany; 2 University of Padova,
Padova, Italy; 3 University
of Gothenburg, Gothenburg,
Sweden; 4 Empa, Swiss Federal
Laboratories for Materials
ScienceandTechnology,
Dübendorf,
Switzerland;
5
Universidad
Autónomade Madrid, Madrid, Spain;
6
Chalmers University of Technology, Gothenburg, Sweden;
7
University of Luxembourg,
Luxembourg,
Luxembourg;8Umeå University, Umeå,SwedenWe study ultrafast dynamics of photocromic molecules
both weakly and strongly coupled to plasmonic nanoantennas. Experiments, verified
by quantum modelling, reveal
sub-ps collapse of molecularpolaritons to intramolecular
dynamics induced by interaction with the plasmons.

CA-4.3 TUE

9:00

Higher-order Visible Vortex
Modes from a Pr3+:YLF
Laser Source Under Intracavity Spherical Aberration∙A.S. Rao1,2,3 , T. Morohashi1 ,W. R. Kerridge-Johns4 , and1
T. Omatsu1,2 ;Graduate
School of Engineering, Chiba
University, Chiba, Japan;
2
Molecular Chirality ResearchCentre, Chiba University,
Chiba, Japan; 3 Institute forAdvanced Academic Research,
Chiba University,
Chiba,
4
Japan;
Photonics Group,
Imperial College London,
London, United Kingdom
We report on the direct generation of higher-order LG
modes at 640 nm (LG0,±31)
and 607 nm (LG0,±17)
wavelengths directly froma Pr3+:YLF laser, which
utilises the presence ofstrong intra-cavity sphericalaberration.

84

CB-3.2 TUE

9:00

Bose-Einstein condensationof photons in a verticalcavity surface-emitting laser∙M. Pieczarka1 , M. Gȩbski2 , A.
Piasecka1 , M. Wasiak2 , and T.
Czyszanowski2 ; 1 Department
of Experimental Physics,
Faculty of Fundamental Problems of Technology, Wrocław
University of Science andTechnology, Wrocław, Poland;
2
Photonics Group, Instituteof Physics, Lodz University ofTechnology, Lodz, Poland
We demonstrate signatures of
Bose-Einstein condensationof photons in a vertical-cavity
surface-emitting laser. We
present condensation andstandard lasing depending on
the relative detuning between
the cavity and the quantum
well resonances in different
devices.

CD-4.3 TUE

9:00

Four-Wave Mixing Enhancement in a Yb-doped
Photonic Crystal Fiber∙B. Krawczyk1 , A. Kudlinski2 ,R. Battle1 , R. Murray1 , andT. Runcorn1 ; 1 Femtosecond
Optics Group, Departmentof Physics, Imperial College,
London, United Kingdom;
2
Universite de Lille, CNRS,UMR 8523-PhLAM–PhysiquedesLasersAtomesetMolecules, Lille, France
We present a novel Yb-doped
PCF and demonstrate that
amplification of FWM pumppulses through stimulated
emission increases the generated anti-Stokes power,
providing a promising route
to increasing conversion
efficiencies beyond nonrare-earth-doped
FWM
PCFs.

CH-3.2 TUE

9:00

Integrated photonics forhigh-precision opticalsensors∙P. Beck1,2 , L. Wynne3 , S.
Iadanza4,5 , L. O’Faolain4,5 ,S.A.
Schulz3 ,andP.
Banzer1,2,6 ; 1 Max Planck Institute for the Science of Light,
Erlangen, Germany; 2 Instituteof Optics, Information andPhotonics,
DepartmentofPhysics,
FriedrichAlexander-University
Erlangen-Nuremberg, Erlangen, Germany; 3 School ofPhysics and Astronomy, SUPA,
University of St Andrews,
St. Andrews, United Kingdom; 4 Centre for Advanced
Photonics & Process Analysis, Munster Technological
University, Cork, Ireland;
5
Tyndall National Institute,Cork, Ireland; 6 Institute ofPhysics, University of Graz,
Graz, Austria
We present a photonic
integrated platform suitablefor various types of highprecision measurements. We
demonstrate measurement of
displacements with a resolution of 7.2nm and discuss
the possible application ofprobing tightly focused vector
beams.

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Room Osterseen ICM

Room 1 Hall B1 (B11)®

/Europe-EQEC 2023

Room 2 Hall B1 (B12)⋅ Tuesday 27 June 2023

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)EA-1.3 TUE

EB-4.2 TUE

Institute of Physics, Faculty ofPhysics, Astronomy and Informatics, Nicolaus Copernicus
University, Grudziadzka 5,
Torun, Poland
We perform Fourier transform cavity ring down spectroscopy of CO using a high finesse cavity and an optical frequency comb. The new stabilization setup allows averaging the broadband spectra
and reaching a high absorption sensitivity.

2

JSVI-1.2 TUE (Invited) 9:00

CF-4.3 TUE (Invited) 9:00

ED-4.3 TUE (Tutorial) 9:00

CG-1.2 TUE

Engineering thermaltransport in lowdimensional systems
Y. Kaur1 , C. Arya1 , S.
Tachikawa1 , A. K. Sivan1 ,G. de Vito1 , R. Swami1 ,J. Trautvetter1 ,D. deMatteis1 , B. Abad1 , and∙I. Zardo1,2 ; 1 Departmentof Physics, University ofBasel, Basel, Switzerland;2
Swiss Nanoscience Institute,
University of Basel, Basel,
Switzerland
In this talk, we present ourachievements on engineeringand probing of phononic
properties
andthermaltransport in nanowires. We
also discuss challenges andprogresses in the measurement of thermal conductivityof nanostructures and low
dimensional systems.

Arbitrary CEP
Manipulation for
Spatiotemporal Control of
Sub-cycle Optical Vortex∙Y.-C. Lin, K. Midorikawa,and Y. Nabekawa; Attoseconds
ScienceResearchTeam,
RIKEN Center for Advanced
Photonics,
2-1 Hirosawa,
Wako, Saitama, Japan
This study shows spatiotemporal control of an arbitrarily
carrier-envelope phase controllable, over-octave bandwidth vortex source with awavelength range of 0.9-2.4
μm and a pulse duration of
4.7 fs, corresponding to 0.9 cycles at the carrier wavelengthof 1.54 μm.

Cavity-Enhanced Precision
Spectroscopy of Molecules∙S.-M. Hu; University of Science and Technology of China, Hefei, China
Cavity-enhanced
spectroscopy methods induce
km-longmolecule-lightinteraction path lengths
andprovidekW-powerlaser fields, which allow for
high-precision spectroscopy
of molecules, with broad
applications in fundamental
physics and beyond.

Nonlinear Light-Induced
Attosecond Magnetization
Dynamics in Non-Magnetic
Materials
O. Neufeld, ∙N. TancogneDejean, U. De Giovannini,
H. Hübener, and A. Rubio;
Max Planck Institute for
the Structure and Dynamics
of Matter and Center for
Free-Electron Laser Science,
Hamburg, Germany
We predict that cascaded
nonlinear-optical processes insolids can convert sub-cycle
light-induced
electronic
currents to transient magnetism, generating the fastest
magnetic response to dateof ~500 attoseconds, paving
the way to new regimes ofmagnetism.

85

9:00

9:00

Catching quantum jumps
through heterodyne
monitoring of a thermal
drive∙G. Hennin1,2
and H.
1
Carmichael1,2 ;Universityof Auckland, Auckland, New
Zealand; 2 Dodd Walls Centre,
Dunedin, New Zealand
The coherence of an atomic
quantum jump triggered by athermal drive is recovered bycontinuously monitoring thesystem emissions using heterodyne detection.

9:00

Non-Adiabatic Holonomic
Quantum Gates∙V. Neef, J. Pinske, M. Heinrich, S. Scheel, and A. Szameit;
Institut for Physics, Universityof Rostock, Rostock, Germany
We present non-adiabatic
holonomic quantum gates
and a quantum algorithm,
paving the way towards
noise-resilient quantum computing in integrated quantum
optics. Their topologicallyprotected
functionalities
are realized solely by meansof non-Abelian geometricphases.

NOTES

CLEO

Room 1 ICM
CM-4.4 TUE

Room 4a ICM
9:15

CK-2.2 TUE®

/Europe-EQEC 2023

Room 4b ICM
9:15

EG-4.3 TUE⋅ Tuesday 27 June 2023

Room 13a ICM
9:15

CA-4.4 TUE

9:15

Room 13b ICM
CB-3.3 TUE

9:15

Room 14a ICM
CD-4.4 TUE

9:15

Room 14b ICM
CH-3.3 TUE

9:15

Adjustable focal zone beam
shaping by using custom
spatially variable waveplates
aimed for laser micromachining∙E. Nacius1,2 , O. Ulčinas2 , J.
Minkevičius1 , S. Orlov1 , and
V. Jukna1,3 ; 1 Center for Physical Sciences and Technology,
Vilnius, Lithuania; 2 Workshop
of Photonics, Vilnius, Lithuania; 3 Laser Research Center,
Vilnius University, Vilnius,
Lithuania
Spatially variable waveplateswith omitted central part are
implemented to transform thebeam intensity distribution at
the focal zone. Such way vector beams with unique intensity distribution patterns canbe created suitable for laser
micromachining.

Plasmonic Nanostructures
for Improved Photodetection∙D. Cristea, R. Tomescu,
P. Obreja, and V. Anastasoaie;
National Institutefor Research and Development in Microtechnologies –IMT Bucharest, Voluntari,
Romania
We present the fabricationand characterization of two
types of plasmonic-enhanced
photodetectors: hot-cariersbased
Schottkysiliconphotodetectors with responsivity up to 50mA/W in SWIR
and solution-processed photodetectors with embedded
nanoparticles, having highresponsivity (0.4...1mA/W)
from UV to SWIR.

Multi-Octave Deep-Strong
Light-Matter Coupling ofMultiple Modes∙J. Mornhinweg1,2 , L. Diebel1 ,M. Halbhuber1 , V. Zeller1 ,J. Riepl1 , T. Inzenhofer1 , D.
Bougeard1 , R. Huber1 , andC. Lange2 ; 1 Department of
Physics, University of Regensburg, Regensburg, Germany;
2
Department of Physics, TU
Dortmund University, Dortmund, Germany
Non-resonant, deep-strong
coupling of multiple matterand light modes allows forrecord strength coupling
equivalent to ΩR /ω c = 3.19
with a spectrum spanning
6 octaves and over 10 intertwined polaritons, resulting
in a virtual photon population>1.

Orange, red and deep red
optical vortex mode
operation in Pr3+:fiber laser∙Y. Yoneda1,2 , W. R. KerridgeJohns3 , S.R. Allam2 , Y.
Fujimoto1 , and T. Omatsu2 ;1
Chiba Institute of Technology,
2
Chiba, Japan;
Graduate
School of Engineering Chiba
University, Chiba, Japan;
3
Photonics Group, The Blackett Laboratory, Departmentof Physics, Imperial College
London, London, United
Kingdom
We demonstrate, for the firsttime, ultracompact visible
vortex fiber laser based on aPr3+:fiber with control of a
3-color (orange, red, and deepred) and handedness of thevortex mode.

Quasi PT-symmetric design
for single-mode high-poweredge-emitting semiconductor lasers∙B. Olyaeefar1 , E. Şeker1 ,S. Şengül1 , K. Dadashi1 ,M.H.
Teimourpour2 ,R.
El-Ganainy2,3 ,andA.
Demir1 ; 1 UNAM - Instituteof Materials Science andNanotechnology,
Bilkent
University, Ankara, Turkey;
2
DepartmentofPhysics,
Michigan Technological University, Houghton, Michigan,
USA; 3 Henes Center for Quantum Phenomena, Michigan
Technological
University,
Houghton, Michigan, USA
Quasi PT-symmetry concept,
with reduced operational sensitivity, is introduced to selectively filter the high-ordermode in high-power edgeemitting lasers. Single-mode
beam emission at high powers above 400mW is demonstrated experimentally.

Experimental study of thestructural dependence of
backward Brillouin gain in
solid-core photonic crystal
fibres∙G. Ji1 , W. He2,3 , Y. Zheng4 ,R. Yin4 , X. Jiang2 , P. Russell2 ,and M. Pang1,2 ; 1 State Key
Laboratory of High Field Laser
Physics and CAS Center for
Excellence in Ultra-intense
Laser Science,
Shanghai
Institute of Optics and Fine
Mechanics (SIOM), CAS,
Shanghai, China; 2 Russell
Centre for Advanced Lightwave
Science,
SIOM-H,
CAS, Hangzhou,
China;
3
Innovation and Integration
Center of New Laser Technology, SIOM, CAS, Shanghai,
China; 4 iFibre Optoelectronics
Technology co. ltd., Ningbo,
China
The Brillouin gain is systematically studied in photonic
crystal fibres with wavelengthscale cores and large air-filling
fractions. For pumping at 1.55
μm, it is found to peak at acore diameter of ~2 μm.

Flip-chip Integration of
Mid-infrared Lab-on-a-chip
for Gas Sensing∙M. Piotrowski, R. Szedlak, J.
Fuchsberger, G. Marschick, B.
Hinkov, and B. Schwarz; Institute of Solid State Electronics,
Technical University of Vienna,
Vienna, Austria
Heterogeneous integration ofa mid-infrared lab-on-a-chipfor gas sensing, consistingof quantum or interband
cascade lasers and respective
detectors, together with afully suspended waveguiding
membrane with an interaction
path length in centimetre
range.

CM-4.5 TUE

CK-2.3 TUE

EG-4.4 TUE

CA-4.5 TUE

9:30

CB-3.4 TUE (Invited) 9:30

CD-4.5 TUE

CH-3.4 TUE

Pump-polarization
dependence of thebipolarization emission in
ytterbium lasers∙H. Akagla1 , N. Chapron1 , P.
Lehoux1 , G. Loas1 , P. Loiko2 ,A. Benayad2 , P. Camy2 , M.
Vallet1 , and M. Brunel1 ;1Univ Rennes, CNRS, Institut
FOTON–UMR 6082, Rennes,
France; 2 Centre de recherche
sur les Ions, les Matériaux etla Photonique (CIMAP), UMR
6252 CEA-CNRS-ENSICAEN,
Université de Caen, Caen,
FrancePump polarization orientation is used to control the
relative powers of two linear,orthogonally polarized, eigenstates in isotropic Yb lasers.

The Berkeley Surface
Emitting Laser (BerkSEL): a
scale-invariant laser?
∙B. Kante; UC Berkeley, Berkeley, USAI will discuss a scalable aperture that solves the six decade
optics challenge of single apertures scaling. I will discuss
the physics of the discovery
that we named Berkeley Surface Emitting Laser (BerkSEL)

Few-cycle, high power, highrepetition rate Yb laser
source based on multidimensional solitary statesin hollow-core fibers∙A. Longa1 , L. Arias 1 , G.
Jargot1 , A. Pomerleau1 , P.
Lassonde1 , G. Fan1,2 , R.
Safaei3 , P.B. Corkum3 , F.
Boschini1 , H. Ibrahim1 , andF. Légaré1 ; 1 Institut Nationald la recherche scientifique,Centre Énergie Matériaux
etTélécommunications,
2Montréal, Canada;
The
Hamburg Centre for Ultrafast
Imaging CUI, Universität
Hamburg, Hamburg, Germany; 3 Department of Physics,
University of Ottawa, Ottawa,
Canada

9:30

Spatially Shaped Femtosecond Laser Pulses for
Micromachining ofMaterials with Dielectric
Microlenses∙C. Florian1,2 and J. Siegel1 ;1Consejo Superior de Investigaciones Cientificas, Madrid,
Spain; 2 Universität Kassel,
Kassel, Germany
Spatially shaped femtosecond
laser pulses are used for lasermachining of silicon using a
direct-laser write system incombination with dielectric
microspheres. By tailoring
the beam wavefront, size andshape of the imprinted pattern
are modified.

9:30

Fast Electrical Modulationof Single Plasmonic
Nano-Rod Resonance
L. Zurak, J. Meier, R. Kullock,
B. Hecht, and ∙T. Feichtner;
Nano-Optics and Biophotonics
Group, Experimentelle Physik
5, JMU Würzburg, Würzburg,
Germany
We charge an electricallycontacted nano particle madefrom gold. Its resonance canthus be shifted with up to 50
kHz on the order of 10−4 .
To explain the experimental
results, a quantum descriptionof the metal surface is needed.

9:30

Polarization Vortex-Driven
Third-Harmonic Generation
in a Single Vertically-Aligned
Semiconductor Nanowire∙S.
Annurakshita1 ,H.
Mäntynen2 , Y. Tamashevich1 ,L. Kallioniemi1 , X. Zang3 , N.
Anttu2,4 , M. Ornigotti1 , H.
Lipsanen2 , and G. Bautista1 ;1
Photonics
Laboratory,
Physics Unit, Tampere University, Tampere, Finland;
2
Department of Electronics
and Nanoengineering, Aalto
University, Espoo, Finland;
3
DepartmentofApplied
Physics, Aalto University, Espoo, Finland; 4 Physics, Facultyof Science and Engineering,Åbo Akademi University,
Turku, Finland

86

9:30

9:30

Silicon nitride 1D photonic
crystal cavity Hybrid Laser
for Refractive Index sensing
in liquid and gaseous media∙T. Oliveira1,2 , S. Iadanza1,2 ,J.H. Mendoza-Castro3 , M.
Grande3 , and L. O’Faolain1,2 ;1Tyndall National Institute,2
Cork, Ireland;
Munster
Technological
University,
Cork, Ireland; 3 Politecnico diBari, Bari, Italy
In this work we show the employment of a novel designof silicon nitride 1D photonic
crystal (PhC) cavity in hybrid
external cavity laser (HECL)
configuration for optical sensing applications, with very
low-detection limits.

CLEO

Room Osterseen ICM

JSVI-1.3 TUE

9:30

Long-Range Surface
Plasmon-Polaritons in
Bilayer Graphene as
Efficient Thermal Energy
Carries∙Y. Kosevich, J. OrdonezMiranda, M. Nomura, and S.
Volz; Institute of Industrial
Science, The University ofTokyo, Tokyo, Japan
Long-range surface plasmonpolaritons can be supported
by bilayer graphene due toits interplane polarizability.
Long-range surface plasmonpolaritons in bilayer graphene
are proposed as efficient
thermal energy carriers withlong propagation length andhigh group velocity.

Room 1 Hall B1 (B11)

CF-4.4 TUE

9:30

Ultrashort pulse characterization over octave spanningspectral range in visible-IR
using amplitude swing∙M. López-Ripa, Í.J. Sola, and
B. Alonso; Grupo de Aplicaciones del Láser y Fotónica(ALF), Universidad de Salamanca, Salamanca, Spain
We demonstrate the capabilityof amplitude swing to characterize ultrashort laser pulses atdifferent spectral regions overan octave spanning in visibleIR without significant modifications. Thus, it can ease theapplications of tunable laser
sources.

®

/Europe-EQEC 2023

Room 2 Hall B1 (B12)⋅ Tuesday 27 June 2023

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)CG-1.3 TUE

EA-1.4 TUE

EB-4.3 TUE

9:15

9:15

9:15

Fourier-Limited Few-Cycle
Attosecond Pulses from
High-Order Harmonic
Generation Assisted by an
Ultraintense Ultrafast
Magnetic Field∙R.
Martín-Hernández1 ,H. Hu2 , A. Baltuska2 , L.
Plaja1 , and C. Hernández1
García1 ;Universidad de
Salamanca,
Salamanca,
Spain; 2 Technische Universität
Wien, Vienna, Austria
We propose a high-orderharmonic generation configuration assisted by strong magnetic fields, generated fromtwo
counter-propagating
high-power lasers.
Our
results demonstrate that near
Fourier-limited, chirp-free,
few-cycle attosecond pulses
are generated in the water
window.

Emergent equilibrium andquantum criticality insystems with two-photon
drive and dissipation∙V.Y. Mylnikov, S.O. Potashin,
G.S. Sokolovskii, and N.S.
Averkiev; Ioffe Institute, St.
Petersburg, Russia
We study nonequilibrium dissipative phase transition of the
optical oscillator with twophoton drive and dissipation.
Quantum criticality is considered at the critical point, andwe obtain emergent equilibrium away from it.

A quantum-bit encoding
converter∙B.E. Asenbeck1 , T. Darras1 ,G. Guccione2 , A. Cavaillès3 , A.
Boyer1 , H. Le Jeannic1 , and J.
Laurat1 ; 1 Laboratoire Kastler
Brossel, Sorbonne Université,
CNRS, ENS-Université PSL,
Collège de France, Paris,
France; 2 Centre for Quantum
Computation and Communication Technology,
The
Australian National University, Canberra, Australia;
3LightOn, Paris, France
We demonstrate an opticalqubit converter, enabling
the faithful conversion ofquantum information fromdiscrete- to continuousvariable qubits. The classicallimit of conversion is exceeded,demonstrating
an essential path to scale
up quantum technology
infrastructures.

CG-1.4 TUE

EA-1.5 TUE

EB-4.4 TUE

9:30

Anisotropic High Harmonic
Generation in Wide Bandgap Dielectrics∙H. Allegre1 , K. Kowalczyk1 ,A. Wyatt2 , E. Springate2 , J.
Marangos1 , J. Tisch1 , and M.
Matthews1 ; 1 Imperial College
London, London, United Kingdom; 2 Central Laser Facility,
Harwell, United Kingdom
We present polarisation dependent harmonics generated
from crystalline samples,
MgO, CaF2 and Al2O3 at
780 nm. We show that eachsample present a specificsymmetry depending on its
crystal structure and latticelayout.

87

9:30

Multi-Mode Frequency
Filtered Photon Correlations of a Driven ThreeLevel Atom∙J.
Ngaha1,2
andH.
1Carmichael1,2 ;The University of Auckland, Auckland,
New Zealand; 2 The DoddWalls Centre for Photonic
and Quantum Technologies,
Dunedin, New Zealand
We have developed a novel
approach to calculating frequency filtered photon correlations. In this work wedemonstrate its effectivenesswhen applied to a three-level
ladder-type atom driven at
two-photon resonance.

9:30

Analog-Digital HybridComputations with Trapped
Ions∙N.M. Linke; Duke Quantum
Center,Duke University,
Durham NC, USA; Joint
Quantum Institute, Universityof Maryland, College Park,USA
The motional modes oftrapped ions represent anunderused quantum resourcethat can encode bosonicdegrees of freedom for
efficient quantum simulation.
In combination with gates
they can create a powerful analog-digital hybrid
quantum machine.

NOTES

CLEO

Room 1 ICM

CM-4.6 TUE

Room 4a ICM

9:45

Galaxy-shaped vortex
surface relief formation byillumination of orthogonal
Laguerre-Gaussian modes∙D. Suzuki1 , A. Tomita1 , A.
Vallés1,2,3 , K. Miyamoto1,2 ,and T. Omatsu1,2 ; 1 Graduate
School of Science and Engineering, Chiba University,
Chiba, Japan; 2 Molecular
Chirality Research Center,
Chiba University,
Chiba,
3
Japan;
ICFO-Institut deCiencies Fotoniques,
The
Barcelona Institute of Scienceand Technology, Barcelona,
Spain
We present the first demonstration of the relief withmultiple spiral arms, named”galaxy-shaped
surfacerelief,” in an azo-polymer
film by employing petal beam
formed of the superpositionof positive and negative
Laguerre-Gaussian modes.

CK-2.4 TUE

9:45

Polariton Smith-Purcell
emission∙L. Prelat1 , E.J.C. Dias1 ,and J. García de Abajo1,2 ;1
ICFO-Institut de Ciencies
Fotoniques,
Castelldefels(Barcelona), Spain; 2 ICREAInstitució Catalana de Recerca
i Estudis Avançats, Barcelona,Spain
We theoretically study the
coupling between free electrons and polaritons mediatedby a single small scatterer,
as well as polariton SmithPurcell emission assisted byscatterer arrays, obtaining
the conditions to maximize
electron–polariton coupling®

/Europe-EQEC 2023

⋅ Tuesday 27 June 2023

Room 4b ICM

Room 13a ICM

We demonstrate the use of
cylindrical vector beams toprobe unambiguously thethird-harmonic
generationfrom a single verticallyaligned GaAs nanowire. The
implications of the techniquein high contrast imaging areshown.

Experimental
observations
in Yb:YAG and Yb:CaF2
are in full agreement witha two-mode rate-equation
model.

We demonstrate pulse compression from 300 fs down to
17 fs up to 20 kHz using multidimensional solitary states ina hollow-core fiber filled withmolecular gas in differential
pressure to mitigate thermal
effects.

EG-4.5 TUE

CA-4.6 TUE

CD-4.6 TUE

9:45

Nonlinearphotoluminescence in gold
thin films∙Á. Rodríguez Echarri1 , F.
İyikanat1 , S. Boroviks2,3 , N.A.
Mortensen2,4,5 , J.D. Cox2,4,5 ,and F.J. García de Abajo1,6 ;1
ICFO - The institute of Photonic Sciences, BARCELONA,
Spain; 2 Center for Nano
Optics, University of Southern
Denmark, Odense, Denmark; 3 Nanophotonics andMetrology Laboratory, Swiss
Federal Institute of Technology
Lausanne (EPFL), Lausanne,
Switzerland; 4 Danish Institutefor Advanced Study, Universityof Southern Denmark, Odense,
Denmark; 5 POLIMA – Center
for Polariton-driven Light–
Matter Interactions, Universityof Southern Denmark, Odense,
Denmark; 6 ICREA – Institució
Catalana de Recerca i Estudis
Avançats, Barcelona, Spain
We investigate nonlinear
photoluminescenceincrystal-quality gold thinfilms using rigorous ab
initio theory supported byexperimental measurements
to reveal the importanceof ultrafast electronic heattransport in the nonlinear
optical response.

9:45

Dynamic control of MEXEL
micro laser modes using aspatially modulated pump
∙G. Kontenis1 , D. Gailevičius1 ,and K. Staliūnas1,2,3 ; 1 Laser
Research Center,
Vilnius,
Lithuania; 2 ICREA, Passeig
Lluís Companys, Barcelona,
Spain; 3 UPC, Dep. de Fisica,
Rambla Sant Nebridi, Terrassa(Barcelona), Spain
We demonstrate the formation of various micro-laser
modes by shaping the pumpbeams
spatialintensity
profile. We dynamically tune
the generated laser beams
shape by application of aprogrammable Spatial Light
Modulator.

88

Room 13b ICM

Room 14a ICM

9:45

Kuramoto transition inharmonically mode-locked
soliton fibre laser based on
optoacoustic interaction in
PCF∙X. Wang1,2 , W. He3,4 , X.
Jiang3 , X. Zhang1,2 , Q.
Huang2 , X. Chang2 , and M.
Pang1,2,3 ; 1 Department of
Optics and Optical Engineering, University of Science andTechnology of China, Hefei,
China; 2 State Key Laboratoryof High Field Laser Physics
and CAS Center for Excellencein Ultra-intense Laser Science,
Shanghai Institute of Optics
and Fine Mechanics (SIOM),
Chinese Academy of Sciences(CAS), Shanghai,
China;
3
Russell Centre for Advanced
Lightwave Science, SIOM and
SIOM-H, CAS, Hangzhou,
4
China;
Innovation andIntegration Center of New
Laser Technology, SIOM, CAS,
Shanghai, China
We report observations andanalytical modelling of theself-organization process ofa harmonically mode-locked
fibre laser based on enhanced
optoacoustic
interactionsin PCF, in which sinusoidal
acoustic interaction between
solitons leads to Kuramototransition.

Room 14b ICM

CH-3.5 TUE

9:45

Near-IR detection using
Photothermal Actuation of
Guided-Mode Resonance
MEMS Structures inGermanium∙P. Rao, D. Rout, and S.K. Selvaraja; Indian Institute of Science, Bangalore, India
We design and demonstratenear-infrared
detection
exploiting the photothermal
and mechanical propertiesof a suspended Ge-based
one-dimensionalguidedmode-resonance(GMR)
structure. This is the first
demonstration of photothermal actuated photodetection
using a GMR.

CLEO

Room Osterseen ICM

JSVI-1.4 TUE

Room 1 Hall B1 (B11)®

/Europe-EQEC 2023

Room 2 Hall B1 (B12)⋅ Tuesday 27 June 2023

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)CG-1.5 TUE

EA-1.6 TUE

EB-4.5 TUE

9:45

Ultrafast Nano Generationof Acoustic Waves in Water:
Thermophone versus
Mechanophone
M. Diego1,2 , M. Gandolfi3,4 ,S. Giordano5 , A. Casto1 , F.M.
Belussi6 , A. Crut1 , F. Vialla1 ,S. Roddaro7 , M. Fasano6 ,F. Vallée1 , P. Maioli1 , N.
Del Fatti1,8 , and ∙F. Banfi1 ;1
Université de Lyon, CNRS,
Université Claude Bernard
Lyon 1, Institut Lumière
Matière, Villeurbanne, France;
2
Institute of Industrial Science,
The University of Tokyo, Tokyo,
Japan; 3 C.N.R-INO, Brescia,
Italy; 4 Department of Information Engineering, Università
di Brescia, Brescia, Italy;
5
Université de Lille, CNRS,
Centrale Lille,
Université
Polytechnique
Hauts-deFrance, Institut d’ElectroniquedeMicroélectroniqueetde Nanotechnologie, Lille,
France; 6 Politecnico di Torino,
Department of Energy, Torino,
Italy; 7 Dipartimento di Fisica”E. Fermi”, Università diPisa, Pisa, Italy; 8 Institut
Universitaire de France, Paris,
FranceThe
photothermoacoustic
launching mechanisms ofwater-immersed nanotransducers
areinvestigatedupon tuning the Kapitza
resistane and the laser pulse
duration. Activation of themechanophone effect allows
launching high frequency
acoustic waves while mimimizing water’s temperature
increase.

CF-4.5 TUE

9:45

Direct Reconstruction of
Two Ultrashort Pulses Basedon Non-InterferometricFrequency-Resolved Optical
Gating∙B. Seifert1,2 , R. RojasAedo1,2 , R.A. Wheatley1,2 ,and D. Hidalgo-Rojas1,2 ;1Facultad de Física, Pontificia
Universidad Católica de Chile,
Santiago, Chile; 2 ANID –Millennium Science Initiative
Program – Millennium Institute for Research in Optics,
Santiago, ChileWe
describeanoninterferometricultrashortpulse measurement techniquebased on frequency-resolved
opticalgating(FROG)
with which pulses can bereconstructed directly, i.e.
non-iteratively.
Only twoslightlydifferent
FROG
spectrograms are measured.

9:45

Generation of topologicalchiral light for robust
enantiosensitive detection
using structured beams∙N. Mayer1 , D. Ayuso2 , E.
Pisanty3 , M. Ivanov1,2,4 , andO. Smirnova1,5 ; 1 Max-BornInstitut, Berlin, Germany;2
Imperial College London,
London, United Kingdom;
3
King’sCollegeLondon,London, United Kingdom;
4
Humboldt Universität zu
Berlin, Berlin, Germany;
5
Technische Universität Berlin,
Berlin, Germany
Combining tailored multicolor structured beams
we create light that displays chirality in time withspatially-varying
handedness, leading to robust andhighly sensitive chiro-opticalresponses with topologicalproperties in chiral molecules.

89

9:45

Autoheterodyne
Characterisation for
Narrowband Photon-Pair
Purity∙V. Prakash1 , A. Sierant 2 ,and M. Mitchell2,3 ; 1 Centerfor
Quantum
Technologies, Singapore, Singapore;2
ICFO-Institut de Ciencies
Fotoniques,
Castelldefels,
Spain; 3 ICREA– Institucio
Catalana de Recerca i Estudis
Avancats, Barcelona, Spain
We report on a quantuminterference based techniqueto characterise very narrowband photon-pairs (≤MHz bandwidth) by highresolution mapping of theirfrequency sum and difference
spectra. This also enables
quantifying their entanglement state and spectral
purities.

9:45

Experimental Study ofTunable Interactions
Between Optically-Trapped
Circular Rydberg Atoms∙P. Méhaignerie, Y. Machu,
A. Durán-Hernández, J.-M.
Raimond, M. Brune, and C.
Sayrin; Kastler Brossel Laboratory, CNRS, ENS-Université
PSL, Sorbonne Université,
Paris, FranceThis work presents the first experimental characterization oftunable interactions between
circular Rydberg atoms, using novel optical engineering
techniques.

NOTES

CLEO

®

/Europe-EQEC 2023

⋅ Tuesday 27 June 2023

Room 1 ICM
10:30 – 11:30

PL-2a.1 TUE (Plenary)PL-2a: EQEC 2023 Plenary talk
Chair: Julien Javaloyes, University of the Balearic Islands,
Spain

Photonic Machines for Large-scale Applications andFundamental Physics∙C. Conti; Department of Physics, University Sapienza,
Rome, Italy

Which is the simplest way to process information withlight? By spatial modulation, we demonstrate combinatorial optimization and natural language processing at
the largest scale. Novel computational paradigms open
the road to new physics and applications with photonics.

Room 1 ICM

Room 13a ICM

Room 13b ICM

10:30

11:30 – 12:30
PL-2b: Award ceremony
Chair: Lukas Gallman, ETH Zurich, Switzerland & Aleksandra Foltynowicz, Umeå University, Sweden

Room 14a ICM

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

PL-3: World of Photonics Plenary

CM-5: Modelling of laser-induced processes

CB-4: Photonic integration I

CD-5: Supercontinuum generation

Chair: Nadezhda Bulgakova, Institute of Physics of the
Czech Academy of Sciences, Prague, Czech republic

Chair: Kamil Pierściński, Łukasiewicz Institute of Microelectronics and Photonics, Ożarów Mazowiecki, Poland

Chair: Christelle Monat, Ecole Centrale Lyon, France

CM-5.1 TUE (Invited)

CB-4.1 TUE (Invited)Supercontinuum Spanning 2.8 Octaves in
4H-Silicon-Carbide Waveguides∙L. Deniel1 , M.A. Guidry2 , D.M. Lukin2 , K.Y. Yang2 , J.
Yang2 , J. Vučković2 , T.W. Hänsch1 , and N. Picqué1 ; 1 Max
Planck Institute of Quantum Optics, Garching, Germany;2
E. L. Ginzton Laboratory, Stanford University, Stanford,USA
A supercontinuum spanning from 0.5 to 3.5 μm is generated in dispersion-engineered silicon-carbide waveguides from 70-fs, 0.19 nJ near-infrared pulses. Low pulse
energy and smooth spectral envelope open up new opportunities for frequency comb spectroscopy.

PL-3.1 TUE (Plenary)

14:00

Laser-driven inertial confinement fusion, powersource of the future?
∙C.L. Haefner1 and T. Ma2 ; 1 Institute for Laser Technology, Aachen, Germany; 2 Lawrence Livermore National
Laboratory (LLNL), Livermore, CA, USA
Fusion ignition has been achieved at the National Ignition Facility at LLNL. This experimental result is a major
scientific breakthrough for laser-driven inertial confinement fusion. This talk presents the experimental results
and technological innovations that made this achievement possible.

14:00

Spatially and time resolved maps of transient
nonequilibrium states in pulsed laser ablation inliquid from large-scale atomistic modeling
C. Chen and ∙L. Zhigilei; University of Virginia, Charlottesville, USA
Spatially and time-resolved maps of transient nonequilibrium states and channels of nanoparticle formation inpulsed laser ablation in liquid are obtained based on the
results of large-scale atomistic simulations.

CM-5.2 TUE

14:00

Monolithic integration of GaSb diode lasers on asilicon photonic circuit∙A. Remis1 , M. Paparella1,2 , L. Monge Bartolomé1 ,A. Gilbert1 , G. Boissier1 , M. Grande2 , A. Blake4 ,L. O’Faolain3,4 , L. Cerutti1 , J.-B. Rodriguez1 , and E.
Tournié1 ; 1 IES, University of Montpellier, C.N.R.S., F34000 Montpellier, France; 2 Department of Electrical andInformation Engineering, Polytechnic University of Bari,
4 Via E. Orabona, IT-70126 Bari, Italy; 3 Center for Advanced Photonics and Process Analysis, Munster Technological University, Bishopstown, IR-T12P928 Cork, Ireland; 4 Tyndall National Institute, Lee Maltings Complex,
Dyke Parade, IR-T12R5CP Cork, Ireland
We report the monolithic integration of mid-infrared
GaSb diode lasers on a Si photonic circuit with around
10% of light coupled into SiN waveguides. This successful demonstration paves the way to fully integrated photonic chips.

14:30

CB-4.2 TUE

Enhanced Energy Absorption and Electron Excitationin Crystalline Silicon Induced by Two-Color Intense
Femtosecond Laser Pulses∙M. Tani, K. Sasaki, Y. Shinohara, and K.L. Ishikawa; The
University of Tokyo, Tokyo, JapanFirst principles simulation shows the energy transferfrom laser to crystalline silicon is dramatically enhancedby mixing IR and UV femtosecond pulses. The dominantmechanism is increase in electron excitation rate assistedby IR component.

14:30

A numerical and experimental butt-coupling analysis
of GaSb diode laser grown on Silicon photonic
integrated circuit∙M. Paparella1,2 , A. Remis1 , L. Monge Barolome1 , J.B. Rodriguez1 , L. Cerutti1 , M. Grande2 , L. O’Faolain3,4 ,and E. Tournié1 ; 1 IES, University of Montpellier, CNRS,Montpellier , France; 2 Department of Electrical and Information engineering, Polytechnic University of Bari,
Bari, Italy; 3 Centre for Advanced Photonics and Process
Analysis, Munster Technological University, Cork, Ireland;
4
Tyndall National Institute, Cork, Ireland
In this work, we model and experimentally demonstrate
the optical coupling between a GaSb diode lasers epitaxially grown on Silicon butt-coupled to passive waveguides. We identify the coupling limits and suggest approaches to mitigate them.
90

CD-5.1 TUE

CD-5.2 TUE

14:00

14:15

Tailored Periodically-Poled Lithium Niobate
Waveguides for Highly Efficient Broadband
Supercontinuum Generation∙F. Ayhan1 , M. Ludwig2 , E. Obrzud3 , D. Grassani3 , V.
Brasch4 , T. Herr2 , and L.G. Villanueva1 ; 1 École Polytechnique Fédérale de Lausanne (EPFL), 1015 Lausanne,
Switzerland; 2 Deutsches Elektronen-Synchrotron DESY,
Notkestr. 85, 22607 Hamburg, Germany; 3 Centre Suisse d’Electronique et Microtechnique SA (CSEM), 2002
Neuchâtel, Switzerland; 4 Q.ant GmbH, Handwerkstraße
29, 70565 Stuttgart, Germany
Using optimized poling patterns and tailored nonlinear
processes, we demonstrate very efficient and broadband
supercontinuum generation in integrated lithium niobate waveguides. The spectra reach the UV and show thegreat potential of such light sources.
CD-5.3 TUE

14:30

Genetic algorithm spectral shaping of supercontinuum over 1550-2000 nm∙M. Hary1,2 , L. Salmela1 , J.M. Dudley2 , and G. Genty2 ;1
Photonics Laboratory, Tampere University, Tampere,
Finland; 2 Université de Franche-Comté, Institut FEMTOST, Besançon, France
We use a genetic algorithm to simultaneously optimize
the intensity in multiple wavelength bands of a supercontinuum from 1550 to 2000 nm. The enhancement factor
varies from 5 to 20 and increases for longer wavelengths.

CLEO

Room 1 ICM®

/Europe-EQEC 2023

⋅ Tuesday 27 June 2023

Room 13a ICM
CM-5.3 TUE

Room 13b ICM
14:45

CB-4.3 TUE

Room 14a ICM
14:45

CD-5.4 TUE

14:45

Ionisation dynamics, damage conditions and surface
patterning in fused silica irradiated with Mid-Infrared femtosecond pulses∙G. Tsibidis1,2 and E. Stratakis1,3 ; 1 Institute of Electronic
Structure and Laser (IESL), Foundation for Research andTechnology (FORTH), Heraklion, Greece; 2 Department ofMaterial Science, University of Crete, Heraklion, Greece;
3
Department of Physics, University of Crete, Heraklion,
GreeceTo elucidate the material response to irradiation with
mid-IR laser sources, a consistent analysis of the interaction of long wavelength femtosecond pulses with dielectric materials is presented

Photonic integration of continuous-wave quantum
cascade lasers with distinct active regions for multispecies gas sensing∙D. Burghart, K. Zhang, A. Koeninger, G. Boemh, and
M.A. Belkin; Technische Universität München, Walter
Schottky Institut and Department of Electrical and Computer Engineering, Garching, Germany
We report the photonic integration of two continouswave quantum cascade lasers with distinct active regions by homogeneous integration on InP. The two colors are further multiplexed to a single output by a passive
evanescent coupler.

High-Power Ultra-Flat Supercontinuum Generation
by Pumping Molecular Gas-Filled Hollow-Core
Fibres in the Green∙A. Lekosiotis, B. Plosz, F. Belli, and J.C. Travers; HeriotWatt University, Edinburgh, United Kingdom
We report the generation of high-power Raman-based
ultra-flat supercontinuum spanning from the ultraviolet to the near-infrared (350-1600 nm) by pumping gasfilled hollow-core anti-resonant fibres in the normal dispersion region at 515 nm.

CM-5.4 TUE

CB-4.4 TUE

CD-5.5 TUE

15:00

15:00

15:00

Laser-induced symmetry breaking in energy absorption of silicon induced by intense femtosecond laser
pulse
J. Sladek1,2 , Y. Levy1 , and ∙T. Derrien1 ; 1 HiLASE Centre Institute of Physics (AS CR), Dolni Brezany, Czech Republic; 2 Faculty of Nuclear Sciences and Physical Engineering- Czech Technical University in Prague, Prague, Czech Republic
Experimental measurements of damage by femtosecond
laser irradiation of silicon were prepared as function of
crystal’s orientation angle with polarization. Quantum
simulations agree with experiments and reveal a symmetry breaking in the crystal’s optical response.

Toward complex GaAs PIC-based laser sources∙J.-P. Koester, O. Brox, H. Wenzel, J. Fricke, P. Della Casa,
A. Maaßdorf, and A. Knigge; Ferdinand-Braun-Institut(FBH), Berlin, Germany
We report on the progression from simple Fabry-Pérotlike diode lasers toward complex GaAs PIC-based laser
sources. This development is illustrated by the resultsof a widely-tunable sampled-grating laser and a dualwavelength laser.

Enhancing Mid-Infrared Supercontinuum Generation at Low Pump Power in SiGe Waveguides∙V. Turpaud1 , N. Koompai1 , T.H.N. Nguyen1 , Y. Yang1 ,J. Frigerio2 , J.-R. Coudevylle1 , D. Bouville1 , C. AlonsoRamos1 , E. Herth1 , L. Vivien1 , G. Isella2 , and D. MarrisMorini1 ; 1 Centre de Nanosciences et de Nanotechnologies,
CNRS, Univ. Paris-Saclay, 91120 Palaiseau, France; 2 LNESS, Dipartimento di Fisica, Politecnico di Milano, Polodi Como, 22100 Como, Italy
We experimentally demonstrate a sub-150 μW averagepump power supercontinuum generation in the midinfrared, ranging from 4 to 10.5 μm wavelength, using
low loss, highly nonlinear graded-index Ge-rich SiGe
waveguides and dispersion management along the propagation.

CM-5.5 TUE

CB-4.5 TUE

CD-5.6 TUE

15:15

Three-Temperature Modeling of Laser Excitation in
Silicon and Parametric Dependence of Damage
Threshold∙P. Venkat1 and T. Otobe1,2 ; 1 Kansai Photon Science Institute, National Institutes for Quantum Science and Technology, Kizugawa (Kyoto), Japan; 2 Photon Science Center,
The University of Tokyo, Bunkyo-ku (Tokyo), Japan
Laser excitation in silicon is studied using threetemperature model (1D-3TM). Calculated damage
thresholds are found to be in reasonable agreement withexperimental data. Effect of laser and target parameters
on damage threshold is also presented.

15:15

Realisation of Multi-Mode Reflector Lasers for
Integrated Photonics∙F.T. Albeladi1,2 , S.-J. Gillgrass1 , J. Nabialek1 , P. Mishra1 ,R. Forrest1 , T.R. Albeladi1,3 , C. Allford1 , M. Tang4 , H.-Y.
Liu4 , S. Shutts1 , and P.M. Smowton1 ; 1 School of Physics
and Astronomy, Cardiff University, Cardiff, United Kingdom; 2 Physics Department, Faculty of Science, University of Jeddah, Jeddah, Saudi Arabia; 3 Physics And Astronomy Department, Faculty of Science, King Saud University, Riyadh, Saudi Arabia; 4 Department of ElectricalEngineering, University College London, London, United
Kingdom
InAs quantum dot multi-mode-interference-reflector(MMIR) lasers with threshold current densities 40%of those of cleaved-cleaved ridge waveguide lasers of
the same cavity length show promise as small footprint
sources for integrated photonics.

91

15:15

Shaped Supercontinuum as a Neural Network
Computing Element
K. Lee and ∙M. Fermann; IMRA America, Inc., Ann Arbor,
USA
We incorporate shaped supercontinuum generation intoa neural network. We are able to perform classification
and autoencoding tasks by phase shaping the seed pulse
and measuring the broadened spectrum.

CLEO

Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Tuesday 27 June 2023

Room 13a ICM

Room 13b ICM

Room 14a ICM

Room 14b ICM

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

CM-6: Laser volume
processing

CK-3: Resonant structures and cavities

EG-5: Single emitters

CB-5: Photonic integration II

CD-6: Mid-IR applications

CH-4: Field applications

Chair: Leonid Zhigilei, University of Virginia, USA

Chair: Emiliano Descrovi, Politecnico di Torino, Italy

CA-5: Diamond lasers
and frequency converters

Chair: Cristina Rimoldi, Politecnico di Torino, Italy

Chair: Haim Suchowski, Tel
Aviv University, Israel

Chair:
Meritxell Vilaseca,
Universitat Politecnica deCatalunya, Terrassa, Barcelona, Spain

CM-6.1 TUE

CK-3.1 TUE

CD-6.1 TUE

16:00

Chair: Christian Kraenkel,
Leibniz-Institut für Kristallzüchtung, Berlin, Germany
16:00

CA-5.1 TUE (Invited) 16:00

CB-5.1 TUE

16:00

CH-4.1 TUE (Invited) 16:00

Femtosecond-Laser Assisted
Selective Etching of Microchannels in Lithium Niobate∙D. Nwatu, D. Kip, and K.
Hasse; Faculty of Electrical Engineering,
HelmutSchmidt University, Hamburg,
Germany
We report on fs-laser assisted selective etching of
microchannels
in
x-cut
LiNbO3 . Up to 1 cm long
microchannels with 10 μm
diameter were etched along
the optical axis within 7 days
using HF(40%) acid.

Enhancing the sensitivity ofsilicon photonic ultrasoundsensors by optimizing thestiffness of polymer cladding∙R.T.
Erdogan1 ,G.A.
Filonenko2 ,S.J. Picken3 ,P.G. Steeneken1 , and W.J.
Westerveld1 ; 1 Department ofPrecision and Microsystems
Engineering, Delft University of Technology, Delft,2
Netherlands;
Departmentof Materials Science andEngineering, Delft Universityof Technology, Delft, Netherlands; 3 Advanced Soft Matter,
Delft University of Technology,
Delft, Netherlands
We
investigate
polymer
claddings to enhance thesensitivity of silicon photonic
ultrasound sensors.
Wetheoretically study the effectof the polymer’s stiffness andexperimentally demonstrate
the enhancement of sensitivity by decreasing polymer
stiffness.

Detection of single ions in a
nanoparticle coupled to afibre cavity
C. Deshmukh1 , E. Beattie1 ,B. Casabone1 , ∙S. Grandi1 ,D. Serrano2 , A. Ferrier2 ,P. Goldner2 , D. Hunger3 ,and H. de Riedmatten1,4 ;1
ICFO - Institut de Ciencies
Fotoniques,
Castelldefels,
Spain; 2 Chimie ParisTech,PSL University, CNRS, Paris,
France; 3 Karlsruher Institut
fur Technologie, Physikalisches
Institut, Karlsruhe, Karlsruhe,
Germany; 4 ICREA - Institució
Catalana de Recerca i Estudis
Avançats, Barcelona, Spain
We report the detection of single erbium ions in a nanoparticle placed in a fiber cavity.
We report a maximum Purcell
factor of 123, as well as saturation of collected counts andan antibunching curve from asingle spectral feature.

A simple pathway to widely
tunable single-frequency
light using monolithic
diamond Raman resonators∙E. Granados; CERN, GENEVE, Switzerland
We demonstrate a simple
methodforgenerating
precisely tunable, singlefrequency nanosecond pulses
using integrated diamondresonators,
suitableforhigh-resolution spectroscopy,
sensing, and quantum optics.
We
measureaccuratelytransitions in Samarium ionsas a proof of its performance.

Tunable Hybrid-Integrated
Diode Laser at 637 nm∙L. Winkler1,2 , K. Gerritsma1 ,A. van Rees1 , P. Schrinner3 ,M. Hoekman3 , R. Dekker3 ,P. van der Slot1 , C. Nölleke2 ,and K.-J. Boller1 ; 1 Universityof Twente, Enschede, Netherlands; 2 TOPTICA Photonics
AG, Gräfelfing, Germany;
3
LioniX International BV,
Enschede, Netherlands
We present a hybridintegrated SiN extended
cavity diode laser with anemission wavelength of 637
nm, the shortest reported forsuch a laser so far. It provides
a record-high mode-hop freetuning range of 43 GHz.

High Conversion Efficiency
Broadband Femtosecond
Mid-IR Optical Parametric
Generation at 10 MHz∙. Sukeert1 , S. Pizzurro2 , A.
Esteban-Martín3 , R. Gotti2 ,L. Carrà4 , G. Piccino4 , A.
Agnesi2 , F. Pirzio2 , C.K.
Suddapalli5 , and M. EbrahimZadeh1,6 ; 1 ICFO-The Instituteof Photonic Sciences, Castelldefels, Spain; 2 Dipartimento
di Ingegneria Industriale edell’Informazione,
Università di Pavia, Pavia, Italy;
3
Departament d’Òptica i
Optometria i Ciències de la
Visió, Universitat de València,
Burjassot, Spain; 4 Bright Solutions Srl, Cura Carpignano,
Italy; 5 Tata Institute of Fundamental Research Hyderabad,
Hyderabad, India; 6 Institució
Catalana de Recerca i Estudis
Avançats (ICREA), Barcelona,
Spain
We report on the generationof broadband mid-IR radiation by exploiting single-passgroup-velocity-matched optical parametric generation of
femtosecond pulses with highconversion efficiency in a 42mm-long MgO:PPLN crystal
at 10 MHz.

Laser-based Sensing forEnergy and Propulsion
Sciences∙R.K. Hanson; Stanford University, Stanford, USA
In this Julius Springer Prize
lecture, I review several
laser-based
sensorandspectroscopic
techniquesdeveloped at Stanford for theadvancement of energy andpropulsion technologies.

CM-6.2 TUE

CK-3.2 TUE

EG-5.2 TUE

CB-5.2 TUE

CD-6.2 TUE

16:15

Selective Laser Etching Dependence on Radiation
Wavelength and Etchant for
Crystalline Materials∙A. Butkute, R. Sirutkaitis, D.
Gailevicius, D. Paipulas, and
V. Sirutkaitis; Vilnius University, Laser Research Center,

16:00

Chair:
Nicolò Maccaferri,Umeå University, Sweden

16:15

Nonlocal Microcapillary
Fibre Sensing Platform∙G. Gardosi and M. Sumetsky; Aston Institute of Photonic
Technologies, Aston University,
Birmingham, United Kingdom
In our proof-of-concept
experiment, we determine

EG-5.1 TUE

16:15

Quantum Imaging Using
Entangled Photon Pairs
from Nonlinear Metasurfaces
J. Ren, ∙J. Ma, J. Zhang, and
A. Sukhorukov; Australian National University, Canberra,
Australia

16:00

16:15

Narrow linewidth ring lasers
for integrated optical gyroscopes∙S. Stopiński1,2,3 , A. Bieniek1 ,S. Latkowski4 ,and R.
Piramidowicz1,2,3 ; 1 Warsaw
University of Technology,
Institute of Microelectronics
92

16:15

Broadband MIR wavelength
conversion in a tapered
silicon core fiber∙D. Wu1 , T. Saini1 , S.
Sun1 ,
M. Huang1 ,L.
Shen2 , T. Hawkins3 , J.
Ballato3 , and A.C. Peacock1 ;1Optoelectronics
ResearchCLEO®

/Europe-EQEC 2023

⋅ Tuesday 27 June 2023

Room Osterseen ICM

Room 1 Hall B1 (B11)

Room 2 Hall B1 (B12)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

JSVI-2: Radiative heattransfer, thermoelectrics& thermochromics, SPP

CF-5: Carrier-envelope
phase metrology andapplications

CE-4: Emission
materials

CG-2: Ultrafast physics
in condensed matter

EB-5: Quantum key
distribution

Chair:
Nadège Courjal,
University of Franche-Comté,
FEMTO-ST, Besançon, France

Chair: Matteo Lucchini, PolItecnico di Milano, Milano,
Italy

CJ-1: Transverse mode
instability in fiber lasers
and amplifiers

Chair: Sebastian Volz, CNRS,The University of Tokyo, Japan

Chair: Nicoletta Haarlammert, Fraunhofer IOF, Jena,
Germany

Chair: Fabian Steinlechner,
University of Jena, Germany

JSVI-2.1 TUE (Invited) 16:00

CF-5.1 TUE (Invited) 16:00

CE-4.1 TUE

16:00

CG-2.1 TUE (Tutorial) 16:00

CJ-1.1 TUE (Invited) 16:00

EB-5.1 TUE

Massive search space
optimization of thermalradiation metamaterials∙J. Shiomi; The University ofTokyo, Tokyo, Japan
We will report recent progresses in applying materials
informatics to optimize thermal radiation metamaterials,
particularly in the scope of extending it to massive search
space, and discuss the capability and remaining challenges
for further development.

Single-Shot CEP Change
Detection in a Nanoantenna
Network∙F. Ritzkowsky1 , M. Yeung2 ,E. Bebeti1 , T. Gebert3,4 , T.
Matsuyama3 , G. Rossi1 , R.
Mainz1,5 , H. Cankaya1,5 , P.
Keathley2 , and F. Kärtner1,5 ;1Deutsches Elektronen Synchrotron, Hamburg, Germany;
2
Massachusetts
Instituteof Technology, Cambridge,
3USA; Max Planck for the
Structure and Dynamics ofMatter, Hamburg, Germany;
4
WiredSense GmbH, Hamburg, Germany; 5 Universität
Hamburg, Hamburg, Germany
We report on the single-shot
carrier-envelope phase change
detection in nanoantenna networks. With a two-cycle midinfrared pulse we generate
sub-cycle electron currents
in ~1000 antennas simultaneously, achieving a carrierenvelope phase dependent
amplitude of 3000 e.

CTH:YAG laser crystal as aspontaneous incoherent
source in the SWIR
L. Lopez, P. Pichon, F. Druon,
P. Georges, and ∙F. Balembois;
Université
Paris-Saclay,
Institut d’Optique Graduate
School, Centre National dela Recherche Scientifique,
Laboratoire Charles Fabry,
Palaiseau, France
CTH:YAGluminescentconcentrator pumped by a
Ce:YAG is demonstrated as
an incoherent source centeredat 2100 nm with a bandwidthof 300 nm. It is more than 20
times brighter spectrally than
SWIR LEDs.

Quantum-coherent
Electron-Light Interactions
in Electron Microscopy∙C. Ropers; Max Planck Institute for Multidisciplinary Sciences, Göttingen, Germany
This tutorial will introduce
principles and applicationsof electron-light scatteringin electron microscopy. Anemphasis will be placedon quantum-coherent processes and recent studies of
spontaneous and stimulated
interactions of free-electron
beams with photonic cavities.

Advances in mode scaling
and TMI suppression in
high-power fibre lasers∙J. Nicholson, J. Pincha, I.
Kansal, R. Windeler, E. Monberg, V. Lukonin, A. Hariharan, G. Williams, A. RosalesGarcia, L. Bansal, and D. DiGiovanni; OFS Laboratories,
Somerset, USA
We present results from new
Yb-doped fibres designedwith increased higher-ordermode loss. The fibres havehightransverse
modeinstability threshold, while
simultaneously maintaining
large mode-field diameter,
allowing for high power
operation
withreducedoptical nonlinearities.

Device-independent
quantum key distribution
using entangled atoms∙T. van Leent1,2 , W. Zhang1,2 ,R. Garthoff1,2 , K. Redeker1,2 ,F. Fertig1,2 , Y. Zhou1,2 , P.
Malik1,2 , R. Schwonnek3,4 , S.
Eppelt1,2 , W. Rosenfeld1,2 , V.
Scarani5,6 , C.C.-W. Lim4,5 ,andH.
Weinfurter1,2,7 ;1
Fakultät für Physik, LMU
Munich, Germany; 2 Munich
Center for Quantum ScienceandTechnology(MCQST), Munich, Germany;3
Naturwiss.-Techn. Fakultät,
Universität Siegen, Germany;
4
Department of Electrical& Computer Engineering,
National University of Singapore, Singapore; 5 Centre forQuantum Technologies, National University of Singapore,
Singapore; 6 Department of
Physics, National University ofSingapore, Singepore; 7 MPQ,
Garching, Germany
Here we present a deviceindependent quantum key
distribution system that enables for secure key exchange
between two users 400 m
apart based on event-readyentanglement of single-atom
quantum memories.

CE-4.2 TUE

16:15

Deterministic Fabrication of
Fluorescent Nanostructures
Exhibiting Magnetic dipolar
Transitions∙M. Rikers1,2,5 , A. Bashiri1,2 ,A. Barreda1,2 , M. Steinert2 ,D.-Y. Choi5 , T. Pertsch2,3,4 ,and I. Staude1,2,4 ; 1 Institute ofSolid-State Physics, Friedrich
Schiller University Jena, Jena,
Germany; 2 Institute of Applied

EB-5.2 TUE

16:00

16:15

Combining quantum cryptographic primitives withhighly-efficient cold-atombased quantum memory∙H. Mamann1 , T. Nieddu1 ,M. Bozzio2 , F. Hoffet3 , F.
Garreau de Loubresse1 , E.
Diamanti4 , A. Urvoy1 , and J.
93

NOTES

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Room 1 ICM

Room 4a ICM

Room 4b ICM

VILNIUS, Lithuania
In this work, we present research on crystalline microprocessing by using femtosecond radiation-induced SLE.
We provide a comparison between various processing protocols and demonstrate structure formation out of crystalline material.

the position of the wateredge moving along thesection of microcapillary
fibre containing a 2 mm long
SNAP (surface nanoscale
axial photonics) microresonator by monitoring the
microresonator spectrum.

We present a combined
quantum ghost and scanning
imaging protocol allowing
2D imaging with 1D detector
array, enabled by strong
spatialcorrelations
andtunable emission angle ofentangled photon pairs emitted from ultrathin nonlinear
metasurfaces.

EG-5.3 TUE

CM-6.3 TUE

16:30

Integrated glass chips for
XUV radiation generationand manipulation∙R.
MartínezVázquez1 ,A.G. Ciriolo1 , G. Crippa1,2 ,M. Devetta1 , D. Faccialà1 ,P. Barbato1,2 , S. Vovla1,2 ,K.A.A.M. Abedin2 , V. Tosa3 ,L. Poletto4 , C. Vozzi1 , R.
Osellame1 , and S. Stagira2 ;1
National Research Council(CNR), Institute for Photonics
and Nanotechnologies, Milan,
Italy; 2 Politecnico di Milano,
Physics Department, Milan,
3
Italy;
National Institutefor R&D of Isotopic andMolecular Technologies, ClujNapoca, Romania; 4 National
Research Council (CNR),
Institute for Photonics andNanotechnologies,
Padova,Italy
We present an integrated glass
platform fabricated by FLICE,
composed of a HHG-chip anda filter for generated XUVradiation. Following hollow
core waveguide concept, we
obtain high photon fluxes andbandwidth non-limited XUVfiltering.

CK-3.3 TUE

16:30

Active Clad Microring Laserwith Diffraction Grating for
Mutual Coupling of Radial
Direction Mode and WGM∙J. Chen1 , A. Nasir1 , A.
Abazi2,3 , A. Eich2,3 , Y.
Tomishige1 , H. Takeda1 , Y.
Mikami1 , N. Tate1 , Y. Oki1 , C.
Schuck2,3 , and H. Yoshioka1 ;1
Kyushu University, Fukuoka,
Japan; 2 University of Münster,
Münster,
Germany;
3
Center for Soft Nano Science,
Münster, Germany
We fabricated active clad microring lasers with a diffraction grating and did the optical characterization. WGM
and radial mode coexist, andthe radial mode can be modulated by adjusting the grating
depth and period.

⋅ Tuesday 27 June 2023

Room 13a ICM

Room 13b ICM

Room 14a ICM

and Optoelectronics, Warsaw,
Poland; 2 LightHoouse Sp. zo.o., Lublin, Poland; 3 VIGO
Photonics S.A., Ożarów Mazowiecki, Poland; 4 Eindhoven
University of Technology,
Eindhoven, Netherlands
We present an InP-based integrated ring laser using AWG
and AMZIs as wavelength filters, with the linewidth of 307
kHz. The laser design is optimized for application in ringlaser gyroscope system.

Centre,UniversityofSouthampton, Southampton,
United Kingdom; 2 Wuhan
National
Laboratory
for
Optoelectronics,
Huazhong
University of Science andTechnology, Wuhan, China;
3
COMSET, Department ofMaterials Science and Engineering, Clemson University,
Clemson, USA
Broadband MIR wavelength
conversion via four-wave
mixing is demonstrated usingadispersion-engineered
tapered silicon core fibre. A
bandwidth of 690nm withamaximum
conversion
efficiency of -23dB is achieved
when pumped at 2.0um.

CB-5.3 TUE

CD-6.3 TUE

16:30

Spontaneous ParametricDown-Conversion in Transition Metal Dichalcogenides
M.A.
Weissflog1 ,∙A.
Fedotova1,2 , Y. Tang3 , B.
1
1
Laudert , F. Abtahi , S.
Shradha1,4 , S. Shinde1 , S.
Saravi1 , I. Staude1,2 , T.
Pertsch1,5 , F. Setzpfandt1,5 ,Y. Lu3 , and F. Eilenberger1,5 ;1Institute of Applied Physics,
Abbe Center of Photonics,
University Jena, Germany;
2
Institute of Solid State
Physics,
University Jena,
Germany; 3 School of Engineering, College of Science
and Computer Science, The
Australian National University, Canberra, Australia;
4
Institute for Condensed
Matter Physics, Technical
University of Darmstadt, Germany; 5 Fraunhofer-Institutefor Applied Optics and Precision Engineering IOF, Jena,
Germany
In this work we experimentally demonstrate spontaneous
parametricdownconversion in transition
metal
dichalchogenides.
Using 3R-MoS2 stacks withthickness 278 nm excited
at 788 nm wavelength we
generate photon-pairs in thetelecom range.

CA-5.2 TUE

16:30

High-power cavity-enhanced diamond Brillouinlaser: a theoretical andexperimental study∙D. Jin1,2 , Y. Wang1,2 , Z. Lu1,2 ,R. P. Mildren3 , and Z. Bai1,2,3 ;1Center for Advanced Laser
Technology, Hebei Universityof Technology, Tianjin, China;
2
Hebei Key Laboratory of Advanced Laser Technology andEquipment, Tianjin, China;
3
MQ Photonics Research Centre, Department of Physics andAstronomy, Macquarie University, NSW, Australia
This paper experimentally andtheoretically investigated thecontinuous-wave resonantly
pumped Brillouin lasers. The
experimental results of thering cavity diamond Brillouinlaser show the first Stokes
output consistent with thetheoretical predictions.

94

16:30

High-speed Direct
Modulation on III-V-on-SOI
Distributed Feedback lasers
with intrinsic electro-optical
bandwidth over 20 GHz∙A. Souleiman1,2 , D. Néel2 ,N. Vaissiere2 , V. Ramez3 , C.
Besancon2 , S. Malhouitre3 , K.
Merghem1 , J. Decobert2 , K.
Hassan3 , D. Bitauld2 , B.-e.
Benkelfat1 , and J.M. Ramirez2 ;1
SAMOVAR, Télécom SudParis, Institut Polytechniquede Paris, Palaiseau, France;
2
III-V Lab, Palaiseau, France;
3
Univ. Grenoble Alpes, CEA,
LETI, Grenoble, France
We present a high-speed IIIV-on-SOI DFB lasers withbackside Bragg gratings. The
laser has achieved an intrinsic
3 dB modulation bandwidthof 21 GHz in the C-band, allowing for direct modulation
at a high speed of 32 Gb/s.

16:30

Pump tuning of a microresonator mid-infrared χ (2)OPO and microcomb
generation at 3.1 μm with
CdSiP2
N. Amiune1 , K. Zawilski2 , P.
Schunemann2 , A. Kordts3 , R.
Holzwarth3 , K. Buse1,4 , and∙I. Breunig1,4 ; 1 Laboratory for
Optical Systems, Departmentof Microsystems Engineering- IMTEK, University ofFreiburg, Germany; 2 BAE
Systems, Inc., Nashua, NH,
USA; 3 Menlo Systems GmbH,
Martinsried,
Germany;4
Fraunhofer Institute for Physical Measurement Techniques,
Freiburg, Germany
With a CdSiP2 microresonator, we demonstrate laser
light tunable from 2.3 to
4.1 μm wavelength pumped
by a compact telecom diodelaser. The same device generates a MIR frequency comb
when operated at degeneracy.

Room 14b ICM

CH-4.2 TUE

16:30

Two-Photon Dual-Comb
LiDAR for Multi-Target
Ranging∙H. Wright1 , A.J.M. Nelson1 ,N.J. Weston2 , and D.T. Reid1 ;1
Heriot-Watt
University,
Edinburgh, United Kingdom;
2
Renishaw Plc, Edinburgh,
United Kingdom
We demonstrate two-photon
dual-comb LiDAR achieving
simultaneous dynamic ranging to three moving targets
driven by sinusoidal, triangular and square waveforms at
0.1 Hz frequency. For stationary targets, we show averaging
to sub-μm precisions in 500
ms.

CLEO

Room Osterseen ICM

Room 1 Hall B1 (B11)®

/Europe-EQEC 2023

Room 2 Hall B1 (B12)⋅ Tuesday 27 June 2023

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Laurat1 ; 1 Laboratoire Kastler
Brossel, Sorbonne Université,
CNRS, ENS-PSL, Collège
de France, Paris, France;
2
Faculty of Physics, Universityof Vienna, VCQ, Vienna,
Austria; 3 ICFO - Institut
de Ciencies Fotoniques, The
Barcelona Institute of Scienceand Technology, Barcelona,
Spain; 4 LIP6, CNRS, Sorbonne
Université, Paris, France
We experimentally performed
a quantum cryptographic
protocol, taking advantage ofour high-efficiency and highfidelity quantum memory
based on cold atoms.

Physics, Abbe Center of Photonics, Friedrich Schiller University Jena, Jena, Germany;
3
Fraunhofer-Institute of Applied Optics and Precision Engineering IOF, Jena, Germany;
4
Max Planck School of Photonics, Jena, Germany; 5 Research
School of Physics, Australia
National University, Canberra,
Australia
Here we present a new twostep electron beam lithography method for the deterministic localization of fluorescentemitters, featuring magnetic
dipolar transition. This is a
critical step in experimentally
studying light-matter interaction on the nanoscale.
JSVI-2.2 TUE

16:30

Plasmon Thermal
Conductance and Thermal
Conductivity of Metallic
Nanofilms∙J. Ordonez-Miranda1 , Y.
Kosevich2 , B.J. Lee3 , M.
Nomura4 , and S. Volz5 ;1
CNRS, The University ofTokyo, Tokyo, Japan; 2 Instituteof Industrial Science, The University of Tokyo, Tokyo, Japan;
3
Department of MechanicalEngineering,Korea Advanced
Institute of Science andTechnology, Daejeon, South
Korea; 4 Institute of Industrial
Science, The University ofTokyo, Tokyo, Japan; 5 CNRS,The University of Tokyo,
Tokyo, JapanThe thermal conductanceand thermal conductivity ofsurface plasmon-polaritons
propagating along a metallic
nanofilm deposited on asubstrate are quantified andanalyzed, as functions of thefilm thickness, length, andtemperature.

CF-5.2 TUE

Room 8 Hall A1 (A12)

16:30

CE-4.3 TUE (Invited) 16:30

CJ-1.2 TUE

Direct CEP Stabilization of ahigh-repetition rate,
few-cycle OPCPA chain witha single feedback loop,
employing a Stereo-ATI∙D. Hoff1,2 , S. Mikaelsson1 ,C. Guo1 , A. L’Huillier1 , C.L.
Arnold1 , and M. Gisselbrecht1 ;1
Department of Physics, Lund
University, Lund, Sweden;
2
Single Cycle InstrumentsUG(hb) & Co. KG, Jena, Germany
We present the direct stabilization of the CEP of a
few-cycle, high-repetition rate
OPCPA laser by employing
a Stereo-ATI pulsemeter for
single-shot detection of the
CEP at full OPCPA repetition
rate and feedback to the oscillator.

Vibrations and Photophysics
in White Light Emitting
Two-Dimensional Metal
Halide Perovskites∙R. Krahne1 , B. Dhanabalan1 ,B. Martin-Garcia2 , D. Spirito3 ,S. Artyukhin1 , M.-L. Lin4 ,Y.-C. Leng4 , P.-H. Tan4 , S.
Kutkan1 , and M. Arciniegas1 ;1
Italian Institute of Technology, Genoa, Italy; 2 CIC
nanoGUNE, San Sebastian,Spain; 3 IHP–Leibniz-Institut
für innovative Mikroelektronik, Frankfurt (Oder),Germany; 4 State Key Laboratory of Superlattices andMicrostructures, IOS, Chinese
Academy of Sciences, Beijing,
China
The symmetries of thephonons in low-dimensional
perovskites are investigatedby angle-resolved Raman
spectroscopy and correlatedwith structural and opticalproperties. This elucidates
the relation of lattice distortions to phonons andelectron-phonon coupling.

Power Scaling Limits ofDiffraction-limited Fibre
Amplifiers Considering
Transverse Mode Instability∙L. Dong, J. Ballato, and J. Kolis; Clemson University, Clemson, USA
An empirical TMI thresholdformula is used to analyse thepower-scaling of ytterbiumdoped fibre amplifiers. This
work serves as a useful extension to earlier works andshines new light on optimal fibre and amplifier designs.

95

16:30

EB-5.3 TUE

16:30

Daylight quantum key
distribution in a free-spacechannel using entangled
photons emitted by aquantum dot device
F. Basso Basset1 , M. Valeri1 ,J. Neuwirth1 , E. Polino1 , M.
Rota1 , D. Poderini1 , C. Pardo1 ,∙G. Rodari1 , E. Roccia1 , S.
Covre da Silva2 , G. Ronco1 ,N. Spagnolo1 , A. Rastelli2 , G.
Carvacho1 , F. Sciarrino1 , and
R. Trotta1 ; 1 Department of
Physics, Sapienza University ofRome, Rome, Italy; 2 Instituteof Semiconductor and Solid
State Physics, Johannes Kepler
University, Linz, Austria
In this word, we implemented
an entanglement-based quantum key distribution across anurban 270m-long free-space
optical link during daylight.
This task has been accomplished for the first time using
a quantum dot device.

NOTES

CLEO

Room 1 ICM
CM-6.4 TUE

16:45

Room 4a ICM
CK-3.4 TUE

16:45

®

/Europe-EQEC 2023

Room 4b ICM
EG-5.4 TUE

16:45⋅ Tuesday 27 June 2023

Room 13a ICM
CA-5.3 TUE

16:45

Room 13b ICM
CB-5.4 TUE

16:45

Room 14a ICM
CD-6.4 TUE

16:45

Room 14b ICM
CH-4.3 TUE

16:45

Micromachining of transparent solids with few-cycle
laser pulses∙J.R. C. Andrade1 ,P.
Sneftrup2 , V. de Michele3 ,L. Rammelt1 , P. Jürgens1 ,M. Vrakking1 , T. Nagy1 ,and A. Mermillod-Blondin1 ;1
Max-Born-Institut, Berlin,
2
Germany;
Departmentof Physics and Astronomy,
Aarhus University, Aarhus,
3
Denmark;
Univ-Lyon,
Laboratoire Hubert Curien(LabHC),Saint-Etienne,
FranceWe present type I modifications in fused silica using 1.5
cycle laser pulses (3.6 fs, center wavelength 710 nm) andcompare them to those induced by typical Ti:Sapphire
50 fs pulses.

Improving the accuracy ofelectron spectroscopy using
calibration with a photonic
integrated circuit-based
microresonator∙B. Weaver1 , A. Sapozhnik1 ,P. Cattaneo1,2 , A. Raja1,3 ,Y. Yang1,3 , R. Wang1,3 , F.
Carbone1 , T. Kippenberg1,3 ,and T. LaGrange1 ; 1 Swiss
Federal Institute of Technology
Lausanne (EPFL), Lausanne,
Switzerland; 2 Dipartimento
di Fisica, Politecnico di
Milano, Milano, Italy; 3 Centerfor Quantum Science andEngineering,
Lausanne,
Switzerland
We present a new methodforcalibrating
electronenergy loss spectrometers
using a photonic integrated
circuit-based microresonator.
The technique’s precision isbetter than previous methods, enabling ultraprecise
spectroscopy of chemical
shifts.

Direct Observation of theOrigin of Spectral Diffusion
in Colloidal Quantum Dots
∙R. Tenne, F. Conradt, V. Bezold, V. Wiechert, and A.
Leitenstorfer; Department of
Physics and Center for Applied
Photonics, University of Konstanz, Konstanz, Germany
Although spectral fluctuations
pose severe limitations on theusability of quantum emitters,
their cause is not entirely clear.
We present a direct observation that spectral diffusion in
colloidal quantum dots resultsfrom stochastic electric-fields

Diode-assisted, continuouswave, nitrogen-vacancy
centre diamond laser system∙L. Lindner1 , F. Hahl1 , T. Luo1 ,G.N. Antonio1 , X. Vidal1 ,M. Rattunde1 , T. Ohshima2 ,M. Capelli3 , B.C. Gibson4 ,A.D. Greentree4 , R. Quay1 ,and J. Jeske1 ; 1 Fraunhofer
Institute for Applied Solid
State Physics IAF, Freiburg,
Germany; 2 National Institutes
for Quantum Science andTechnology (QST), Takasaki,
Japan; 3 School of Science,
RMIT University, Melbourne,
Australia; 4 ARC Centre of
Excellence for Nanoscale BioPhotonics, School of Science,
RMIT University, Melbourne,
Australia
We present a diode-assisted
continuous-wave
laser
system based on nitrogenvacancy centres in diamondfor high-sensitivity laser
threshold magnetometry. The
linear cavity comprising anantireflective coated red laser
diode and an NV-diamondshows lasing behaviour.

Frequency Agile Hybrid
Si3 N4 -MEMS Photonic
Integrated Circuit Based
Laser
∙A.
Voloshin1,2,3 ,A.
Bancora1,2,3 , G. Lihachev2,3 ,V. Snigirev2,3 , H. Tian4 ,J.
Riemensberger2,3 ,V.
Shadymov2,3 , A. Siddharth2,3 ,A.
Attanasio4 ,R.N.
Wang2,3 , S. Bhave4 , andT. Kippenberg2,3 ; 1 DeepLight
SA, Lausanne, Switzerland;
2Institute of Physics, Swiss
Federal Institute of Technology
Lausanne (EPFL), Lausanne,
3
Switzerland;Center of
Quantum Science and Engineering (EPFL), Lausanne,
4
Switzerland;
OxideMEMS
Lab, Purdue University, West
Lafayette, USA
We demonstrate double-ringVernier laser with fast linear
frequency tuning of 2.5 GHz
at 100 kHz and wavelengthswitching with 7 ns rise timeusing silicon nitride photonic
chip with monolithically integrated PZT actuator.

Mid-IR All-Optical Polingin Silicon Nitride Waveguides∙O. Yakar1 , C. Lafforgue1 , A.
Ayan1 , J. Faugier-Tovar2 , P.
Chausse3 , C. Petit-Etienne3 ,E. Pargon3 , Q. Wilmart2 , andC.-S. Brès1 ; 1 Ecole Polytechnique Fédérale de Lausanne,
Photonic Systems Laboratory(PHOSL), STI-IEL, Station
11, Lausanne, Switzerland;2
Univ. Grenoble Alpes, CEA,
LETI, Grenoble,
France;33Grenoble Alpes, CNRS,
CEA/LETI-Minatec, Grenoble
INP, LTM, Grenoble, France
We report the inscriptionofquasi-phase-matchinggratings for second harmonic
generation through all-opticalpoling in the mid-infrared
wavelengths
enabledbysilicon-rich silicon nitride
waveguides that was notpossible by stoichiometricsilicon nitride waveguides.

Noninvasive quantitative
assessment of collagendegradation in parchmentsby polarization-resolved
SHG microscopy∙G. Galante1,2 , M. Schmeltz1 ,S. Heu-Thao2 , L. Robinet2 ,M.-C. Schanne-Klein1 , and
G. Latour1,3 ; 1 Laboratoired’Optique et Biosciences,
CNRS, Inserm, Ecole Polytechnique, Institut Polytechniquede Paris, Palaiseau, France;
2
Centre de Recherche sur laConservation, CNRS, MNHN,
Ministère de la Culture,
Paris, France; 3 Université
Paris-Saclay, Gif-sur-Yvette,
FrancePolarization-resolved second
harmonic generation (P-SHG)
is a modality to extract quantitative information about theorganization of fibrillar collagen. P-SHG is used to characterize the degradation of collagen within historical parchment.

CM-6.5 TUE

CK-3.5 TUE

17:00

EG-5.5 TUE (Invited) 17:00

CA-5.4 TUE

CB-5.5 TUE

CD-6.5 TUE

CH-4.4 TUE

Near-ultraviolet high-Q
whispering-gallery-modes
microresonators for laser
frequency stabilization
G. Perin, Y. Dumeige, P. Féron,and ∙S. Trebaol; Univ Rennes,
CNRS, Institut FOTON - UMR
6082, Lannion, France
We report a study on high-Q
whispering gallery mode microsphere at 420 nm. Q factor up to 10^8 is reported.
Pound-Drever-Hall stabilization of a diode laser on awhispering gallery mode isdemonstrated.

Deep Ultraviolet Nanophotonics to enhance the sensitivity of autofluorescence
spectroscopy on label-freeproteins∙P. Roy, J.B. Claude, and J.
Wenger; Aix Marseille Univ,
CNRS, Centrale Marseille, Institut Fresnel, AMUTech, Marseille, France
We developed a new label-freemethod for detecting single
proteins in DUV range using
optical horn antenna, improving signal and allowing detection of single tryptophan level,
opening up study of a wide
range of proteins.

Proof-of-principle demonstration of a diamond
Raman amplifier at >1.5μm∙P. Julien1 , V. Savitski2 ,Ł.
Dziechciarczyk1 ,G.
Demetriou1 , and A. Kemp1 ;1
University of Strathclyde,
Glasgow, United Kingdom;
2
Fraunhofer
CentreforApplied Photonics, Glasgow,
United Kingdom
We report a maximum amplification factor of 1.4 from anovel diamond master oscillating power amplifier at theeye-safe range and the current
progress towards the optimisation of this setup.

17:00

Femtosecond Bessel Beams
for the efficient generationof volume diffraction gratings in glass∙J. Fantova1,2 , A. Rodriguez1,2 ,G. Garcia-Mandayo1,2 , and
1
S.M. Olaizola1,2 ;CEITBasqueResearchandTechnology Alliance (BRTA),
San
Sebastian,Spain;
2
Universidad de Navarra,
Tecnun, San Sebastian, Spain
Using femtosecond Bessel
Beams, volume diffraction
gratings
were
generatedwithin three different glass
substrates of high refractive
index change, yielding opticalelements of up to 70% combined first order diffraction
efficiency.

96

17:00

17:00

Low loss InP U-bend gain
waveguides for hybrid integration with silicon photonics∙H. Tuorila1 , J. Viheriälä1 , J.W. Lee2 , M. Harjanne2 , M.
Cherchi2 , T. Aalto2 , and M.
Guina1 ; 1 Tampere University,
Tampere, Finland; 2 VTT Technical Research Centre of Finland, Espoo, Finland
We present a low loss U-bend
InP travelling wave semiconductor optical amplifier designed for improved controlof the high precision alignment required for hybrid integration with silicon photonics platforms. Analysis on Ubend structure and the hybrid
integration are presented.

17:00

Coherently driven active
resonator frequency combs
in the mid-infrared∙D. Kazakov1 , T. Letsou1,2 ,M. Piccardo1,3 , M. Beiser4 , L.
Columbo5,6 , M. Brambilla7 ,F. Prati8 , L. Lugiato8 , M.
Pushkarsky9 ,D. Caffey9 ,T. Day9 , B. Schwarz1,4 ,and F. Capasso1 ; 1 Harvard
University, Cambridge, USA;2
Massachusetts
Instituteof Technology, Cambridge,
USA; 3 Fondazione Istituto
Italiano di Tecnologia, Milan,
Italy; 4 TU Vienna, Vienna,
Austria; 5 Politecnico di Torino,
Turin, Italy; 6 CNR-Istituto di
Fotonica e Nanotecnologie,
Bari, Italy; 7 Universit‘a e
Politecnico di Bari, Bari, Italy;

17:00

QCL-based FMCW ranging
and free-space opticalcommunication in the midinfrared∙B. Martin1,2 , P. Feneyrou3 ,E. Rodriguez2 , T. Bonazzi2 ,D. Gacemi2 , N. Berthou1 ,A. Martin3 , and C. Sirtori2 ;1Thales SIX France, Gennevilliers, France; 2 Laboratoirede Physique de l Ecolenormale Superieure, Paris,
France; 3 Thales research andtechnology, Palaiseau, France
We demonstrate the first
results of QCL-based FMCW
ranging in the mid-infrared.
Thanks to state-of-the-art
quantum devices, we performed
preciseoutdoorranging up to 30 m, andCLEO

Room Osterseen ICM

Room 1 Hall B1 (B11)

JSVI-2.3 TUE

CF-5.3 TUE

16:45

Spectral coherence properties of continuum generation in bulk crystals under
spatial phase fluctuations∙B. Maingot1,2 , G. Chériaux1 ,N. Forget2 , and A. Jullien1 ;1
Institut Physique de Nice, Valbonne, France; 2 Fastlite, Antibes, France
The stability of the phase difference between two whitelight continua, generated fromthe same 180-fs pulses at 1035
nm, is assessed by a modified Bellini-Hänsch interferometer. The impact of spatial
phase fluctuations on spectralphase is quantified.

JSVI-2.4 TUE

CF-5.4 TUE

17:00/Europe-EQEC 2023

Room 2 Hall B1 (B12)⋅ Tuesday 27 June 2023

Room 6 Hall B3 (B32)

16:45

Ab initio calculations of thethermoelectric phonon drageffect in semiconductor
nanostructures
R. Sen, N. Vast, and ∙J. Sjakste; Laboratoire des Solides
Irradiés, CEA-DRF-IRAMIS,
École Polytechnique, CNRSUMR 7642, Institut Polytechnique de Paris, Palaiseau,
FranceIn order to understand thephonon drag effect at thenanoscale, we have studied,using density functional theory and the linearized Boltzmann Transport Equation, theeffect of direction-dependentnano-structuring on the Seebeck coefficient of silicon.

Advances in Photothermal
Science and Techniques: aroute for NDT from Macro
to Nanoscale∙R. Li Voti, G. Leahu, E.
Petronijevic, M.C. Larciprete,
A. Belardini, M. Centini, and
C. Sibilia; Sapienza Univesità
di Roma, Department of Basicand Applied Science for Engineering, Rome, Italy
Recent advances for nondestructive evaluation andtesting of chiral materials,
ordered/disordered
nanowires/spheres by photothermal techniques are
summarized. IR radiometry
is introduced to measure
the thermal property at a
nanoscopic scale

®

17:00

Carrier-Envelope Offset
Frequency Characterizationof a 100 MW-Level ThinDisk Oscillator∙Y. Kopp, S. Goncharov, G.
Hehl, and O. Pronin; Helmut
Schmidt University, Hamburg,
Germany
The detection and characterization of the carrier-envelope
offset frequency of a 100 MWlevel Kerr-lens mode-locked
thin-disk oscillator is presented. The carrier-envelope
phase stabilization of thisoscillator is on the way.

CE-4.4 TUE

17:00

Ce:LYSO, from scintillator
to solid-state lighting as a
blue luminescent concentrator
L. Lopez1 , P. Pichon1 , P.
Loiseau2 , B. Viana2 , R.
Mahiou3 , F. Druon1 , P.
Georges1 , and ∙L. Lopez1 ;1Université
Paris-Saclay,
Institut d’Optique Graduate
School, Centre National dela Recherche Scientifique,
Laboratoire Charles Fabry,
Palaiseau, France; 2 Université
PSL,
ChimieParisTech,
CNRS, Institut de Recherchede Chimie Paris, Paris,
France; 3 Université Clermont
Auvergne,
CNRS,
Clermont Auvergne INP, ICCF,
Clermont-Ferrand, France

CG-2.2 TUE

17:00

Light-Driven Attosecond
Photoinjection in Germanium∙G. Inzani1 , L. Adamska2 , A.
Eskandari-asl3 , N. Di Palo1 ,G.L. Dolso1 , B. Moio1 , L.J.
D’Onofrio2 , A. Lamperti4 , A.
Molle4 , R. Borrego-Varillas5 ,M. Nisoli1,5 , S. Pittalis2 , C.A.
Rozzi2 , A. Avella3,6,7 , and M.
Lucchini1,5 ; 1 Department of
Physics, Politecnico di Milano,
Milano, Italy; 2 CNR - Istituto
Nanoscienze, Modena, Italy;
3
Dipartimento di Fisica ”E.
R. Caianiello”, Università degliStudi di Salerno, Fisciano (SA),
Italy; 4 CNR - IMM, Unit ofAgrate Brianza, Agrate Brianza (MB), Italy; 5 Institute for
Photonics and Nanotechnolo97

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)CJ-1.3 TUE

EB-5.4 TUE

16:45

16:45

Polarization Dependence ofTransverse mode Instability
in Yb-doped LMA PM
Fibers∙G.
Palma-Vega1,2 ,D.
Häßner1 , S. Kuhn1 , J. Nold1 ,F. Möller1 , C. Jáuregui2 ,A.
Tünnermann1,2 ,N.
Haarlammert1 ,andT.
Schreiber1 ; 1 Fraunhofer Institute for Applied Optics andPrecision Engineering, Jena,
Germany; 2 Institute of Applied
Physics,
Friedrich-Schiller
University, Jena, Germany
We investigate the dependence of transverse mode
instabilities on the linear
input polarization angle in a
PM fiber amplifier. A mitigation strategy by detuning
the polarization angle fromthe slow-axis of the fiber ispresented.

A continuous-variable
quantum secure directcommunication protocol
with squeezed states∙I. Paparelle1 , F. Mousavi2,3 ,F. Scazza2,3 , M. Paris4 , A.
Bassi2 , and A. Zavatta5 ;1
Ecole Normale Supérieure, Paris, France; 2 Universitàdegli Studi di Trieste, Trieste,
Italy; 3 Istituto Nazionale di
Ottica, Consiglio Nazionaledelle Ricerche, Trieste, Italy;
4
Università degli Studi diMilano, Milano, Italy; 5 Istituto
Nazionale di Ottica, Consiglio
Nazionale delle Ricerche,Firenze , ItalyWe
proposeanovel
continuous-variable quantum
secure direct communication
protocol,investigate its
security, implement it via
coherent and squeezed states
through the optical fiber, anddemonstrate the benefits ofsqueezed states for achieving
higher secrecy.

CJ-1.4 TUE

EB-5.5 TUE

17:00

Transverse Mode Instabilities in kW-class Tm-doped
Fiber Amplifier∙F. Möller, T. Lühder, B. Yildiz,
C. Schmittner, T. Walbaum,and T. Schreiber; Fraunhofer
Institute for Applied Optics
and Precision Engineering IOF,
Jena, Germany
We present a monolithic,
beam-combinable Tm fiber
amplifier at 2036 nm with an
output power of >800 W in
a 25/400 μm fiber geometry.
The
pumpwavelengthdependent TMI threshold will
be investigated.

17:00

Single-emitter quantum key
distribution over 175 km
fibre with optimised finite
key rates∙J. Ho1 , C.L. Morrison1 , R.G.
Pousa2 , F. Graffitti1 , Z.X.
Koong1 , P. Barrow1 , N.G.
Stoltz3 , D. Bouwmeester4,5 ,J. Jeffers2 , D.K.L. Oi2 , B.D.
Geradot1 , and A. Fedrizzi1 ;1
Institute of Photonics andQuantum Sciences, HeriotWatt University, Edinburgh,2
United Kingdom;
SUPA
Departement of Physics, University of Strathclyde, Glasgow,
United Kingdom; 3 Materials
Department, University ofCalifornia, Santa Barbara,
USA; 4 Huygens-Kamerlingh
Onnes Laboratory, Leiden

NOTES

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Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

Room 4b ICM⋅ Tuesday 27 June 2023

Room 13a ICM

Room 13b ICM

Room 14a ICM

Room 14b ICM

Universit‘adell’Insubria,
Como, Italy; 9 DRS Daylight
Solutions, San Diego, USA
Passive Kerr resonators enableagile frequency comb generators in the visible and thenear-infrared. We demonstrate coherently driven active
ring resonators with an effective Kerr nonlinearity arisingfrom gain saturation, paving
the way to reconfigurable frequency combs in the midinfrared.

evidence the feasibility ofsimultaneous communication
and ranging.

CD-6.6 TUE

CH-4.5 TUE

8

CM-6.6 TUE

17:15

Femtosecond laser fabrication of gradient refractive
index micro-lenses in chalcogenide glass for applications in visible and infrared
region∙T. Le Phu1 , D. Le Coq2 , and
P. Masselin1 ; 1 Universitédu Littoral Côte d’Opale,
Dunkerque, France; 2 Institut
des Sciences Chimiques deRennes, Rennes, France
We report a direct laser
writing process to fabricate
gradient refractive index
micro-lenses inside chalcogenide glass for both visible
and infrared applications.
The working distance canbe controlled by selecting
writing
parametersandsubstrate thickness.

CK-3.6 TUE

17:15

Extremely narrow, sharppeaked resonances at theedge of the continuum∙I.
Lukosiunas1 ,L.
Grineviciute2 , J. Nikitina1 ,D. Gailevicius1 , and K.
Staliunas1,3,4 ; 1 Vilnius University, Vilnius, Lithuania;
2
Center for Physical Sciences
and Technology,
Vilnius,3
Lithuania;
ICREA, Passeig Llu’ıs Companys 23,
4
Barcelona, Spain;
UPC,
Dep. de Fisica, Rambla Sant
Nebridi, Barcelona, Spain
We report a newly observed
phenomenon, specifically of a
critical narrowing of Fano resonance in a driven potential
well. The resonances obtain
unusual sharp-peak shapes atthe continuum boundary inside dielectric thin films.

CA-5.5 TUE

17:15

Enhanced diamond
Brillouin scattering basedon cascaded Raman conversion∙H. Chen1,2 , Y. Wang1,2 , Z.
Lu1,2 , R.P. Mildren3 , and Z.
Bai1,2,3 ; 1 Center for Advanced
Laser Technology, Hebei University of Technology, Tianjin,
China; 2 Hebei Key Laboratoryof Advanced Laser Technology
and Equipment,
Tianjin,
China; 3 MQ Photonics Research Centre, Departmentof Physics and Astronomy,
Macquarie University, Sydney,
Australia
We report a diamond Raman
Brillouin laser, and realize a
1.2/1.5 μm cascade Raman
Brillouin laser output with
controllable order by controlling its output transmittanceand cavity length98

CB-5.6 TUE

17:15

Design optimization of onchip III-V/SiN quantum
well/dot lasers∙E. Alkhazraji1 , W.W. Chow2 ,F. Grillot3 , J.E. Bowers4,5 ,S. Madaras2 , M. Gehl2 , E.
Skogen2 , and Y. Wan1 ; 1 King
Abdullah University of Scienceand Technology,
Thuwal,2
Saudi
Arabia;SandiaNational Laboratories, Albu3
querque, USA; LTCI, Télécom
Paris, Institut Polytechniquede Paris, Palaiseau, France;
4
Institute for Energy Efficiency, University of California- Santa Barbara, Santa
Barbara, USA; 5 Materials
Department, University ofCalifornia - Santa Barbara,
Santa Barbara, USA
A parametric analysis anddesign-operation
optimization are presented for
integrated III-V quantum welland quantum dot lasers with
SiN microring resonators
to maximize the power andminimize the linewidth,
which is crucial for several
applications.

17:15

11-μJ picosecond-pulsed
hollow-core-fibre-feedback
optical parametric oscillator∙Y. Wu, S. Liang, Q. Fu, F. Poletti, D.J. Richardson, and L.
Xu; Optoelectronics ResearchCentre, Southampton, United
Kingdom
A fibre-laser-pumped hollowcore-fibre-feedback
opticalparametric oscillator operating at 1-MHz repetition-rate
and generating 130-ps-pulsed
signals and idlers at wavelengths of 1600 nm and 2950
nm, with a record overallpulse energy of 11.4 μJ is
presented.

17:15

Full-Field Hyperspectral
Imaging of a Painting in the
Mid-Infrared∙J. Charsley1 , M. Botticelli2 ,V. Risdonne3 , T. Visser2 ,C. Young2 , M. Smith2 , M.
Rutkauskas1 , Y. Altmann1 ,and D. Reid1 ; 1 Heriot-Watt
University, Edinburgh, United2
Kingdom;
University ofGlasgow, Glasgow, United
3
Kingdom; Victoria & AlbertMuseum, London, United
Kingdom
A compact and cost-effective
mid-infrared hyperspectral
imager(700-1400cm-1
bandwidth) capable of fastacquisition and material
identification through stateof-the-art signal processing
strategies is demonstrated ona painted cultural heritage
object for technical art
history.

CLEO

Room Osterseen ICM

JSVI-2.5 TUE

17:15

Temperature Tunable VO2
Perfect Absorber via W
doping∙D. ceneda1 , M.C. Larciprete1 ,M. Centini1 , R. Li Voti1 , D.
Scirè2 , M. Mosca2 , D. Persano
Adorno3 , R. Macaluso2 , T.
Cesca4 , G. Mattei4 , K. Aydin5 ,and C. Sibilia1 ; 1 Departmentof Basic and Applied Sciencesfor Engineering, Sapienza,
Rome, Italy; 2 Departmentof Engineering, Universityof Palermo, Palermo, Italy;
3
DepartmentofPhysics
and Chemistry, Universityof Palermo, Palermo, Italy;
4
DepartmentofPhysics
and Astronomy, Universityof Padova, Padova, Italy;
5
Department of Electricaland Computer Engineering,Northwestern
University,
Evanston, USA
We performed infrared optical characterization of Wdoped VO2 films at increasing W doping percentage, deposited by PLD on sapphire
substrates, obtaining a temperature tunable VO2 perfect absorber reaching a reflectance of 0.02% at room
temperature.

Room 1 Hall B1 (B11)CF-5.5 TUE

17:15

Carrier-envelope phasetuned nonlinear optical
dynamics of single-cycle
pulses generated in hollowcore photonic-crystal fiber∙I. Savitsky1 , E. Stepanov1,2 ,A. Voronin1,2 , A. Lanin1,2 ,and A. Fedotov1,2 ; 1 M. V.
Lomonosov Moscow State
University, Moscow, Russia;
2
Russian Quantum Center,
Moscow, Russia
We demonstrate a source ofhigh peak power single-cycle
near-to-mid-IR phase stablepulses based on soliton
self-compression in an antiresonant hollow-core fiber.
These pulses are shown tobe well suited for ultrafast
light–matterinteractions
analysis.

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/Europe-EQEC 2023

⋅ Tuesday 27 June 2023

Room 2 Hall B1 (B12)

Room 6 Hall B3 (B32)

Understanding the potential
and limitations of the first
Ce:LYSO luminescent concentrator pumped by UV
LEDs thanks to simulations
and experiments. New sourcewith better performance thanthe best blue LEDs on themarket.

gies, IFN - CNR, Milano, Italy;
6
CNR - SPIN, UoS di Salerno,
Fisciano (SA), Italy; 7 Unità
CNISM di Salerno, Universitàdegli Studi di Salerno, Fisciano(SA), Italy
We investigate a novel
ultrafast charge photoinjection regime in undoped
monocrystalline germanium
with attosecond transientreflectivity spectroscopy. We
decouple several physicalphenomena with different
timing within the pump envelope, while intra-band motion
hinders charge injection.

CE-4.5 TUE

CG-2.3 TUE

17:15

Persistent luminescence in
Ce,Cr-doped garnet crystals
T. Delgado1 , D. Rytz2 , L.
Giordano1 , G. Cai1 , M. Allix3 ,E. Veron3 , and ∙B. Viana1 ;1
PSL University,
ChimieParisTech, IRCP-CNRS,, Paris,
France; 2 BREVALOR Sàrl,
1669, Les Sciernes, Switzerland; 3 CNRS, CEMHTI UPR
3079, Univ. Orléans, , Orleans,
FranceCe,Cr-doped GYAGG single
crystalswith
persistentluminescence have been
elaborated. Single crystals canbe useful to better understandthe mechanism.
Volumeeffects have been shown
whereas surface polishingshould be controlled toenhance light extraction

17:15

Ultrafast Transition fromState-Blocking Dynamics toElectron Localization inTransition Metal β-Tungsten
E.W. de Vos, S. Neb, A. Niedermayr, F. Burri, M. Hollm,∙L. Gallmann, and U. Keller;
Department of Physics, ETH
Zürich, Zürich, Switzerland
We describe an ultrafast transition of the electronic response of optically excited
β-Tungsten.
The response
moves from a regime wherestate-filling of the excited carrier population dominates towards localization of carriers
onto the outer d-orbitals

99

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)
University, Leiden, Netherlands; 5 Department of Physics,
University of California, Santa
Barbara, USA
We report on experimental
results for fibre-based quantum key distribution using
frequency-converted single
photons from a quantum dot.
We exploit improved theoretical techniques for finite-key
analysis enabling practical
QKD over metropolitan
distances.

CJ-1.5 TUE

17:15

Mitigation of Transverse
Mode Instability (TMI) withHigh Beam Quality using
Multimode Fiber Amplifiers
C.-W. Chen1 , K. Wisal2 , Y.
Eliezer1 , A.D. Stone1 , and ∙H.
Cao1 ; 1 Department of Applied
Physics, Yale University, New
Haven, USA; 2 Department of
Physics, Yale University, New
Haven, USA
We demonstrate numericallyand theoretically that thetransverse-mode stability ofa high-power fiber amplifieris greatly enhanced by simultaneously exciting manyhigh-order modes, while theamplified light maintains highspatial coherence and beam
quality.

EB-5.6 TUE

17:15

Localizing eavesdroppers
inside a quantum channel
using stimulated Brillouinscattering∙A. Popp1,2,3 , B. Stiller1,2 ,and C. Marquardt1,2,3 ; 1 Max
Planck Institute for the Scienceof Light, Erlangen, Germany;
2
DepartmentofPhysics,
Friedrich-Alexander
Universität Erlangen-Nürnberg,
3Erlangen, Germany; SAOT,
Graduate School in Advanced Optical Technologies,
Erlangen, Germany
We present a novel approach
to localize eavesdroppers inside a quantum channel using distributed Brillouin scattering. Applying BOCDA, we
are able to localize evanescentoutcoupling down to 1% in astandard fiber channel.

NOTES

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⋅ Tuesday 27 June 2023

Hall B0
13:00 – 14:00

CD-P.5 TUE

CD-P.9 TUE

CD-P: CD Poster session

Time-frequency analysis of dark-waves∙L. Vamos1 , C. Hensel1 , I. Tyulnev1 , L. Maidment1 , U.
Elu1 , M. Enders1 , and J. Biegert1,2 ; 1 ICFO - Institut deCiencies Fotoniques, Castelldefels, Spain; 2 ICREA - Institució Catalana de Recerca i Estudis Avançats, Barcelona,
Spain
We demonstrated the depolarization effect in athmospheric pulse propagation by high quality fits onto the induction decay part of field-resolved measurements. The
time-frequency analysis reveals coupling effects amongrotational modes in a 60ps range.

Comparison of Dark Temporal Cavity Solitons inFabry-Pérot and Ring Resonators with Normal
Dispersion∙G.N. Campbell1 , L. Hill2 , P. Del’Haye2,3 , and G.-L.
Oppo1 ; 1 University of Strathclyde, Glasgow, United Kingdom; 2 Max Planck Institute for the Science of Light, Erlangen, Germany; 3 Friedrich Alexander University ErlangenNuremberg, Erlangen, Germany
We characterize dark vectoral temporal cavity solitons
for a Fabry-Pérot resonator with normal dispersion andmake comparison with an equivalent ring resonator system. The Fabry-Pérot offers advantages in the generationof frequency combs.

CD-P.1 TUE

Power-efficient hyperparametric oscillation via
bound states in the continuum∙F. Lei, Z. Ye, K. Twayana, Y. Gao, M. Girardi, Ó.B. Helgason, P. Zhao, and V. Torres-Company ; Department ofMicrotechnology and Nanoscience, Chalmers Universityof Technology, Gothenburg, Sweden
We present a hyperparametric oscillation with record
high power efficiency in an integrated silicon nitride
microring-waveguide system, which is realized by utilizing the concept of bound states in the continuum.
CD-P.2 TUE

Efficient Generation of Vacuum-Ultraviolet Light inan Ultracompact Setup for Applications in Molecular
and Nuclear Spectroscopy∙M. Seitz1 , J. Al-Nuwaider2 , F. Belli3 , L. Silletti1 , V.
Wanie1 , F. Calegari1,4 , and A. Trabattoni1,2 ; 1 Center
for Free-Electron Laser Science, Deutsches ElektronenSynchrotron DESY, Hamburg, Germany; 2 Institute of
Quantum Optics, Hannover, Germany; 3 Heriot-Watt
University, School of Engineering and Physical Sciences,
Edinburgh, United Kingdom; 4 Physics Department, Universität Hamburg, Hamburg, Germany
This contribution presents an innovative and efficientvacuum ultraviolet light source, employing consecutive
nonlinear frequency conversion in nonlinear crystals
and up-conversion in a hollow core fiber via four-wave
mixing.
CD-P.3 TUE

Increasing brightness in multiphoton microscopy
with low-repetition-rate, wavelength-tunable
femtosecond fiber laser∙J. Bogusławski, A. Kwaśny, D. Stachowiak, and G. Soboń;Laser & Fiber Electronics Group, Wrocław University of
Science and Technology, Wrocław, Poland
We show an improved brightness in multiphoton microscopy using a custom-built fiber laser. The laser offers
versatile output parameters, including wavelength (760800nm) and pulse-repetition-rate (1-25MHz) tunability,
at short sub-90 fs duration and high energy (>1nJ).
CD-P.4 TUE

High Energy Burst Pulsed KGW Raman Laser∙A. Tarasov and H. Chu; Laseroptek, Seongnam, SouthKorea
We realized for the first time burst pulse generation in
KGW Raman laser with energy 13 J, 11.6 J and 8.5 J at
the wavelengths 559, 589 and 621 nm correspondingly,
operating at 1 Hz

CD-P.6 TUE

Photonic Generation and Band-selection ofMulti-Carrier Chirped Waveforms through
Stimulated Brillouin Scattering∙R. Dhawan, D. Parida, and A. Choudhary; Ultrafast Optical Communications and High-performance Integrated
Photonics (UFO-CHIP) group, Department of ElectricalEngineering, Indian Institute of Technology (IIT), Delhi,
New Delhi, India
Photonic frequency-multiplication of the RF frequencyof linear frequency modulated waveforms by 4X andmulti-band LFM generation is demonstrated though asimple modulation technique. Selection of individual
bands is also achieved through flexible Brillouin filtering
CD-P.7 TUE

Laser guiding of consecutive meter-scale discharges
in air
P. Walch, L. Arantchouk, B. Mahieu, M. Lozano, Y.B. André, A. Mysyrowicz, and ∙A. Houard; Laboratoired’Optique Appliquée – ENSTA Paris, Ecole Polytechnique,
CNRS, Institut Polytechnique de Paris , Palaiseau, France
We study the evolution of meter-scale long-lived laser
guided electric discharges and the interaction between
consecutive discharges in the perspective of creating aquasi-permanent conductive channel induced by femtosecond laser filamentation.
CD-P.8 TUE

Energy Conversion Efficiency Improvement of a
MgO:PPLN-based Subnanosecond OpticalParametric Generator Using a Supercontinuum Seed
∙J. Banys, S. Armalytė, V. Tamulienė, V. Jarutis, and J.
Vengelis; Laser Research Center, Faculty of Physics, Vilnius University, Vilnius, Lithuania
We propose seeding the MgO:PPLN crystal-based subnanosecond micro-laser pumped optical parametric
generator with supercontinuum generated in a photonic
crystal fiber - an idea that significantly increases the energy conversion efficiency while preserving good output
beam quality.

CD-P.10 TUE

IDFG in GaSe and LGS, we covered a spectral range between 3 and 18 μm.
CD-P.13 TUE

Switchable Ultraviolet Harmonic Beam Manipulation
via Spatial Phase Modulation of Near-infrared
Driving Beam
∙S. Won, S. Choi, T. Kim, B. Kim, S.-W. Kim, and Y.-J.
Kim; Korea Advanced Institute of Science and Technology,
Daejeon, South Korea
We present the polarization-resolved ultraviolet (UV)harmonic beam pattern manipulation via spatial phasemodulation of the driving beam. Our work enables thearbitrary control of UV laser pulses in UV optical hologram and encryption.

Critical coupling in Cavity Resonator Integrated
Grating Filters (CRIGFs) for SHG control
O. Gauthier-Lafaye1 , P. Dubreuil1 , ∙S. Calvez1 , A.
Monmayrant1 , E. Hemsley2 , A.-L. Fehrembach2 , and E.
Popov2 ; 1 LAAS-CNRS, Toulouse, France; 2 Institut Fresnel, Marseille, France
We demonstrate experimentally critical coupling for
nonlinear conversion in grating-coupled Fabry-Pérot
planar microcavities known as Cavity-Resonant Integrated Grating Filters. Novel asymmetric designs offer
Q-factors from 1000 to 8000 and allow critical couplingwith maximised SHG.

CD-P.14 TUE

CD-P.11 TUE

CD-P.15 TUE

Ultrafast third-order nonlinear optical response of
2D NbS2 , NbSe2 , ZrTe2 , and MoS2 LTMDs insuspension∙A.J.A. Carvalho1 , D. Valente1 , C.L.A.V. Campos1 , A.M.
Jawaid 2 , R. Busch2 , R.A. Vaia2 , and A.S.L. Gomes1 ;1Physics Department, Universidade Federal de Pernambuco, 50670-901, Recife, Brazil; 2 Materials and Manufacturing Directorate, Air Force Research Laboratories,
WPAFB, 45433, Recife, USA
We investigated the ultrafast third-order nonlinearity of
2D transition-metal dichalcogenides based on the optical Kerr gate technique and discuss the physical mechanism responsible for the effect. Measured nonlinear coefficients ranged from 8.6 × 10−19 m2 /W to 5.3 ×
10−18 m2 /W.
CD-P.12 TUE

Mid-infrared generation in GaSe and LGS with
few-cycle pulses compressed by cascaded multipass
cells∙J.G. Meyer, S. Goncharov, A. Zablah, and O. Pronin;
Helmut-Schmidt-Universität, Hamburg, Germany
We generated 7 fs pulses at 1 μm wavelength from two
cascaded multipass cells after a Pharos laser. By driving

100

A New Approach to OPCPA Idler Pulse Energy
Build-up at 2.3 μm by Transient Stimulated Raman
Chirped-Pulse Amplification∙A. Petrulėnas, P. Mackonis, and A. Rodin; State research
institute Center for Physical Sciences and Technology , Vilnius, Lithuania
The combination of OPCPA and transient stimulated Raman amplification of chirped pulses in KGW demonstrates a new approach for idler energy buildup in the
SWIR range. After SRA idler energy increase 33% withnearly transform-limited 53 fs pulses after compression.
Parametric Amplification in Dual-Core Fibers Via
Intermodal Four-wave Mixing∙M. Shi1 , V. Ribeiro1,2 , and A.M. Perego1 ; 1 Aston Institute of Photonic Technologies, Aston University, B4 7ET,
Birmingham, United Kingdom; 2 Kets Quantum Security
Ltd. BS15 4PJ, Bristol, United Kingdom
We demonstrate analytically and numerically a novel
dual-core fiber based optical parametric amplifier operating via intermodal four-wave mixing and featuring afrequency asymmetric spectrum with signal and idlers
generated into two different supermodes.
CD-P.16 TUE

Thermal and non-thermal optical nonlinearities of
2D layered transition metal dichalcogenides insuspension∙C.L.A.V. Campos1 , J.E.Q. Bautista1 , C.B. de Araújo1 ,A.M. Jawaid2 , R. Busch2 , R.A. Vaia2 , and A.S.L. Gomes1 ;1Departamento de Física, Universidade Federal de Pernambuco, , 50670-901 , Recife, Brazil; 2 Materials andManufacturing Directorate, Air Force Research Laboratories, WPAFB, 45433, Ohio, USA
We investigate the nonlinear optical response of bidimensional transition-metal dichalcogenide in suspen-

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Hall B0
sion due to intensity-dependent Kerr-type nonlinearityand explained the origin of the slow (thermal) and ultrafast (nonthermal) nonlinearities

frared while suppressing stationary background, and remarkable ability of detection in the visible range.

CD-P.17 TUE

Theory of Parametric Amplification in two Coupled
Waveguides: Frequency-Dependent Coupling andResilience to Pump Fluctuations∙M. Shi1 , V. Ribeiro1,2 , and A.M. Perego1 ; 1 Aston Institute of Photonic Technologies, Aston University, B4 7ET,
Birmingham, United Kingdom; 2 Kets Quantum Security
Ltd. BS15 4PJ, Bristol, United Kingdom
We present a comprehensive theoretical framework fordual waveguides based parametric amplifiers description, highlighting the role of frequency dependent coupling for dispersion engineering and the robustness of
the amplification scheme with respect to pump fluctuations.

Assessment of the Feasibility of Employing Chaos
Synchronization in Two Cascaded Microresonators
for Secure Data Transmission∙D. Lemcke1,2 , D. Moreno1,3 , S. Fujii4 , A. Nakashima1 , A.
Uchida5 , and T. Tanabe1 ; 1 Department of Electronics andElectrical Engineering, Faculty of Science and Technology,
Keio University, Yokohama, Japan; 2 RWTH Aachen University, Aachen, Germany; 3 Polytechnic University of Valencia, Valencia, Spain; 4 Department of Physics, Facultyof Science and Technology, Keio University, Yokohama,Japan; 5 Department of Information and Computer Sciences, Saitama University, Saitama, JapanTo employ chaos synchronization in actual transmission
systems we use differential binary shift keying modulation to analyze the degree of synchronization of two cascaded microresonator frequency combs simulated utilizing the modified Lugiato-Levefer equations.
CD-P.18 TUE

Few-cycle ultra-broadband beam scanningmicroscope prototype∙C. Maibohm1 , H. Sebastião1 , J. Martins1 , M.L. Ribeiro1 ,M. Miranda2 , P.T. Guerreiro2 , R. Romero2 , H. Crespo2,3 ,and J.B. Nieder1 ; 1 INL - International Iberian Nanotechnology Laboratory, Braga, Portugal; 2 Sphere Ultrafast
Photonics, Porto, Portugal; 3 IFIMUP-IN and Dept. ofPhysics and Astronomy, University Porto,, Porto, Portugal
SyncRGB-FLIM beam scanning microscope, where asub-10 fs pulsed laser is maintained at the focus pulse allowing for efficient imaging of various labelled and labelfree markers across the full visible wavelength spectrum.
CD-P.19 TUE

Nonlinear-crystals-based optical transient detection
system with femtosecond pulses∙. Sukeert1 , C.K. Suddapalli2 , P.G. Schunemann3 , G.J.
de Valcárcel4 , M. Ebrahim-Zadeh1,5 , and A. EstebanMartín1,4 ; 1 ICFO—Institut de Ciències Fotòniques,
Castelldefels (Barcelona), Spain; 2 Tata Institute of Fundamental Research Hyderabad, Hyderabad (Telangana),
India; 3 BAE Systems Inc, Nashua (New Hampshire),
USA; 4 Departament d’Òptica i Optometria i Ciències dela Visió, Universitat de València, Burjassot (Valencia),
Spain; 5 Institució Catalana de Recerca i Estudis Avançats(ICREA), Barcelona, Spain
We report a nonlinear-crystals-based up-converted optical transient detection system with femtosecond pulses
for phase measurement of a dynamic signal in the in-

CD-P.20 TUE

CD-P.21 TUE

Resonance-enhanced Third Harmonic Generation in
Mn+-dominated Laser-induced Plasmas∙M. Oujja1 , J.J. Camacho2 , M. Castillejo1 , and R.
de Nalda1 ; 1 Instituto de Quimica Fisica Rocasolano CSIC, Madrid, Spain; 2 Facultad de Ciencias, Universidad
Autónoma, Madrid, Spain
A laser-induced plasma of metallic manganese is diagnosed by optical emission spectroscopy and its properties are correlated with its high nonlinear optical response in a third order harmonic generation experiment.

CD-P.23 TUE

CD-P.27 TUE

MIR Supercontinuum Using Gain-Switched andModelocked Pumping∙C.R. Smith1 , C.R. Petersen1,2 , and O. Bang1,2,3 ; 1 DTU
Electro, Technical University of Denmark, Kgs. Lyngby,
Denmark; 2 NORBLIS ApS, Virum, Denmark; 3 NKT Photonics A/S, Birkerød, Denmark
We obtain a supercontinuum spectrum extending beyond 4μm with RIN below 13% from ZBLAN pumped
by a homebuilt flexible amplified gain-switched 1950nm
diode. These promising results are compared withpumping by a commercial modelocked laser.

Deterministic soliton crystal dual-microcomb
generation in coupled nonlinear microcavities bytuning the coupling coefficient∙Z. Cheng1,2 , D. Huang2,3 , F. Li1,2 , C. Lu1,2 , and P.K.A.
Wai1,2,4 ; 1 Photonics Research Centre, Department ofElectronic and Information Engineering, The Hong Kong
Polytechnic University, Hong Kong, China; 2 The Hong
Kong Polytechnic University Shenzhen Research Institute,Shenzhen, China; 3 Photonics Research Centre, Department of Electrical Engineering, The Hong Kong Polytechnic University, Hong Kong, China; 4 Department of
Physics, Hong Kong Baptist University, Kowloon Tong,
Hong Kong, China
We propose a novel dual-frequency comb generation
scheme in two coupled nonlinear microcavities by tuning the coupling coefficient between the two microcavities. Synchronously tuning of the two pumps is not required for dual-microcomb generation.

CD-P.24 TUE

Optical switches in thin film coatings based on highly
nonlinear materials∙M. Steinecke1 , K. Kiedrowski1 , M. Jupé1,2 , A. Wienke1,2 ,and D. Ristau1,2,3 ; 1 Laser Zentrum Hannover e.V.,
Hanover, Germany; 2 Cluster of Excellence PhoenixD(Photonics, Optics and Engineering - Innovation AcrossDisciplines), Hanover, Germany; 3 Leibniz University
Hannover, Institute of Quantum Optics, Hanover, Germany
A concept for a fast, passive optical switch based on the
optical Kerr-effect in thin film interference coatings ispresented. The materials, manufacturing and successful validation of optical switching is presented and discussed.
CD-P.25 TUE

CD-P.22 TUE

Measuring nonlinearities under high dispersion andloss∙D. Castelló-Lurbe1,2,3 , C. Cuadrado-Laborde4 , E.
Silvestre1,5 , A. Díez1,2 , and M.V. Andrés1,2 ; 1 Institut
Universitari de Ciències dels Materials, Universitat
de València, Catedrático Agustín Escardino 9, 46980
Paterna, Spain; 2 Departament de Física Aplicada i Electromagnetisme, Universitat de València, Dr. Moliner
50, 46100 Burjassot, Spain; 3 Brussels Photonics, Department of Applied Physics and Photonics, Vrije Universiteit
Brussel, Pleinlaan 2, 1050 Brussel, Belgium; 4 Institutode Física Rosario (CONICET-UNR), Blvr. 27 de Febrero210bis, S2000EZP Rosario, Argentina; 5 Departamentd’Òptica i Optometria i Ciències de la Visió, Universitat
de València, Dr. Moliner 50, 46100 Burjassot, Spain
Accuracy limitations on the nonlinear coefficient measurement when dispersion and loss cannot be neglected
are overcome. We demonstrate our approach experimentally propagating pulses along a kilometer-longstandard fiber pumped close to 2 μm.

Conical Odd Harmonic Generation Induced by
Femtosecond Filamentation in LiSAF∙R. Grigutis, V. Jukna, G. Tamošauskas, and A. Dubietis; Laser Research Center, Vilnius University, Vilnius,
Lithuania
We report on conical odd-harmonics generation that
accompany supercontinuum generation in LiSAF using
femtosecond pulses due to filament inscribed nanograting, justified by the measurements of time evolution
and angle-resolved spectra of supercontinuum and oddharmonics emissions.
CD-P.26 TUE

Direct measurement of the two-photon excitation
cross-section of xenon by laser absorption∙C. Drag1 , F. Marmuse2 , and C. Blondel1 ; 1 Laboratoirede Physique des Plasmas, Palaiseau, France; 2 European
Spatial Agency, Noordwijk, Netherlands
The two-photon excitation cross-section is a key parameter for the TALIF method, which is commonly used
to measure atomic densities for plasma diagnostics. We
present a new method for cross-section measurements
applied to Xe.

101

CD-P.28 TUE

Heat-induced variation of second-harmonic
generation in silicon oxynitride thin films∙J. Lukeš1,2 and K. Žídek1 ; 1 Research Center TOPTEC,
Institute of Plasma Physics of the Czech Academy of Sciences, Prague, Czech Republic; 2 Technical University in
Liberec, Faculty of Mechatronics, Informatics and Interdisc. Studies, Liberec, Czech Republic
Efficient optical enhancement of second harmonic generation on thin silicon nitride and silicon oxynitride
films is presented. Thermal-induced changes in mechanical stress are proposed as the main cause, but other effects are also discussed.
CD-P.29 TUE

The efficient intermodal four-wave mixing process ina few-mode fibers∙K. Michal and U.A. Laudyn; Warsaw University of Technology, Faculty of Physics, Warsaw, Poland
The work presents an intermodal four-wave mixing in a
few-mode fiber within the visible wavelength band anda sub-nanosecond regime. A high conversion efficiency(over 40%) was obtained in a stimulated nonlinear process.
CD-P.30 TUE

Spectral broadening in concave-convex multipass
cells in gas and solid medias∙K. Schwarz1 , N. Kovalenko1 , V. Hariton2 , K. Fritsch1,3 ,and O. Pronin1 ; 1 Helmut Schmidt University, Hamburg,
Germany; 2 Instituto Superior Técnico, Lisbon, Portugal;
3n2-Photonics GmbH, Hamburg, Germany
Convex-concave multipass cell operating with 0.2 mJ,
260 fs input pulses is demonstrated with solid-state and

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Hall B0gas media. The pulses are broadened and compressed tosub-60 fs paving the way to high energy foldable convexconcave cells.
CD-P.31 TUE

Linear and Nonlinear Optical Properties of
Aluminum∙M. Scalora1 , M. Belchovski2 , S. Mukhopadhyay3 , K.
Hallman4 , R. Vilaseca3 , C. Cojocaru3 , J. Trull3 , and M.A.
Vincenti2 ; 1 Aviation and Missile Center, US Army CCDC
- 35898-5000, Redstone Arsenal, AL , USA; 2 Department
of Information Engineering – University of Brescia, Via
Branze 38, 25123 , Brescia, Italy; 3 Department of Physics,
Universitat Politècnica de Catalunya, Rambla Sant Nebridi 22, 08222 , Terrassa , Spain; 4 PeopleTec, Inc. 4901-I
Corporate Dr, 35805, Huntsville, AL, USA
We report our theoretical results of second and third harmonic generation from a flat Al layer. Our results suggests that the intrinsic properties of Al may be more pronounced compared to other plasmonic materials.

13:00 – 14:00
CF-P: CF Poster session
CF-P.1 TUE

Simultaneous measurement of sub-femtosecond
timing jitter in two frequency channels by using time
stretched self-coherent detection∙Y. Li1,2 , D. Huang1,2 , F. Li2,3 , and P.K.A. Wai2,3,4 ;1
Photonics Research Institute, Department of Electrical Engineering, The Hong Kong Polytechnic University,
Hong Kong, China; 2 The Hong Kong Polytechnic University Shenzhen Research Institute, Shenzhen, China;
3
Photonics Research Institute, Department of Electronic
and Information Engineering, The Hong Kong Polytechnic
University, Hong Kong, China; 4 Department of Physics,
Hong Kong Baptist University, Hong Kong, China
We demonstrate simultaneous measurement of subfemtosecond timing jitter in two frequency channels bytime stretched self-coherent detection. The phase information of the beating-frequency signal of the chirped
pulses is utilized to determine the timing jitter.
CF-P.2 TUE

Linearity of High-Sensitivity Infrared Electro-Optic
Sampling∙Z. Wei1,2 , C. Hofer1,2,3 , D. Gerz1,2,4 , N. Karpowicz1,2 ,and I. Pupeza1,2,4 ; 1 Ludwig Maximilians University
Munich, Garching, Germany; 2 Max Planck Instituteof Quantum Optics, Garching, Germany; 3 Center for
Molecular Fingerprinting, Molekuláris-Ujjlenyomat Kutató Közhasznú Nonprofit Kft., Budapest, Hungary;

CD-P.32 TUE

Chalcogenide-ring fiber design for Brillouin
Scattering with OAM modes
D. Yadav, K. Aggarwal, ∙A. Choudhary, and V.
Venkataraman; Indian Institute of Technology Delhi,
New Delhi, India
We demonstrate the excitation of strong backward stimulated Brillouin scattering using orbital angular momentum modes in a chalcogenide-ring silica optical fiber design through simulations and discuss the momentum
conservation between the optical and acoustic modes.
CD-P.33 TUE

Image Upconversion System by THG of a
Self-illuminated and Self-synchronized Passively
Q-Switched Laser∙A.J. Torregrosa1 , M.L. Rico2 , and J. Capmany1 ; 1 Dpto.
de Ingeniería de Comunicaciones and I3E, Universidad
Miguel Hernández, Elche, Spain; 2 Dpto. de Tecnología

Leibniz Institute of Photonic Technology - Member ofthe research alliance “Leibniz Health Technologies“, Jena,
Germany
Electro-optic sampling (EOS) holds the records for sensitivity and dynamic range for infrared detection. Here,
we investigate the linearity of EOS and discuss how highgate-pulse energies benefit both sensitivity and linearityof field-sensitive detection.
4

CF-P.3 TUE

Tunable ultrafast mid-IR source intensity noiseproperties
Q. Bournet1,2 , ∙M. Natile2 , F. Guichard2 , Y. Zaouter2 ,M. Jonusas3 , A. Bonvalet 3 , M. Joffre3 , F. Druon 1 ,M. Hanna1 , and P. Georges1 ; 1 Université Paris-Saclay,
Institut d’Optique Graduate School, CNRS, Laboratoire
Charles Fabry, Palaiseau, France; 2 Amplitude, Pessac,
France; 3 Laboratoire d’Optique et Biosciences, Ecole Polytechnique, CNRS, INSERM, Institut Polytechnique deParis, Palaiseau, France
We report on extensive noise characterization of widely
tunable (3.5-10 μm), high repetition rate (100 kHz),
mid-IR few-cycle sources.
CF-P.4 TUE

High-power ultrashort pulse amplification with an
Yb:YScO3 crystal∙N. Torcheboeuf1 , C. Hofer1 , L. Karlen1 , C. Kränkel2 , A.
Uvarova2 , L. Huelshoff2 , M. Gaponenko3 , G. Spühler3 ,B. Eiermann4 , D. Zadravec4 , F. Fink5 , H. Schlich5 , andS. Lecomte1 ; 1 Centre Suisse d’Electronique et de Mi-

Informática y Computación, Universidad de Alicante, Alicante, Spain
We present a self-illuminated and self-synchronizedinfrared-to-visible image upconversion system based on
intracavity third harmonic generation in a passively QSwitched YVO4:Nd3+ laser oscillating at 1342 nm resulting in a 447 nm upconverted image.
CD-P.34 TUE

DC Kerr effect modulators in silicon for cryogenic
mid-infrared applications∙M. Radulovic1,2 , B.D.J. Sayers1,2 , S.G. Currie1,2 , D.A.
Quintero Dominguez1 , and J.W. Silverstone1 ; 1 Big Photon Lab, H. H. Wills Physics Laboratory and Department of Electrical and Electronic Engineering, Universityof Bristol, Bristol, United Kingdom; 2 Quantum Engineering Centre for Doctoral Training, H. H. Wills Physics Laboratory and Department of Electrical and Electronic Engineering, University of Bristol, Bristol, United Kingdom
We iteratively design and implement silicon photonic

crotechnique (CSEM), Neuchâtel, Switzerland; 2 LeibnizInstitut für Kristallzüchtung (IKZ), Berlin, Germany;
3
NKT Photonics Switzerland GmbH, Regensdorf, Switzerland; 4 WZW Optic AG, Balgach, Switzerland; 5 MaTeck
Material Technologie & Kristalle GmbH, Jülich, Germany
A Yb:YScO3 crystal was fabricated and tested as abooster stage in an amplified femtosecond laser. Its
unique properties allowed to reach power levels of 93.5
W for MHz repetition rates with sub-300fs pulse duration.
CF-P.5 TUE

Ultra-compact system to synthesize space-time lightsheets∙M. Yessenov1 , O. Mhibik1 , L. Mach1 , T. Hayward2 , R.
Menon2 , L. Glebov1 , I. Divliansky1 , and A. Abouraddy1 ;1
CREOL, University of Central Florida, Orlando, USA; 2
Department of Electrical and Computer Engineering, University of Utah, Salt Lake City, USA
We introduce an ultra-compact and robust system togenerate space-time wave packets based on chirped volume Bragg gratings to spatially resolve the spectrum,
which reduced the volume of the synthesis setup down
to 25x25x8 mm3.
CF-P.6 TUE

Analysis of wavelength dependent wavefront
deformation in thin plate compressors for energetic
single-cycle laser pulses∙L. Lehotai1 , S. Tóth1 , I. Seres1 , J. Csontos1 , V. Pajer1 ,Á. Börzsönyi1 , K. Osvay2 , and R.S. Nagymihály1 ;1
ELI ALPS, ELI-HU Non-Profit Ltd, Szeged, Hun-

102

modulators based on DC Kerr effect in the 2μm band
and we compare them and consider their performancein the quantum photonics applications.
CD-P.35 TUE

Novel scheme for a broadband SRS microscope withsparse-wavenumber acquisitions based on the
Hadamard transform∙L. Genchi, S.P. Laptenok, and C. Liberale; King Abdullah
University of Science and Technology (KAUST), Thuwal,
Saudi Arabia
We present a novel scheme for multiplexed stimulated
Raman scattering microscopy based on the Hadamardtransform. It uses an acousto-optic tunable filter and isdriven by a femtosecond oscillator and a picosecond optical parametric oscillator.

gary; 2 National Laser-initiated Transmutation Laboratory, University of Szeged, Szeged, Hungary
A novel 3+1D numerical simulation for spatio-temporal
couplings in high energy post-compression systems wasdeveloped and validated with experimental results. Our
method helps to identify and minimize spatio-temporal
distortions to achieve energetic single-cycle laser pulses.
CF-P.7 TUE

Multi-heterodyne Differential Phase Measurement ofMicrocombs∙K. Twayana1 , I. Rebolledo-Salgado1,2 , M. Girardi1 , F.
Lei1 , Ó.B. Helgason1 , M. Karlsson1 , and V. TorresCompany1 ; 1 Chalmers University of Technology, Gothenburg, Sweden; 2 RISE Research Institutes of Sweden, Borås,SwedenWe report differential phase measurement and reconstruction of 100 GHz soliton microcombs assisted byelectro-optic down-conversion using another (uncalibrated) soliton microcomb as an optical reference.
CF-P.8 TUE

Tunable Dual-Wavelength Laser at 1.8 μm Based on
SESAM and NOLM
∙X. Wen1 , T. Qiao1 , M. Zhou1 , H. He1 , Y. Zhou1 , andK.K.-Y. Wong1,2 ; 1 The University of Hong Kong, Department of Electrical and Electronic Engineering, Hong Kong,
China; 2 Advanced Biomedical Instrumentation Centre,
Hong Kong Science Park, Hong Kong, China
A tunable dual-wavelength all-fiber laser at 1.8 μm utilizing SESAM and NOLM was demonstrated for the firsttime. Two typical mode-locked regimes of the dual-

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Hall B0
wavelength signal varying from single-pulse/singlepulse to single-pulse/multi-pulse were observed.
CF-P.9 TUE

Highly sensitive, highly versatile, 100-kHz vis-NIR
ultrafast pump-probe setup based on aninterferometric spectrometer∙A. Villa1 , A. Ross1 , V. Policht1 , O. Dogadov1 , and
F. Scotognella1,2 ; 1 Politecnico di Milano, Milan, Italy;
2
Center for Nano Science and Technology@PoliMi, Istituto Italiano di Tecnologia, Milan, Italy
We present a high sensitivity ultrafast pump-probe setup
running at 100 kHz and achieving shot-to-shot detection
through an interferometric spectrometer. Wide pumptunability and high temporal resolution are reported,along with sensitivities up to 10-5.
CF-P.10 TUE

Stable harmonic modelocked laser operation bydamping the temporal displacement of optical pulses
in analogy to Brownian particles∙M. Laçin1 , P. Repgen1 , A. Şura2 , Ç. Şenel3 , and F.Ö.
İlday1,2,4 ; 1 Department of Physics, Bilkent University,
Ankara, Turkey; 2 Department of Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey;
3TÜBİTAK National Metrology Institute (UME), Kocaeli, Turkey; 4 UNAM-National Nanotechnology Research Center and Institute of Materials Science and Nanotechnology, Bilkent University, Ankara, Turkey
In analogy to the damping of the movement of a Brownian particle through a viscous liquid, we damp the temporal displacement of harmonic modelocked pulses in alaser cavity for superior short-term stability.
CF-P.11 TUE

Temporal Characterization of Ultra-Short Laser
Pulses Using Third-Order Nonlinear Process with
Perturbation∙H. Cao1,2 , P. Huang1 , H. Yuan1,2 , H. Wang1,2 , X.
Wang1,2 , Y. Wang1,2 , W. Zhao1,2 , and Y. Fu1,2 ; 1 Center
for Attosecond Science and Technology, State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of
Optics and Precision Mechanics, Xi’an, China; 2 Universityof Chinese Academy of Sciences, Beijing, China
We propose a simple method to temporal characterize
the few-cycle laser pulses. The method is based on introducing perturbation to the third-order nonlinear processes, including transient grating in solid plates and
THG in air.

CF-P.16 TUE

CF-P.12 TUE

1-MHz mode-locked all-fiber linear-cavity laser
based on two SESAMs at 1.7 μm for multiphoton
microscopy∙T. Qiao1 , M. Zhou1 , X. Wen1 , and K.K.-Y. Wong1,2 ; 1 The
University of Hong Kong, Department of Electrical andElectronic Engineering, Hong Kong, China; 2 Advanced
Biomedical Instrumentation Centre, Hong Kong Science
Park, Hong Kong, China
A 1.7-μm mode-locked all-fiber laser with a repetition
rate of about 1 MHz was demonstrated. It is modelocked by two semiconductor saturable absorber mirrors
and employs a compact linear cavity for the first time.
CF-P.13 TUE

High-speed Time Stretch LIDAR at 780nm with asingle-pixel silicon avalanche photodetector∙C. Stock1 , T.F. Kutscher1 , A. Gruber1 , P. Lamminger1 , C.
Leonhardt1 , F. Sommer1,2 , J. Jurkevicius1 , and S. Karpf1 ;1
Universität zu Lübeck, Lübeck, Germany; 2 LeibnizInstitut für Virologie, Hambrug, Germany
We present an inertia-free, high-speed time-stretch LIDAR system based on a new swept source pulsed laser
at 780nm. This enables detection using a single-pixel
avalanche photodiode. We present 3D scene acquisitionsat 2 kHz rate.
CF-P.14 TUE

Coupled active cavities for all-fiber optical frequency
comb generation∙C. Simon, N. Englebert, F. Leo, and S.-P. Gorza; Université libre de Bruxelles (ULB), Bruxelles, Belgium
We introduce a design of active resonators hosting cavity
solitons, that overcomes the saturation power limitationof the intracavity amplifier. This paves the way to highbrightness fiber frequency comb sources based on active
cavity solitons
CF-P.15 TUE

Nonlinear compression of mJ-level pulses via
double-pass loose focusing in air∙F. Zhang1,2 , A. Pelekanidis1,2 , M. Du1,2 , K. Eikema1,2 ,and S. Witte1,2 ; 1 Advanced Research Center for
Nanolithography (ARCNL), Amsterdam, Netherlands;
2
Department of Physics and Astronomy, Vrije Universiteit, Amsterdam, Netherlands
We report on a novel double-pass-based scheme for nonlinear pulse compression, which overcomes the pulse energy limitation and beam quality degradation, and features extreme simplicity, high compression efficiency,
and average power scaling capabilities.

Broadband Auston-Type Photoconductive Field
Sampling in Gallium Phosphide∙N. Altwaijry1,2 , M. Qasim1,2 , M. Mamaikin1,2 , J.
Schötz1,2 , K. Golyari1,2 , M. Heynck1,2 , E. Ridente1,2 ,V.S. Yakovlev1,2 , N. Karpowicz1,2 , and M.F. Kling1,2,3,4 ;1
Max Planck Institute of Quantum Optics, Garching, Germany; 2 Ludwig-Maximilians-Universität, Garching, Germany; 3 SLAC National Accelerator Laboratory, Menlo
Park, USA; 4 Applied Physics Department, Stanford University, Stanford, USA
We present an Auston-type technique for sampling nearinfrared fields by applying a short visible-UV gate pulse
to a common semiconductor. The gate pulse causes anappreciable change in carrier density (within femtoseconds) permitting field detection.
CF-P.17 TUE

Few Cycle Pulse Compression and White Light
Generation in Cascaded Multipass Cells∙S. Goncharov1 , K. Fritsch2 , and O. Pronin1 ; 1 Helmut
Schmidt University, Holstenhofweg 85, 22043, Hamburg,
Germany; 2 n2-Photonics GmbH, Hans-Henny-JahnnWeg 53, 22085, Hamburg, Germany
We report supercontinuum generation and pulse compression in two cascaded multipass cells based on dielectric mirrors. The 230 fs long-, 12 μJ pulses were compressed to 7 fs, corresponding to 1.0 GW peak power andthroughput of 84%.
CF-P.18 TUE

Characterizing ultrashort laser pulses with atime-dependent polarization state using the d-scan
technique∙D. Díaz Rivas, A.-K. Raab, C. Guo, A. L’Huillier, and C.
Arnold; Department of Physics, Lund University, Lund,
SwedenIn this work, a polarization gate is generated using ultrashort pulses with a duration of 6 femtoseconds and characterized with the dispersion scan technique. The temporal reconstruction confirms the creation of the timedependent polarization state.
CF-P.19 TUE

High Power Ultrafast Pulsed Laser at 2060 nm from a
Stabilized Doubly Resonant Optical Parametric
Oscillator∙H. Rao1,2 , C.M. Dietrich1,2 , J.R.C. Andrade3 ,R. Mevert1,2 , F.J. Geesmann1 , A. Demircan1,2 , I.
Babushkin1,2,3 , and U. Morgner1,2 ; 1 Leibniz University Hannover, Institute of Quantum Optics, Hannover,Germany; 2 Cluster of Excellence PhoenixD, Hannover,Germany; 3 Max Born Institute, Berlin, Germany

103

A high power 2-μm femtosecond laser source is demonstrated by a doubly resonant optical parametric oscillator. Under a pump power of 18.7 W, a stable output
power of 4.9 W is observed.
CF-P.20 TUE

Passive mode-locking of a fiber laser using a V4C3
MXene based saturable absorber at 1910 nm∙S.-y. Kwon, K. Lee, T. Woo, J. Ryu, J. Jung, and J.H. Lee;
School of Electrical and Computer Engineering, University
of Seoul, Seoul, South Korea
The saturable absorption property of V4C3 MXene wasinvestigated at 2-um wavelengths. A saturable absorber
was fabricated with a ~13% modulation depth. A fiber
laser mode-lcoked by the device produced ~1.1-ps pulses
at ~1912 nm.
CF-P.21 TUE

Status of the ELI-ALPS High repetition rate (HR)laser systems
P. Jójárt1 , ∙I. Seres1 , Z. Bengery1 , B. Gilicze1 , Z.
Várallyay1 , Á. Börzsönyi1 , E. Shestaev2 , N. Walther2 , M.
Tschernajew2 , C. Grebing2 , S. Breitkopf2 , T. Eidam2 , and
J. Limpert2 ; 1 ELI-ALPS, Szeged, Hungary; 2 Active Fiber
Systems GmbH, Jena, Germany
The ELI-ALPS High Repetition rate laser systems provide millijoule level, few-cycle laser pulses at 100 kHz
repetition rate. HR-1 is available for user experiments,and HR-2 is expected to reach specifications by summer
2023.
CF-P.22 TUE

Ultrafast Spectroscopy at Artemis∙R.T. Chapman, A.S. Wyatt, Y. Zhang, J.O.F. Thompson,
C.E. Sanders, G.M. Greetham, and E. Springate; Central
Laser Facility, Harwell, United Kingdom
The recent expansion of the Artemis facility to house
both a high pulse energy laser and a high repetition ratelaser for extreme ultraviolet generation has been realised
and the first results are presented here.
CF-P.23 TUE

Dispersion Management in Vulcan OPCPA Petawatt
Laser Using a Grating-prism Compressor∙V. Aleksandrov, M. Galimberti, I. Musgrave, N. Stuart,and C. Hernandez-Gomez; Central Laser Facility, Scienceand Technology Facilities Council, Didcot, United Kingdom
We design an additional grating-prism compressor to
manage the dispersion in Vulcan OPCPA Petawatt Laser
up to the fifth order. Transmission gratings are used tofurther improve the temporal contrast of the 16 fs pulses.

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Hall B0
13:00 – 14:00
CK-P: CK Poster session
CK-P.1 TUE

Ultra-low-loss broadband multiport optical splitters∙P. Vildoso1,2 , R.A. Vicencio1,2 , and J. Petrovic3 ;1
Departamento de Física, Facultad de Ciencias Físicas y Matematicas, Universidad de Chile, Santiago,
Chile; 2 Millenium Institute for Research in Optics-MIRO,
Concepción, Chile; 3 Vinča Institute of Nuclear Sciences,
National Institute of the Republic of Serbia, University ofBelgrade, Belgrade, Serbia
Novel near-zero-loss 1xN optical splitters are inverse designed and demonstrated by laser writing in glass. The
20-60 nm FWHM bandwidth at 640 nm, <0.5 dB imbalance and downscalable footprint demonstrate advantage
over other design methods.
CK-P.2 TUE

Bi-Layer Grating Couplers for Hybrid SixNy - Si3N4
Photonics with Sub-Decibel Coupling Efficiency∙V. Vitali1,2 , C. Lacava2 , T. Domínguez Bucio1 , F.Y.
Gardes1 , and P. Petropoulos1 ; 1 Optoelectronics ResearchCentre, University of Southampton, Southampton , United
Kingdom; 2 Electrical, Computer and Biomedical Engineering Department, University of Pavia, Pavia , Italy
A general strategy for the design of bi-layer SixNySi3N4 grating couplers is presented. Coupling efficiencies exceeding -0.5 dB are numerically demonstrated for
a 400nm-thick bottom Si3N4 waveguide using different
top-layer SixNy materials.
CK-P.3 TUE

Ion-implanted diced ridge waveguides in Pr:YLF∙K. Hasse1 , S. Suntsov1 , S. Püschel2 , H. Tanaka2 , C.
Kränkel2 , I. Bányász3 , and D. Kip1 ; 1 Helmut Schmidt
University, Hamburg, Germany; 2 Leibniz-Institut fürKristallzüchtung (IKZ), Berlin, Germany; 3 Wigner Research Centre for Physics, Budapest, Hungary
We demonstrate the first ion-implanted waveguides in
Pr:YLF. Ridge waveguides diced into the surface of ionimplanted Pr:YLF enable single and multimode guiding
with transmission losses of 0.4 – 2.5 dB/cm depending
on wavelength and waveguide dimensions.
CK-P.4 TUE

Laser based Methods for Photoluminescence
Enhancement of Silicon Nanocrystals in a Silicon
Suboxide Matrix∙L.J. Richter and J. Ihlemann; Institut für Nanophotonik
Göttingen e.V., Göttingen, Germany
Silicon nanocrystals offer an opportunity for the implementation of silicon-based photonics and thus integration into microelectronics processes. Here, results

are presented for laser-based methods for photoluminescence enhancement of silicon nanocrystals in a silicon
suboxide matrix.
CK-P.5 TUE

All-Optically Adressable Sub-Micron Pixels∙M. Crouzier1,3 , V. Yam1 , G. Magno2 , T. Lopez3 , and
B. Dagens1 ; 1 Université Paris-Saclay, CNRS, Centre deNanosciences et de Nanotechnologies, Palaiseau, France;2
Department of Electrical and Information Engineering,
Polytechnic University of Bari, Bari, Italy; 3 Stellantis,
Centre technique de Vélizy, Vélizy-Villacoublay, France
We numerically study the coupling between plasmonic
chains deposited above a waveguide array. This structure allows the independent and local excitation of plasmonic nanostructures defining submicrometer pixels foraddressable optical traps or spatial light modulators.
CK-P.6 TUE

Design and Fabrication of Angled MMI-Based
Duplexer for Sensing Applications∙A. Thottoli1 , A.S. Vorobev 1,2,3 , G. Biagi2,4 , S.
Iadanza2,3,5,6 , G. Magno1 , L. O’Faolain2,3 , and M.
Grande1 ; 1 Department of Electrical and Information
Engineering, Politechnico di Bari, Bari, Italy; 2 Centre
for Advanced Photonics and Process Analysis, Munster Technological University, Cork, Ireland; 3 Tyndall
National Institute, T12 PX46 Cork, Ireland., Cork, Ireland; 4 PolySenSe Lab, Physics Department, Universityof Bari, Bari, Switzerland; 5 Laboratory of Nano andQuantum Technologies, Paul Scherrer Institut, Villigen,
Switzerland; 6 IBM Research Zurich, Zurich, Switzerland
We propose a compact, low-loss, broadband angled
multi-mode interference based duplexer coupler as an
optical component for integrating multiple wavelengths
with higher optical output power transmittance for multiple gas sensing applications.
CK-P.7 TUE

Modified Photonic Band Gap Via Thermal Shrinkage
of Two-photon Polymerized Distributed Bragg
Reflectors∙Y.-S. Chen1 , M. Taverne2 , C.-C.K. Huang3 , Y.-L.D.
Ho2 , and J.G. Rarity1 ; 1 University of Bristol, Bristol,
United Kingdom; 2 Northumbria University, Newcastle
upon Tyne, United Kingdom; 3 University of Southampton, Southampton, United Kingdom
Thermal shrinkage is applied on the polymer-based distributed Bragg reflectors (DBR) template to reduce theperiod. A uniform shrinkage is observed on the template, which modified the photonic band gap to a shorter
wavelength.

CK-P.8 TUE

CK-P.11 TUE

Apodized Chirped Bragg Gratings in a Silicon
Nitride-on-Insulator Platform at Short-Wave
Infrared Wavelengths∙M. Sinobad1 , J. Lorenzen1 , A. Berg1 , H. Francis2 , J.
Carreira2 , M.A. Gaafar1 , T. Herr1,3 , N. Singh1 , and F.X.
Kärtner1,3 ; 1 Deutsches Elektronen-Synchrotron, Hamburg, Germany; 2 Ligentec SA, Ecublens, Switzerland;
3
Universität Hamburg, Hamburg, Germany
We report on apodized chirped Bragg gratings in a silicon nitride-on-insulator platform. Applications for thisdevice include nonlinear photonics, specifically dispersion compensation in mode-locked lasers operating inthe short-wave infrared wavelength band.

Inverse Design of Low-Loss Subwavelength Grating
Couplers∙S. Hooten1 , T. Van Vaerenbergh2 , M. Fiorentino1 , and R.
Beausoleil1 ; 1 Hewlett Packard Labs, Milpitas, CA, USA;
2
Hewlett Packard Labs, HPE Belgium, Diegem, Belgium
The AI-enhanced inverse design of low-loss, highbandwidth subwavelength grating couplers (SWGCs) ispresented. We obtain 3D-simulated 0.7dB insertion loss
and 40nm 1dB-bandwidth at λ=1550nm.

CK-P.9 TUE

MIRPIC – a rising photonic integration platform for
mid-infrared∙R. Piramidowicz1,2,3 , S. Stopiński1,2,3 , K. Anders1,2,3 , A.
Jusza1,3 , M. Lelit1,4 , A. Połatyński1,5 , P. Wiśniewski4 , M.
Słowikowski1,4 , M. Juchniewicz4 , K. Pavłov4 , M. Żbik2 , J.
Jureńczyk2 , K. Pierściński6 , and D. Pierścińska6 ; 1 Warsaw
University of Technology, Institute of Microelectronics andOptoelectronics, Warsaw, Poland; 2 VIGO Photonics S.A.,Ożarów Mazowiecki, Poland; 3 LightHouse Sp. z o.o.,
Lublin, Poland; 4 Warsaw University of Technology, Centre for Advanced Materials and Technologies CEZAMAT,
Warsaw, Poland; 5 VPIphotonics GmbH, Berlin, Germany;6Łukasiewicz Research Network - Institute of Microelectronics and Photonics, Warsaw, Poland
We present and discuss the results of the development of
the first integrated photonic platform for mid-IR spectral
range (MIRPIC), based on heterogeneously integratedof QCLs, Ge-on-Si waveguiding components, and antimonide super lattice mid-IR detectors.
CK-P.10 TUE

Generalized Vectorial Light Transmission Control
Using Bilayer Metasurfaces with Fully Designable
Anisotropy and Chirality∙T. Chang1,2 , J. Jung1 , and J. Shin1 ; 1 Department of Materials Science and Engineering, KAIST, Daejeon, South Korea; 2 Centre for Disruptive Photonic Technologies, SPMS
and TPI, Nanyang Technological University, Singapore,
Singapore
We realize bilayer dielectric metasurfaces that enable
complete passive vectorial linear control on light transmission for a specific wavelength. We demonstratepolarization-multiplexed holographic techniques thatwere not possible previously, and propose a metasurfacebased optical platform.

104

CK-P.12 TUE

Arbitrary 3D beam delivery from planar opticalwaveguides for quantum technology∙D.-W. Ko, Q.S. Ahmed, J.W. Field, J.C. Gates, and P.
Horak; University of Southampton, Southampton, United
Kingdom
We design 2D holographically written grating couplers
for the generation of arbitrarily shaped free-space beams
from integrated planar waveguides. Local grating periods and index modulations depend on target field, pumpbeam profile and pump depletion.
CK-P.13 TUE

Laser-engineered nanocomposites for SERS
applications∙M. Hoffmann, S. Wackerow, A. Abdolvand, and S.A.
Zolotovskaya; Materials Science & Engineering Research
Cluster, School of Science and Engineering, University of
Dundee, Dundee , United Kingdom
A rapid and scalable approach to sub-micron periodic
array deposition of Ag and Au nanoparticles is presented. Multiscale plasmonic effects in the Ag/AuNPTiO2 arrays enabled substantial SERS performance improvement with the enhancement factors reaching 10^7.
CK-P.14 TUE

Efficient Phase Tuning of Silicon Photonic Devices
Using Alignment Assisted Liquid Crystal Tuners∙S. Kumari, R. Kallega, S. Shelwade, A. Keloth, and S.K.
Selvaraja; Indian Institute of Science Bangalore, Bangalore, India
We demonstrate a groove-assisted liquid crystal phasetuner integrated over a silicon Mach-Zehnder interferometer. The fabricated device offers a phase tuning efficiency of 2.25π/mW, which is 30% more efficient than agroove-less device.
CK-P.15 TUE

Thermal Crosstalk Alleviated Silicon Microring
Switches∙R. Cubas Heim1 , S. De1,2 , R. Das1 , K. Singh1 , T. KleineOstmann2 , and T. Schneider1 ; 1 TU Braunschweig, Braunschweig, Germany; 2 PTB Braunschweig, Braunschweig,
GermanyCLEO®

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Hall B0
We demonstrate simulation results for densely packed
photonic chips for a routed optical switching network.
As we show, by a deep trench design, the thermal
crosstalk between the switches can be drastically reduced.

We study thin film broadband perfect absorbers withcopper nanoparticles. We have simulated and fabricatedsamples of the perfect broadband absorbers. It turns out
we can achieve almost 90% light absorption over a broad
range.

CK-P.16 TUE

CK-P.20 TUE

Impurity-generated wavepackets in one dimensional
photonic lattices∙B. Real1,2 , D. Guzmán-Silva1,2 , and R.A. Vicencio1,2 ;1Departamento de Física, Facultad de Ciencias Físicas
y Matemáticas, Universidad de Chile, Santiago, Chile;
2
Millenium Institute for Research in Optics, Santiago,
Chile
We propose a method to create on-chip wavepackets
with well-defined quasimomentum by exploiting theleaky mode of an impurity in one-dimensional photonic
lattices

Deformed Polymer Microcavities to Enhance
Dynamical Properties of Semiconductor Lasers∙R. de Mey1 , K. Vanmol1 , J. Van Erps1 , S.W. Jolly1,2 , and
M. Virte1 ; 1 Brussels Photonics (B-PHOT), Dept. of Applied Physics and Photonics, Vrije Universiteit Brussel,
Brussels, Belgium; 2 Service OPERA-Photonique, Université Libre de Bruxelles, Brussels, Belgium
We investigate the use of deformed polymer microcavities to achieve time-distributed optical feedback in semiconductor lasers. We analyze how the geometry of thecavity impacts the laser dynamics and the properties of
the generated chaos.

CK-P.17 TUE

Isotropic double Dirac cones in the electromagnetic
dispersion relation detected by high-resolution
angle-resolved reflection spectroscopy
A. Begum1,2 , Y. Yao1,2 , T. Kuroda1 , E. Watanabe1 , N.
Ikeda1 , Y. Sugimoto1 , H. Koyama1 , Y. Takeda1,2 , and∙K. Sakoda1 ; 1 National Institute for Materials Science,
Tsukuba, Japan; 2 University of Tsukuba, Tsukuba, Japan
We successfully fabricated SOI photonic crystal slabs
by EB lithography that materialized electromagnetic
isotropic double Dirac cones in the zone center, whichwere confirmed by high-resolution angle-resolved reflection spectroscopy in the mid IR range.

CK-P.21 TUE

CK-P.18 TUE

Photonics for Single Photon Sources FabricatedUsing Nanoimprint Lithography∙Y. Li, J. Qian, and J.M. Smith; University of Oxford, OXFORD, United Kingdom
We fabricate the planar-hemispherical optical microcavities for single photon sources using nanoimprint lithography. Clear optical confinement modes are observed intransmission spectra through microcavities. We aim toembed emitters later to create cavity-coupled single photon sources.

Polarization coupling in thin film lithium niobate
waveguide∙D. Fu, H.R. Fergestad, A. Prencipe, T. Li, and K. Gallo;
KTH Royal Institute of Technology, Stockholm, Sweden
A thin film lithium niobate waveguide with two tapers
is fabricated and measured with controlled polarization.
40 % longitudinal coupling between fundamental TE
and TM modes is observed at telecom wavelengths.
CK-P.19 TUE

Broadband perfect absorbers based on copper
nanoparticles thin films∙N. Perdana1 , K. Rogall2 , J. Drewes2 , A. Vahl2 ,T. Strunskus2 , M. Abdelaziz2 , F. Faupel2 , and C.
Rockstuhl1,3 ; 1 Institute of Theoretical Solid State Physics,
Karlsruhe Institute of Technology (KIT), Karlsruhe, Germany; 2 Institute of Material Science, Chair for Multicomponent Materials, Kiel University, Kiel, Germany;3
Institute of Nanotechnology, Karlsruhe Institute of Technology (KIT), Karlsruhe, Germany

Diamond ”Sawfish” photonic crystal cavities∙M.E. Stucki1,2 , T. Pregnolato1,2 , J.M. Bopp1,2 , M. van der
Hoeven1 , and T. Schröder1,2 ; 1 Ferdinand-Braun-InstitutegGmbH, Berlin, Germany; 2 Department of Physics, Humboldt University of Berlin, Berlin, Germany
In order to enhance spectral properties and photon
collection of color centers in diamond, we fabricate“Sawfish” photonic crystal cavities using quasi-isotropic
under etching and demonstrate their performance spectroscopically.
CK-P.22 TUE

CK-P.23 TUE

Advanced optical interfaces for silicon-nitride-based
bio-photonic platform operating in visible spectral
range∙M. Lelit1,2 , K. Anders1,3 , M. Słowikowski1,2 , M.
Juchniewicz2 , B. Stonio1,2 , S. Stopiński1,3 , and R.
Piramidowicz1,3 ; 1 Warsaw University of Technology, Institute of Microelectronics and Optoelectronics, Warsaw,
Poland; 2 Warsaw University of Technology, Centre forAdvanced Materials and Technologies CEZAMAT, War-saw, Poland; 3 VIGO Photonics S.A., Ożarów Mazowiecki,
PolandAdvanced optical interfaces developed for SiN-based
visible passband photonic platform intended forbiosensing applications is being reported in this work.
Results for 3D-tapers assisted edge couplers and lightleakage-shielded grating couplers are presented.
CK-P.24 TUE

Surface second harmonic generation from AB-type
stacks of dielectric nanolaminates∙F. Abtahi1 , P. Paul1,2 , A. Kuppadakkath1 , A. Pakhomov1 ,A. Szeghalmi1,2 , F. Setzpfandt1,2 , and F. Eilenberger1,2,3 ;1Friedrich Schiller University Jena, Institute of Applied
Physics, Abbe Center of Photonics, Jena, Germany;
2
Franhofer-Institute for Applied Optics and Precision Engineering IOF, Jena, Germany; 3 Max Plank School of Photonics, Jena, Germany
We investigate the second harmonic generation responseof artificial optical surfaces functionalized with subwavelength stacks of dielectric, amorphous media which multiply the number of surfaces experienced by an electricfield dramatically.
CK-P.25 TUE

Photon Confinement in 3D Photonic Band Gap
Superlattices∙M. Kozon1,2 , M. Schlottbom2 , J.J.W. van der Vegt2 , andW.L. Vos1 ; 1 Complex Photonic Systems (COPS), MESA+
Institute for Nanotechnology, University of Twente, Enschede, Netherlands; 2 Mathematics of Computational Science (MACS), MESA+ Institute for Nanotechnology, University of Twente, Enschede, Netherlands
We present an extensive analysis of photon confinement
properties of 3D inverse woodpile photonic band gap
crystals with respect to their structural parameters. We
also analyze their potential for cavity quantum electrodynamics.
CK-P.26 TUE

Mode-locking System of Coupled Microcavities with
Gain and Nonlinear Loss
∙R. Imamura1 , S. Fujii2 , A. Nakashima1 , and T. Tanabe1 ;1
Department of Electronics and Electrical Engineering,
Faculty of Science and Technology, Keio University, Yokohama, Japan; 2 Department of Physics, Faculty of Scienceand Technology, Keio University, Yokohama, Japan
We numerically study the mode-locking regime in a system in which a gain-doped resonator is coupled to anonlinear loss-functionalized resonator. In this system,
mode-locking is possible even with low gain and relatively low Q.

105

CK-P.27 TUE

Experimental Observation of Radiance Phenomena
in One-Dimensional Photonic Lattices∙D. Román-Cortés1,2 , J. Cubillos1,2 , C. Cid-Lara1,2 ,I. Salinas1,2 , P. Solano3 , and R.A. Vicencio1,2 ;1Departamento de Física, Facultad de Ciencias Físicas y Matemáticas, Universidad de Chile, Santiago, Chile;
2
Millennium Institute for Research in Optics - MIRO,
Santiago, Chile; 3 Departamento de Física, Facultad deCiencias Físicas y Matemáticas, Universidad de Concepción, Concepción, Chile
We experimentally observe both super-radiance and thegeneration of bound states in the continuum when two
photonic “atoms” emit towards a continuum-like 1Dphotonic lattice, depending on the specific separationand phase between them.
CK-P.28 TUE

Robust reverse chiral light dynamics around
conjugate exceptional points in1D photonic bandgap
waveguides∙S. Dey and S. Ghosh; Indian Institute of Technology Jodhpur, Jodhpur, India
We report the hosting of conjugate exceptional points(EPs) in two complementary gain-loss assisted 1D photonic bandgap waveguides and explore the robust chiraland reverse chiral mode conversion phenomena following dynamical EP encirclement schemes.
CK-P.29 TUE

Study on bifurcating light trajectory in a distorted
photonic crystal with multiple slip dislocations∙Y. Kawamoto1 , J. Hashizume1 , H. Kitagawa1 , and K.
Kitamura1,2 ; 1 Kyoto Institute of Technology, Kyoto, Japan;
2
Japan Science and Technology, Saitama, Japan
We have numerically analyzed light propagation in the
distorted photonic crystal which possesses multiple slip
dislocations and shown the trajectory repeated curvatureand bifurcation, in which can explain by potential twounits lattice shapes change.
CK-P.30 TUE

Discontinuous Galerkin Method to Model Light
Propagation in Photonic Crystals of Any Size
∙M. Kozon1,2 , L.J. Corbijn van Willenswaard1,2 , M.
Schlottbom2 , W.L. Vos1 , and J.J.W. van der Vegt2 ;1Complex Photonic Systems (COPS), MESA+ Institute for
Nanotechnology, University of Twente, Enschede, Netherlands; 2 Mathematics of Computational Science (MACS),MESA+ Institute for Nanotechnology, Enschede, Netherlands
We present a discontinuous Galerkin method for lightpropagation through large photonic crystals by utilizing their local periodicity, allowing us to treat the wholecrystal as one finite element with Bloch basis functions.

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⋅ Tuesday 27 June 2023

Hall B0
CK-P.31 TUE

Radiation phenomena in kagome photonic lattices
I. Salinas1,2 , J. Cubillos1,2 , A. Szameit3 , P. Solano4 , and∙R. Vicencio1,2 ; 1 D. Fisica, FCFM, Universidad de Chile,
Santiago, Chile; 2 Millenium Institute for Research in Optics - MIRO, Santiago, Chile; 3 Institute of Physics, University of Rostock, Rostock, Germany; 4 D. Fisica, FCFM,
Universidad de Concepcion, Concepcion, Chile
We study radiation, super and sub radiance phenomena
in a 2D kagome photonic lattice. We show that an in (outof) phase atoms emission drastically improves (reduces)the energy radiated to the lattice.
CK-P.32 TUE

Q-factor optimization in photonic crystal nanobeam
cavities based on elliptical nanopillars for refractive
index sensing∙J.H. Mendoza-Castro1,2 , A.S. Vorobev1,3,4 , S. Iadanza3,4 ,B. Lendl2 , M. Grande1 , and L. O’Faolain3,4 ; 1 Department
of Electrical and Information Engineering, Politecnico diBari, Via E. Orabona, 4, 70126 , Bari, Italy; 2 Institute ofChemical Technologies and Analytics, TU Wien, Getreidemarkt 9/164,1060 , Vienna, Austria; 3 Centre for Advanced Photonics and Process Analysis, Munster Technological University, T12 T66T Bishopstown , Cork, Ireland;
4
Tyndall National Institute, T12 PX46 , Cork, Ireland
We present a compact and flexible Photonic Crystal
Nanobeam Cavity (PhCNC) design in which optimization of the calculated Q-factor (106 ) is achieved by elliptically shaped Si3 N4 nanopillars
CK-P.33 TUE

Fabrication of 3D Photonic Band Gap Crystals from
Silicon
M.J. Goodwin1,2 , C.A.M. Harteveld1 , L.J. Corbijn
van Willenswaard1 , T.J. Vreman1 , A.S. Schulz1 , D.A.
Grishina1 , and ∙W.L. Vos1 ; 1 Complex Photonic Systems(COPS), MESA+ Institute for Nanotechnology, Universityof Twente, Enschede, Netherlands; 2 MESA+ Nanolab,
University of Twente, Enschede, Netherlands

13:00 – 14:00
EG-P: EG Poster session
EG-P.1 TUE

Electron decoherence and distant object detection∙C.I. Velasco1 , V. Di Giulio1 , and F.J. García de
Abajo1,2 ; 1 ICFO - Institut de Ciencies Fotoniques, The
Barcelona Institute of Science and Technology, Castelldefels (Barcelona), Spain; 2 ICREA - Institucio Catalana deRecerca i Estudis Avancats, Barcelona, Spain
We show that two-path decoherence of a single-electron

A method of creating 3D, inverse woodpile, photonic
crystals in silicon by reactive ion etching. The crystals
were characterized by various tomography and imaging
techniques.
CK-P.34 TUE

Integrated Circuits with Optical Injection Locking ofRing Lasers for QKD and QPSK Applications
D. Massella1 , M. Wallace2 , R. Broeke2 , F. Diaz1,3 , and ∙N.
Pinto1 ; 1 Universidade de Vigo, Vigo, Spain; 2 Bright Photonics, Eindhoven, Netherlands; 3 AtlanTTic research center, Vigo, Spain
The present work demonstrates the design and experimental implementation of two monolithically integrated
ring laser circuits, based on the optical injection locking technique. Preliminary characterization results showthat locking is achievable under current designs.
CK-P.35 TUE

Stable soliton comb from dual ring microresonators∙A.n. Karunakaran1,2 , A. Manetta1 , P. Varming1 , O.B.
Helgason3 , P. Montague1 , M. Pu2 , V. Torres-Company3 ,and K. Yvind2 ; 1 NKT Photonics A/S, Birkerod, Denmark;2
DTU Electro, Technical University of Denmark, Kgs.
Lyngby, Denmark; 3 Department of Microtechnology andNanoscience, Chalmers University of Technology, Gothenburg, Sweden
We present a packaged SiN dual-ring resonator for frequency comb generation. Using an ultra-stable pumplaser and active temperature stabilization we alleviatefrequency drifts and detuning fluctuations. The resulting solitons are stable over several hours.
CK-P.36 TUE

Towards the Simultaneous Coupling and Enhancement of hBN Based Single Photon Emission with
Si3 N4 Photonic Structures∙B. Laudert1 , J.P. Berti Ligabo1 , and F. Eilenberger1,2 ;1Institute of Applied Physics, Friedrich Schiller University
Jena, Jena, Germany; 2 Fraunhofer-Institute for Applied

beam caused by inelastic interaction with a material
structure is driven by infrared divergences, which are encapsulate in quantum interactions that leave traces up to
macroscopic distances.
EG-P.2 TUE

Particle-in-Cell simulations of ultrashort opticallaser pulses for magnetic field enhancement andelectric field suppression∙L. Grünewald1,2 ,R. Martín-Hernández3 ,E.
Gangrskaia4 , V. Shumakova4 , C. Hernández-García3 ,and S. Mai1 ; 1 Institute for Theoretical Chemistry, Faculty

Optics and Precision Engineering IOF, Jena, Germany
A proposed scheme for the simultaneous enhancement
and coupling for hBN based single-photon emission
with Si3 N4 photonic structures. In FDTD simulations
we have achieved a Purcell factor of 7.9 and a coupling
efficiency of 35%.
CK-P.37 TUE

Photonic Energy Density and Scattering from
Random and Periodic Arrays of Silicon Pillars
M.J. Goodwin1,2 , O. Akdemir1 , M.D. Truong1 , L. Bitenc1 ,A. Lagendijk1 , and ∙W.L. Vos1 ; 1 Complex Photonic
Systems (COPS), MESA+ Institute for Nanotechnology,
University of Twente, Enschede, Netherlands; 2 MESA+
Nanolab, University of Twente, Enschede, Portugal
A range of randomly and periodically arrange pillars
have been fabricated to study photonic energy density
and localization in scattering media.
CK-P.38 TUE

Computation of Optical Properties of Real Photonic
Band Gap Crystals as Opposed to Utopian Ones
L.J. Corbijn van Willenswaard1,2 , S. Smeets3 , N. Renaud3 ,M. Schlottbom2 , J.J.W. van der Vegt2 , and ∙W.L. Vos1 ;1Complex Photonic Systems (COPS), MESA+ Insitute for
Nanotechnology, Universiteit Twente, Enschede, Netherlands; 2 Mathematics of Computational Science (MACS),MESA+ Insitute for Nanotechnology, Universiteit Twente,
Enschede, Netherlands; 3 Netherlands eScience Center,
Amsterdam, Netherlands
Manufacturing deviations of real photonic crystals are
not included in predictive models. Here we present thenumerical transmission spectrum computed from tomographically reconstructed crystal and compare this witha utopian model without these deviations.

B. Brecht1 , and T. Zentgraf1 ; 1 Paderborn University,
Paderborn, Germany; 2 Karlsruhe Institute of Technology,
Karlsruhe, Germany
We present a scheme for topologically noise-protectedtransport of light at 1550 nm in a Silicon on Insulator
Platform. We report the design, fabrication and characterization of our structures.
CK-P.40 TUE

Butt-Coupling Optical Probe Card for Wafer-Scale
Photonic-Integrated-Circuits Test with Polarization
Control
C.-Y. Wu1 , ∙M.-C. Lee1 , M.-J. Lu2 , S.-Y. Mu2 , J. Chen2 ,and C.-S. Cheng2 ; 1 National Tsing Hua University,
Hsinchu, Taiwan; 2 Advanced Semiconductor Engineering
Inc., Kaohsiung, Taiwan
A Si photonics optical probe card is presented for onwafer testing photonic integrated circuits via a butt coupling scheme. This probe card can characterize thepolarization-dependent loss of devices under test.
CK-P.41 TUE

An Integrated Passively Q-switched Nanophotonic
Laser in the NIR Based on Two-Dimensional
Materials
G. Nousios1 , T. Christopoulos1 , ∙O. Tsilipakos2 , and E.
Kriezis1 ; 1 Aristotle University of Thessaloniki, Thessaloniki, Greece; 2 National Hellenic Research Foundation,
Athens, Greece
We propose and analyze a nanophotonic Q-switched lasing element utilizing 2D materials for optically pumped
gain and saturable absorption. Lasing is rigorously evaluated with a temporal coupled-mode theory frameworkand mW peak power is predicted.

CK-P.39 TUE

Topological Valley Photonic Crystals for on-chiptransport of light∙E. Narváez Castañeda1 , A. Khanda2 , M. Brauckmann1 ,of Chemistry, University of Vienna, Vienna, Austria;
2
Vienna Doctoral School in Chemistry (DoSChem),
University of Vienna, Vienna, Austria; 3 Grupo de Investigacíon en Aplicaciones del Láser y Fotónica, Departamento de Física Aplicada, University of Salamanca,
Salamanca, Spain; 4 Photonics Institute, TU Wien, Vienna, Austria
We report simulations of electromagnetic fields of ultrashort, azimuthally polarized laser beams interacting withmetal apertures of different shape, providing magnetic
field enhancement and electric field suppression near the
beam axis for magneto-only optical spectroscopy.

106

EG-P.3 TUE

Designing plasmonic sensors using Babinet’s
principle∙J.A. Riley1,2 , M. Horák3,4 , V. Křápek3,4 , and V. PachecoPeña1 ; 1 School of Mathematics, Statistics and Physics,
Newcastle University, Newcastle Upon Tyne, United Kingdom; 2 School of Engineering, Newcastle University, Newcastle Upon Tyne, United Kingdom; 3 Central European
Institute of Technology, Brno University of Technology,
Brno, Czech Republic; 4 Institute of Physical Engineering,
Brno University of Technology,, Brno, Czech Republic

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⋅ Tuesday 27 June 2023

Hall B0
Université Côte d’Azur, Valbonne, France
The Photonic Atom Probe allows the correlative measurement of Atom Probe Tomography and Photoluminescence data. In this contribution, both the laser absorption and PL emission properties of the nanometricspecimen are investigated.

Numerical and experimental, studies of complementary
plasmonic sensors designed using Babinet’s principle ispresented. Spectral changes in the localised surface plasmons resonances are demonstrated when introducing
variations in the parameters of a nearby dielectric analyte.

2EG-P.4 TUE

EG-P.6 TUE

Low-temperature plasmonically enhanced
single-molecule spectroscopy of fluorescent proteins∙O. Evans1 , V. Singh1 , O. Aksakal2 , D. Jones2 , P. Borri2 ,and W. Langbein1 ; 1 Cardiff University, School of Physics
and Astronomy, Cardiff, United Kingdom; 2 Cardiff University, School of Biosciences, Cardiff, United Kingdom
We present plasmonically enhanced single-molecule
cryo-spectroscopy of far-red fluorescent protein,mRhubarb. The temporal switching and jitter of thespectra provide information on the conformational
dynamics of the chromophore and fluorescent protein.

Towards Plexcitonic Systems of Gold Nano-Antennas
and J-aggregates∙A.M. Jumbo Nogales1 , M. Grzelczak2 , and Y. Rakovich3 ;1Materials Physics Center, Donostia, Spain; 2 Donostia International Physics Center, Donostia, Spain; 3 Ikerbasque,
Basque Foundation for Science, Bilbao, Spain
The coupling of gold nano-structures and J-aggregatesprovides interesting applications due to their uniqueproperties. We used gold nano-bipyramids and JC-1 Jaggregates in strong coupling to characterize plexcitonic
systems and evaluate their potential for applications.

EG-P.5 TUE

EG-P.7 TUE

Development of the Far-Field Photoluminescenceemission from a Quantum Well during its Field
Evaporation in a Tomographic Atom Probe∙E.M. Weikum 1 , G. Beainy1 , J. Houard1 , S. Moldovan1 ,J.-M. Chauveau2 , M. Hugues2 , D. Lefebvre2 , A. Vella 1 ,and L. Rigutti1 ; 1 Université de Rouen , Rouen, France;

Probing the Position Resolved Energy Density Inside
Photonic Scattering Slabs with Strong Absorption
and Anisotropy∙O. Akdemir1 , L. Bitenc2 , I.L. Maxwell1 , M. Goodwin1 ,M.D. Truong1 , A. Lagendijk1 , and W.L. Vos1 ; 1 Complex

Photonic Systems (COPS), University of Twente, Enschede, Netherlands; 2 University of Ljubljana, Ljubljana,
Slovenia
We present experiments to probe the positiondependent energy density inside strongly absorbing
and anisotropic scattering samples. Common analytical approximations fail to describe such samples. We
compare experiments to analytical approximations andMonte Carlo simulations.
EG-P.8 TUE

Uncovering the Physics of Ultraslow Hot-exciton
Relaxation and Interparticle Auger Coupling in HgTe
Quantum Dots
∙K. Fan1 , K.A. Sergeeva2 , A.A. Sergeev1 , L. Zhang1 ,C.C.S. Chan1 , Z. Li2 , X. Zhong2 , S.V. Kershaw2 , J. Liu1 ,A.L. Rogach2 , and K.S. Wong1 ; 1 Department of Physics,
The Hong Kong University of Science and Technology,
Hong Kong, China; 2 Department of Materials Science andEngineering, City University of Hong Kong, Hong Kong,
China
Transient absorption measurement reveals ultraslow
hot-exciton cooling in HgTe quantum dots. Auger recombination is significantly enhanced by interparticle
excitonic coupling at reduced ligand length. The discovery contributes to developing high-performance optoelectronic materials with confinement-bulk duality.

NOTES

107

EG-P.9 TUE

All-Silicon Topology Optimized Two-Photon
Absorption Detector for On-chip Interconnects∙A.N. Kamel1,2 , M.R.A. Newman1,2,3 , A. Marchevsky1,2,4 ,R.E. Christiansen2,5 , A.N. Babar1,2 , P.T. Kristensen1,2 ,O. Sigmund2,5 , S. Stobbe1,2 , J. Mørk1,2 , and K. Yvind1,2 ;1DTU Electro, Technical University of Denmark, Kgs.
Lyngby, Denmark; 2 NanoPhoton - Center for Nanophotonics, Kgs. Lyngby, Denmark; 3 Interuniversity Microelectronics Centre (IMEC), Leuven, Belgium; 4 Microsoft
Danmark ApS, Kg. Lyngby, Denmark; 5 Department ofCivil and Mechanical Engineering, Technical Universityof Denmark, Kgs. Lyngby, Denmark
We present and all-silicon, topology-optimized, resonant two-photon PIN detector for on-chip interconnects. Using topology optimization, the field enhancement necessary for efficient two-photon detection is possible at moderate quality factor and thus does not limit
speed.

CLEO

Room 1 ICM

Room 4a ICM®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 4b ICM

Room 13a ICM

Room 13b ICM

Room 14a ICM

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

CM-7: Laser written waveguides and gratings

CK-4: Active components

EG-6: Nanomanipulation,nano-organization andcorrelation

CA-6: Visible and UV lasers

JSI-1: Nonlinear X-ray wavemixing

CD-7: Spectroscopy applications

Chair: Giuseppe Sansone, University
of Freiburg, freiburg, Germany

Chair: Aurelien Houard, ENSTA
Paris, France

JSI-1.1 WED (Invited)CD-7.1 WEDChair: Robert Thomson, HeriotWatt University, Edinburgh, United
KingdomCM-7.1 WED

8:30‘Designer Glasses’ for Ultrafast
Laser-Inscribed Low-Loss Optical
Waveguides
T.T. Fernandez1,2 , A. Ross-Adams1 ,M. Bakovic3 , M.J. Withford1,3 , and∙S. Gross3,4 ; 1 MQ Photonics Research Centre, School of Mathematical and Physical Sciences, Macquarie
University, NSW 2109, Sydney, Australia; 2 University of South Australia, Laser Physics and Photonics
Devices Laboratories, SA 5095, Adelaide, Australia; 3 Modular Photonics Pty Ltd, Sydney, Australia; 4 MQ
Photonics Research Centre, School ofEngineering, Macquarie University,
NSW 2109, Sydney, Australia
The composition of the glass substrate when creating optical waveguides using Ultrafast Laser Inscription is crucial for the formationof high-quality waveguides. We
present tailored glass compositions
enabling ~0.05 dB/cm propagationloss.

CM-7.2 WED

8:45

Femtosecond inscription of aspectral array of seven fiber Bragg
gratings at the same spot using asingle uniform phase-mask∙A. Halstuch and A.A. Ishaaya;
School of Electrical and Computer
Engineering, Ben-Gurion Universityof the Negev, Beer-Sheva, Israel
A spectral array of seven fiber-

Chair: Stefano Pelli, CNR-IFAC,
Sesto Fiorentino, Italy

Chair: Takunori Taira, RIKEN
SPring-8 Center (RSC), Japan

Chair: Michele Celebrano, Politecnico di Milano, Italy
CK-4.1 WED (Invited)

8:30

Photophysics of single color
centers in silicon∙A. Dréau; Laboratoire Charles
Coulomb, Montpellier, FranceWith a view to developing quantum applications, we fabricate single color centers in silicon, associated with the so-called G-center,and investigate their single-photon
emission to understand their photophysics and interactions with theirlocal environment.

EG-6.1 WED

8:30

CA-6.1 WED

8:30

Hyper Rayleigh Scattering of
Liquids : an Insight into
Nanoscale organization of Liquids∙F. Rondepierre1 , J. Duboisset2 ,and P.-F. Brevet1 ; 1 Institut Lumière
Matière, UMR CNRS 5603,Université Claude Bernard Lyon 1,
Villeurbanne, France; 2 Aix Marseille
Université,
C.N.R.S.,
Centrale
Marseille, Institut Fresnel, F-13013
Marseille, France, Marseille, France
Second Harmonic Scattering isdemonstrated to probe aqueous
electrolyte nanoscale orientationalcorrelations undergoing long toshort-range transition with salt
concentration. These experimental
results are described within atheoretical framework involving theliquid correlation function.

UV-diode-pumped green andyellow Tb3+ lasers∙M. Badtke, S. Kalusniak, H.
Tanaka, and C. Kränkel; LeibnizInstitut für Kristallzüchtung (IKZ),
Berlin, Germany
We investigated the visible laser performance of Tb3+ :LiLuF4 under different UV-pump wavelengths using a 2ω-Ti:sapphire. Furthermore,
we demonstrated the first UV-laserdiode pumped Tb3+ -laser, whichshows promise as a compact and efficient yellow laser source.

EG-6.2 WED

CA-6.2 WED

8:45

Inducing electron-photon
correlations at an integrated
photonics microresonator
A. Feist1,2 , G. Huang3,4 , G. Arend1,2 ,Y. Yang3,4 , ∙J.-W. Henke1,2 , A.S.
Raja3,4 , F.J. Kappert1,2 , J. Pan3,4 , H.
Lourenco-Martins1,2 , Z. Qiu3,4 , J.
Liu3,4 , O. Kfir1,2 , T.J. Kippenberg3,4 ,and C. Ropers1,2 ; 1 Max Planck

8:45

Diode-pumped Q-switched
Alexandrite Laser as an emitter in
a compact general purpose lidar
system for atmosphericmeasurements∙S. Scheuer1 , A. Munk1 , M.
Strotkamp1 , B. Jungbluth1 , J.
Höffner2 , J. Froh2 , T. Mense2 ,1
and A. Mauer2 ;Fraunhofer

108

8:30

X-ray Transient Grating experiments at Free Electron Lasers∙C. Svetina; Instituto Madrileño deEstudios Avanzados en Nanociencia (IMDEA Nanociencia), Madrid,
Spain
Optical transient grating is a fourwave-mixing method implemented
to investigate transport phenomena
and diffusion processes. I will show
results in developing X-ray Transient Grating at X-ray Free Electron
Lasers and discuss the challenges
and perspectives.

8:30

High harmonic spectroscopy ofquantum phases in a high-Tc
superconductor
J. Alcalà1 , U. Bhattacharya2 , M.
Ciappina3,4 , U. Elu2 , T. Graß2 , P. T.
Grochowski2,5,6,7 , M. Lewenstein2,8 ,A. Palau1 , T. P. H. Sidiropoulos2 ,T. Steinle2 , ∙I. Tyulnev2 , and J.
Biegert2,8 ; 1 ICMAB-CSIC - Institut de Ciència de Materials deBarcelona, Barcelona, Spain; 2 ICFO
- Institut de Ciencies Fotoniques,
The Barcelona Institute of Scienceand Technology, Barcelona, Spain;
3
Guangdong Technion - Israel
Institute of Technology, Shantou,
China; 4 Technion - Israel Instituteof Technology, Haifa, Israel; 5 Center
for Theoretical Physics, Polish
Academy of Sciences, Warsaw,
Poland; 6 Institute for Quantum
Optics and Quantum Information,
Austrian Academy of Sciences,
Innsbruck, Austria; 7 Institute for
Theoretical Physics, University of
Innsbruck, Innsbruck, Austria;
8
ICREA - Institución Catalana deInvestigación y Estudios Avanzados,
Barcelona, Spain
We report on the new non–linear
optical signatures of quantum phasetransitions in the high-temperature
superconductor YBCO, observed
through high harmonic generation
spectroscopy.
CD-7.2 WED

8:45

Bright phase-stable waveforms
covering the entire infraredmolecular fingerprint region∙H. Kassab1 , S. Gröbmeyer2 , C.
Hofer1,3,4 , W. Schweinberger2,3 ,P. Steinleitner1,2 , M. Högner1 , T.
Amotchkina1 , M. Knorr5 , R. Huber5 ,F. Krausz1,2,3 , N. Karpowicz1,2 , andI. Pupeza1,2,6 ; 1 Max Planck InstituteCLEO

Room 14b ICM

Room Osterseen ICM®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

CH-5: Optical frequency
combs

EE-1: Ultrafast spectroscopy
of solids

CF-6: New trends inpost-compression I

CI-1: Fibers for telecommunications

CJ-2: Beam combination offiber lasers and amplifiers

EB-6: Integrated quantum
opticsChair: Arnaud Mussot, University ofLille, France

Chair:
Lenard Vamos,
Castelldefels, Spain

ICFO,

Chair:
Oleg Pronin, HelmutSchmidt-Universität / Universität
der Bundeswehr Hamburg, Germany

Chair: Katarzyna Krupa, Instituteof Physical Chemistry PAS, Warsaw,
PolandChair: Liang Dong, Clemson University, Clemson, USA

Chair: Nicolas Fabre, Telecom Paris,
FranceCH-5.1 WED (Tutorial)

EE-1.1 WED

8:30

CF-6.1 WED

CI-1.1 WED

CJ-2.1 WED (Invited)EB-6.1 WED

8:30

Optical frequency comb applications beyond frequency metrology
using versatile control of opticalwaves∙K. Minoshima; The University ofElectro-Communications,
Chofu,
Japan
Optical frequency comb provides
powerful tools in broad area using
its versatile phase controllability. In
this tutorial, our recent works on
various metrology applications suchas highly functional spectroscopy,
quantum optics, and imaging arepresented.

8:30

8:30

Following phase transition in
niobium dioxide by time-resolved
high-harmonic spectroscopy∙Z. Nie1 , L. Guery1 , P. Juergens1,2 ,and P. Kraus1,3 ; 1 Advanced Research Center for Nanolithography,
Amsterdam, Netherlands; 2 MaxBorn-Institute for Nonlinear Optics
and Short Pulse Spectroscopy, Berlin,
Germany; 3 Department of Physics
and Astronomy, and LaserLaB,
Vrije Universiteit,
Amsterdam,
Netherlands
Robust experimental evidence ofultrafast insulator-to-metal transition in niobium dioxide has beenfound in time-resolved high harmonic spectroscopy and such sensitive methodology based on extreme
nonlinearity could be generalized toany phase transitions.

Low-Noise Tunable Source for
Stimulated Raman Scattering
Imaging∙I. Martin1,3 , S. Bux1 , T. Sylvestre2 ,S. Metais3 , H. Rigneault3 , and N.
Forget1 ; 1 Fastlite, Antibes, France;
2
Institut FEMTO-ST, Besançon,France; 3 Institut Fresnel, Marseille,
FranceWe present a low-noise tunable(0.78-1μm) OPA at 40 MHz,pumped by a Kerrlens mode-locked
Ytterbium laser. The RIN is shotnoise-limited (-160 dB/Hz) at~3MHz and we were able to acquire
SRS images.

The Impact Of Zero-Dispersion
Wavelength Fluctuations In A
Parametric Amplifier Based On
Dual Core Fibers
V. Ribeiro1 , M. Shi2 , and ∙A.M.
Perego2 ; 1 Kets Quantum Security
Ltd, Bristol, United Kingdom;
2
Aston University, Birmingham,
United Kingdom
We present a theory of the zerodispersion wavelength fluctuations
impact on a dual core fiber parametric amplifier gain, demonstrating
agreement with Montecarlo simulations and superior resilience compared to standard single core fiber
optical parametric amplifiers.

EE-1.2 WED

CF-6.2 WED

CI-1.2 WED

8:45

Signature of diabatic transition ofdressed excitons in monolayer
WSe2∙K. Uchida1 , S. Kusaba1 , K. Nagai1 ,T.N. Ikeda2 , and K. Tanaka1 ;1
Department of Physics, Kyoto
University, Kyoto, Japan; 2 Instituteof Solid State Physics, University ofTokyo, Kashiwa, Japan

8:45

Taming light bullets in thehollow-fiber compressor∙G. Steinmeyer1 , T. Nagy1 , I.
Babushkin2 , and C. Mei3 ; 1 MaxBorn-Institut, Berlin, Germany;
2
Institute of Quantum Optics,
Leibniz University , Hannover,Germany; 3 University of Science andTechnology, Beijing, China

8:45

Generalized angle-OAM Talbot
effect in ring-core fibers∙M. Eriksson1 , J. Hu2 , S. Gigan2 ,and R. Fickler1 ; 1 Physics Unit, Photonics Laboratory, Tampere University, Tampere, Finland; 2 Laboratoire
Kastler Brossel, ENS-Université PSL,
CNRS, Sorbonne Université, Collège
de France, Paris, France

109

8:30

Coherently combined high power
multicore fibers∙J. Limpert; Institute of Applied
Physics, University Jena, Jena,
Germany; Helmholtz-Institute Jena,
Jena, Germany; 3Fraunhofer Institute for Applied Optics and Precision
Engineering, Jena, Germany
The basics, the progress and the perspectives of the coherent combination of amplifying multicore fibers
with high core count will be reviewed.

8:30

High-fidelity on chip four-photon
GHZ states∙M. Pont1 , G. Corrielli2 , A.
Fyrillas3 , I. Agresti4,5 , G. Carvacho4 ,N. Maring3 , P.-E. Emeriau3 , F.
Ceccarelli2 , R. Albiero2 , P.H.D.
Ferreira2,6 , N. Somaschi3 , J.
Senellart3 ,M. Morassi1 ,A.
1Lemaitre , I. Sagnes1 , P. Senellart1 ,F. Sciarrino4 , M. Liscidini7 , N.
Belabas1 , and R. Osellame2 ; 1 C2N,
CNRS, Universite Paris-Saclay, UMR
9001, Palaiseau, France; 2 IFN-CNR,
Milano, Italy; 3 Quandela, Massy,
France; 4 Dipartimento di Fisica,
Sapienza Universita di Roma, Rome,
Italy; 5 University of Vienna, Facultyof Physics, Vienna, Austria; 6 Physics
Department, Federal Universityof Sao Carlos, Sao Carlos, Brazil;
7
Dipartimento di Fisica, Universita
di Pavia, Pavia, Italy
We use a quantum-dot based singlephoton source to demonstrate ahigh-fidelity high-rate generation of
4-photon quadri-partite GHZ stateswith an integrated photonic circuit.
Our experimental platform paves
the way towards photonic intermediate scale quantum computation.

EB-6.2 WED

8:45

High bandwidth homodyne
detection in a monolithic ePIC
process
J. Frazer, J.F. Tasker, ∙G. Ferranti,
and J.C.F. Matthews; Quantum Engineering Technology Labs, H. H. Wills
Physics Laboratory and Department
of Electrical & Electronic Engineering, University of Bristol, Bristol,CLEO

Room 1 ICM

Room 4a ICM

Bragg-gratings is inscribed with asingle-uniform phase-mask at thesame spot. These gratings are inscribed with a femtosecond laser,
while the wavelength tunability isachieved by defocusing and phasemask movement.

CM-7.3 WED

9:00

High-efficiency fibre couplingfrom laser-written waveguides
using partially overlapping
multi-pass inscription∙M. Ehrhardt, M. Heinrich, and A.
Szameit; Institute for Physics, University of Rostock, Rostock, Germany
We shape the mode field of femtosecond laser-written waveguides
in fused silica via the partial overlap of multiple inscription passes.
Judicious tuning of exposure parameters facilitates near-unity mode
overlap and coupling to standard
single-mode fibers.

CK-4.2 WED

9:00

A Photonic Integrated CircuitBased Erbium-doped Waveguide
Amplifier∙Y. Liu1,2 , Z. Qiu1,2 , X. Ji1,2 ,A. Lukashchuk1,2 , J. He1,2 , J.
Riemensberger1,2 , M. Hafermann3 ,R.N. Wang1,2 , J. Liu1,2 , C. Ronning3 ,and T.J. Kippenberg1,2 ; 1 Instituteof Physics, Swiss Federal Instituteof Technology Lausanne (EPFL),
Lausanne, Switzerland; 2 Centerfor Quantum Science and Engineering,Swiss
FederalInstituteof Technology Lausanne (EPFL),
Lausanne, Switzerland; 3 Institute ofSolid State Physics, Friedrich Schiller
University Jena, Jena, Germany
We demonstrate an Erbium-doped
waveguide amplifier by erbium ion
implantation in Si3 N4 photonic integrated circuits, achieving 145 mW
on-chip output power and morethan 30 dB small-signal gain, on parwith Erbium-doped fiber amplifiers.

®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 4b ICM

Room 13a ICM

Institutefor
Multidisciplinary
Sciences, Göttingen, Germany; 2 4th
Physical Institute, University of
Göttingen, Göttingen, Germany;3
Institute of Physics, Swiss Federal
Institute of Technology Lausanne(EPFL), Lausanne, Switzerland;
4
Center for Quantum Science andEngineering, Swiss Federal Instituteof Technology Lausanne (EPFL),
Lausanne, Switzerland
We couple free electrons to the optical modes of a high-Q photonic
chip-based microresonator. Inelastic scattering leads to the generation of single photons in the cavity
modes, correlated to an energy-lossof the electrons.

Institute for Laser Technology
ILT, Aachen, Germany; 2 Leibniz
Institute of Atmospheric Physics IAP,
Kühlungsborn, Germany
We present the design and performance of four prototypes of narrowbandwidth emitters based on diodepumped Alexandrite lasers for atmospheric Doppler-Mie, -Rayleighand -resonance lidars. Furthermore,
first results for efficient frequencydoubling into UV are presented.

EG-6.3 WED

CA-6.3 WED

9:00

Midinfrared optical force for
sorting materials depending on
their chemical structures
Y.A. Darmawan1 , T. Goto1 , T.
Yanagishima2 , T. Fuji1 , and ∙T.
Kudo1 ; 1 Laser Science Laboratory,
Toyota Technological Institute,
Nagoya, Japan; 2 Department of
Physics, Graduate School of Science,
Kyoto University, Kyoto, Japan
Optical force is resonantly enhanced
when a midinfrared quantum cascade laser excites molecular vibrational modes of target materials. We
experimentally discovered that particles are sorted accordingly to theirchemical structures using a midinfrared optical force.

Room 13b ICM

9:00

375-400nm UV Generation via an
Alexandrite laser and Zn-indiffused MgO-doped PPLN Waveguides∙G. Tawy1 , N. Palomar Davidson1 ,P.L. Mennea1 , G. Churchill1 , L.D.
Wright2 ,R.H.S. Bannerman1 ,P.G.R. Smith1 , J.C. Gates1 , M.J.
Damzen3 , and C.B.E. Gawith1 ;1
Optoelectronics Research Centre,
Southampton, United Kingdom;
2
Covesion Ltd.,Southampton,
United Kingdom; 3 Imperial College
London, London, United Kingdom
We present the very first demonstration of a widely tunable UV laser
source from an Alexandrite laser using second-harmonic-generation in
PPLN waveguides. Waveguide efficiency, spectra and mode profiles
are presented.

110

Room 14a ICM
of Quantum Optics, Garching,
Germany; 2 Ludwig Maximilian
University Munich,
Garching,
Germany; 3 Center for MolecularFingerprinting, Budapest, Hungary; 4 Quantum Matter Institute,
University of British Columbia,
Vancouver, Canada; 5 . Departmentof Physics, University of Regensburg,
Regensburg, Germany; 6 Leibniz
Institute of Photonic Technology- Member of the research alliance“Leibniz Health Technologies“, Jena,
Germany
Modern Yb-based MHz-repetitionrate lasers readily provide 10fs-scale pulses with 100-W-levelaverage powers. Using such a laser,
we simultaneously cover the entire
infrared molecular fingerprint
region with passively-phase-stable
130-mW-average-power
waveforms, via multi-crystal intrapulse
difference-frequency mixing.

JSI-1.2 WED

9:00

All X-ray four-wave mixing on agas phase sample∙A.S. Morillo-Candas1 , A. AlHaddad1 ,S. Augustin1 ,A.
Cannizzo2 , Y. Deng1 , T. Feurer2 ,J. Knurr1,3 , C. Ott4 , E. Prat1 ,M. Rebholz4 , A. Sarracini1 , K.
Schnorr1 , Z. Sun1 , X. Xie1 , N.
Yang1,3 , S. Zedane1 , H. Zhang1,3 ,T. Pfeifer4 , C. Bostedt1,3 , and G.
Knopp1 ; 1 Paul Scherrer Institute,Villigen, Switzerland; 2 Institute ofApplied Physics, Bern, Switzerland;
3
Ecole Polytechnique Federal deLausanne , Lausanne, Switzerland;
4
Max Planck Institut für Kernphysik,
Heidelberg, Germany
An all X-ray - four wave mixing(FWM) experiment has been successfully demonstrated at the SwissFEL free electron laser in an atomicgas (Ne) by using a “folded BOX”
configuration, which ensures temporal and spatial overlap of the Xray beams.

CD-7.3 WED

9:00

Broadband Dual-Comb Spectroscopy in the Near-Ultraviolet
Spectral Region∙L. Fürst, A. Kirchner, A. Eber,
F. Siegrist, R. di Vora, and B.
Bernhardt; Institute of Experimental
Physics, Graz, Austria
We demonstrate direct ultraviolet
dual-comb spectroscopy using two
broadened frequency-tripled frequency comb outputs. Absorption
spectroscopy of formaldehyde wasaccomplished with complete state
resolution at 100 μs acquisition
time and 133 GHz resolution.

CLEO

Room 14b ICM®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room Osterseen ICM

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

We observed the signature of diabatic transition between different
Floquet eigenstates in monolayer
WSe2 by irradiating with intense
mid-infrared light.

Spatio-temporal soliton formation
is discussed in a fully analytical approach, solving the eigenvalue problem of the nonlinear Schrödinger
equation in the Fourier domain. Resulting scaling rules and design considerations are presented.

We show the first experimental
demonstration of the generalized
angle-OAM Talbot effect in ringcore fibers, combining the selfimaging effects in both angular and
OAM domains, which may enablenovel quantum and classical information manipulation in the future.

EE-1.3 WED

CF-6.3 WED

CI-1.3 WED (Invited)

9:00

Direct signatures of light-driven
bands in ultrafast nonlinear
optical excitations∙A. Galler, A. Rubio, and O. Neufeld;
Max Planck Institute for the Structure and Dynamics of Matter, Hamburg, Germany
We theoretically show that strongfield nonlinear-optical transitions
in solids, which are the basis fora plethora of physical phenomena, map the structure of the Floquet light-dressed electronic bands,
opening new possibilities for ultrafast spectroscopy.

9:00

Generation of Tuneable Vacuum
Ultraviolet Pulses Through Resonant Dispersive Wave Emission
With an Ytterbium-based Laser∙C. Brahms and J.C. Travers; HeriotWatt University, Edinburgh, United
Kingdom
We generate tuneable ultrafast
pulses in the vacuum ultraviolet
down to 145 nm through resonant dispersive wave emission
in a gas-filled hollow-core fibre
pumped by compressed pulses
from a commercial high-powerytterbium-based drive laser.

9:00

Optical Communications: a
Hollow Future ahead?
∙F. Poletti1,2 , G. Jasion1 , E.
Numkam Fokoua1,2 , H. Sakr1,2 ,and I. Davidson1 ; 1 Optoelectronics
Research Centre, University ofSouthampton,
Southampton,
2
United Kingdom;
Lumenisity,
Southampton, United Kingdom
Hollow core fibre technology has
progressed very rapidly in recent
years, to the point that its optical performance has reached levels compatible with those requiredfor optical communications. We
will review state-of-the-art and future prospects.

111

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)
United Kingdom
We demonstrate a monolithic homodyne detector with a 3 dB bandwidth of 19.8 GHz and shot noise
clearance of 16 dB. This result highlights the potential of monolithic integration to improve performance ofdevices for quantum technologies.

CJ-2.2 WED

9:00

32 mJ, 158 fs pulses from a coherently combined ytterbiumdoped fiber laser system∙H. Stark1,2 , M. Benner1 , J. Buldt1 ,A. Klenke1,3,4 , and J. Limpert1,2,3,4 ;1Friedrich Schiller University Jena,
Abbe Center of Photonics, Institute of Applied Physics, Jena, Germany; 2 Fraunhofer Institute for Applied Optics and Precision Engineering, Jena, Germany; 3 HelmholtzInstitute Jena, Jena, Germany; 4 GSI
Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
We present a high-energy fiber
chirped-pulse amplification laser
system based on spatial and temporal coherent combination of 128
pulse replicas. A pulse energy of
32 mJ at 158 fs pulse duration and
20 kHz repetition rate is achieved.

EB-6.3 WED

9:00

Quantum enhanced integrated
single photon nonlinear interferometer∙K.-H. Luo, M. Santandrea, M. Stefszky, H. Herrmann, and C. Silberhorn; Integrated Quantum Optics
Group, Institute for Photonic Quantum Systems (PhoQS), Paderborn
University, Paderborn, Germany
We have experimentally studied an
integrated nonlinear SU(1,1) interferometer at the single photon level.
The Fisher information deduced
from interference fringes of singles
reveals quantum advantage even ina lossy device.

CLEO

Room 1 ICM
CM-7.4 WEDRoom 4a ICM
9:15

CK-4.3 WED®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 4b ICM
9:15

EG-6.4 WEDRoom 13a ICM
9:15

CA-6.4 WEDRoom 13b ICM
9:15

JSI-1.3 WEDRoom 14a ICM
9:15

CD-7.4 WED

9:15

DUV laser written gratings onzinc doped lithium niobate waveguides∙R.H.S. Bannerman1 , J.W. Field1 ,Q.S. Ahmed1 , P.C. Gow1 , J.C. Gates1 ,P.G.R. Smith1 , and C.B.E. Gawith1,2 ;1Optoelectronics Research Centre, University of Southampton,
Southampton, United Kingdom;
2
Covesion Ltd.,Southampton,
United Kingdom
Gratings are fabricated on 40mm
long single-mode zinc-indiffusedridge PPLN waveguides using a
focused holographic process and ananosecond pulsed 213nm laser.
Damage-free gratings are madewith fluences from 30 mJ/cm2 to
6 kJ/cm2 .

Integrated Germanium-on-Silicon Ring Resonator with HighQ-factor in the Mid-Infrared∙R. Armand1 , M. Perestjuk1,2 ,A. Della Torre1 , M. Sinobad1 ,A. Mitchell2 , A. Boes2,3 , J.-M.
Hartmann4 , J.-M. Fedeli4 , V.
Reboud4 , C. Monat1 , and C. Grillet1 ;1
Institut des Nanotechnologies deLyon, Ecully, France; 2 RMIT, Melbourne, Australia; 3 The Universityof Adelaide, Adelaide, Australia;
4
CEA-Leti, Grenoble, France
We report a high-Q ring resonator in the mid-infrared in a
germanium-on-silicon chip-based
platform. The side-coupled ringexhibits a loaded Q-factor of
154,000 at the operating wavelengtharound 4.18 μm.

Accurate transfer of individual
nanoparticles onto single
photonic nanostructures∙J. Redolat1 , M. Camarena1 , A.
Griol1 , M. Kovylina1 , A. Xomalis2,3 ,J. Baumberg2 , A. Martinez1 , and
E. Pinilla1 ; 1 Universitat Politècnica de València, Nanophotonics
Technology
center.,Valencia,
2
Spain;
NanoPhotonics Centre,
Cavendish Laboratory. Universityof Cambridge, Cambridge, United
Kingdom; 3 Empa, Swiss Federal
Laboratories for Materials Scienceand Technology, , Thun, Switzerland
We present a reproducible, singlestep, and cost-effective method forthe controlled nanopositioning of
single metallic nanoparticles (NPs)onto lithographically fabricatedphotonic nanostructures with
sub-micron accuracy.

Deep-red laser operation ofcleaved single-crystal plates of
Eu:CsGd(MoO4)2 molybdate∙A. Baillard1 , P. Loiko1 , A. Pavlyuk2 ,A. Braud1 , and P. Camy1 ; 1 Centre deRecherche sur les Ions, les Matériaux
et la Photonique (CIMAP), UMR
6252 CEA-CNRS-ENSICAEN, Université de Caen Normandie, Caen,
France; 2 A.V. Nikolaev Instituteof Inorganic Chemistry, Siberian
Branch of Russian Academy of
Sciences, Novosibirsk, RussiaA
deep-red
17at.%
Eu:CsGd(MoO4)2 laser basedon cleaved single-crystal plates
generates 212 mW at 703.1 nm(the 5D0→7F4 transition) with aslope efficiency of 30.1%, a laser
threshold of 51 mW and a linear
polarization.

Nanoscale Transient Magnetization Dynamics With Extreme
Ultraviolet Transient Gratings∙L. Foglia; Elettra Sincrotrone Trieste
S.C.p. A. , Trieste, Italy
We review the recent advanceson investigating and controlling
nanoscale ultrafast magnetization
dynamics using EUV transient
gratings, which is paramount forunderstanding
light-controlled
ultrafast magnetic data processing
and storage applications.

Spectroscopy of Heteronuclear
Xenon-noble Gas Dimers - Towards Bose-Einstein Condensation of Vacuum-UV Photons∙E. Boltersdorf, T. vom Hövel, F.
Vewinger, and M. Weitz; Institut fürAngewandte Physik, Bonn, Germany
We report experimental work aimed
at extending the applicability of
Bose-Einstein-condensation of photons from current visible spectral
range experiments to the vacuumultraviolet (100nm-200nm) regime.
For this, spectroscopic experiments
investigating dense xenon-noble gas
mixtures are presented.

CM-7.5 WED

CK-4.4 WED

EG-6.5 WED

CA-6.5 WED

JSI-1.4 WED

CD-7.5 WED

9:30

Ultrafast Laser Written Waveguide Chips for Quantum Applications∙B. Sun1 , A. Sotirova2 , V.D. Cruz2 ,C. Ballance2 , E. Mer3 , R.B. Patel3 ,I.A. Walmsley3 , and M.J. Booth1,4 ;1Department of Engineering Science,
University of Oxford, Oxford ,2
United Kingdom;
Departmentof Physics, University of Oxford,
Oxford , United Kingdom; 3 Ultrafast
Quantum Optics group, Departmentof Physics, Imperial College London,
London, United Kingdom; 4 Erlangen
Graduate School in Advanced
OpticalTechnologies(SAOT),Friedrich-Alexander-University
Erlangen-Nürnberg,
Erlangen,Germany
Waveguide-based chips created by
SPIM-WG technique enabled several new functionalities in quantum applications. Scalable devices
with high index contrast, closely
stacked waveguide array and low
crosstalk demonstrated applicationin trapped ion quantum computation.

9:30

Towards on-chip ultrafast pulse
amplification∙M.A. Gaafar1 , K. Wang2 , M.
Ludwig1 , T. Wildi1 , M. Sinobad1 ,J. Lorenzen1 , H. Francis3 , M.
Geiselmann3 , F.X. Kärtner1,4 , S.M.
Garicia-Blanco2 , N. Singh1 , andT. Herr1,4 ; 1 Deutsches ElektronSynchrotron DESY, Notkestraße 85,
Hamburg, Germany; 2 Integrated
Optical Systems, MESA+ Institutefor Nanotechnology,
Universityof Twente, 7500AE, Enschede,
Netherlands; 3 LIGENTEC SA, EPFL
Innovation Par L, Chemin de laDent-d’Oche 1BB, Switzerland CH1024 Ecublen, Ecublen, Switzerland;
4
Physics Department, Universität
Hamburg, Luruper Chaussee 149,
22761, Hamburg, Germany
Here we demonstrate a broadband,large mode area thulium-based
integrated amplifier with tailoredgroup-velocity dispersion.
Wemeasure up to 10 dB signal pulse
net gain at 1820 nm inside a 5
cm-long waveguide.

9:30

Recoil and Quantum Effects in theInteraction of Low-Energy Free
Electrons with Illuminated Planar
Surfaces∙A.P. Synanidis1 , P.A.D. Gonçalves1 ,C. Ropers2 , and F.J. García de
Abajo1,3 ; 1 ICFO – Institut deCiències Fotòniques, The Barcelona
Institute of Science and Technology,
08860 Castelldefels (Barcelona),
Spain; 2 Max Planck Institute forMultidisciplinary Sciences, Germany, 37077 Göttingen, Germany;
3
ICREA – Institució Catalana
de Recerca i Estudis Avançats,Passeig Lluís Companys 23, 08010
Barcelona, Spain
We present a theoretical framework
to describe electron-light-matter interactions for low-energy electrons,
encompassing quantum and recoil
effects, and allowing us to predict
exciting phenomena during electron
scattering from illuminated planar
surfaces and surface optical modes.

9:30

Acousto-optic Q-switched Alexandrite Laser with Wavelength
Tuning and Second Harmonic
Generation∙M. Liang1 , A. Minassian2 , and
M. Damzen1 ; 1 Imperial College
London, London, United Kingdom;
2
Unilase, London, United Kingdom
We present the first ever AcoustoOptic Q-switched Alexandrite laser.
We demonstrate 290 microJoules
pulse energy at 5 kHz, wavelengthtuning from 734 – 783 nm, and second harmonic generation in LBO(and BBO) crystal to generate tunable ultraviolet.

112

9:30

Time Resolved Hard X-ray/
Optical Transient Grating
Spectroscopy on a Liquid Jet
A.S. Morillo-Candas1 , A. AlHaddad1 , S. Augustin1 , C. Bacellar1 ,A. Cannizzo2 , C. Cirelli1 , D.
Fainozzi3 , T. Feurer2 , P. Johnson1 ,T. Mamyrbayev1 , A. Maznev4 , K.
Nelson4 , K. Schnorr1 , C. Svetina5 ,J. Vila-Comamala1 , M. Chergui6 ,C. Bostedt1 , and ∙G. Knopp1,6 ;1Paul Scherrer Institute, Villigen ,Switzerland; 2 Institute of Applied
Physics, University of Bern, Bern,
3
Switzerland;
Elettra-Sincrotrone
Trieste, Trieste, Italy; 4 Massachusetts
Institute of Technology, Cambridge,
5
USA;
IMDEA
nanociencia,
Madrid, Spain; 6 École polytechnique
fédéral de Lausanne, Lausanne,
Switzerland
We demonstrate for the first time
the feasibility of hard X-ray/opticaltransient grating spectroscopy (XOTG) on a liquid jet system at SwissFEL and use it for the investigation of the chemical dynamics of anaqueous ferrioxalate solution.

9:30

Harmonic generation from silicon
membranes at visible and ultraviolet wavelengths∙L. Rodríguez1 , K. Hallman2 ,J. Trull1 , C. Cojocaru1 , M.A.
N. Akozbek4 ,R.
Vincenti3 ,Vilaseca1 ,and M. Scalora5 ;1
Department of Physics, Universitat
Politècnica de Catalunya, Terrassa,
Spain; 2 PeopleTech, Inc., Huntsville,
USA; 3 Department of Information
Engineering - University of Brescia,
Brescia, Italy; 4 US Army Space& Missile Defense Command,
Tech Center, Redstone Arsenal,
Huntsville, USA; 5 DEVCOM Aviation and Missile Center, Redstone
Arsenal, Huntsville, USA
We report an experimentaltheoretical study of harmonic
generation in silicon nanomembranes that allows us to determine
physical properties of the material.
With this, we are able to predict
harmonic efficiencies in more
complex structures.

CLEO

Room 14b ICM

Room Osterseen ICM
EE-1.4 WED

CH-5.2 WED

9:30

High speed mid-infrared dual
comb spectroscopy with a single
optical parametric oscillator∙D. Long1 , M. Cich2 , C. Mathurin3 ,A. Heiniger2 , G. Mathews3 , A.
Frymire3 , and G. Rieker3 ; 1 National
Institute of Standards and Technology , Gaithersburg, MD, USA;
2
Toptica Photonics, Pittsford, NY,
USA; 3 Precision Laser Diagnostics
Laboratory, University of Colorado,
Boulder, CO , USA
A pair of mid-infrared frequency
combs were simultaneously generated in a single optical parametric oscillator. The resulting combs
exhibited high power, high mutual
coherence, and allowed for quantitative spectroscopy on nanosecond
timescales.

9:15

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)CF-6.4 WEDRoom 6 Hall B3 (B32)

9:15

Landau Transitions and BerryCurvature Effects in Optically
Induced Anomalous Hall Current
C. Dresler1 , ∙S. Priyadarshi1 ,J. Hübner2 , and M. Bieler1 ;1Physikalisch-Technische
Bundesanstalt, Braunschweig, Germany;
2
Institutfür
Festkörperphysik,
Leibniz
Universität
Hannover,Hannover, Germany
We induce anomalous Hall currents
in bulk GaAs by ultrafast opticalexcitation of Landau levels. An
analysis of the resulting THz radiation suggests that both, Berry curvature and scattering contribute to theAHC.

GW-scale pulse compression at
multi-MHz-rate via all-bulk
quasi-waveguide spectral
broadening∙S. Gröbmeyer1 , K. Fritsch1,2 , V.
Pervak1 , F. Krausz1,3 , and K.F.
1
Mak3 ;
Ludwig-MaximiliansUniversität München, München,2
Germany;
Helmut-SchmidtUniversität/Universität der Bundeswehr Hamburg,
Hamburg,
Germany; 3 Max-Planck-Institut für
Quantenoptik, Garching, Germany
We present spectral broadening via
a distributed quasi-waveguide, withwhich we generated 10.8 fs pulses at
100 W of average power and 0.64
GW of peak power with excellent
temporal and spatial fidelity.

EE-1.5 WED

CF-6.5 WED

9:30

Probing ultrafast carrier dynamics in perovskite wide bandgap
oxides∙H.-Y. Chen1,2,3 , R. Versteeg1 ,P. Marsik4 , and M. Chergui1,3 ;1Laboratory of Ultrafast Spectroscopy(LSU), École polytechnique
fédérale de Lausanne (EPFL),
Lausanne, Switzerland; 2 Laboratory
for Ultrafast Microscopy andElectron Scattering(LUMES), École
polytechnique fédérale de Lausanne(EPFL), Lausanne, Switzerland;
3
Lausanne Centre for Ultrafast Science (LACUS), École polytechnique
fédérale de Lausanne (EPFL), Lausanne, Switzerland; 4 Departmentof Physics, Faculty of Science andMedicine, University of Fribourg,
Fribourg, Switzerland
We studied wide bandgap perovskite oxides by ultrafast transientreflectivity. Clear excitonic bleaching and enhancement as wellas giant acoustic phonon wasobserved. A hot carrier coolinglifetime below 1 ps was revealed.

⋅ Wednesday 28 June 2023

9:30

Generation of picosecond pulses
from tapered laser diodes withover 40 W peak power at wavelengths of 780 nm and 830 nm∙S. Wohlfeil, H. Christopher, J.
Fricke, P. Della Casa, A. Maaßdorf,
H. Wenzel, A. Knigge, and G.
Tränkle; Ferdinand-Braun-Institut(FBH), Berlin, Germany
We present two monolithic diodelasers with tapered gain sections
emitting at 780 nm and 830 nm.
Picosecond pulses with over 40 W
peak power are measured in passivemode-locking operation.

Room 7 Hall A1 (A11)CJ-2.3 WED

CI-1.4 WED

9:30

High efficiency interface between
multi-mode and single-mode
fibers∙O. korichi,
M. Hiekkamäki,
and R. fickler; Tampere University,Photonics Laboratory, Physics
Unit, Tampere, Finland
We present a method capable ofachieving MMF–SMF coupling efficiencies from 30% to 70% using a multi-plane light conversion
scheme (MPLC).

113

9:15

Room 8 Hall A1 (A12)EB-6.4 WED

9:15

Coherent beam combining andtelecom modulation: reciprocal
impact∙P. Pichon1 , B. Rouzé1 , M. Gay2 ,L. Bramerie2 , L. Lombard1 , and
A. Durécu1 ; 1 DOTA, ONERA,
Université Paris Saclay, Palaiseau,
France; 2 Institut Foton, CNRSUMR 6082, Université de Rennes,
Lannion, FranceThis work explores the compatibility
between 1) coherent beam combining in MOPA configuration using
frequency-tagging locking and 2) a
telecom signal relying on either amplitude modulation (NRZ) or phasemodulation (DPSK).

Integrated photonics for quantum
communication on a CubeSat∙J. Pudelko1,2 , Ö. Bayraktar1,2 ,I. Khan1,2 , W. Boxleitner3 , S.
Petscharnig3 , C. Pacher3 , G.
Leuchs1,2 , and C. Marquardt1,2 ;1Max-Planck-Institutefor
theScience of Light, Erlangen, Germany;
2
Friedrich-Alexander-Universität
Erlangen-Nürnberg,
Erlangen,Germany; 3 AIT Austrian Instituteof Technology GmbH, Center for
Digital & Safety, Vienna, Austria
We present a photonic integrated
CubeSat payload consisting of asender for weak coherent states anda quantum random number generator, intended to demonstrate two
important building blocks for satellite based quantum communicationfrom space.

CJ-2.4 WED

EB-6.5 WED

9:30

Optimized multicore fiber designs
for coherent combination∙C. Jauregui 1 , A. Klenke1,2,3 ,A. Steinkopff1 , C. Aleshire1 , M.
Bahri1 , J. Nold4 , S. Kuhn4 , N.
Haarlammert4 , T. Schreiber4 , and J.
Limpert1,2,3,4 ; 1 Institute of Applied
Phyiscs, Friedrich-Schiller University
Jena, Jena, Germany; 2 HelmholtzInstitute Jena, Jena, Germany; 3 GSI
Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany;
4
Fraunhofer Institute for Applied
Optics and Precision Engineering,
Jena, Germany
The interconnection between the
different design parameters for multicore fibersis presented andguidelines to obtain optimized multicore fiber designs for high-power,
coherently-combined systems are
discussed.

9:30

Nitrogen-vacancy centres integrated with foundry silicon
nitride photonics∙H.-C. Weng, J. Monroy-Ruz, J.C.F.
Matthews, J.G. Rarity, K.C. Balram,
and J.A. Smith; Quantum Engineering Technology Labs, H. H. Wills
Physics Laboratory and Department
of Electrical and Electronic Engineering, University of Bristol, Bristol,
United Kingdom
We demonstrate the coupling of NV
centres in nanodiamond to foundry
optimised silicon nitride photonics
in an all-integrated device. The NV
centres show a fluorescence lifetimeof order 10 ns through the waveguide channel.

CLEO

Room 1 ICM
CM-7.6 WEDRoom 4a ICM
9:45

CK-4.5 WED®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 4b ICM
9:45

EG-6.6 WEDRoom 13a ICM
9:45

CA-6.6 WEDRoom 13b ICM
9:45

JSI-1.5 WEDRoom 14a ICM
9:45

CD-7.6 WED

9:45

244nm Direct UV Written
Gratings in SiNx layers∙A.I. Flint, G. De Paoli, S.T. Ilie,
R.H.S. Bannerman, P.C. Gow, J.C.
Gates, F.Y. Gardes, and P.G.R.
Smith; University of Southampton,
Optoelectronics Research Centre
Southampton, Southampton, United
KingdomInterferometric
244nm
laser
inscription with is used to write
550nm period holographic gratings
into SiNx layers. We present thecharacterisation of the fabrication
process and optimisation grating
response in etched and diced
waveguides.

A lithographically defined quantum dot with simultaneous subwavelength confinement of light∙G. Kountouris, L. Vestergaard, A.S.
Darket, J. Mørk, and P.T. Kristensen;
Technical University of Denmark,Kongens Lyngby, Denmark
We present a design for deterministic fabrication of a lithographicallydefined quantum dot in a dielectric cavity with deep sub-wavelength
confinement of light and characterize the performance by quantifying
the achievable radiative rate and efficiency.

Moulding optical tweezers for 3D
enhanced trapping∙C. Sharp1 , U.G. Butaite1 , M.
Horodynski2 , G.M. Gibson3 , S.
Rotter2 , J.M. Taylor3 , and D.B.
Phillips1 ; 1 Department of Physics
and Astronomy, University of Exeter,
Exeter, United Kingdom; 2 Institutefor Theoretical Physics, Vienna
University of Technology, Vienna,
Austria; 3 School of Physics andAstronomy, University of Glasgow,
Glasgow, United Kingdom
We experimentally demonstrate 3D
enhanced optical trapping. For constant laser power, our enhanced
optical traps reduce the motion a
trapped particle by an order ofmagnitude, when compared with aGaussian beam.

Detailed optomechanical designof a 150 mJ single frequency UVlaser for the Aeolus-2 mission∙D. Esser1 , M. Giesberts1 , B.
Erben1 , S. Nyga1 , R. Kasemann1 ,C. Wührer2 , S. Hahn2 , M.
Leyendecker1 , J. Eßer1 , W. Wirz1 ,S. Klein1 , M. Traub1 , J. Klein1 ,W. Brandenburg1 , M. Höfer1 , D.
Mohr1 , L. Pérez Prieto2 , and H.-D.
Hoffmann1 ; 1 Fraunhofer Institut f.
Lasertechnik, Aachen, Germany;
2
Airbus Defense & Space GmbH,
München, Germany
The detailed design of a demonstrator for a laser transmitter for ESA’s
Aeolus-2 mission is presented. The
laser is capable to generate 150 mJ
pulses at 355 nm wavelength andbeam propagation factor < 2.

Polarization gratings at the nanoscale: a new tool to study dichroic
samples∙R. Mincigrucci, F. Bencivenga, L.
Foglia, G. Perosa, and C. Masciovecchio; Elettra Sincrotrone Trieste SCpA, Trieste, Italy
We hereby present a new class oftransient gratings that can be generated by two crossed polarized extre
ultraviolet beams. Possible applications to dichroic samples will be discussed.

Mid-infrared Spontaneous andStimulated Raman Scattering in a
Silicon Core Fiber∙M. Huang1 , S. Sun1 , T.S. Saini1 , Q.
Fu1 , L. Xu1 , D. Wu1 , H. Ren2 , L.
Shen3 , T.W. Hawkins4 , J. Ballato4 ,and A.C. Peacock1 ; 1 Optoelectronics
Research Centre, University ofSouthampton, Southampton, United
Kingdom; 2 School of Optoelectronic
Engineering and Instrumentation
Science, Dalian University ofTechnology, Dalian, China; 3 Wuhan
National Laboratory for Optoelectronics, Huazhong University of
Science and Technology, Wuhan,
China; 4 Centre for Optical Materials
Science and Engineering Technologies and Department of Materials
Science and Engineering, Clemson
University, Clemson, USA
Raman scattering beyond 2.2 μm is
measured for the first time in a silicon core fiber. Both spontaneousand stimulated effects are observed,
with a gain of 30 dB achieved via apulsed pump laser.

Room 4a ICM

Room 4b ICM

Room 13a ICM

Room 13b ICM

Room 14a ICM

Room 14b ICM

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

CK-5: Silicon nitride systems
and devices

JSIV-1: Photo(electro)chemistry and desalination

CA-8: High-power lasers andfacilities

JSI-2: X-ray source developments

CD-8: Nonlinear dynamics I

CH-6: Imaging at the nanoscale

Chair: Béatrice Dagens, Université
Paris-Saclay, France

Chair: Giulia Tagliabue, EPFL, Lausanne, Switzerland

Chair: Marc Brunel, Institut FOTON, Université de Rennes, France

Chair: Christoph Bostedt, EPFL,
Lausanne, Switzerland

CK-5.1 WED

10:30

JSIV-1.1 WED (Invited) 10:30

CA-8.1 WED (Invited)

JSI-2.1 WEDRoom-temperature Sputtered
Ultralow-loss Silicon Nitride∙S. Zhang1 , T. Bi1,2 , I. Harder1 , O.
Lohse1 , F. Gannott1 , A. Gumann1 ,Y. Zhang1 , and P. Del’Haye1,2 ;1Max Planck Institute for the
Science of Light, Erlangen, Germany; 2 Department of Physics,
Friedrich-Alexander-Universität
Erlangen-Nürnberg,
Erlangen,Germany
We demonstrate a new process for
integrated silicon nitride photonic
devices based on reactive sputtering. We achieve propagation losses

Plasmonic bimetallic metasurfaces for large-scale solar
Hydrogen production∙E. Cortes; University of Munich(LMU), Munich, Germany
Optimization strategies for the synthesis and design of plasmonic catalysts: from understanding mechanistic details at the single particle
level to the fabrication of cm2 supercrystals towards large-scale Hydrogen production.

High-Power Q-switched Near
Infrared Cryogenic Lasers∙M. Ganija1,2 , K. Boyd1,2 , and J.
Munch1 ; 1 CADR-USPL, Faculty of
SET, The University of Adelaide, Adelaide, Australia; 2 Directed Energy
Technologies and Effects, Defence
Science and Technology Group, Adelaide, Australia
We report diffraction limited
beam quality, continuous andpulsed Ho:YAG at 80 % efficiency
with respect to pump power. We
demonstrated average powers above

10:30

10:30

Self-Seeding Systems at theEuropean XFEL
∙G. Geloni; European XFEL, Schenefeld, Germany
On behalf of the FEL R&D group,in this contribution I will discusspresent capabilities and future possibilities of Self-Seeding systems at
the European X-ray Free-Electron
Laser.

114

Chair: François Leo, Université librede Bruxelles, Belgium

CD-8.1 WED (Invited)

10:30

Laser-guided lightning using kHz
filamentation at 1030 nm∙A. Houard1 , P. Walch1 , T. Produit2 ,V. Moreno2 , B. Mahieu1 , A.
Sunjerga3 , C. Herkommer4 , A.
Mostajabi3 , U. Andral2 , Y.-B.
André1 , M. Lozano1 , L. Bizet1 ,M.C. Schroeder2 , G. Schimmel2 , M.
Moret2 , O. Maurice5 , B. Esmiller5 ,K. Michel4 , W. Haas6 , T. Metzger4 ,M. Rubinstein7 ,F. Rachidi3 ,8
V. Cooray , A. Mysyrowicz1 , J.
Kasparian2,9 , and J.-P. Wolf2 ;1
Laboratoire d’Optique Appliquée –Chair: Thomas Chaigne, Fresnel Institute, Marseille, France

CH-6.1 WED

10:30

Multi-Wavelength Ptychography
for Wavefront Sensing∙A. Pelekanidis1,2 , M. Du1 , X. Liu1,2 ,F. Zhang1 , K.S.E. Eikema1,2 , and S.
Witte1,2 ; 1 Advanced Research Center for Nanolithography, Amsterdam,
Netherlands; 2 Department of Physics
and Astronomy, Vrije Universiteit,
Amsterdam, Netherlands
We use multi-wavelength ptychography to reconstruct and characterize extreme ultraviolet wavefronts
generated via high harmonic generation (HHG). We demonstrate theaberration transfer between the fun-

CLEO

Room 14b ICM
CH-5.3 WEDRoom Osterseen ICM
9:45

EE-1.6 WED

9:45

®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)CF-6.6 WEDRoom 6 Hall B3 (B32)

9:45

CI-1.5 WED

9:45

Room 7 Hall A1 (A11)CJ-2.5 WED

9:45

Room 8 Hall A1 (A12)EB-6.6 WED

9:45

Detection Sensitivity of DualComb Spectroscopy∙M. Roiz1 , S. Larnimaa1 , J. Karhu1,2 ,and M. Vainio1,3 ; 1 Department ofChemistry, University of Helsinki,
Helsinki, Finland; 2 Metrology Research Institute, Aalto University, Espoo, Finland; 3 Photonics Laboratory, Physics Unit, Tampere University, Tampere, Finland
We have built a passively coherent
dual-comb spectrometer to study
different aspects that affect detection sensitivity in dual-comb spectroscopy as well as demonstrate possible ways to improve it.

Ultrafast Interband Transition inGold Probed by a Femtosecond
Plasmonic Wavepacket∙B. Lovász1 , P. Sándor1 , Z. Pápa1,2 ,J. Budai2 , and P. Dombi1,2 ; 1 Wigner
Research Centre for Physics, Budapest, Hungary; 2 ELI-ALPS Research Institute, ELI-HU Nonprofit
Kft, Szeged, Hungary
We measured hot electron population decay induced by ultrafast
interband transition in gold witha novel free-space-pump plasmonprobe setup. Hot electrons thermalized with 117-fs and the lattice with
5-ps time constant.

Complete analysis of picosecond
optical pulses by using the offset
frequency intensity modulation∙K. Oguchi1 , S. Nitanai2 , and Y.
Ozeki1 ; 1 Department of ElectricalEngineering and Information Systems, The University of Tokyo, 7-31 Hongo, Bunkyo-ku, Tokyo, Japan;
2
Department of Electrical and Electronic Engineering, The Universityof Tokyo, 7-3-1 Hongo, Bunkyo-ku,
Tokyo, Japan
We propose a method of characterizing picosecond optical pulses
using offset-frequency intensity
modulation and spectral measurement. We experimentally measure
the chirp of picosecond Ti:sapphirelaser pulses, which was difficult
to be characterized by previous
methods.

Proposal for Multiport Photon
Routing using Photonic Crystal
Cavity Phase Shifters∙M. Heuck; Technical University ofDenmark, Kgs. Lyngby, Denmark
We propose compact multiportphoton routers based on static mixing circuits and dynamic photonic
crystal cavity phase shifters. We
discuss optimized mixing circuits
and sensitivity to imperfections for
implementations in lithium niobate
on insulator.

Phase Combination of 12 Fibers
Using Multi-Plane Light Conversion Device∙R. Demur1 , E. Turpin1,2 , L.
Leviandier1 , J. Bourderionnet1 ,and E. Lallier1 ; 1 Thales Research& Technology, Palaiseau, France;
2
C2N Centre de Nanosciences etde Nanotetchnologies, Palaiseau,
FranceWe present the coherent beam combination of 12 fibers using a multiplane light conversion device. We
evaluate the combination efficiencyof the device and comment thesteering performances compared tothe theory.

Generation of spatially entangledstates of light in nonlinear waveguide arrays
A. Raymond1 , S. Francesconi1 , J.
Palomo2 , P. Filloux1 , M. Morassi3 ,A. Lemaître3 , F. Raineri3,4 , M.
Amanti1 , S. Ducci1 , and ∙F.
Baboux1 ; 1 Université Paris Cité,
Paris, France; 2 Université PSL,
Paris, France; 3 CNRS/Université
Paris-Saclay, Palaiseau, France;
4
Université Côté d’Azur, Nice, France
We demonstrate a nonlinear waveguide array, where photon pairs generated by SPDC are simultaneously
spread over the whole array throughcascaded quantum walks. This concept implements a compact and versatile source of spatially entangledstates.

Room Osterseen ICM

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)NOTES

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

CM-LIM: Lightmatter interaction

CF-7: Ultrafast laser technology I

CI-2: Frequency combs

CJ-3: Mode-locked fiber
lasersEB-7: Quantum sensing

Chair:
Emmanuel Stratakis,
FORTH, Institute of Electronic
Structure and Laser, Heraklion,
Crete

Chair: Hanieh Fattahi, MPI for the
Science of Light, Erlangen, Germany

CM-LIM.1 WED

CF-7.1 WED

10:30

Defect-rich Nanocatalysts from
Pulsed Laser Diffusion Enhancement in Liquids∙S. Barcikowski, K. Lau, S. Zerebecki, C. Rehbock, A. Ziefuß, and
S. Reichenberger; Chemical Technology and Center for NanoIntegration
Duisburg-Essen CENIDE, Universityof Duisburg-Essen, Essen, Germany
Laser Particle Processing in Liquid allows to enhance diffusion processes on a nanosecond time scaleby precise and efficient laser excitation allowing to write catalytically active defects with single-

10:30

Single-cavity dual-comb Yb:YAG
laser operating at 250 MHz withultra-low noise∙J. Pupeikis, B. Willenberg, C.
Bauer, S. Camenzind, A. NussbaumLapping, C. Phillips, and U. Keller;
ETH Zurich, Zurich, Switzerland
We demonstrate a 250 MHz singlecavity dual-comb laser delivering 2
W average power per comb with 100
Hz radio-frequency comb linewidthand 22 fs relative timing jitter over
[10 Hz – 8.25 kHz].

Chair: Alessandro Tonello, University of Limoges, France

CI-2.1 WED (Tutorial)

10:30

Microcombs for Optical Communications∙V. Torres Company; Chalmers University of Technology, Gothenburg,
SwedenThis tutorial will give an overview
of the enabling characteristics of
microcombs in wavelength divisionmultiplexing and coherent communication systems.

Chair: Alex Fuerbach, Macquarie
University, Sidney, Australia

CJ-3.1 WED

10:30

Towards a self-starting all-fibre
all-normal dispersion Mamyshev
Oscillator in the 2 μm band
∙D.C. Kirsch1 , M.E. Likhachev2 ,S.S. Aleshkina2 , M.V. Yashkov3 ,and M. Chernysheva1 ; 1 Leibniz
Institute of Photonic Technology,
Jena, Germany; 2 Prokhorov General
Physics Institute of the Russian
Academy of Sciences, Dianov Fiber
Optics Research Center, Moscow,
Russia; 3 Institute of Chemistryof High Purity Substances of theRussian Academy of Sciences,
Nizhny Novgorod, Russia

115

Chair: Gerd Leuchs, Institute for the
Science of Light, Erlangen, GermanyEB-7.1 WED

10:30

Ultrasensitive Photonic Quantum
Noise Sensing by Frequent-measurement Nonlinear Filtering∙G. Kurizki1 , O. Firstenberg1 ,T. Opatrný2 , D.B.R. Dasari3 , F.
Caruso4 , F. Piacentini5 , and M.
Genovese5,6 ; 1 Weizmann Instituteof Science, Rehovot, Israel; 2 Palacky
University , Olomouc, Czech Republic; 3 University of Stuttgart, Stuttgart, Germany; 4 University of Florence,
Sesto Fiorentino, Italy; 5 Istituto
Nazionale di Ricerca Metrologica,
Torino, Italy; 6 INFN (sez. Torino),
Torino, ItalyCLEO

Room 4a ICM

Room 4b ICM/Europe-EQEC 2023

Room 13b ICM

100 W and pulse energies 470 mJ at
high repetition rate.

10:45

JSI-2.2 WED

Semiconductor Laser Frequency
Stabilization based on a Silicon
Nitride Photonic Integrated
Circuit
A. Brugnoni1 , A.E. Kaplan1,2 , V.
Vitali1,2 , M. Re3 , ∙C. Lacava1,2 , and
I. Cristiani1 ; 1 Photonics Group, Department of Electrical, Computerand Biomedical Engineering, Pavia,
Italy; 2 Optoelectronics Research Centre, Southampton, United Kingdom;
3
Huawei Technologies Italia S.r.l.,
Milano, Italy
The design and experimental characterization of a fully-integrated silicon nitride frequency stabilizer ispresented. A C-band semiconductor laser stabilization with a maximum frequency deviation of 60
MHz from the nominal value wasdemonstrated.

CK-5.3 WED

11:00

Ultra-high-quality factor microring resonator based on silicon
nitride∙S. Cui1,2 , K. Cao1,2 , Y. Yu1,2 , and X.
Zhang1,2 ; 1 Wuhan National Laboratory for Optoelectronics and School of
Optical and Electronic Information,
Huazhong University of Science andTechnology, Wuhan, China; 2 Optics
Valley Laboratory, Wuhan, China
We demonstrated a highly multimode MRR to achieve ultra-low
propagation loss. Our method eliminates the requirement for chemicalmechanical planarization and canbe applied to different material platforms, thus greatly relaxing the fabrication processing requirements.

⋅ Wednesday 28 June 2023

Room 13a ICM

of less than 3.5 dB/m after 800 ∘ Cannealing, enabling resonators with
Q>10million for soliton generation.

CK-5.2 WED

®

10:45

Status and near future plans forgenerating pulses with shorter
wavelengths and duration by the
FERMI FEL
∙M.B. Danailov; Elettra-Sincrotrone
Trieste SCpA, Trieste, Italy
An overview of the status and ongoing upgrades of FERMI is presented,
with emphasis on the roots to expand the current FEL parameters toshorter wavelengths and pulses. Ongoing seed laser upgrade will be discussed.

JSIV-1.2 WED

11:00

Monocrystalline Plasmonic Nanostructures for Hot Carrier Photochemistry∙F. Kiani and G. Tagliabue; École
Polytechnique Fédérale de Lausanne,
Lausanne, Switzerland
We study quantum efficiency spectra of a redox reaction for monocrystalline gold nano-antennas having different thicknesses on TiO2coated glass substrates. The results
unravel the role of metal properties and plasmon excitation effects
in plasmonic photocatalysis.

CA-8.2 WED

11:00

Progress on Laser Development at
the Extreme Photonics Applications Centre∙P. Mason, N. Stuart, J. Phillips, R.
Heathcote, S. Buck, A. Wojtusiak,
M. Galimberti, T. de Faria Pinto, S.
Hawkes, S. Tomlinson, R. Pattathil,
T. Butcher, C. Hernandez-Gomez,
and J. Collier; Central Laser Facility,
STFC, Didcot, United Kingdom
Progress on the development of astate-of-the-art petawatt laser driver
operating at 30 J, 30 fs and 10 Hz
pulse rate at the Extreme Photonics
Applications Centre

JSI-2.3 WED

11:00

Development of Two-Colour SubFemtosecond Pump/Probe Techniques with X-ray Free-Electron
Lasers∙Z. Guo; SLAC National Accelerator
Laboratory, Menlo Park, USA; Department of Applied Physics, Stanford University, Stanford, USA
We report the attosecond control
and diagnosis of gigawatt-level
two-colour (ω/2ω) attosecond
pump/probe pulse pairs withtunable sub-femtosecond delays at
the Linac Coherent Light Source(LCLS).

116

Room 14a ICM

Room 14b ICM

ENSTA Paris, Ecole Polytechnique,
CNRS, IP Paris , Palaiseau, France;
2
Groupe de Physique Appliquée,
Université de Genève, Geneva,
Switzerland; 3 EMC Laboratory,
Electrical Engineering Institute,
Ecole Polytechnique Fédérale deLausanne, Lausanne, Switzerland;
4
TRUMPF Scientific Lasers GmbH+ Co. KG, Unterföhring, Germany;
5
ArianeGroup, Les Mureaux, France;
6
Swisscom Broadcast AG, Bern,
Switzerland; 7 School of Managementand Engineering Vaud, University ofApplied Sciences and Arts Western
Switzerland,
Yverdon-les-Bains,
Switzerland; 8 Department of Electrical Engineering, Uppsala University,
Uppsala, Sweden; 9 Institute forEnvironmental Sciences, Universitéde Genève, Geneva, Switzerland
We demonstrate the guiding oflightning over a distance of 50 mby laser filamentation of a highrepetition-rate terawatt laser.

damental laser and the harmonics,
and chromatic aberration inherent
during HHG.

CD-8.2 WED

11:00

UV Pulse Compression in Hollow
Core Fibers using XPM∙J.P. Messerschmidt1,2 , Y. Jiang1 ,G.M. Rossi1,2 , and F.X. Kärtner1,2 ;1Center for Free-Electron Laser
Science,
Deutsches ElektronenSynchrotron
DESY,
Hamburg,
Germany; 2 Physics Department and
The Hamburg Centre for Ultrafast
Imaging, University of Hamburg,
Hamburg, Germany
UV pulse self-compession to below 7 fs and μJ-level pulse energy
is achieved via cross-phase modulation in a hollow-core fiber compressor. Further energy scaling andpulse compression down to few-fs iscurrently being investigated.

CH-6.2 WED

10:45

Nanoscale Material-specific
Imaging Using an Extreme
Ultraviolet Table-top Light Source∙C. Liu1,2,3 ,W. Eschen1,2,3 ,L. Loetgering1,2,3 , D.S. Penagos Molina1,2,3 , R. Klas1,2,3 , V.
Schuster1,2,3 , A. Kirsche1,2,3 , L.
Berthold4 , A. Iliou5 , M. Steinert2 , F.
Hilmann5 , M. Krause4 , J. Limpert2,6 ,and J. Rothhardt1,2,3,6 ; 1 Helmholtz
Institute Jena, Jena, Germany;
2
Institute of Applied Physics,
Friedrich-Schiller-University Jena,
Jena, Germany; 3 GSI Helmholtzzentrum für SchwerionenforschungGmbH, Darmstadt,
Germany;4
Fraunhofer Institute for Microstructure of Materials andSystems IMWS, Halle, Germany;
5
Leibniz Institute for Natural Product Research and Infection Biology,
Jena, Germany; 6 Fraunhofer Institute for Applied Optics and Precision
Engineering IOF, Jena, Germany
We present our latest results ontable-top ptychographic imaging at
13.5 nm. Quantitative amplitudeand phase images were obtainedwith sub-20 nm spatial resolution.
Investigations of silicon-based
semiconductor samples and microorganisms are enabled withexcellent material-specificity.
CH-6.3 WED

11:00

Shape Measurement of Gold Nanorods in Water Using Microcavities∙Y. Yin, A. Trichet, and J. Smith;
University of Oxford, Oxford, United
Kingdom
We characterize aspect ratios of
single gold nanorods in water using open-access microcavities. By
measuring Stokes parameters of atransmitted beam, we obtain theanisotropic particles’ perturbation

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laser-pulse-precision into nanoparticles.

CM-LIM.2 WED

10:45

CF-7.2 WED

10:45

®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)The self-starting of a Thulium-based
Mamyshev oscillator in all-fibre andall-normal dispersion configuration
is explored. The first studies of
the unoptimised, free-running laser
demonstrate the generation of 200ps pulses with up to 6 nJ energy.

We report novel methods for detecting quantum noise signatures via
nonlinear filtering of quantum noise
by frequent measurements of single
quanta probes. Unparalleled sensitivity is reported for spin and photon probes.

CJ-3.2 WED

EB-7.2 WED

10:45

10:45

High-temperature laser absorption of steel∙J. Volpp; Luleå University of Technology, Luleå, Sweden
It was possible to measure laser absorption values at high temperaturesusing a radiometric setup. Measurement data show a general trendof increasing absorption at increasing temperature with an absorption
drop just above boiling temperature.

High-speed optical sampling by
dynamic repetition rate tuning ofan optically injected mode-locked
laser diode∙A.F. Ribeiro1 , T. Gomes1,2 , and
M.A. Cataluna1 ; 1 Institute of
Photonics and Quantum Sciences,
Heriot-Watt University, Edinburgh,
United Kingdom; 2 IFIMUP and Departamento de Física e Astronomia,
Faculdade de Ciências, Universidade
do Porto, Porto, Portugal
We demonstrate high-speed opticalsampling by cavity tuning (OSCAT),
with record scan rates of up to 20
MHz, enabled by the wide and dynamic repetition rate tuning of adual-tone optically-injected modelocked quantum-dot laser diode.

E-band Fourier domain mode
locked laser and its application in
optical coherence tomography∙Y. Shi1,2 , D. Huang1,2 , Y. Li1,2 , F.
Li2,3 , and P.K.A. Wai2,3,4 ; 1 Photonics
Research Institute, Department ofElectrical Engineering, The Hong
Kong Polytechnic University, Hong
Kong, China; 2 The Hong Kong
Polytechnic University Shenzhen
Research Institute, Shenzhen, China;
3
Photonics
Research
Institute,
Department of Electronic and Information Engineering, The Hong Kong
Polytechnic University, Hong Kong,
China; 4 Department of Physics,
Hong Kong Baptist University, Hong
Kong, China
We demonstrate for the first timean E-band Fourier domain mode
locked laser with a 50 kHz sweep
rate and a 90 nm sweep range, andits application in swept-source optical coherence tomography.

Nonlinear filtering of thermal
excitations from Quantum spin
ensembles by Quantum spinprobe measurements∙D.B.R. Dasari1 , S. Yang2 , A.
Chakrabarti3 , A. Finkler3 , G.
Kurizki3 , and J. Wrachtrup1 ; 1 3.
Physics Institute, University of
Stuttgart,
Stuttgart,
Germany;2
Department of Physics, The Hong
Kong University of Science andTechnology, Clear Water bay,
Hong Kong, China; 3 Departmentof Chemical Physics, Weizmann
Institute of Science, Rehovot, Israel
We report nonlinear purification of
Quantum spin ensembles by frequent measurements of a coupled
Quantum Probe. Quantum StateEngineering and Quantum Random
walks follow as a natural consequence in both the ensemble andprobe dynamics.

CM-LIM.3 WED

CF-7.3 WED

CJ-3.3 WEDEB-7.3 WED

11:00

Exploration of the ultimate
limitation of Moore’s law using
Lloyd’s Mirror interference
lithography∙S. Santra1 , K. M. Dorney2 , F.
Holzmeier2 , J. Petersen2 , S. De
Gendt1,2 , and E. W. Larsen2 ; 1 KU
Leuven, Leuven, Belgium; 2 imec,
Leuven, Belgium
We demonstrate the utilization ofa tabletop high harmonic generation EUV source to perform interference lithography of ∼20 nm
pitch line/space patterns in a spinon metal-oxide photoresist by deploying a Lloyd’s mirror interference lithography setup.

11:00

Monolithic
Kerr-Lens-Modelocked 2.2-GHz
Yb:Y2O3 Oscillator, Amplified bya Semiconductor Optical
Amplifier∙H. Ostapenko1 , Y. Feng1 , T.
Lamour2 , R. McCracken1 , O.
Mandel2 , D. Weise2 , and D.T. Reid1 ;1
Heriot-Watt University, Edinburgh,
United Kingdom; 2 Airbus Defence
and Space GmbH, Immenstaad,
Germany
We present a fully bonded 2.2-GHz
low-noise Yb:ceramic laser oscillator with 189 fs pulses which arethen amplified through the chirpedpulse amplification in a semiconductor optical amplifier to 69 mW of
average power.

11:00

Coherence Breakdown Within the
Ultra-Stable Regime of Fourier
Domain Mode-Locked Lasers
Under Increasing Intracavity
Power∙Ö.E. Aşırım1 , R. Huber2 , and C.
Jirauschek1 ; 1 Technical Universityof Munich, Munich, Germany;
2
University of Lübeck, Lübeck,Germany
The high coherence of FDML lasers
is demonstrated to gradually deteriorate in the ultra-stable regime
above a threshold power whose
value depends on the fiber parameters. The numerical results are in excellent agreement with experiment.

117

11:00

Rotation sensing with structured
photons and multi-planelight-conversion∙R. Fickler1 , M. Hiekkamäki1 ,M. Eriksson1 , A.Z. Goldberg2,3 ,F. Bouchard2 , and L.L. Sánchez1
Soto4,5 ;Tampere University,
Tampere, Finland; 2 National Research Council of Canada, Ottawa,
Canada; 3 University of Ottawa,
Ottawa, Canada; 4 Max-PlanckInstitut für die Physik des Lichts,
Erlangen, Germany; 5 Departamentode Óptica,, Madrid, Spain
Using the structured photons, we
generate twisted N00N-states toperform super sensitive angularmeasurements.
We further use
them to encode high-dimensional
King states for simultaneous mul-

NOTES

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Room 13a ICM

Room 13b ICM
JSI-2.4 WEDRoom 14a ICM

Ultrasmall Submicrometer Sized
Periodic Deposition on the Silicon
Nitride Microring with Nanodispensing Technique∙H. Takeda1 , A. Abazi2,3 , A. Eich2,3 ,Y. Tomishige1 , K. Hiramoto1 , J.
Chen1 , Y. Mikami1 , N. Tate1 ,Y. Oki1 , C. Schuck2,3 , and H.
1
Yoshioka1 ;Kyushu University,
Fukuoka, Japan; 2 University ofMuenster, Muenster, Germany;
3
Center for Soft Nano Science,
Muenster, Germany
For use in the telecommunication
band (around 1.55 micrometer), a
second-order Bragg grating (grating
period is shorter than 1 micrometer) was printed on an optical microring using nanodispensing technique and spectroscopic measurement showed spectral shift.

Plasmonic Cu2SSe Nanocrystals:
Chemical Synthesis and Applications∙N. Manwar and J.C. Colmenares Q.;
Institute of Physical Chemistry, Polish Academy of Sciences (IPC-PAS),
Warsaw, Poland
We are exploring the cuprous
sulfide selenide (Cu2SSe) alloyNCs for plasmon induced catalytic(PIC) applications. Nevertheless,the chemical synthesis route isused to prepare the Cu2S, Cu2Se,
and Cu2SSe nanocrystals andcharacterized those in detailed.

Femtosecond Precision Synchronization of Independent Laser
Systems for Pump-Probe
Experiments∙E.C. Erdman1,2 ,J. Novák1 ,1
R. Antipenkov , L. Indra1,3 , B.
Tykalewicz1 , M. Horáček1 , J. Fara1 ,J.A. Naylon1 , P. Bakule1 , and B.
Rus1 ; 1 The Extreme Light Infrastructure ERIC, ELI Beamlines Facility,
Dolní Březany, Czech Republic;
2
Charles University in Prague,
Prague, Czech Republic; 3 Czech
Technical University in Prague,
Prague, Czech Republic
A new laser (F-SYNC) operating at
13mJ, 1kHz, and compressible to<20fs has been developed. Here, we
describe our work on its synchronization to a second 1kHz laser (L1Allegra) with fs-level precision andarbitrary delay.

CK-5.5 WED

JSIV-1.4 WED

CA-8.4 WED

JSI-2.5 WED

11:15

11:30

Perfect soliton crystal linear-wave
scattering in a Si3N4 microring
resonator∙H. Zhang1 , L. Lu1,2 , J. Chen1,2 ,and L. Zhou1,2 ; 1 State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai, China; 2 SJTU-Pinghu Instituteof Intelligent Optoelectronics, Shanghai, China
We investigate the perfect soliton
crystal linear-wave scattering by injecting an extra probe laser in a
Si3N4 microring resonator. With aproperly set probe laser, the comb
spectrum is adjusted in the experiments.

JSIV-1.3 WED

11:15

11:30

Record efficient and stable Sibased photoanodes enabled byultrathin transition-metal alloy
film for solar-assisted water
splitting∙F. Xiang, N. Li, A. Burguete-Lopez,
Z. He, M. Elizarov, and A. Fratalocchi; King Abdullah University of Science and Technology (KAUST), Jeddah province, Thuwal city, Saudi
ArabiaWe report an ultrathin transitionmetal alloy coating strategy on Si
photoanodes for efficient and stablesolar-assisted water splitting. This
technique extended the device lifetime to above 200 hours with aworld-record efficiency of 4.25%.

CA-8.3 WED

11:15

11:30

High Contrast Front-End for High
Repetition Rate 100 TW-Class
Laser System∙L. Indra1,2 , A. Špaček1,2 , J.T.
Green1 ,J. Bartoníček1,3 ,J.
Eisenschreiber1,4 , M. Fibrich1,2 ,B. Tykalewiz1 , M. Horáček1 , J.A.
Naylon1 , and B. Rus1 ; 1 The Extreme
Light Infrastructure ERIC, ELI
Beamlines Facility, Dolní Břežany,Czech Republic; 2 Faculty of Nuclear
Sciences and Physical Engineering,
Czech Technical University in
Prague, Czech Republic; 3 Facultyof Mechanical Engineering, Czech
Technical University in Prague,
Czech Republic; 4 Charles University,
Faculty of Mathematics and Physics,
Prague, Czech Republic
We present an overview of a frontend, which seeds a 100TW-classlaser and provides a synchronizedmulti-mJ, 2.2μm, 2kHz auxiliary
output. Both branches are seeded
via supercontinuum generated andamplified by a single regenerative
amplifier.

11:30

An attosecond timing tool forphase-resolved experiments at
free-electron lasers∙P.K.
Maroju1 , M. Di Fraia2 ,O. Plekan2 , M. Bonanomi3,4 , B.
Merzuk1 , D. Busto1,5 , I. Makos1 ,M. Schmoll1 , R. Shah1 , P.R. Ribic2 ,L. Giannessi2,6 , G. De Ninno2,7 ,C. Spezzani2 , G. Penco2 , A.
Demidovich2 , M. Danailov2 , M.
Coreno2,6,8 , M. Zangrando2 , A.
Simoncig2 , M. Manfredda2 , R.J.
Squibb9 , R. Feifel9 , S. Bengtsson5 ,E.R. Simpson5 , T. Csizmadia10 ,M. Dumergue10 , S. Kuehn10 , K.
Ueda11 , J. Li12 , K.J. Schafer12 ,F. Frassetto13 , L. Poletto13 , K.C.
Prince2 ,J. Mauritsson5 ,C.
2Callegari , and G. Sansone1 ;1
Physikalisches Institut, AlbertLudwigs-Universität,
Freiburg,2Germany;
Elettra-Sincrotrone,
Trieste, Italy; 3 Dipartimento di
Fisica Politecnico, Milano, Italy;
4
Istituto di Fotonica e Nanotecnologie CNR-IFN, Milano, Italy;
5
Department of Physics, Lund Uni-

118

to the cylindrically symmetric resonance modes.

11:15

Spectral phase interferometry fordirect electric-field reconstructionof XUV synchrotron light∙T. Fuji1 , T. Kaneyasu2 , M.
Fujimoto3 , Y. Okano3 , E. Salehi3 ,M. Hosaka4,5 , Y. Takashima4 , A.
Mano4 , Y. Hikosaka6 , S.-i. Wada7 ,and M. Katoh7,3 ; 1 Toyota Technological Institute, Nagoya, Japan; 2 SAGALight Source, Tosu, Japan; 3 Institutefor Molecular Science, Okazaki,
Japan; 4 Nagoya University, Nagoya,Japan; 5 University of Science andTechnology of China, Hefei, China;
6
University of Toyama, Toyama,
7
Japan;
Hiroshima University,
Higashi-Hiroshima, Japan
We have demonstrated the characterization of XUV synchrotron lightusing spectral phase interferometry for direct electric-field reconstruction. A tandem undulator wasused to generate a spectrally sheared
replica of the original wave packet.

CK-5.4 WEDRoom 14b ICM

CD-8.3 WED

11:15

CH-6.4 WED

11:15

Experimental realization of acoherent Raman comb
∙J. Ignacchiti1 , A. Reigue1 , F.
Amrani1,2 ,B. Debord1,2 ,F.
Gérôme1,2 , and F. Benabid1,2 ;
1GPPMM Group, Xlim Institue,
CNRS UMR 7251, Universitéde Limoges, Limoges, France;
2
GLOphotonics, Limoges, France
Working in the transient regime ofstimulated Raman scattering in H2filled hollow core fiber, we demonstrate the phase locking of the generated Raman comb, in quantitative
agreement with the numerical resolution of the Maxwell-Bloch equations.

Single-Molecule Image Scanning
Microscopy∙E. Slenders, S. Patil, A. Bucci, L.
Bega, M. Donato, M. Held, and G.
Vicidomini; Istituto Italiano di Tecnologia, Genoa, Italy
We present single-molecule image
scanning microscopy, a technique
for single-molecule localization microscopy that combines structured
illumination with structured detection. We show that this technique
has several advantages over PALM,
MINFLUX, and RASTMIN.

CD-8.4 WED

CH-6.5 WED

11:30

Spatial Multiplexing of Temporal
Localized Structures in
Degenerate Optical Cavities
A. Bartolo1 , N. Vigne2 , M. Marconi1 ,G. Beaudoin3 , K. Pantzas3 , I.
Sagnes3 , A. Garnache2 , and ∙M.
Giudici1 ; 1 Université Côte d’Azur,
Centre National de La Recherche
Scientifique, UMR7010 Institut
de Physique de Nice, Valbonne,
France; 2 Institut d’Electronique etdes Systèmes, UMR5214, Centre
National de la Recherche Scientifique, University of Montpellier,Montpellier, France; 3 Centre for
Nanosciences and Nanotechnology,
Centre National de la Recherche
Scientifique UMR9001, Université
Paris-Saclay, Palaiseau, France
We have implemented spatially independent sources of temporal localized structures in the transverse
plane of a degenerate cavity VECSEL. A large variety of spatiotemporal light states can be obtained
and controlled all-optically.

11:30

Subatomic Optical Localizationand Metrology with Topologically
Structured Light
T. Liu1 , ∙C.-H. Chi1 , J.-Y. Ou1 , K.
MacDonald1 , and N. Zheludev1,2 ;1UniversityofSouthampton,
Southampton, United Kingdom;
2
Nanyang Technological University,
Singapore, Singapore
The first realization of optical picomotion metrology is reported. The
position of a nanowire is localizedwith ‘sub-Brownian’ precision better than 100 picometers via deeplearning analysis of topologicallystructured light scattering from thenanowire.

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/Europe-EQEC 2023

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Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)tiparameter sensing of a rotation
around a randomly chosen axis.

CM-LIM.4 WED

11:15

CF-7.4 WED

11:15

Investigation on the influence ofbeam steering frequency on keyhole behaviour using a dynamic
beam laser
F. Hugger1 , ∙R. Sättele1 , E. Punzel1 ,A. Bürger1 , and J. Wagner2 ; 1 BBW
Lasertechnik GmbH, Prutting, Germany; 2 Institut für Strahlwerkzeuge(IFSW), Stuttgart, Germany
Dynamic beam lasers enable rapidchanges in intensity distributions at
MHz frequencies. The influence ofvarious thermal cycles on the dynamic response of the capillary surface is analytically investigated andcompared to high-speed images.

Towards deep UV spectroscopy
with a high-power single-cavity
dual-comb thin-disk oscillator∙T. Hofer, K. Fritsch, and O. Pronin;
Helmut Schmidt University, Hamburg, Germany
Frequency-doubling our highpower dual-comb spectrometerbased on a single-cavity thin-disk
oscillator enables simultaneous
spectroscopic measurements in
two spectral domains in order toevaluate and discuss the further
frequency conversion towards deep
UV dual-comb spectroscopy.

CM-LIM.5 WED

CF-7.5 WED

11:30

Direct writing of silver-seed paths
for electroless copper deposition
using laser-induced forward
transfer∙M. Domke1 ,S. Stroj1 ,J.
Landsiedel2 ,and N. AguilóAguayo2 ; 1 Research Center for
Microtechnology, Vorarlberg University of Applied Sciences, Dornbirn,
Austria; 2 Research Institute of Textile Chemistry and Textile Physics,
University of Innsbruck, Dornbirn,
Austria
A laser-induced forward transfer of
Ag nano and micro particle is utilized to generate seed paths for thegrowth of conductive lines on textiles via electroless copper deposition.

11:30

Mode-locked Pulses with
Narrowband Comb-like Peaks
Formed by Intracavity Amplitude
Modulation from Gaseous
Molecules∙D. Okazaki1,2 , W. Song1 , I.
Morichika1 , and S. Ashihara1 ;1Institute of Industrial Science, The
University of Tokyo, Tokyo, Japan;
2
Institute for Chemical Research,
Kyoto University, Kyoto, JapanThe mode-locked oscillation withintense narrowband spectral peaks
is observed in Cr:ZnS laser with intracavity gaseous molecules. The
shape of peaks varies inside the cavity because of intracavity narrowband amplitude modulation understrong nonlinearity.

CJ-3.4 WED

CI-2.2 WED

11:30

Active Feedback Stabilization ofSuper-efficient Microcombs∙I. Rebolledo-Salgado1,2 , O. Bjarki
Helgason1 , M. Girardi1 , M. Zelan2 ,and V. Torres-Company1 ; 1 Dept.
Microtechnology and Nanoscience,
Chalmers University of Technology,
Gothenburg, Sweden; 2 Measurement
Science and Technology, RISE Research Institutes of Sweden, Borås,SwedenWe report the long-term operationof a super-efficient microcomb. We
use the soliton power to maintain afixed pump detuning. The microcomb operates over 25 hours using athermal control in a packaged module.

11:15

EB-7.4 WED

11:15

1550 nm FDML-MOPA laser withkilowatt wavelength-swept pulses∙T. Kutscher, A. Gruber, P. Lamminger, C. Leonhardt, M. Wiggert,
C. Stock, and S. Karpf; Institute of
Biomedical Optics, Lübeck, Germany
We present a swept-source FDMLMOPA laser at 1550nm with 60ps
pulses at 1kW peak power. The
326kHz sweep rate is modulated
to 80 MHz pulse rate to enablehigh-speed imaging using inertiafree spectro-temporal line scanning.

Coherent two-photon LIDAR withincoherent thermal light∙C.-H. Lee1 , Y. Kim1 , D.-G. Im1 ,U.-S. Kim1 , V. Tamma2 , and Y.-H.
Kim1 ; 1 Department of Physics,
Pohang University of Science andTechnology, Pohang, South Korea; 2 School of Mathematics andPhysics, University of Portsmouth,
Portsmouth, United Kingdom
We demonstrate a coherent twophoton LIDAR with thermal lightthat exploits the counterintuitive
emergence of second-order interference beyond the coherence length.
We expect our LIDAR scheme canplay a crucial role in remote sensing.

CJ-3.5 WEDEB-7.5 WED

11:30

Four-wave mixing fast wavelength
sweeping FDML laser with kW
peak power at 900 nm and 1300
nm
∙P. Lamminger1 , H. Hakert1 , S.
Lotz1 , J.P. Kolb2 , T. Kutscher1 , S.
Karpf1 , and R. Huber1,2 ; 1 Instituteof Biomedical Optics, Universität
zu Lübeck, Luebeck, Germany;
2
Medizinisches
Laserzentrum
Lübeck GmbH, Luebeck, Germany
Here presented is a fast wavelength
sweeping fiber laser with kilowatt
peak power at 900nm built of a
1064nm MOPA laser and a 1300nm
FDML laser using four-wave mixing
in a photonic crystal fiber.

119

11:30

Vector Magnetometry Based on
Polarimetric Optically Detected
Magnetic Resonance
P. Reuschel1 , M. Agio1,2 , and ∙A.M.
Flatae1 ; 1 Laboratory of Nano-Optics,
University of Siegen, Siegen, Germany; 2 National Institute of Optics(INO), National Research Council(CNR), Sesto Fiorentino, Italy
We introduce vector magnetometry
based on polarimetric optically detected magnetic resonance of ensembles of nitrogen-vacancy centersin diamond without a magnetic bias
field. The approach is general forother spin-1 color centers with C3v
symmetry.

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CK-5.6 WEDRoom 4b ICM

11:45

Spectrally asymetric frequency
conversion with pulsed four-wave
mixing in graphene covered Si3 N4
waveguides∙P. Demongodin1 , H. El Dirani2 , S.
Kerdilès2 , J. Lhuillier1 , T. Wood1 ,C. Sciancalepore2 , and C. Monat1 ;1
Université de Lyon, Ecole Centralede Lyon, INSA Lyon, Universit’e
Claude Bernard Lyon 1, CPE Lyon,
CNRS, INL, UMR5270, Ecully,
France; 2 Universitté Grenoble-Alpes,
CEA-LETI, Grenoble, France
We investigate the nonlinear response of Si3 N4 waveguides locallycovered by graphene with pulsed
degenerate FWM at telecom wavelength. Our measurements highlight a strong asymmetry in the
power of the generated idler withgraphene.

JSIV-1.5 WED®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 13a ICM

11:45

Large-Scale Decentralized Photothermal Desalination: A Blueprint to Make Efficient Off-Grid
Technologies a Reality
W. Schmid, A. Machorro-Ortiz, P.
Dongare, N. Halas, and ∙A. Alabastri; Rice University, Houston, TX,
USA
Our general approach for large-scalesolar-driven photothermal desalination (SDPD), emphasizing the positive feedback relationship between
evaporative power transfer and heatrecovery, guides the discussion ofrecent advancements toward efficient and modular day-long water
purification.

CA-8.5 WEDRoom 13b ICM

11:45

A variable output 100 Hz laser
system with few-cycle and TW
level pulses∙P. Gaal1 , B. Nagyilles1 , M.
Karnok1 ,A.P. Kovacs1,2 ,T.
Gilinger1 , M. Fule1,3 , C. Kiraly1 , R.
Nagymihaly1,4 , I. Seres1,4 , S. Toth1,4 ,and K. Osvay1,2 ; 1 National LaserInitiated Laboratory, University ofSzeged, Szeged, Hungary; 2 Dept
Optics and Quantum Electronics,
University of Szeged, Szeged, Hungary; 3 Dept. Experimental Physics,
University of Sz, Szeged, Hungary;
4
ELI-ALPS, Szeged, Hungary
A versatile 100Hz laser system basedon negatively and positively chirped
CPA has been developed. The few
cycle output provides pulses with
9.2fs and 0.3mJ, while the power
output supports 26fs pulses with
36mJ.

Room 14a ICM

versity, Sweden; 6 INFN Laboratori
Nazionali di Frascati, Rome, Italy;
7
Laboratory of Quantum Optics,
University of Nova Gorica, Slovenia;
8
ISM-CNR, Istituto Struttura della
Materia, Trieste, Italy; 9 Departmentof Physics, University of Gothenburg,
Sweden; 10 ELI ALPS, ELI-HU,
Szeged, Hungary; 11 Institute ofMultidisciplinary
Researchfor
Advanced Materials, Tohoku, Japan;
12Department of Physics and Astronomy Louisiana State University,
Baton Rouge, USA; 13 Istituto di
Fotonica e Nanotecnologie, Padua,
Italy
We will present a novel attosecond
timing tool for the single-shot characterization of the relative phase of
an attosecond pulse train and an infrared laser field. A resolution of one
atomic unit (24 as) is demonstrated.
JSI-2.6 WED

11:45

FLASH2020+: Providing newopportunities for excellent FEL
experiments∙L. Schaper, M. Beye, M. Gühr, I.
Hartl, and S. Schreiber; Deutsches
Elektronen-Synchrotron
DESY,
Hamburg, Germany
By 2025 the FLASH facility will betransformed to simultaneously deliver high intensity SASE and spectrally clean Fourier limited externally seeded FEL pulses driving next
generation FEL experiments in the
XUV to soft X-ray regime.

CD-8.5 WEDRoom 14b ICM

11:45

Enhancing Ising Machine Robustness Through Period-2 Dynamics
in Optical Resonators∙L. Quinn1,2 , G. Xu3 , Y. Xu1,2 ,J. Fatome4 , S. Murdoch1,2 , M.
Erkintalo1,2 ,and S. Coen1,2 ;1Physics Department, University of
Auckland, Auckland, New Zealand;2
he Dodd-Walls Centre for Photonic and Quantum Technologies,
Otago, New Zealand; 3 School of
Optical and Electronic Information,
Huazhong University of Scienceand Technology, Wuhan, China;
4
ICB, UMR 6303 CNRS, Université
Bourgogne-Franche-Comté, Dijon,
FranceHere we propose a novel coherent
Ising machine (CIM) based upon
spontaneous symmetry-breaking(SSB) in a driven Kerr resonator. We
demonstrate enhanced robustness
due to the utilization of period-2
symmetry-breaking dynamics.

CH-6.6 WED

11:45

A Photonic Atom Probe allowing
for super-resolution photoluminescence spectroscopy and contactless optical piezo-spectroscopy
L. Rigutti1 , E. Di Russo1 , P.
Dalapati1 , L. Venturi1 , J. Houard1 ,I. Blum1 , S. Moldovan1 , J.-M.
Chauveau2 , M. Huges2 , D. Blavette1 ,F. Vurpillot1 , and ∙A. Vella1 ; 1 Univ
Rouen Normandie, INSA Rouen
Normandie, CNRS, Groupe dePhysique des Matériaux UMR
6634, Rouen, France; 2 Centre deRecherche sur l’Hétéro-Epitaxie et
ses Applications, UPR10 CNRS ,Valbonne, France
We present the Laser-assisted Atom
Probe Tomography coupled within-situ micro-photoluminescencebench as a new instrument for
in-situ correlative microscopy
with improuved optical resolution and contactless opticalpiezospectroscopy.

Room 4a ICM
12:00 – 12:52
PP-2: Early-stage Researcher (ESR) session Poster pitches II
Chair: Emiliano Descrovi, European Optical Society,
Palaiseau, France
PP-2.1 WED (Poster pitch of CC-P.1)

12:00

400 kHz repetition rate THz-TDS with 24 mW of average power driven by a compact industrial Yb-laser∙C. Millon1 , S. Houver2 , and C.J. Saraceno2 ; 1 Ruhr University Bochum, Bochum, Germany; 2 Paris Cite University, Paris, France
We demonstrate a 24 mW average power THz-TDS at
400 kHz repetition rate, driven directly by a commercial

fs-laser. We show no thermal effects on the generated
THz while varying the repetition rate.

to 1625 nm is achieved at deposition temperature as low
as 300 ∘ C.

which combines the bonding beam delivery and microscopy channels.

PP-2.2 WED (Poster pitch of CE-P.2)

PP-2.3 WED (Poster pitch of CE-P.3)

PP-2.4 WED (Poster pitch of CG-P.2)

12:04

Low-temperature and hydrogen-free silicon dioxidecladding for next-generation integrated photonics
Z. Li1,2 , ∙Z. Qiu1,2 , R.N. Wang1,2 , M. Divall1,2 , and T.
Kippenberg1,2 ; 1 Swiss Federal Institute of Technology Lausanne (EPFL), Lausanne, Switzerland; 2 Center for Quantum Science and Engineering, EPFL, Lausanne, Switzerland
We demonstrate a hydrogen-free low-loss silicon dioxide
film deposited with SiCl4 for cladding of photonic integrated circuits. A very wide low-loss window of 1260 nm

12:08

Laser-Assisted Bonding Prototype Equipment for
Hybrid Integration of Silicon Photonic Circuits∙A. Vlasov, T. Uusitalo, E. Lepukhov, H. Virtanen, S.-P.
Ojanen, J. Viheriälä, and M. Guina; Tampere University,
Physics Unit, Optoelectronic Research Centre, Korkeakoulunkatu 3, Tampere, FinlandHybrid integration on silicon substrate is promising way
towards increased density and enhanced functionality.
We introduce the self-developed laser-assisted bonding setup with bottom coaxial irradiation architecture,

120

12:12

Attosecond Optical Spectroscopy of Monocrystalline
Diamond∙G.L. Dolso1 , S.A. Sato2 , N. Di Palo1 , G. Inzani1 , R.
Borrego-Varillas3 , M. Nisoli1,3 , and M. Lucchini1,3 ;1Department of Physics, Politecnico di Milano, Italy;
2
Center for Computational Sciences, University ofTsukuba, Japan; 3 Institute for Photonics and Nanotechnologies, IFN-CNR, Milano, Italy, Italy
We measured attosecond electron dynamics in singlecrystalline diamond induced by few-femtosecond opti-

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Room Osterseen ICM
CM-LIM.6 WED

11:45

Inscription of Waveguides andBeam Splitters in Borosilicate
Glass using a Femtosecond Laserwith a Long Focal Length∙T. Willburger, S. Funken, M.-J.
Kleefoot, and H. Riegel; Aalen University, Aalen, Germany
In this work, we present the potential for the microfabrication of
direct written optical components
such as waveguides and beam splitters into the volume of borosilicate
glass using femtosecond laser with along focal length.

Room 1 Hall B1 (B11)CF-7.6 WED

11:45

Self-Starting Kerr-Lens-Modelocked 1-GHz Ti:sapphire Oscillator Pumped by a Single Laser
Diode∙H. Ostapenko, T. Mitchell, P. CastroMarin, and D.T. Reid; Heriot-Watt
University, Edinburgh, United Kingdom
We present a 1-GHz self-starting
Ti:Sapphire laser oscillator pumped
by a single green diode, achieving
106 mW of average output power at
1W of pump with 111 fs pulses andlow-noise performance.

®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 6 Hall B3 (B32)
CI-2.3 WEDRoom 7 Hall A1 (A11)

11:45

Direct-modulation optoelectronic
oscillator for optical frequency
comb and pulse generation∙B. Sinquin, M. Vallet, M. Alouini,
and M. Romanelli; Univ. Rennes,
CNRS, Institut FOTON UMR 6082,
Rennes, France
We propose a direct-modulation optoelectronic oscillator to generate simultaneously ultra-pure RF signals
and low jitter picosecond opticalpulses. We demonstrate a phasenoise of -123 dBc/Hz at 10 kHz anda broad optical spectrum.

CJ-3.6 WED

11:45

Frequency-Shifted-Feedback
Mode-Locked Fibre Laser with
Tuneable Repetition Rate
∙J.-B. Lecourt1 , A. Baylon2 , S.
Boivinet1 , T. Cassim2 , F. Défossez1 ,A. Gognau1 , J.-P. Yehouessi1 , and
Y. Hernandez1 ; 1 Multitel Innovation Center, Mons, Belgium;2Euro-Multitel SA, Mons, Belgium
A Frequency Shifted Feedback
mode-locked fiber laser is developed. The laser can operate atdifferent repetition rates, fundamental frequency imposed by cavity
length and harmonics, thanks todynamic control of the transmissionof the Acousto-Optic-Modulator

Room 8 Hall A1 (A12)EB-7.6 WED

NOTES

11:45

Time-frequency quantum metrology∙N. Fabre; Telecom Paris, Institut
Polytechnique de Paris, 19 Place
Marguerite Perey, 91120, Palaiseau,
France
The engineering of the spectral distribution of photon pairs, and theinfluence of the scaling with thenumber of photons, are investigated
for the measurement of time andfrequency delay.

Room 4a ICM
cal light pulses. Our results, supported by TDDFT simulations, validate macroscopic models and identify thecontribution of individual sub-bands to the total opticalresponse.
PP-2.5 WED (Poster pitch of CG-P.3)

12:16

Optical levitation of reflective shells using an LG01
vortex beam
∙A.-H. Munj, R. Smith, and W. Kerridge-Johns; Imperial
College, London, United Kingdom
We present optical levitation of reflective silver-coatedglass shells ranging from 53-93μm in diameter, at large
working distances (40-100mm) using a LG01 vortex
laser. Minimum levitation powers ranged from 50mW
to 100mW.

∙E. Bodo, V. Bello, and S. Merlo; Dep. of Electrical, Computer & Biomedical Engineering, University of Pavia, Italy
We provide the proof of concept of urea concentration
detection by means of amplitude measurement, specifically exploiting the urea absorption band around λ =2.15 μm, that can provide valuable information about
dialysis efficiency.
PP-2.8 WED (Poster pitch of CL-P.2)

12:28

Multiple Scattering Layers As Physical Unclonable
Functions For Optical Wireless Communication∙A. Rates1 , J. Vrehen2 , B.L. Mulder1 , W.L. IJzerman2,3 ,and W.L. Vos1 ; 1 Complex Photonic Systems (COPS),MESA+ Institute for Nanotechnology, University ofTwente, Enschede, Netherlands; 2 Signify, Eindhoven,
Netherlands; 3 Department of Mathematics and Computer
Science, Eindhoven University of Technology, Netherlands
We study the correlation of light speckle between multiple scattering layers. Based on this, we propose an opticalwireless communication scheme using scattering media
as physical unclonable functions.

Classification of clinically significant prostate cancer
using Raman spectroscopy and Support Vector
Machine classification∙S.J. van Breugel1,2,3 , I. Low4 , M.L. Christie4 , M.R.
Pokorny4 , H.U. Holtkamp1,3 , M.K. Nieuwoudt1,2,3 ,M.C. Simpson1,2,3,5 , K. Zargar-Shoshtari4,6 , and C.
Aguergaray2,3,5 ; 1 School of Chemical Sciences, Universityof Auckland, Auckland, New Zealand; 2 The DoddWalls Centre for Photonic and Quantum Technologies,
Dunedin, New Zealand; 3 The Photon Factory, Universityof Auckland, New Zealand; 4 Counties Manukau District
Health Board, Auckland, New Zealand; 5 Department of
Physics, University of Auckland, New Zealand; 6 Facultyof Medical and Health Sciences, University of Auckland,
New Zealand
Raman spectroscopy and support vector machine classification are combined to detect clinically significant
prostate cancer on a data set of 152 patients. The reported cohort and classification performance are thehighest reported to date.

PP-2.7 WED (Poster pitch of CL-P.1)

PP-2.9 WED (Poster pitch of EB-P.1)

PP-2.6 WED (Poster pitch of CI-P.13)

12:20

12:24

Towards the development of a SWIR-LEDs based
optoelectronic system for urea monitoring duringhaemodialytic therapy

12:32

Deep Learning Based TEMPEST Attacks on a
Quantum Key Distribution Sender∙A. Baliuka1,2 , M. Stöcker1 , M. Auer1,2,3 , P. Freiwang1,2 ,H. Weinfurter1,2,4 , and L. Knips1,2,4 ; 1 LMU, Munich, Germany; 2 MCQST, Munich, Germany; 3 Univ. der Bundeswehr München, Neubiberg, Germany; 4 MPQ, Garching, Germany
A side-channel attack on the electronics of a quantum
key distribution sender is demonstrated analyzing radiofrequency emissions using neural networks. It can extract almost all secret key at a few centimeters from thedevice.
PP-2.10 WED (Poster pitch of EC-P.1)

12:36

Observation of interaction-induced topological
doublon states∙J. Beck1 , H. Drüeke1 , M.J. Meschede1 , M. Heinrich1 ,F.S. Piccioli1,2 , S. Weidemann1 , D. Bauer1 , and A.
Szameit1 ; 1 Institute for physics, University Rostock, Germany; 2 INO-CNR BEC Center and Dipartimento di
Fisica, Universita‘ di Trento, Italy
We present the first observation of propagating topologically protected doublon states in an anomalous Floquet
driven 1D array. Using dimensional mapping, the two
repulsive interacting particles in 1D were observed in 2D
laser-written waveguide lattices.
PP-2.11 WED (Poster pitch of EH-P.1)

12:40

Holographic Optical Metasurfaces with High Trap Stiffness∙T. Plaskocinski, J. Xiao, M. Biabanifard, S. Persheyev,
and A. Di Falco; University of St Andrews, UK
Photonic metasurfaces have been proposed to create
on-chip solutions for optical trapping applications. We
present a metasurface-enabled on-chip system, capableof trapping extended objects, with performance comparable to a system using high numerical aperture objectives.

121

PP-2.12 WED (Poster pitch of EH-P.16) 12:44

Self-Assembled Deep Ultraviolet Rhodium nanogap
antenna to enhance single protein autofluorescence∙P. Roy1 , S. Zhu2 , J.B. Claude1 , J. Liu2 , and J. Wenger1 ;1
Aix Marseille Univ, CNRS, Centrale Marseille, Institut Fresnel, AMUTech, Marseille, France; 2 Department ofChemistry, Duke University, Durham, USA
Self-assembled label-free detection platform for single
proteins in DUV range using natural autofluorescenceand Rh Dimer gap antenna design, showing 2 orders
higher enhancement than confocal methods and 1 orderhigher than current state-of-the-art techniques.
PP-2.13 WED (Poster pitch of EI-P.6)

12:48

Second-order nonlinearity of excitons in
hBN-encapsulated monolayer transition metal
dichalcogenides∙S. Takahashi1 , S. Kusaba1 , K. Watanabe2 , T. Taniguchi3 ,K. Yanagi4 , and K. Tanaka1,5 ; 1 Department of Physics,
Kyoto University, Kyoto, Japan; 2 Research Center for
Functional Materials, National Institute for Materials Science, Tsukuba, Japan; 3 International Center for Materials Nanoarchitectonics, National Institute for Materials
Science, Tsukuba, Japan; 4 Department of Physics, Tokyo
Metropolitan University, Tokyo, Japan; 5 Institute for Integrated Cell-Material Sciences, Kyoto, Japan
P-series excitons besides s-series were observed by sum
frequency generation spectroscopy in monolayer transition metal dichalcogenides. New insights into nonlinear
optical responses were obtained from energy level structures and polarization dependences.

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Room 4b ICM

Room 13a ICM

Room 13b ICM

Room 14a ICM

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

JSI-3: Imaging geometric andelectronic structures

CK-6: Integrated opticaldevices I

JSIV-2: Thermal radiationand photovoltaics

CA-7: Power scaling

CB-6: Integrated photonics
and frequency combs

CD-9: Nonlinear dynamics II

Chair: Cristian Svetina, IMDEA,
Madrid, Spain

Chair: Joyce Poon, Max-PlanckInstitute for Microstructure Physics,
Halle, Germany

Chair:
Esther Alarcon Llado,
AMOLF, Amsterdam, The Netherlands

JSI-3.1 WED (Invited)

CK-6.1 WED (Invited)

14:00

JSIV-2.1 WED (Invited) 14:00

CA-7.1 WED (Tutorial) 14:00

CB-6.1 WED (Keynote) 14:00

CD-9.1 WEDLighting up the brain: Implantable neural probes using waferscale integrated photonics∙J. Poon; Max Planck Institute of Microstructure Physics, Halle (Saale),Germany; University of Toronto,
Toronto, Canada
I will present silicon photonic integrated circuits operating in thevisible spectrum that miniaturize
today’s microscopy and fiber optic
tools to enable unique multiphysical and multifunctional interfaces tothe brain for optogenetics and fluorescence imaging.

Incandescent Metasurfaces∙J.-J. Greffet; Université Paris-Saclay,
Institut d’Optique Graduate School,
Palaiseau, France
We introduce the basic concepts ofan incandescent metasurface emphasizing the differences with usual
metasurfaces. We then discuss recent results demonstrating control
of directivity, emission spectrum,
polarization and fast modulation.

Prospects in power scaling of fiber
lasers and amplifiers∙A. Tuennermann; Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany; Friedrich Schiller University
Jena, Institute of Applied Physics,
Jena, Germany
The state of the art of science andtechnology in fiber lasers and amplifiers is reviewed. The prospects
for future developments using advanced fiber designs in combination
with modern laser and amplifier architectures are discussed.

Ultra-low loss hybrid silicon
nitride integrated photonics:
from chipscale frequency combs,
frequency agile lasers to Erbium
amplifiers on chip
∙T.J. Kippenberg; EPFL, Lausanne,
Switzerland
Recent advances allowed to create
ultra-low-loss, meter-long waveguides in silicon nitride. I will review advances of this technology,
from chipscale frequency combs,
parametric amplifiers, ultra-narrow
linewidth lasers with fiber lasercoherence, and erbium amplifierson chip.

Ultrasensitive Dispersive Fourier
Transform Characterization of
Nonlinear Instabilities∙L. Sader1 , S. Bose2,3 , A. Khodadad
Kashi2,3 , Y. Boussafa1 , R. Dauliat1 ,P. Roy1 , M. Fabert1 , A. Tonello1 ,V. Couderc1 , M. Kues2,3 , and B.
Wetzel1 ; 1 XLIM Research Institute,
CNRS UMR 7252, University of
Limoges, Limoges, France; 2 Instituteof Photonics, Leibniz University
Hannover, Hannover, Germany;3
Cluster of Excellence PhoenixD,
Leibniz
University
Hannover,Hannover, Germany
We report on a dispersive Fouriertransform characterization technique using single photon detectors.
We show that this ultrasensitive approach allows the characterizationof nonlinear noise-driven dynamics
with ultra-high resolution andtheoretically unlimited dynamic
range.

14:00

Imaging ultrafast electron dynamics in isolated nanoparticles
B. Senfftleben1 , J. Zimmermann1,2 ,A. Colombo2 , E. Hassanpour
Yesaghi2 , L. Hecht2 , A. Hoffmann1 ,M. Kretschmar1 , K. Kolatzki2 ,B. Kruse3 , B. Langbehn4 , N.
Monserud1 , T. Nagy1 , M. Sauppe2 ,R.M. Tanyag1,4 , J. Tümmler1 ,A. Ulmer4 , T. Möller4 , I. Will1 ,T. Fennel3 , M.J.J. Vrakking1 , A.
Rouzée1 , B. Schütte1 , and ∙D.
Rupp1,2 ; 1 Max Born Institute,
Berlin, Germany; 2 NUX, DPHYS,ETH Zürich, Zürich, Switzerland;
3
Institut für Physik, Uni Rostock,
Rostock, Germany; 4 IOAP, TU
Berlin, Berlin, Germany
We image isolated nanoparticles infree flight with intense pulses from
X-ray free electron lasers and highharmonic sources. The recent advent of intense attopulses even allows to resolve ultrafast changes of
the nanoparticles’ electronic structure.

Chair: Clara Saraceno, University of
Bochum, Bochum, Germany

Chair: Benedikt Schwarz, Technical
University, Wien, Austria

Chair: Ayhan Demircan, Leibnitz
University Hannover, GermanyCD-9.2 WED

14:00

14:15

Genetic algorithm optimization ofbroadband operation in a noiselike pulse fiber laser∙M. Hary1,2 , C. Lapre2 , F. Meng3 , C.
Finot4 , G. Genty1 , and J.M. Dudley2 ;1
Photonics Laboratory, Tampere
University,
Tampere,Finland;2
Université de Franche-Comté,
Institut FEMTO-ST, CNRS UMR
6174, Besançon, France; 3 State Key
Laboratory of Integrated Optoelectronics, College of Electronic Science& Engineering, Jilin University, Jilin,
China; 4 Université de Bourgogne,
Laboratoire
Interdisciplinaire
Carnot de Bourgogne, CNRS UMR
6303, Dijon, France
We use a genetic algorithm to locate the optimal broadband states of
122

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/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

CH-7: Instrumentation for
optical sensing and microscopy

EF-1: Complex fiber dynamics I

CF-8: Ultrafast laser technology II

CI-3: Ultrafast telecommunications

EB-8: Quantum imaging

Chair: Gian-Luca Oppo, Universityof Strathclyde, United Kingdom

Chair: Takao Fuji, Toyota Technological Institute, Nagoya, Japan

Chair: Alessandro Tonello, University of Limoges, France

CJ-4: Specialty fiber characterisation techniques andcomponents

14:00

EF-1.1 WED (Tutorial) 14:00

CF-8.1 WED (Invited)

CI-3.1 WED (Invited)

Fabrication of Chequerboard
Diffraction Grating for Robustand Single-Shot Phase-Shifting
Digital Holography∙T. Maeda1,2 , S. Yanase1,2 , H.
Sotobayashi1 , and K. Akahane2 ;1
AoyamaGakuinUniversity,
2
Sagamihara, Japan;
National
Institute of Information and Communications Technology, Koganei,Japan
A chequerboard diffraction grating
was fabricated to demonstrate robust and single-shot phase-shifting
digital holography. In the experiment, the phase distribution of light
was successfully measured with thesame accuracy as the conventional
four-shot method.

Nonlinear Multimode Fiber
Optics∙S. Wabnitz; Sapienza University ofRome, Rome, Italy
This tutorial will present an
overview of recent research
progress in the field of nonlinear
multimode fiber optics. Phenomena such as multimode solitons,
geometric parametric instability
and beam self-cleaning lead to newtechnological applications.

Novel ultrafast laser technology
for generating gigawatt-classisolated attosecond pulses∙E. Takahashi; RIKEN, Wako, Japan
We introduce two novel lightsources; one is a 6-TW single-cycle
laser system via dual-chirped
optical parametric amplification,and the other is GW-scale isolated
attosecond pulse driven by ahigh-energy 3-channel waveform
synthesis.

Chair: Marco Grande,Politecnico diBari, Italy
CH-7.1 WED

CH-7.2 WED

14:00

14:00

Graphene Plasmonics – A Beyond
100 GHz Technology∙J. Leuthold, S.M. Koepfli, P.
Ma, X. Zhang, M. Baumann, S.
Nashashibi, J. Smajic, U. Koch, and
Y. Fedoryshyn; ETH Zurich, Zurich,
Switzerland
Novel approaches towards new
generations of graphene plasmonic
modulators and detectors withresponses of 500 GHz and beyond are introduced. Important
performance parameters such as
losses, efficiency or responsivity
are addressed by combining thetechnologies.

14:15

Metasurface Confocal – Enablinga Shift in Optical Instrumentation∙D.J. Townend, J. Williamson, D.
Tang, N. Sharma, A.J. Henning, H.
Martin, and X. Jiang; University of
Huddersfield, Huddersfield, United
Kingdom
We present our results showing thecreation of an ultra-compact andlightweight confocal sensor basedon a single metasurface. When
deployed as an integrated sensor
this will help realise smarter andmore automated manufacturing
processes.

Chair:
Laurent Bigot,
University of Lille, France

CNRS-

CJ-4.1 WED

14:00

EB-8.1 WED

14:00

Fiber-modes characterization
using singular value decomposition∙Y. Tu1,2,3 , C.
Pfleghar1 , C.
Jauregui1 , and J. Limpert1,2,3,4 ;1Friedrich-Schiller-Universität Jena,
Institute of Applied Physics, Abbe
Center of Photonics, Albert-EinsteinStr.
15,07745, Jena, Germany;2
Helmholtz Institute Jena, Fröbelstieg 3, 07743 , Jena, Germany;
3
GSI Helmholtzzentrum für Schwerionenforschung,Planckstraße
1, 64291 , Darmstadt, Germany;
4
Fraunhofer Institue for Applied
Optics and Precision Engineering,
Albert-Einstein-Str. 7, 07745 , Jena,
Germany
A novel experimental fiber-modes
characterization method is proposed. This method, unlike theexperimental methods before, canoperate with any light source andany fiber length, which can be used
to characterize more fibers.

Quantum image distillation with
undetected photon beam
J. Fuenzalida1,2 , M. Gilaberte
Basset2,3 , S. Töpfer1,2 , J.P. Torres4 ,and ∙M. Gräfe1,2,3 ; 1 Institute of Applied Physics, Technical University ofDarmstadt, Germany; 2 Fraunhofer
Institute for Applied Optics andPrecision Engineering IOF, Jena,
3
Germany;Friedrich Schiller
University Jena, Abbe Center of
Photonics, Jena, Germany; 4 ICFOInstitut de Ciencies Fotoniques,
The Barcelona Institute of Scienceand Technology and Dept. Signal
Theory and Communications, Universitat Politecnica de Catalunya,
Castelldefels/Barcelona, Spain
We present quantum image distillation of objects in presence ofstrong noise. Our approach is basedon quantum holography with undetected light and exploits quantum
correlated photon pairs and induced
coherence in a nonlinear interferometer.

CJ-4.2 WED

EB-8.2 WED

14:15

Picometer-resolution and highdynamic-range profilometer forhollow-core fiber surface
roughness characterization∙A. Dhaybi1 , J. Osório1 , K. Vasko1 , F.
Amrani1,2 , G. Tessier3 , B. Debord1,2 ,F. Gérôme1,2 , and F. Benabid1,2 ;
1GPPMM Group, XLIM Institute,
CNRS UMR 7252, Limoges, France;
2
GLOphotonics, Limoges, France;
3
Institut de la Vision, CNRS UMR
7210, INSERM, Sorbonne University,
Paris, France
Large dynamic and picometerresolution
surface-roughnessprofilometer for varied types of
HCPCF is reported.
Measurement of the two surfaces HCPCF
cladding-silica-membrane is ob123

Chair: Miles Padgett, University ofGlasgow, UK

14:15

Mid-infrared quantum scanningmicroscopy with visible light∙J.R. León-Torres1,2 , J. Fuenzalida1 ,M. Gilaberte Basset1 , S. Töpfer1 , and
M. Gräfe3 ; 1 Fraunhofer Instituteof Applied Optics and Precision
Engineering IOF, Jena, Germany;
2
Institute of Applied Physics,
Friedrich-Schiller-Universität Jena,
Jena, Germany; 3 Institute of Applied
Physics,
Technische Universität
Darmstadt, Jena, Germany
A label-free quantum scanning
imaging system is presented,
capable of detecting in the visible
regime, while illuminating with
undetected light in the Mid-IR
region by exploiting the quantum
correlations of photon-pairs.

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Room 4b ICM

Room 13a ICM

Room 13b ICM

Room 14a ICM
a noise-like pulse fiber laser around1550 nm. The broadest bandwidths
spanning 100’s of nm are automatically found within only a few generations.

JSI-3.2 WED

14:30

Visualization of Light-induced
Transitions in Dielectric-metallic
Nanoparticles with Intense X-ray
Pulses∙Z. Sun1 , K. Schnorr1 , A. Al
Haddad1 , S. Augustin1 , A.S. Morillo
Candas1 , G. Knopp1 , J. Knurr1,2 ,A. Sarracini1 , X. Xie1 , N. Yang1,2 ,H. Zhang1,2 , and C. Bostedt1,2 ;1Paul Scherrer Institut, Villigen PSI,
Switzerland; 2 Ecole PolytechniqueFédérale de Lausanne, Lausanne,
Switzerland
We demonstrated time-resolved
single-shot single-particle imaging
of ultrafast laser induced phasetransitions of free-flying dielectricmetallic core-shell nanoparticles
from femto- to nanosecond withintense X-ray free-electron lasers at
SwissFEL.
JSI-3.3 WED

14:45

Imaging laser-driven dynamics inmaterials with atomic resolution
and in real time with ultrashort
x-ray pulses∙D. Gorelova; I. Institute for Theoretical Physics, University of Hamburg,
Hamburg, Germany
Based on a rigorous theoretical analysis, we propose a novel method ofimaging real-time optically-driven
electron dynamics in materials bymeans of attosecond x-ray pulses.

CK-6.2 WED

14:30

JSIV-2.2 WED

14:30

CD-9.3 WED

Mid-infrared photonic integrated
platform based on Fe-doped
InGaAs buried in InP∙M. Montesinos Ballester, E. Jöchl, R.
Wang, P. Täschler, Z. Wang, E. Gini,
M. Beck, and J. Faist; Institute forQuantum Electronics, ETH-Zurich,
Zürich, Switzerland
In this work we present a midinfrared photonic integrated platform based on Fe-doped InGaAs
waveguides buried in InP, demonstrating propagation losses as low as
0.57 dB/cm at 4.6 μm wavelength in
TM polarization.

The contribution has been withdrawn.

CK-6.3 WED

14:45

JSIV-2.3 WED (Invited) 14:45

CB-6.2 WEDOptical Power Splitters for Integrated Multimode Photonics∙J. Haines1 ,V. Vitali1 ,P.
Petropoulos1 , C. Lacava1,2 , K.
Bottrill1 , M. Gandolfi3 , C. De
Angelis3 , Y. Franz1 , and M.
Guasoni1 ; 1 Optoelectronics ResearchCentre, University of Southampton,
Southampton, United Kingdom;2
Department of Electrical, Computer and Biomedical Engineering,
University of Pavia, Pavia, Italy;
3
CNR-INO and Department ofInformation Engineering, Universityof Brescia, Brescia, Italy
Compact 1xN integrated power
splitters for both the fundamental
and higher order modes are fabricated and tested. Our devices
are based on arrays of coupledwaveguides with non uniform
spacing allowing for arbitrary
power splitting.

Diffused light concentration forenhanced solar energy yield∙R. Saive; University of Twente, Enschede, Netherlands
We report on a photonic system capable of collimating diffuse light infree space and investigate how sucha system can open up new possibilities for harvesting solar energy
through light emission onto solar
panels.

Self-generation of opticalfrequency combs in III-V/SiN
external cavity laser withfrequency-selective mirror∙C. Rimoldi, L.L. Columbo, and M.
Gioannini; Dipartimento di Elettronica e Telecomunicazioni, Politecnico di Torino, Torino, Italy
We theoretically and numericallyinvestigate the mechanism behindthe spontaneous generation of frequency comb regimes in III-V SiN
hybrid lasers with a narrowband
mirror, displaying both amplitudeand frequency modulation.

124

14:30

Dynamics of Raman Cavity Solitons in Passive Kerr Resonators∙Z. Li1 , Y. Xu1 , S. Shamailov1 , X.
Wen2 , W. Wang2 , X. Wei2 , Z. Yang2 ,S. Coen1 , S.G. Murdoch1 , and M.
Erkintalo1 ; 1 Department of Physics
and The Dodd-Walls Centre, University of Auckland, Auckland, New
Zealand; 2 School of Physics and Optoelectronics, South China Universityof Technology, Guangzhou, China
In this contribution, we explore themulti-pulsing dynamics of the dissipative Raman solitons, demonstrating that a variety of multi-soliton
states can be deterministically generated and that the resultant solitons
display complex behaviours.
14:45

CD-9.4 WED

14:45

Two-frequency pulse compounds
in presence of a zero-nonlinearity
point∙O. Melchert1,2 , S. Bose2,3 , S.
Willms1,2 , I. Babushkin1,2 , U.
Morgner1,2 , and A. Demircan1,2 ;1Leibniz Universität Hannover,Institute of Quantum Optics,
Hannover, Germany; 2 Cluster of
Excellence PhoenixD, Hannover,3
Germany;
Leibniz Universität
Hannover, Institute of Photonics,
Hannover, Germany
We discuss the complex propagation dynamics of two-frequency
pulse-compounds in waveguides
with single zero-dispersion andzero-nonlinearity points.
We
demonstrate that under the impactof the Raman effect, a higher-ordertrapped state transitions into thegroundstate.

CLEO

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/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)tained for the first-time. The results
confirm the newly-developed technique to reduce surface-roughness
with shear-stress.
CH-7.3 WED

14:30

CF-8.2 WED

14:30

CI-3.2 WED

14:30

CJ-4.3 WED

14:30

Frequency-Controlled Dot
Pattern Projection of Ultrashort
Pulse using Optical Phased Array
Based on Optical Frequency
Comb∙T. Kato1,2 and K. Minoshima1 ;1The
UniversityofElectroCommunications (UEC), Tokyo,
2
Japan; PRESTO, JST, Tokyo, JapanWe demonstrated a dot patternprojection of ultrashort pulse bypulse-to-pulse interference using an
optical-phased array based on an
optical frequency comb by changing
the ratio of two frequency parameters of the comb.

Intra-Cavity Femtosecond
Standing Waves for Multi-Photon
Pump-Probe Experiments at
100 MHz∙T. Heldt1,2 , J.-H. Oelmann1,2 , L.
Guth1,2 , N. Lackmann1 , J. Nauta1,2 ,T. Pfeifer1 , and J.R. Crespo LópezUrrutia1 ; 1 Max-Planck-Institut fürKernphysik, Heidelberg, Germany;2
Heidelberg Graduate School for
Physics, Heidelberg, Germany
Enhancing frequency combs in cavities adds to their high coherence andmegahertz repetition rate the highintensities needed for strong-field
physics. Our approach also generates femtosecond standing waves atthe cavity focus.

Ultra-broadband UTC-PD using
well-optimized InGaAs/InP active
layer toward 200-GHz bandwidthand beyond∙T. Umezawa, S. Nakajima, A. Matsumoto, K. Akahane, and N. Yamamoto; National Institute of Information and Communications Technology, Tokyo, Japan
We present an ultra-broadband
high-speed UTC-PD using welloptimized and extremely thin
active layers to achieve 200-GHz
bandwidth and beyond.
Thecharacteristics of the fabricateddevice are discussed, along with thesimulation results.

Fibre Bragg Gratings Inscribed in
Dy-doped InF3 Fibre Using Talbot
Interferometer and Vis-fs-Laser∙K. Grebnev and M. Chernysheva;
Leibniz Institute of Photonic Technology, Jena, Germanyn this work we present inscription
Bragg grating in Dy-doped InF3
fiber using Talbot interferometerand visible femtosecond laser. Optical properties, process of thermal
annealing and ways of inscription
optimization are described.

CH-7.4 WED

CF-8.3 WED

CI-3.3 WED

CJ-4.4 WED

14:45

Birefringent elements for optical
microscopy by ultrafast laser
writing∙Y. Lei1 , P. Kazasky1 , and M.
Shribak2 ; 1 Optoelectronics ResearchCentre, University of Southampton,
Southampton, United Kingdom;
2
Marine Biological Laboratory,
University of Chicago, Woods Hole,
MA, USA
Geometric phase prisms (GPprisms) and retardance gradientprisms (X prisms) are demonstrated
by ultrafast laser writing in silica
glass and are used for differential
interference contrast imaging, withthe potential to replace Wollaston
prisms.

14:45

Nanojoule-level spectrally tunable
all-PM mode-locked Yb:fiber laser∙S. Ebrahimzadeh1 , S. Adnan1 ,V. Shumakova2,3 , V.F. Pecile2,4 ,J. Fellinger2 , M. Leskowschek2 ,P.E.C. Aldia2,4 , A.S. Mayer2 ,L.W. Perner2,4 , S. Salman5,7,8 , S.
Schilt6 , C.M. Heyl5,7,8 , I. Hartl5 ,O.H. Heckl2 , and G. Porat1,9 ;1Department of Electrical andComputer Engineering, Universityof Alberta, Edmonton, Alberta
T6G 1H9,, Edmonton, Canada;
2
Christian Doppler Laboratory
for Mid-IR Spectroscopy and
Semiconductor Optics,
Faculty
Center for Nano Structure Research,
Faculty of Physics, University of
Vienna,1090, Vienna, Austria;
3
Photonics Institute, TU Wien,1040,
Vienna, Austria; 4 Vienna Doctoral
School in Physics, University of
Vienna, 1090, Vienna, Austria;
5
Deutsches Elektronen-Synchrotron
DESY, 22607, Hamburg, Germany;
6
Laboratoire
Temps-Fréquence,
Université de Neuchâtel, CH-2000,
7
Neuchâtel,Switzerland;
GSI

14:45

SOA-Based Power Equalisationfor 100 Gb/s Passive Optical
Network∙F. Jamali, S.L. Murphy, C. Antony,and P.D. Townsend; Tyndall National Institute, University College
Cork, Cork, Ireland
SOA-based optical power equalisation using variable bias and control
light injection are investigated for
100 Gb/s PAM4 PON. A high dynamic range of 23 dB is achieved,and gain saturation induced patterning effects are studied.

125

14:45

Spatial coherence characterizationin multimode fibers∙J. Li, P. Ryczkowski, and G. Genty;
tampere university, Tampere, Finland
We characterize experimentally thespatial coherence of a step-index
multimode fiber coupled broadband
light across the full beam profile. Our experimental observations
agree with numerical simulations
using a random mode coupling theoretical model.

EB-8.3 WED

14:30

Experimental separation estimation of incoherent optical sources
reaching the Cramér-Rao bound∙C. Rouvière1 , D. Barral1 , A.
Grateau1 ,G.
Sorelli1,2 ,I.
Karuseichyk1 , M. Walschaers1 ,and N. Treps1 ; 1 Laboratoire Kastler
Brossel, ENS-Université PSL, CNRS,
Sorbonne Université, Collège deFrance, Paris, France; 2 Fraunhofer
IOSB, Ettlingen, Fraunhofer Instituteof Optronics, System Technologies
and Image Exploitation, Ettlingen,Germany
We experimentally implement the
separation estimation between toincoherent optical sources. Our
method, relying on spatial-mode
demultiplexing and intensity measurements, saturates the CramérRao bound, with five orders ofmagnitude gain compared to theRayleigh limit.
EB-8.4 WED

14:45

Resolution of quantum imaging
with undetected photons via
position correlations∙M. Gilaberte Basset1,2 ,R.
Sonderheimer1,3 , J. Fuenzalida4 ,A. Vega2 , S. Töpfer4 , E. Santos2 , F.
Setzpfandt2 , F. Steinlechner1,2 , and
M. Gräfe1,2,4 ; 1 Fraunhofer Institutefor Applied Optics and Precision
Engineering IOF, Jena, Germany;
2
Friedrich-Schiller-University,
Institute of Applied Physics, Jena,
3
Germany;Friedrich-SchillerUniversity, Institute of Condensed
Matter Theory and Optics, Jena,
Germany; 4 Institute of Applied
Physics, Technical University ofDarmstadt, Darmstadt, Germany
We present experimental resolution
results for imaging with undetected
photons via position correlations.
These support the theory published
to date, nevertheless showing theCLEO

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⋅ Wednesday 28 June 2023

Room 4b ICM

Room 13a ICM

Room 13b ICM

Room 14a ICM

15:00

Ultrafast orbital tomography of amolecular film at a FEL∙M. Scholz1 , K. Baumgärtner2 , N.
Wind3 , M. Reuner4 , M. Heber1 ,D. Kutnyakhov1 , L. Wenthaus1 ,M. Beye1 , F. Reinert2 , F. Roth5 ,K. Niki6 , D. Popova-Gorelova4 ,and K. Rossnagel1,7 ; 1 Deutsches
Elektronen-Synchrotron
DESY,
Notkestraße 85, Hamburg, Germany; 2 Experimentelle Physik 7,
Julius-Maximilians-Universität, Am
Hubland, Würzburg, Germany;3
Institut für Experimentalphysik,
Universität Hamburg,
Luruper
Chaussee 149, Hamburg, Germany;
4
I. Institute for Theoretical Physics,
Universität Hamburg,
Luruper
Chaussee 149, Hamburg, Germany; 5 Institute of Experimental
Physics, TU Bergakademie Freiberg,
Leipziger Straße 23, Freiberg, Germany; 6 Graduate School of Scienceand Engineering, Chiba University,
1-33 Yayoi-cho, Inage-ku, Chiba,
Japan; 7 Institut für Experimentelle
und Angewandte Physik, ChristianAlbrechts-Universität zu Kiel, Kiel,
Germany
Flow of charge and energy acrossthe molecule-substrate interface areof essential importance for surface
chemistry and novel devices. By
shooting a ‘molecular movie’ at a
FEL, we disentangle electronic andstructural dynamics.
JSI-3.5 WED

®

15:15

Sub-wavelength Charge Dynamics
in Textured Infrared and Free
Electron Lasers
J. Wätzel1 , P.R. Ribič2 , M. Coreno2,3 ,M.B.
Danailov2 , C. David4 ,A. Demidovich2 , M. Di Fraia2 ,L.
Giannessi2,5 , K.
Hansen6 ,Š. Krušič7 , M. Manfredda2 , M.
Meyer8 , A. Mihelič7 , N. Mirian2,9 ,O. Plekan2 , B. Ressel10 , B. Rösner4 ,A. Simoncig2 , S.
Spampinati2 ,M. Stupar10 , M. Žitnik7 , M.
Zangrando2,11 , C. Callegari2 , G.D.
Ninno2,10 , and ∙J. Berakdar1 ;1
Martin-Luther University Halle-CK-6.4 WED

15:00

CA-7.2 WEDUltra-low loss mid-infrared
frequency conversion insilicon-on-insulator waveguides∙D.A. Sulway1 , Y. Yonezu2,3 , L.M.
Rosenfeld1 , P. Jiang1 , T. Aoki3 , andJ.W. Silverstone1 ; 1 Quantum Engineering Technology Labs, Bristol, United Kingdom; 2 NTT Basic
Research Laboratories, Kanagawa,Japan; 3 Waseda University, Tokyo,
Japan
We demonstrate stimulated fourwave mixing with the use of ultralow loss adiabatic fibre-chip couplers at 2.1 microns in silicon. We
measure -0.48 dB of coupler transmission, and subsequently a broad
40 nm four-wave mixing bandwidth.

CK-6.5 WED

15:15

Resonant Micro-Opto-Mechanical
Phase Modulator Fabricated in
Glass by a Femtosecond Laser
R. Memeo1,2 , ∙A. Crespi1,2 , and R.
Osellame2,1 ; 1 Dipartimento di Fisica- Politecnico di Milano, Milano,
Italy; 2 Istituto di Fotonica e Nanotecnologie - Consiglio Nazionale delle
Ricerche (IFN-CNR), Milano, Italy
We demonstrate an integrated optics modulator based on the elastooptic effect, exploiting the resonant
oscillations of a mechanical microstructure and operating at megahertz frequency. The device is en-

JSIV-2.4 WED

15:15

Light management forphotovoltaics and a European PV
industry∙A. Polman; NWO Institute AMOLF,
Amsterdam, Netherlands
We present novel light management strategies to develop flexible, integrated and ultra-high efficiency photovoltaics using spectrum splitting, contact cloaking, radiative cooling and triple-junction
tandems and promote a new European PV industry.

15:00

CB-6.3 WED

15:00

CD-9.5 WED

15:00

Q-switched Ho:YAG Master
Oscillator Power Amplifier with85 W Average Output Power at 2.1
μm
M.J. Barber, P.C. Shardlow, and∙W.A. Clarkson; Optoelectronics Research Centre, Southampton, United
Kingdom
We report on a two-stage Ho:YAG
MOPA where the pump power isprovided by ten spatially-combined
1907 nm thulium fibre lasers, producing 85 W of average output
power for 320 W of combined pump
power.

Dynamics of Integrated
Multi-Wavelength Lasers with
Optical Frequency Comb
Injection∙S. Abdollahi, P. Marin-Palomo, and
M. Virte; Brussels Photonics Team
(B-PHOT), Vrije Universiteit Brussel, Brussels, Belgium
We demonstrate experimentallythat subjecting multi-wavelength
lasers to frequency comb injection
leads to broadening and multiplication of the original comb. We
achieve comb multiplication up to
a 1 THz and highlight the mode
coupling impact.

Unveiling the Volumetric Orbital
Angular Momentum Density Flowof Light by Symmetry Breaking of
its Second Harmonic∙O. Yesharim1 , I. Hurvitz1 , S.
Pearl1,2 , A. Karnieli1 , and A. Arie1 ;1
Tel Aviv University, Tel Aviv, Israel;
2
Soreq NRC, Yavne, Israel
Optical orbital angular momentum
beams exhibit hidden rotational energy flow that varies in three dimensional space. We present a nearlynon-destructive measurement thatallows for volumetric orbital density
flow determination using nonlinear
optical symmetry breaking.

CA-7.3 WED

CB-6.4 WED

CD-9.6 WED

15:15

All optical-parametric-amplification technic based high-energy
laser front-end∙L. Lafargue1,2 , G. Dalla-Barba1 ,F. Scol1 , F. Audo1 , O. Vanvincq2 ,G. Bouwmans2 , and E. Hugonnot1 ;1Commissariat à l’Énergie Atomiqueet aux Énergies Alternatives, Centred’Études Scientifiques et Techniques
d’Aquitaine, Le Barp, France; 2 Univ.
Lille, CNRS, UMR 8523 - PhLAM- Physique des Lasers Atomes etMolécules, Lille, France
We set up a high-energy laser frontend which consists of μJ-range

126

15:15

Study of noise transfer in semiconductor frequency combs∙T. Steshchenko, V. Roncin, and F.
Du-Burck; Laboratoire de Physiquedes Lasers,
C.N.R.S./Université
Sorbonne Paris Nord, Villetaneuse,FranceThe noise transfer from the supply
current to the optical modes and the
RF beat of a mode-locked FabryPerot Qdash laser is studied experimentally and the results are interpreted from the theory.

15:15

4-Field Symmetry Breakings in
Microresonator-Based Photonic
Molecules∙A. Ghosh1,2 , L. Hill1,3 , G.-L.
Oppo3 , and P. Del’Haye1,2 ; 1 Max
Planck Institute for the Science ofLight, 91058 Erlangen, Germany;
2
Friedrich Alexander University
Erlangen-Nuremberg, 91058 Erlangen, Germany; 3 University ofStrathclyde, G4 0NG Glasgow,
United Kingdom
We study two different arrangements of photonic molecules andshow nested and sequential symme-

CLEO

Room 14b ICM

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/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt,
Germany; 8 Helmholtz-Institute Jena,
07743, Jena, Germany; 9 Departmentof Physics, University of Alberta,
Edmonton, Alberta T6G 2E1,
Edmonton, Canada
We report on a self-starting all-PM
Yb:fiber laser, based on a phasebiased nonlinear amplifying loop
mirror. The laser wavelength is tunable from 1017nm to 1071nm, withup to 110mW average power and
1.42nJ pulse energy.
CH-7.5 WED

15:00

Single pumped superluminal laser∙Y. Sternfeld1 , Z. Zhou2 , S.
Shahriar2,3 , and J. Scheuer4 ; 1 Tel
Aviv University, Department of
Physics and Astronomy, Tel Aviv,
Israel; 2 Northwestern University,
Department of Electrical andComputer Engineering, Evanston,
USA; 3 Northwestern University, Department of Physics and Astronomy,
Evanston, USA; 4 Tel Aviv University,
School of Electrical Engineering, TelAviv, Israel
We present a new approach for realizing superluminal ring laser using a single isotope of atomic Rbvapor by producing electromagnetically induced transparency (EIT) in
self-pumped Raman gain.

EF-1.2 WED (Invited)

15:00

Guided Brillouin interactions from optical vortex isolators to
extreme thermodynamics∙B. Stiller; Max Planck Institutefor the Science of Light, Erlangen, Germany; University ErlangenNuremberg, Erlangen, Germany
We
investigate
BrillouinMandelstam
interactionsofvortex modes with application tononreciprocal devices and lasers intwisted photonic crystal fibers. In
liquid-core fibers, we use optoacoustics to experimentally explore
different thermodynamic regimes
such as negative pressure.

CF-8.4 WED

15:00

Room 8 Hall A1 (A12)use for a more general analytical expression that we also provide.

CI-3.4 WED

15:00

CJ-4.5 WED

15:00

Conversion of Mode-Locked
States within an Empty Optical
Resonator∙M. Zwilich, F. Schepers, and C. Fallnich; University of Münster, Instituteof Applied Physics, Münster, Germany
A longitudinal mode-locked beam
is converted to a transverse modelocked beam by an empty optical resonator.
Equivalently, anamplitude-modulated beam is converted to a beam periodically moving across the transverse plane.

Graphene photonics nested
Mach-Zehnder modulator foradvanced modulation formats∙V. Sorianello1 , A. Montanaro1 ,M.A. Giambra2 ,N. Ligato2 ,W. Templ3 , P. Galli4 , and M.
Romagnoli1 ; 1 Photonic Networks
and Technologies Lab – CNIT,
Pisa, Italy; 2 CamGraPhIC srl,
INPHOTEC, Pisa, Italy; 3 Nokia BellLabs, Stuttgart, Germany; 4 Nokia
Solutions and Networks Italia,
Vimercate, Italy
We show the first graphene photonics I/Q modulator based on electroabsorption modulators on silicon
photonic waveguides. We show
40Gb/s QPSK modulation with very
compact design able to operate fromthe O-band to L-band and beyond.

Hybrid Silica-Fluoride
Side-polished Fiber Pump
Combiner∙B. Perminov and M. Chernysheva;
Leibniz Institute of Photonic Technology, Thüringen - Jena, Germany
In this work we present the hybrid
silica-fluoride side-polished fiber
pump combiner.
By adjusting
their relevant position via X-Y
and rotation stage maximum
coupling coefficient of 60% has
been achieved.

CF-8.5 WED

CI-3.5 WED

CJ-4.6 WED

EB-8.5 WEDEB-8.6 WED
CH-7.6 WED

15:15

Miniature spectrometer based ona rotated chirped volume Bragg
grating∙M. Yessenov, O. Mhibik, L. Mach,
L. Glebov, A. Abouraddy, and I. Divliansky; CREOL, University of Central Florida, Orlando, USA
We introduce a compact spectrum
analyzer based on a new opticalcomponent – rotated chirped volume Bragg grating – with a compact
footprint capable of pulse stretching
and compression without the needfor free space propagation.

15:15

Intra-pulse Intensity Noise
Shaping in a Mode-locked Fiber
Oscillator∙M. Edelmann1,2 , M. Pergament1 ,and F.X. Kärtner1,2 ; 1 Deutsches
Elektronen-Synchrotron
DESY,
Center for Free-Electron Laser
Science CFEL, Hamburg, Germany;
2
Department of Physics, Universität
Hamburg, Hamburg, Germany
We demonstrate intra-pulse intensity noise shaping in a mode-locked
fiber oscillator.
The intrinsic
re-shaping of intra-pulse intensity
noise distributions enables efficient

15:15

All-Optical Hard Limiter Using
Quantum-Dot SOA-based MZIs
∙H. Yashima and Y. Uji; Tokyo University of Science, Tokyo, JapanAn all-optical hard limiter using
quantum-dot semiconductor optical amplifier-based Mach-Zehnderinterferometers is proposed. We
show that the proposed device has
characteristics close to those of an
ideal hard limiter and eliminates
noise.

127

15:15

Femtosecond laser-written waveguides and couplers for integrated
mid- infrared photonic devices
T. Fernandez1,2 , S. Gross3 , M.
Withford1 ,B. Johnston1 ,T.
Gretzinger1 , S. Rehman1 , and ∙A.
Fuerbach1 ; 1 School of Mathematicaland Physical Sciences, Macquarie
University,
Sydney,Australia;
2
University of South Australia,
Laser Physics and Photonics Devices
Laboratories, Adelaide, Australia;
3
School of Engineering, Macquarie
University, Sydney, Australia
We report the fabrication of fiber-

15:00

Compact Infrared Imaging Using
Undetected Visible Photons With
Rapid Analysis∙E. Pearce1 , N.R. Gemmell1 , J.
Flórez1 , J. Ding1 , C.C. Phillips1 ,R.F. Oulton1 , and A.S. Clark1,2 ;1Department of Physics, Blackett
Laboratory, Imperial College London, London, United Kingdom;
2
Quantum Engineering Technology
Labs, University of Bristol, Bristol,
United Kingdom
We present a compact, portablenonlinearinterferometerforinfrared imaging with visible
detection, including rapid data
analysis of transmission and phase.
The device is robust to operation
outside the laboratory.
15:15

Fourier-transform mid-infrared
spectroscopy using nonlinear
interferometers∙J. Kunz, C. Lindner, S. Herr, S.
Wolf, J. Kiessling, and F. Kühnemann; Fraunhofer IPM, Freiburg,
Germany
Nonlinear interferometers basedon correlated photon pairs allow
mid-infrared spectroscopy with
only near-infrared detection. We
use this measurement concept
in combination with Fouriertransform processing to perform
spectroscopic analysis of multi-gas
samples.

CLEO®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 ICM

Room 4a ICM

2

Wittenberg,
Halle,
Germany;
Elettra-Sincrotrone, Trieste, Italy;
3
ISM-CNR, in Basovizza Area
Science Park, Trieste, Italy; 4 Paul
Scherrer Institut, Villigen-PSI, Villigen, Switzerland; 5 INFN-LNF, Via
E. Fermi 40, Frascati , Italy; 6 Center
for Joint Quantum Studies andDepartment of Physics, School of Science, Tianjin University, China; 7 J.
Stefan Institute, Jamova cesta, Ljubljana, Slovenia; 8 European XFEL,
Hamburg, Germany; 9 Deutsches
Elektronen-Synchrotron(DESY),
Hamburg, Germany; 10 University
11of Nova Gorica, Slovenia; Istituto
Officina dei Materiali, Consiglio
Nazionale delle Ricerche, Trieste,
Italy
Combining structured XUV and infrared laser pulses allow the control
of localized and delocalized chargecurrent distributions on femtoseconds/nanometer time-length scales
within the laser spots. Applications
to ultrafast spintronic and quantum
information are presented.

tirely realized in glass by femtosecond laser micromachining.

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

JSI-4: Nonlinear and ultrafast X-ray spectroscopy

CK-7: Integrated opticaldevices II

EH-1: Temporal and topological metamaterials

CA-9: Waveguide lasers

CB-7: Diode laser frequency
combs

CD-10: Resonant structures

Chair: Rebecca Boll, EuXFEL, Schenefeld, Germany

Chair: Stefano Pelli, CNR-IFAC,
Sesto Fiorentino, Italy

Chair: Nicolò Maccaferri, UmeåUniversity, Sweden

JSI-4.1 WED

CK-7.1 WED (Invited)EH-1.1 WED (Invited)

16:00

Following site-selective chemicalbond changes via ultrafast X-ray
photoelectron spectroscopy
A. Al Haddad1 , S. Oberli2 , A.
Picon3 , J. Knurr1,2 , S. Augustin1 , G.
Knopp1 , A.S. Morillo-Candas1 , E.
Prat1 , Z. Sun1 , K. Schnorr1 , and ∙C.
Bostedt1,2 ; 1 Paul Scherrer Institute,Villigen PSI, Switzerland; 2 Ecole
Polytechnique Federale de Lausanne(EPFL), Lausanne, Switzerland;
3
Universidad Autonoma de Madrid,
Madrid, Spain
We demonstrate howto trackelectronic and nuclear dynamics
on the femtosecond time scalewith site selectivity using ultrafast
time-resolved photoelectron spec-

Room 4b ICM

16:00

Femtosecond-Laser Written
Universal Photonic Processors∙F. Ceccarelli1 , C. Pentangelo2,1 ,N. Di Giano2,1 , R. Arpe2 , S.
Piacentini1,2 , A. Crespi2,1 , and
R. Osellame1 ; 1 Istituto di Fotonica e Nanotecnologie - Consiglio
Nazionale delle Ricerche (IFNCNR), Milano, Italy; 2 Dipartimento
di Fisica - Politecnico di Milano,
Milano, Italy
Universal photonic processors(UPPs) are an enabling technology
for many applications. Two 6-mode
UPPs (785 and 1550 nm) fabricatedby femtosecond laser micromachining show an unprecedented
reconfiguration fidelity.
Their

Room 13a ICM

Room 13b ICM

Room 14a ICM

FOPCPA source coupled to a poweramplifier free-space OPCPA, to get
more than 200 mJ at 1053-nmcentral-wavelength with a repetition
rate of 2 Hz.

16:00

Topological Phases of Spacetime
Crystals
J. Serra and ∙M. Silveirinha; University of Lisbon, Lisboa, Portugal
Heuristically, nontrivial topologies
are associated with some form ofangular momentum.
Surprinsingly, here, we find that nontrivial topological phases and synthetic
spacetime-rotations can be engineered in temporal-crystals that imitate a translational motion withuniform velocity.

Chair: Michael Damzen, Imperial
College London, United Kingdom

CA-9.1 WED

16:00

Multi-GHz Femtosecond Modelocking and Noise Characterization of fs-laser-inscribed Waveguide Lasers∙J.E. Bae1 , M. Hyun2 , X. Mateos3 ,M. Aguiló3 , F. Díaz3 , C. Romero4 ,J.R.V. de Aldana4 , J. Kim2 , and
F. Rotermund1 ; 1 Department of
Physics, KAIST, Daejeon, South
Korea; 2 Department of MechanicalEngineering,
KAIST, Daejeon,South Korea; 3 Universitat Rovira
i Virgili (URV), Tarragona, Spain;
4
University of Salamanca, Spain
Multi-GHz femtosecond modelocked Yb:KLuW waveguide lasers
and their characteristics of noise
spectra are investigated.
The

128

try breakings along with switching
regimes. The results show the possibility of developing all optical fourway optical switches.

Chair: Michael Haider, Technical
University of Munich, Germany
CB-7.1 WED

16:00

Subharmonic Optical Injection
Locking of a Mode-locked Laser
Diode∙A.F. Ribeiro1 , T. Gomes1,2 , and
M.A. Cataluna1 ; 1 Institute of
Photonics and Quantum Sciences,
Heriot-Watt University, Edinburgh,
United Kingdom; 2 IFIMUP and Departamento de Física e Astronomia,
Faculdade de Ciências, Universidade
do Porto, Porto, Portugal
We demonstrate subharmonic dualtone optical injection locking of a
20GHz quantum-dot mode-locked
laser diode, at driving frequencies of
10, 5, and 2.5GHz. Broad repetition
rate tunabilities (hundreds of MHz)are achieved for all orders.

Chair: Ingo Breunig, University ofFreiburg, Germany

CD-10.1 WED

16:00

Investigation on Optical Parametric Oscillators Based on Different
Silicon Nitride Waveguide Geometries∙M. Gao1 , N.M. Lüpken1 , K.-J.
Boller2,1 , and C. Fallnich1 ; 1 Instituteof Applied Physics, University of
Münster, Germany; 2 University ofTwente, MESA+ Institute for Nanotechnology, Enschede, Netherlands
We identify synchronously pumped
silicon nitride waveguide-based optical parametric oscillators, showing
a significantly improved output energy of 255 pJ and conversion efficiency of 17 % while achieving 176
nm wavelength tunability at around1.15 μm.

CLEO

Room 14b ICM

Room Osterseen ICM®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

periodic noise suppression of thecirculating intra-cavity pulse.

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)

coupled integrated photonic devices
in three different mid-infrared compatible glasses using the femtosecond laser direct-write technique anddiscuss the physical origin of the induced refractive index change.

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

CH-8: Methods in opticalsensing and microscopy

EF-2: Kerr solitons andfrequency combs I

CF-9: Ultrafast spectroscopy

CI-4: Fibers for telecommunications and THz

CJ-5: Novel fiber lasers

EB-9: Quantum communication

Chair: Meritxell Vilaseca,Universitat
Politecnica de Catalunya, Terrassa,
Barcelona,Spain

Chair: Svetlana Gurevich, Universityof Münster, Germany, Münster, GermanyCH-8.1 WED

EF-2.1 WED (Invited)

16:00

Telecentric Correlation Holography: A Novel Method to Record
Fresnel Incoherent Correlation
Holograms∙T. Spellauge and T. Hellerer; Multiphoton Imaging Laboratory, University of Applied Sciences Munich,Lothstr. 34, 80335 Munich, Germany
We present a novel holographic system capable of generating laterally
shift-invariant holograms using incoherent sources like LEDs. Our
self-referencing interferometer contains windows with carefully chosen properties, which enable nearperfect spatio-temporal superposition of both light fields.

16:00

Thermal Effects in Kerr-Microresonator Optical Frequency Combs∙T. Drake, G. Colacion, L. Rukh, E.
Perez de Juan, and B. Stone; University of New Mexico, Albuquerque,USA
We present an experimental investigation of thermodynamic instabilities in Kerr-microresonator opticalfrequency combs. By understanding
and harnessing the coupling of thermal effects to properties of the comb
light, we can improve comb precision and performance.

Chair: Birgitta Bernhardt, University of Technology, Graz, Austria

CF-9.1 WED

16:00

High-sensitivity coherent dualcomb spectroscopy with singlecavity dual-comb OPO operating
at 250 MHz∙C. Phillips, C. Bauer, J. Pupeikis,
B. Willenberg, and U. Keller; ETH
Zurich, Zurich, Switzerland
We demonstrate high-sensitivity
dual-comb spectroscopy from afree-running optical parametricoscillator pumped by a picosecond
solid-state laser.
Both cavities
leverage spatial multiplexing toobtain two combs in one cavity withultralow noise and high power.

Chair: Peter Horak, University ofSouthampton, United Kingdom

Chair: Jayanta Sahu, Univ ofSouthampton, Southampton, United
Kingdom

CI-4.1 WED

CJ-5.1 WED

16:00

Optimizing the Capacity ofStandard Cladding Diameter
Multicore Fiber Systems using S,
C, and L Bands∙R. Luis, G. Rademacher, B. Puttnam, J. Sakaguchi, and H. Furukawa; NICT, Koganei, Japan
We optimize the core count in standard cladding diameter multicore
fibers to maximize capacity by exploiting the crosstalk wavelength
dependency. Introducing the S bandin C+L band systems increases the
optimum core count to 5.

129

16:00

Radially polarized picosecond
MOPA system based on doubleclad ytterbium-doped spun
tapered fiber with ring-shaped
active core
∙I. Zalesskaia1 , E. Motorin2 , V.
Ustimchik2 , F. Lindner3 , V. Reichel3 ,K. Wondraczek3 , Y. Lei4 , P. G.
Kazansky4 , R. Gumenyuk1,2 , and
V. Filippov2 ; 1 Tampere University,
Tampere, Finland; 2 Ampliconyx Ltd,
Tampere, Finland; 3 Dept. Leibniz
Institute of Photonic Technology e.V.,
Jena, Germany; 4 Optoelectronics Research Centre, Southampton, United
Kingdom
We have demonstrated the successful direct amplification of a

Chair: Birgit Stiller, Max Planck Institute for the Science of Light, Erlangen, GermanyEB-9.1 WED

16:00

Multiplexed quantum teleportation from a telecom qubit to amatter qubit through 1 km of
optical fibre
D. Lago-Rivera1 , J.V. Rakonjac1 , ∙S.
Grandi1 , and H. de Riedmatten1,2 ;1Institut de Ciencies Fotoniques,
The Barcelona Institute of Scienceand Technology, Castelldefels, Spain;
2
Institucio Catalana de Recerca i
Estudis Avançats, Barcelona, Spain
We report temporally multiplexed
quantum teleportation from a telecom qubit onto a solid-state quantum memory separated by 1 km of
optical fibre. An active feed-forward
scheme is implemented on the teleported qubit.

CLEO

Room 1 ICM

Room 4a ICM

troscopy with an x-ray pump / x-ray
probe approach at a free-electron
laser source.

performance dramatically improvesin vacuum.

JSI-4.2 WED®

/Europe-EQEC 2023

Room 4b ICM

Room 13a ICM

16:15

CA-9.2 WED

16:30

Unraveling Rabi dynamics with aseeded FEL at XUV wavelength∙S. Nandi1 , E. Olofsson2 , M.
Bertolino2 , S. Carlström2 , F.
Zapata2 , D. Busto2 , C. Callegari3 ,M. Di Fraia3 , P. Eng-Johnsson2 ,R. Feifel4 , G. Gallician5 , M.
Gisselbrecht2 ,S. Maclot2 ,L.
Neoričić2 , J. Peschel2 , O. Plekan3 ,K.C. Prince3 , R.J. Squibb4 , S.
Zhong2 , P.V. Demekhin6 , M.
Meyer7 , C. Miron5 , L. Badano3 ,M.B. Danailov3 , L. Giannessi3 , M.
Manfredda3 , F. Sottocorona3 , M.
Zangrando 3 , and J.M. Dahlström2 ;1
Université de Lyon, Université
Claude Bernard Lyon 1, CNRS,
Institut Lumière Matière, Villeurbanne, France; 2 Department of
Physics, Lund University, Lund,
Sweden; 3 Elettra-Sincrotrone Trieste, Trieste, Italy; 4 Department of
Physics, University of Gothenburg,
Gothenburg, Sweden; 5 Université
Paris-Saclay, CEA, CNRS, LIDYL,
Gif-sur-Yvette, France; 6 Institute ofPhysics and CINSaT, University ofKassel, Kassel, Germany; 7 European
XFEL, Schenefeld, Germany

CK-7.2 WED

16:30

Fabrication of AlGaN Integrated
Photonic Devices∙S. Gundogdu1,2 , T. Pregnolato1,2 , T.
Kolbe2 , S. Hagedorn2 , S. Pazzagli1 ,M. Weyers2 , and T. Schröder1,2 ;1
Humboldt Universitat zu Berlin,
2
Berlin, Germany;
FerdinandBraun-Institut, Berlin, Germany
AlGaN is a promising material forphotonics due to its wide bandgap,
high electro-optic coefficient, andnonlinearity.
We demonstratewaveguides, tapers, directional
couplers, ring resonators, andMach-Zender interferometers for
operating at 632 nm.

Room 13b ICM

Room 14a ICM

measured timing jitter is comparedwith the numerical estimation
depending on cavity parameters
including repetition rates andsaturable absorber types.

Ultrafast Electron Dynamics
Measured with an Attosecond
X-Ray Free-Electron Laser∙T. Driver; Stanford PULSE Institute,
Menlo Park, USA; Linac Coherent
Light Source, SLAC National Accelerator Laboratory, Menlo Park, USA
We present the generation of attosecond x-ray free-electron laser
pulses and pulse pairs and their application to measurements of ultrafast coherent electron dynamics inboth core-excited neutral moleculesand valence ionized molecular ions.

JSI-4.3 WED⋅ Wednesday 28 June 2023

EH-1.2 WED

16:30

Metamaterial Continuous Time
Crystal - A New State of Photonic
Matter
T. Liu1 , V. Raskatla1 , J.-Y. Ou1 , ∙K.
MacDonald1 , and N. Zheludev1,2 ;1UniversityofSouthampton,
Southampton, United Kingdom;
2
Nanyang Technological University,
Singapore, Singapore
A continuous time crystal state
can be realised in a nano-optomechanical metamaterial - light resonant with the metamolecules’ plasmonic mode triggers a spontaneoustransition to a state characterised bytransmissivity oscillations resulting
from many-body interactions.

16:15

CB-7.2 WED

16:15

CD-10.2 WED

16:15

Improved thermal performancesof resonant reflection waveguidegrating structure∙A. Boubekraoui1 , D. Bashir1 ,G. Mourkioti2 , J.I. Mackenzie2 ,T. Graf1 ,and M. Abdou
Ahmed1 ; 1 Institut für Strahlwerkzeuge,Universität Stuttgart, Pfaffenwaldring 43, 70569 , Stuttgart,
Germany; 2 Optoelectronics ResearchCentre, University of Southampton,,
Southampton, S017 1BJ, United
Kingdom
We present laser and thermal performances of resonant grating used
in a thin-disk laser resonator emitting 191W of output power. Grating surface temperature of 32∘ C wasrecorded for a power density of
kW
52 cm
2.

Improvement of laser diode chaos
properties by optical comb injection∙Y. Doumbia, T. Malica, D. Wolfersberger, and M. Sciamanna; CentraleSupélec, Metz, France
We experimentally study the optical injection dynamics of frequency
combs in lasers diode. We observe
chaotic dynamics with a bandwidthof 33 GHz and a spectral flatness up
to 0.83.

Multiply-resonant Waveguide
Gratings for Enhanced Secondharmonic Generation∙M. Mekhael, S. Bej, A. PanahPour, R. Fickler, and M.J. Huttunen;
Photonics Laboratory, Physics Unit,
Tampere University, Finland
We design a resonant waveguidegrating structure for enhanced nonlinear optical processes. We findthat rectangular lattice structureswith L-shaped protrusions can
support two simultaneous high-Q
resonances at pump and secondharmonic wavelengths, providing
multiresonant enhancement.

CA-9.3 WED

CB-7.3 WED

CD-10.3 WED

16:30

Room-temperature Distributed
Feedback FAPbBr3 Perovskite
Nanocrystal Laser Integrated on
Silicon Nitride Waveguide
Platform∙F. Fabrizi1,2 , P. Cegielski1 , M.
Runkel3 , V. Morad4 , D. Dirin4 , S.
Suckow1 , T. Riedl3 , M. Kovalenko4 ,S.B. Anantharaman1 , and M.C.
Lemme1,2 ; 1 AMO GmbH, Aachen,
Germany; 2 RWTH Aachen University, Aachen, Germany; 3 Bergische
Universität Wuppertal, Wuppertal,
Germany; 4 ETH Zürich, Zürich,
Switzerland
Colloidal
halideperovskite
nanocrystals, due to their exceptional optical properties, are prime
candidate materials for on-chip
visible light sources. Here, we

130

16:30

Frequency Comb Broadening by
Optical Noise Injection in a Semiconductor Laser∙A. Borodkin1 , A. Kovalev2 , M.
Giudici1 , G. Huyet1 , A. Ramdane3 ,M. Marconi1 , and E. Viktorov2 ;1
Université Côte d’Azur, Centre National de La Recherche Scientifique,
Institut de Physique de Nice, F06560 Valbonne, France; 2 ITMO
University, 197101 St. Petersburg,
Russia; 3 Centre de Nanosciences etde Nanotechnologies, CNRS UMR
9001, Université Paris-Saclay, 91120
Palaiseau, France
We demonstrate experimentally aspectral broadening induced by optical noise injection in a InAs/InP
quantum dash frequency comb laser
and relate it to the nearly instanta-

16:30

Tunable dual comb source in a
Kerr microresonator∙P.C. Qureshi1,2 , V. Ng1,2 , F.
Azeem1,3 , L.S. Trainor1,3 , H.G.L.
Schwefel1,3 ,S. Coen1,2 ,M.
Erkintalo1,2 , and S.G. Murdoch1,2 ;1The Dodd-Walls Centre for
Photonic and Quantum Technologies, Dunedin, New Zealand;
2
Department of Physics, University of Auckland, Auckland, New
Zealand; 3 Department of Physics,
University of Otago, Dunedin, New
Zealand
We show two new tuning techniques
for microresonator dual-comb setups. By selecting the number of
azimuthal modes between the two
pumps, and by varying their relative detunings, discrete (coarse)

CLEO

Room 14b ICM

Room Osterseen ICM®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)cylindrical-vector beam in a picosecond MOPA system, which carries 10 ps pulses at 1030 nm with a
91 kW peak power and 0.97 μJ pulse
energy.
CH-8.2 WED

16:15

CF-9.2 WEDApplication of superconducting
nanowire detector arrays inmolecular beam research andmass spectroscopy∙R. Gourgues; Single Quantum,
Delft, Netherlands
We report on the fabrication andcharacterization of arrays of Superconducting Nanowire Detectors
made of NbTiN. We employ thesedevices for the detection of large single charged molecules with low kinetic energy.

CH-8.3 WED

16:30

Plasmonic-Based Non-Invasive
In-Operando Technique for theCharacterization of MoS2 Nanoswitches∙J. Symonowicz1 , D. Polyushkin 2 ,T. Mueller 2 , and G. Di Martino1 ;1
Department of Materials Scienceand Metallurgy, University of Cambridge, Cambridge, United Kingdom;
2
Vienna University of Technology,
Institute of Photonics, Vienna, Austria
We develop the first non-destructive
plasmonic-based technique to characterize nanoswitches in-operando
and under ambient conditions.
With our method we describe
nano-kinetics of electrical switches
based on MoS2 nanosheets.

EF-2.2 WED

16:30

Parametrically-driven cavity solitons in a pure Kerr microresonator
G. Moille1,2 , M. Leonhardt3 , D.
Paligora3 , N. Englebert4 , F. Leo4 , J.
Fatome3,5 , K. Srinivasan1,2 , and ∙M.
Erkintalo3 ; 1 Joint Quantum Institute, NIST/University of Maryland,College Park, USA; 2 Microsystems
andNanotechnology
Division,
National Institute of Standards andTechnology, Gaithersburg, USA;3
Department of Physics and The
Dodd-Walls Centre, University of
Auckland, New Zealand; 4 Service
OPERA-Photonique, Universite librede Bruxelles, Belgium; 5 Laboratoire
Interdisciplinaire
CarnotdeBourgogne CNRS-Universite deBourgogne, Dijon, France
We report on the first experimen-

16:15

CI-4.2 WED

16:15

CJ-5.2 WED

16:15

EB-9.2 WED

16:15

Generation of Tunable
Narrowband Azimuthally
Polarized Pulses for Magnetic
Excitation of Eu3+ Ions
∙E. Gangrskaia1 , V. Shumakova1 ,A. Bellissimo1 , E. Kaksis1 , L.
Grünewald2,3 ,S. Mai2 ,A.
Baltuška1,4 , and A. Pugžlys1,4 ;1Photonics Institute, TU Wien,
Vienna, Austria; 2 Institute ofTheoretical Chemistry, University of
Vienna, Vienna, Austria; 3 Vienna
Doctoral School in Chemistry(DoSChem), University of Vienna,
Vienna, Austria; 4 Center for Physical Sciences & Technology, Vilnius,
Lithuania
In order to induce the selective excitation of magnetic-dipole transitions in Eu3+ ions, we generatenarrowband wavelength-tunable azimuthally polarised pulses by combining spectral shifting via stimulated Raman scattering and spectral
focusing.

Rate Optimized Probabilistic
Shaping-based Transmission overField Deployed Coupled-Core
4-Core-Fiber
A. Nespola1 , M.A. Amirabadi2,3 , R.
Ryf4 , M. Mazur4 , N.K. Fontaine4 ,L. Dallachiesa4 , T. Hayashi5 , M.H.
Kahaei3 , S.A. Nezamalhosseini3 ,A. Marotta6 , A. Mecozzi6 , C.
Antonelli6 , and ∙A. Carena2 ;1Links Foundation, Turin, Italy;
2
Politecnico di Torino, Turin, Italy;
3
Iran University of science andtechnolog, Tehran, Iran (the Islamic
Republic of).; 4 Nokia Bell Labs,
Murray Hill, NJ, USA; 5 Sumitomo
Electric Industries, Ltd, Yokohama,Japan; 6 Universita Degli Studi
Dell’Aquila, L’Aquila, ItalyWe
demonstrateprobabilistic
shaping-based long-haul transmission
overfield-deployedcoupled-core
multi-core-fibers.
Results show that probabilistic
shaping maintains its gain overuniform QAM over long distances.

Pr3+ vortex fibre laser with interferometric output coupler in red
and orange∙W.R.
Kerridge-Johns1,2 ,A.S.
Rao2,3 , Y. Fujimoto4 , and T.
Omatsu2 ; 1 Department of Physics,
Imperial College, London, United
Kingdom; 2 Graduate School ofEngineering,
Chiba University,
Chiba, Japan; 3 Institute for Advanced Academic Research, Chiba
University, Chiba, Japan; 4 Chiba
Institute of Technology, Chiba, Japan
We construct a Pr3+:waterproof
fluoro-aluminate glass fibre laser
with first order vortex output using an interferometric Gaussian tovortex mode converting output coupler. We find multiple laser wavelengths in orange (606nm-615nm),
red (635nm-640nm), and infrared(695nm-700nm).

Tomography of distant single
Atoms∙F. Fertig1,2 , Y. Zhou1,2 , P.
Malik1,2 , T. van Leent1,2 , and H.
Weinfurter1,2,3 ; 1 Fakultät für Physik,
Ludwig-Maximilians-Universität,
2
Munich,Germany;
MunichCenter for Quantum Science andTechnology (MCQST), Munich,Germany; 3 Max-Planck-Institut für
Quantenoptik, Garching, Germany
We report on the generation andtomographic reconstruction of anentangled state of two single-atoms
separated by 400 meters, and detailon the evaluation of the entangledstate fidelity.

CF-9.3 WED

CI-4.3 WED

CJ-5.3 WEDEB-9.3 WED

16:30

Speeding up field-resolved spectroscopy by Compressed Sensing∙K. Scheffter1,2 , J. Will1,2 , C. Riek3 ,H. Jousselin4 , S. Coudreau4 , N.
Forget4 , and H. Fattahi1,2 ; 1 Max
Planck Institute for the Scienceof Light, Erlangen, Germany;
2
Friedrich-Alexander
University
Erlangen-Nürnberg,
Erlangen,Germany; 3 Zurich Instruments Germany, Munich, Germany; 4 Fastlite,
Antibes, France
We experimentally demonstratecompressed sensing in fieldresolved spectroscopy for the firsttime. Our method based on rapid,
random sampling allows for signal
reconstruction beyond the Nyquist
limit, accelerating measurement
speed by three orders of magnitude.

16:30

Effects of Fluctuations in Dispersion of Transmission Lines on
Optical Eigenvalue Communication∙T. Motomura, A. Maruta, and K.
Mishina; Osaka University, Suita,Japan
We evaluate effects of longitudinalfluctuations of dispersion parameter on eigenvalue transmission by
numerical simulations. A longdistance transmission suppressing
an eigenvalue shift using an NZDSF is achieved by selecting effective eigenvalues.

131

16:30

Tapered Fiber Amplifier Operated
Near 1030 nm with 430 kW Peakand 50 W Average PowerK. Bobkov1 , E. Mikhailov1 , A.
Levchenko 1 , V. Velmiskin 1 , D.
Khudyakov1 , S. Aleshkina1 , T.
Zaushitsyna1 , M. Bubnov1 , D.
Lipatov2 , and ∙M. Likhachev1 ;1
Prokhorov General Physics Instituteof the Russian Academy of Sciences,
Moscow, Russia; 2 G.G. Devyatykh
Institute of chemistry of high purity
substances of the Russian Academyof Sciences, Nizhny Novgorod ,RussiaTapered Yb-doped fiber amplifier
was optimized for operation near
1030 nm. Output peak power of
430 kW in 5.2-ps-pulses with average power of 32 W was obtained.

16:30

Experimental anonymous
conference key agreement∙J. Webb1 , J. Ho1 , F. Grasselli2 ,G. Murta2 , A. Pickston1 , A.
Ulibarenna1 , and A. Fedrizzi1 ;1Heriot-Watt University, Edinburgh,
United Kingdom; 2 Heinrich-HeineUniversität Düsseldorf, Düsseldorf,
Germany
Experimental
fully-anonymous
conference key agreement ina six-user network, where allusers’ identities are hidden. The
conference key rates for all groupconfigurations show the key rateadvantagewhen
multipartite
entanglement is used.

CLEO

Room 1 ICM

Room 4a ICM

Despite being a cornerstone ofquantum physics, Rabi dynamics
in light-matter interaction has only
been studied at long wavelengths.
Here, we present the first demonstration of Rabi dynamics at XUVwavelengths using a seeded FEL.
JSI-4.4 WED

16:45

Photoelectron Signatures ofNonperturbative Dynamics in
Resonant Two-photon Ionizationof Helium∙E. Olofsson and J.M. Dahlström; Division of Mathematical Physics, Lund
University, Lund, Sweden
Motivated by recent experimental results from the FERMI freeelectron laser, we study photoionization from a Rabi-oscillating He
atom using an effective Hamiltonian
approach. We investigate the interference between resonant and nonresonant ionization processes.

JSI-4.5 WED

17:00

Atomic two-color XUV interferometer∙M. Žitnik1,2 , A. Mihelič1,2 , K.
Bučar1,2 , Š. Krušič1,2 , J. Turnšek1,2 ,R. Squibb3 , R. Feifel3 , I. Ismail4 ,P. Lablanquie4 , J. Palaudoux4 , O.
Plekan5 , M. Di Fraia5 , N. Pal5 ,M. Coreno5,6 , M. Manfredda5 ,A. Simoncig5 , P.R. Ribič5,7 , F.
Sottocorona5 , E. Allaria5 , K.C.
Prince5 , C. Callegari5 , and F.
Penent4 ; 1 Jožef Stefan Institute,
Ljubljana, Slovenia; 2 Faculty ofMathematics and Physics, Universityof Ljubljana, Ljubljana, Slovenia;
3
University of Gothenburg, De-

CK-7.3 WED®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 4b ICM

16:45

EH-1.3 WED

16:45

Room 13a ICM

Room 13b ICM

Room 14a ICM

demonstrate a room-temperature
integrated distributed feedback
nanocrystal laser with ultranarrow
FWHM upon optical pumping.

neous carrier relaxation process in
the Q-dash inhomogeneous material.

and continuous (fine) tunings aredemonstrated.

CA-9.4 WED

CB-7.4 WED

CD-10.4 WED

16:45

16:45

16:45

Precision-machined hollow-corewaveguides for extreme-ultraviolet wavelengths∙T. Strobl1,2 , L. Hein1,2 , T.W.
Hänsch1,2 ,T.
Udem1,2 ,T.
Sukegawa3 , M. Koyama3 , andA. Ozawa1 ; 1 Max-Planck-Institut
für Quantenoptik, 85748 Garching,
Germany; 2 Fakultät für Physik,
Ludwig-Maximilians-Universität
München,80799
München,Germany; 3 Canon Inc., 30-2,
Shimomaruko 3-choume, Ohta-ku,
Tokyo, Japan
Waveguides for extreme-ultraviolet
wavelengths are demonstrated.
Hollow-core waveguides were fabricated on a metal substrate using
a precision machining centre andtested with 123.6 nm radiation. This
technology enables miniaturisationof XUV frequency comb metrology
experiments.

Optical time diffraction as awindow into Epsilon Near Zerodynamics∙R. Tirole1 , S. Vezzoli1 , E. Galiffi2 ,B. Tillman3 , P.A. Huidobro4 , A.
Alu2,5 , S.A. Maier1,3,6 , J.B. Pendry1 ,and R. Sapienza1 ; 1 The Blackett
Laboratory, Department of Physics,
Imperial College London, United
Kingdom; 2 Photonics Initiative,
Advanced Science Research Center, City University of New York,
USA; 3 Chair in Hybrid Nanosystems,
Nanoinstitut
Munchen,Ludwig-Maximilians-Universitat
Munchen, Germany; 4 Institutode Telecomunicacoes,
Instituto
Superior
Tecnico-UniversityofLisbon, Portugal; 5 Physics Program,
Graduate Center, City University of
New York, USA; 6 School of Physics
and Astronomy, Monash University,
Clayton, Australia
In a pump-probe experiment withan Indium Tin Oxide thin film, a
temporal analogue of Young’s double slit experiment is demonstrated.
The generated spectral oscillations
give insight on the nonlinear dynamics within the epsilon-near-zero
platform.

Femtosecond-laser-written
depressed-cladding waveguidelaser in Tm3+:CaF2∙P. Loiko1 , K. Eremeev1 , C. Romero2 ,J.R.V. de Aldana2 , X. Mateos3 , A.
Benayad1 , P. Camy1 , and A.
Braud1 ; 1 Centre de Recherche
sur les Ions, les Matériaux et la
Photonique (CIMAP), UMR 6252
CEA-CNRS-ENSICAEN, Universitéde Caen Normandie, Caen, France;
2
University of Salamanca, Salamanca, Spain; 3 Universitat Rovira i
Virgili (URV), Tarragona, Spain
Depressed-cladding low-loss (0.3dB/cm) buried waveguides were
fabricated in a bulk Tm3+:CaF2
crystal by femtosecond Direct Laser
Writing.
The 50 μm-diameterwaveguide laser delivered 385
mW at 1.87 μm with 41.1% slope
efficiency.

Dual-comb interferometer basedon densified gain-switched laser
diodes for high-resolution sensing
applications∙C. Quevedo-Galán1 , A. Rosado1,2 ,P. López-Querol1 ,A. PérezSerrano1 , J.M. García Tijero1 , and I.
Esquivias1 ; 1 CEMDATIC - E.T.S.I.
Telecomunicación,
Universidad
Politécnica de Madrid (UPM),
Madrid, Spain; 2 Instituto de Óptica’Daza de Valdes’, IO-CSIC, Madrid,Spain
A dual-comb interferometer basedonexternally-densified
gainswitched optical frequency combs
has been employed to measure thetransmission profile of an etalon,
paving the way for applications
requiring ultra-high resolution.

Magnesium Fluoride PhotonicBelt Resonators For Generating
Broadband Frequency Combs∙V. Ng1,2 , P.C. Qureshi1,2 , F.
Azeem1,3 , L.S. Trainor1,3 , H.G.L.
Schwefel1,3 ,S. Coen1,2 ,M.
1,2Erkintalo , and S.G. Murdoch1,2 ;1The Dodd-Walls Centre for Photonic and Quantum Technologies,
Dunedin, New Zealand; 2 Universityof Auckland, Auckland, New
Zealand; 3 University of Otago,
Dunedin, New Zealand
We consider photonic belt resonators which support only a few
optical modes. These resonators are
dispersion engineered to generatebroadband
opticalfrequency
combs, free from spectral defects,
and extended by dispersive waves.

CK-7.4 WED

EH-1.4 WED

CA-9.5 WEDCB-7.5 WED

CD-10.5 WED

17:00

High-Extinction Reconfigurable
Mach-Zehnder Interferometer
Based on Silicon Photonic MEMS
∙D.U. Kim1 , M.G. Lim1 , Y.J. Park1 ,D.J. Choi1 , M.J. Her1 , M.S. Hong1 ,Y. Jeong2 , K. Yu2 , and S. Han1 ;1
Department of Robotics Engineering, Daegu Gyeongbuk Institute of
Science and Technology, Daegu,
South Korea; 2 School of ElectricalEngineering,
Korea Advanced
Institute of Science and Technology(KAIST), Daejeon, South Korea
We propose and demonstrate ahigh-extinction
reconfigurable
Mach-Zehnder interferometer with

17:00

How to exploit light-matter interactions in space (x,y,z) and time(t) to enable spatiotemporal
effective materials?
∙V. Pacheco-Peña1 and N. Engheta2 ;1School of Mathematics, Statistics
and Physics, Newcastle University,
Newcastle Upon Tyne, NE1 7RU,
United Kingdom; 2 Department ofElectrical and Systems Engineering,
University of Pennsylvania, Philadelphia, PA 19104, USA
We discuss how temporally modulated media єr (t) within spatially inhomogeneous multilayers can be exploited to achieve space-time effec-

17:00

High-energy pulse laser system at1540 nm using an Er,Yb:glass
planar waveguide amplifier forcoherent doppler wind lidar∙J. Nomura1 , W. Yoshiki1 , K.
Hirosawa1 ,T.
Yanagisawa2 ,N. Ohata1 , S. Imamura3 , D.
Sakaizawa3 ,and N. Tomii3 ;1
Mitsubishi Electric Corporation,
Information Technology R & D
Center, 5-1-1 Ofuna Kamakura
Kanagawa
247-8501,
Japan;
2
Mitsubishi Electric Corporation,
Communication System Center,
8-1-1 Tsukaguchi-Honmach Amagasaki Hyogo 661-8661, Japan;

132

17:00

Accurate measurement of thelinewidth enhancement factor ofsemiconductor lasers by a simple
technique∙B. Sinquin and M. Romanelli; Institut FOTON, UMR 6082, Rennes,
FranceWe propose a simple, precise and reliable method for the measurementof the linewidth enhancement factor
in semiconductor lasers. We show
experimentally 3% uncertainty. This
technique is of interest in the context of microwave photonics.

17:00

Symmetry breaking in high-Q
silicon nitride resonators∙Y. Zhang1 , S. Zhang 1 , T. Bi1,2 ,G.N. Ghalanos1,3 , H. Yan1,2 , and P.
Del’Haye1,2 ; 1 Max Planck Institutefor the Science of Light, 91058
Erlangen, Germany; 2 Departmentof Physics, Friedrich-AlexanderUniversität
Erlangen-Nürnberg,
91058 Erlangen, Germany; 3 Blackett
Laboratory, Imperial College London, SW7 2AZ London, United
Kingdom
Symmetry breaking of counterpropagating light in microresonators has
many applications, ranging from

CLEO

Room 14b ICM

CH-8.4 WEDRoom Osterseen ICM

16:45

High-sensitivity Hyperspectral
Fourier-plane Microscopy by an
Ultrastable Common-path
Interferometer
A. Genco1 , C. Cruciano1 , M. Corti1 ,B. Ardini1 , K. McGhee3 , L. Sortino4 ,L. Hüttenhofer4 , T. Virgili2 , D.G.
Lidzey3 , S.A. Maier4,5,6 , A. Bassi1 ,G. Valentini1 , G. Cerullo1,2 , and1∙C. Manzoni2 ;Dipartimento
di Fisica, Politecnico di Milano,
Milano, Italy; 2 IFN CNR, Milano,
Italy; 3 Department of Physics andAstronomy, University of Sheffield,
Sheffield, United Kingdom; 4 Facultyof Physics, Ludwig-MaximiliansUniversität München,
Munich,Germany; 5 School of Physics andAstronomy, Monash University,
Clayton,Victoria,
Australia;
6
Department of Physics, Imperial
College London, London, United
Kingdom
A common-path birefringent interferometer produces hyperspectral
images of the k-space of optical microcavities and metasurfaces, obtaining a simultaneous angular andspectral view of the samples, retrieving 3D maps of their angular dispersions with optimal resolution.
CH-8.5 WED

17:00

Nanosecond compressive FLIM
via Random Temporal Signals
with direct lifetime retrieval∙J. Junek and K. Žídek; Regional Center for Special Optics and Optoelectronic Systems TOPTEC, Institute of
Plasma Physics of the CAS, Prague 8,
Czech Republic
We present the novel RATS method
for time-resolved spectroscopy. We
tuned overall method performance
while maintaining low cost. We
outline an alternative FLIM reconstruction algorithm that shortens
the post-processing time, making
the method more attractive.

tal observation of parametricallydriven cavity solitons (PDCSs) in apure Kerr resonator. Bichromatic
pumping of a silicon nitride microresonator results in PDCS frequency combs in between the twopump frequencies.
EF-2.3 WED

16:45

Soliton Generation in a Gallium
Phosphide Photonic Crystal
Cavity∙A. Davydova1 , A. Nardi2 , N.
Kuznetsov1 , C. Möhl2 , M.H.
Anderson1 , J. Riemensberger1 , T.J.
Kippenberg1 , and P. Seidler2 ; 1 Swiss
Federal Institute of Technology
Lausanne(EPFL),
Lausanne,
Switzerland; 2 IBM Research Europe,
Zurich, Switzerland
We demonstrate a broadband
dispersion-engineered
photonic
crystalFabry-Perot
resonator
based on Gallium phosphide withrecord-high quality factor. Withsubharmonic pulsed pumping,
we achieve generation of stabledissipative Kerr frequency combs.

EF-2.4 WED

17:00

Electrically-driven platform forsoliton generation∙N. Opačak1,2 , D. Kazakov2 , L.
Columbo3 , M. Beiser1 , F. Pilat1 ,M. Brambilla4 , F. Prati5 , M.
Piccardo2,6 , F. Capasso2 , and B.
Schwarz1,2 ; 1 Institute of Solid StateElectronics, TU Wien, Vienna,
Austria; 2 John A. Paulson School ofEngineering and Applied Sciences,
Harvard University, Cambridge,
USA; 3 Dipartimento di Elettronica
e Telecomunicazioni, Politecnico di
Torino, Torino, Italy; 4 Dipartimento
di Fisica Interateneo and CNR-IFN,
Universitá e Politecnico di Bari,®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)

Average power scalability to 50 W
was demonstrated.

CF-9.4 WED

16:45

CI-4.4 WED

16:45

CJ-5.4 WED

16:45

EB-9.4 WED

16:45

Sub-20-fs UV Pump - XUV Probe
Beamline for Ultrafast Molecular
Spectroscopy∙A. Crego1,2 , S. Severino3 , F.
Medeghini3 , L. Mai3 , F. Frassetto4 ,L. Poletto4 , M. Lucchini1,3 , M.
Reduzzi3 , M. Nisoli1,3 , and R.
Borrego-Varillas1 ; 1 Institute for
Photonics and Nanotechnologies,
IFN-CNR, Piazza Leonardo da Vinci
32, 20133, Milano, Italy; 2 Grupo deInvestigación en Aplicaciones delLáser y Fotónica, Departamentode Física Aplicada, Universidad de
Salamanca, E-37008, Salamanca,
Spain; 3 Dipartimento di Fisica,
Politecnico di Milano, Piazza
Leonardo da Vinci 32, 20133, Milano, Italy; 4 Institute for Photonics
and Nanotechnologies, IFN-CNR,
via Trasea 7, 35131, Padova, Italy
We developed a unique UV–XUV
spectroscopy beamline with sub-20fs temporal resolution, unambiguously characterized by in-situ photoelectron cross-correlation. We
present its application to resolve forthe first time the ultrafast S2/S1 passage in acetylacetone.

On the Influence of Gating on
Computational Complexity and
Performance of Recurrent Neural
Networks-based Equalizers∙D. Argüello Ron; Aston Institute of
Photonic Technologies, Aston University, Birmingham, United Kingdom
Low computational complexity variants of bi-LSTM and bi-GRU models are proposed and successfully
used to compensate the nonlinearities from the transmission of DP
34.4 Gbaud 16QAM over 450km of
TWC fiber without sacrificing performance.

Tunable Brillouin/Neodymium
fiber laser with non-resonant
pumping∙R. Prakash1 , D. Darwich1 , C.
Dixneuf2 , G. Guiraud2 , K. Le
Corre3 , T. Robin3 , R. Florentin4 ,M. Laroche4 , G. Santarelli1 , and
A. Hilico1 ; 1 LP2N, IOGS, CNRS
and Université de Bordeaux,2Talence, France;
Azur Light
Systems, Pessac, France; 3 Exail(formerly iXblue), Lannion, France;
4
CIMAP, ENSICAEN-CNRS-CEA,
Normandie Université, Caen, France
We demonstrate a high power,
polarization maintaining, lownoise, single frequency, tunable
Neodymium-doped fiber laser andits subsequent use as a non-resonant
Brillouin fiber laser pump.

Transmission of light-matterentanglement over a metropolitan
network
J.V. Rakonjac1 , ∙S. Grandi1 , S.
Wengerowsky1 , D. Lago-Rivera1 , F.
Appas1 , and H. de Riedmatten1,2 ;1
ICFO-Institut de Ciencies Fotoniques,
Castelldefels,
Spain;2
ICREA-Institució Catalana de Recerca i Estudis Avançats, Barcelona,
Spain
We report entanglement between amultimode quantum memory anda photon, after propagation in a
metropolitan fibre link. The detection setup is then placed in a remotelocation while detection events aresent back through optical fibres.

CF-9.5 WED

CI-4.5 WED

CJ-5.5 WEDEB-9.5 WED

17:00

Laser-induced Nonthermal Spin
Dynamics in Ferromagnetic
Materials Probed by Ultrafast
Magneto-optic Spectroscopy∙I.C. Yu1 , J.-H. Shim2 , B.-G. Park3 ,K.-J. Kim1 , D.-H. Kim4 , J.H. Oh1 ,K.-J. Lee1 , and F. Rotermund1 ;1
Department of Physics, Korea
Advanced Institute of Scienceand Technology (KAIST), 34141
Daejeon, South Korea; 2 Departmentof Physics and Center for Attosecond
Science and Technology, POSTECH,
37673 Pohang,South Korea;
3
Department of Materials Scienceand Engineering, Korea Advanced

17:00

THz-range all-optical wavelength
conversion using a feedbackcontrolled multi-wavelength laser∙P. Marin-Palomo, S. Abdollahi, and
M. Virte; Brussels Photonics Team
(B-PHOT), Vrije Universiteit Brussel, Brussels, Belgium
We demonstrate wavelength conversion of up to 10.5 nm (1.36 THz)through single optical injection ina multi-wavelength laser. The proposed scheme enables amplificationand control of the frequency shift
without additional optical input.

133

17:00

Fabrication and characterisationof few mode DBR BrillouinRaman lasers∙R.H.S. Bannerman1 , A.I. Flint1 ,J.C. Gates1 , N.G.R. Broderick2 ,C.B.E. Gawith1,3 , and P.G.R.
Smith1 ; 1 Optoelectronics ResearchCentre, University of Southampton,
United Kingdom; 2 Dodd Walls
Centre for Photonics and Quantum Technologies, Department of
Physics, The University of Auckland,
New Zealand; 3 Covesion Ltd.,Southampton, United Kingdom
We present our work on the
fabrication and characterization of

17:00

Efficient interface between ultrafast and nanosecond opticalquantum systems∙F. Sośnicki, M. Mikołajczyk, A.
Golestani, and M. Karpiński; University of Warsaw, Warszawa, Poland
We experimentally demonstratelarge-scale spectral bandwidthcompression by over two orders ofmagnitude of broadband heralded
single photons, from 0.56 nm to
4 pm, increasing a photon flux
through a 3.6 pm filter by a factorof 16.

CLEO®

/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Room 1 ICM

Room 4a ICM

Room 4b ICM

partment of Physics, Gothenburg,
Sweden; 4 LCP-MR (UMR 7614),
Sorbonne Universit’e and CNRS,Paris, France; 5 Elettra-Sincrotrone
Trieste, Trieste, Italy; 6 Consiglio
Nazionale delle Ricerche –Istituto
di Struttura della Materia, Trieste,
Italy; 7 Laboratory of Quantum
Optics, University of Nova Gorica,
Nova Gorica, Slovenia
We report on using helium(ω1 + ω1 )/(ω3 − ω1 ) XUV interferometer to detect phase shift of
the fundamental radiation tuned to
the 4s −1 5p window resonance after
passing 5 m long gas attenuator
filled with krypton.

MEMS-based tunable couplers
and phase shifter. The measured
extinction ratio at 1550 nm and1560 nm is 41.76 dB and 41.25 dB,
respectively.

tive materials, opening a new direction for a full manipulation of lightmatter interactions in both space
and time.

3

JSI-4.6 WED

CK-7.5 WED

EH-1.5 WED

CA-9.6 WED

17:15

Impulsive X-ray Raman in liquid
water∙O. Alexander1 , F. Egun1 , D.
Garratt2 , L. Rego1,3 , J. Cryan2,4 ,T. Driver2,4 , J.P. Marangos2,4 , A.
Marinelli4 , R. Coffee4 , D. Deponte4 ,D. Haxton5 , E. Thierstein2,4 , J.
Lee1 , J. Turner1 , K. Kowalczyk1 ,K. Zhao1 , M.-F. Lin4 , N. Berrah6 ,P. Bucksbaum2 , R.-P. Wang7 ,S. Beauvarlet6 , S. Moeller2,4 , J.
Oneal2,4 , G. Dakovski4 , and K.
Larsen2,4 ; 1 Imperial College London, London, United Kingdom;
2
Stanford Pulse Institute, California,
USA; 3 University of Salamanca,
Salamanca, Spain; 4 Linac Coherent
Light Source, California, USA;5KLA Corporation,
California,
USA; 6 University of Connecticut,
Connecticut, USA; 7 Universität
Hamburg, Hamburg, Germany
We observe impulsive X-ray Raman emission from micrometerthick liquid water jets using intense 350 as X-ray XFEL pulses, atthe oxygen K-edge. Our calculation predict valence states excitations, with populations dependent
on the propagation length.

17:15

Amorphous Silicon based Crosstalk Resilient Photonic Phase
Shifters∙S. De1,2 , R. Das1 , K. Singh1 , Y.
Mandalawi1 , T. Kleine-Ostmann2 ,and T. Schneider1 ; 1 TU Braunschweig, Braunschweig, Germany;
2
PTB Braunschweig, Braunschweig,
Germany
We show that the phase crosstalk in
amorphous silicon based integrated
photonic devices is much smaller
than in crystalline ones and can befurther mitigated by deep trenches.

Room 13a ICM

17:15

Edge Modes, Symmetries, and Zak
Phases: Analysis via Bloch
Impedance∙I. Tsukerman1 and V. Markel2 ;1
Department of Electrical andComputer Engineering, The University of Akron, Akron, Ohio,
USA; 2 Departments of Radiology
and Bioengineering, University ofPennsylvania, Philadelphia, PA,USA
Unidirectional modes exist at interfaces of topologically different
periodic structures. In photonics, a general proof of this bulkboundary correspondence principle
is still lacking. This paper provides
such a proof, along with illustrative
numerical examples.

Room 13b ICM

Room 14a ICM

Japan
Aerospace
Exploration
Agency, 6-13-1 Osawa Mitaka Tokyo
181-0015, Japan
We have developed a high-energy
pulse laser system at 1540 nm using an Er,Yb:glass planar waveguide
amplifier that outputs pulses withenergy exceeding 40 mJ for coherent
doppler wind lidar.

17:15

High energy passively Q-switchedlaser on a CMOS platform∙N. Singh1 , J. Lorenzen1 , M.
Sinobad1 , K. Wang2 , A. Liapis3 , H.
Frankis4 , M. Gaafar1 , S. Haugg5 ,H. Francis6 , J. Carreira6 , M.
Geiselmann6 , T. Herr1 , J. Bradley4 ,Z. Sun3 , S. Garcia-Blanco2 , and F.
Kärtner1,7 ; 1 Center for Free-Electron
Laser Science CFEL, Hamburg,
Germany; 2 University of Twente,
Enschede, Netherlands; 3 Aalto University, Espoo, Finland; 4 McMaster
University, Hamilton, Canada;
5CHyn, University of Hamburg,
Hamburg, Germany; 6 LIGENTEC,
Ecublens, Switzerland; 7 Departmentof Physics, Universität Hamburg,
Hamburg, Germany
We demonstrate CMOS-compatiblehigh energy Q-switched laser in theeye-safe window, with an on-chip
output pulse energy over 150 nanojoules at a repetition rate of ~1 MHz
in the fundamental optical mode in
a compact footprint.

134

isolators to memories and gyroscopes. We report symmetry breaking in a high-Q silicon nitride resonator at a threshold power below 4mW.

CB-7.6 WED

17:15

Detection and investigation ofpulse asymmetries in passively
mode-locked quantum-dot laser
diodes using dispersion-scan∙T.d.S. Gomes1,2 , H. Crespo2,3 ,and M.A. Cataluna1 ; 1 Institute of
Photonics and Quantum Sciences,
Heriot-Watt University, Edinburgh,
United Kingdom; 2 IFIMUP and
Departamento de Física e Astronomia, Faculdade de Ciências
da Universidade do Porto, Porto,
3
Portugal;
Blackett Laboratory,
Imperial College, London, United
Kingdom
We demonstrate a dispersion-scansetup to characterize and compress
pulses from a quantum-dot modelocked laser diode, studying the influence of drive current and reverse
bias on pulse asymmetry and compressing the pulses to sub-ps durations.

CD-10.6 WED

17:15

Polarization-Based Idler Elimination: Enhancing the Efficiency of
Optical Parametric Amplification∙G. Jansonas1,2 , R. Budriūnas1,2 ,G. Valiulis1 , and A. Varanavičius1 ;1
Vilnius University, Laser ResearchCenter, Vilnius, Lithuania; 2 Light
Conversion Ltd., Vilnius, Lithuania
This study presents a novel way toincrease the energy conversion efficiency of optical parametric amplification by eliminating the idler wave
from the interaction using consecutive type-I and type-II amplification
processes.

CLEO

Room 14b ICM

CH-8.6 WED

17:15

Sensing of Dynamic Light-LiquidInteraction with Dual Beam
Thermal Lens Spectroscopy∙J.L.
Domínguez-Juárez1,2 ,R.
Quintero-Torres1 , J.L. Aragón1 ,M.A. Quiroz-Juárez 1 , and J.
Villatoro3,4 ; 1 Centro de Física
Aplicada y Tecnología Avanzada,
Universidad Nacional Autónoma deMéxico, , 76230, Juriquilla, Querétaro, México; 2 Cátedras CONACyT,Centro de Física Aplicada y Tecnología Avanzada, UNAM, 76230, Juriquilla, Querétaro, México;3
Department of Communications
Engineering, University of theBasque Country UPV/EHU, 48013,
Bilbao, Spain; 4 Ikerbasque-BasqueFoundation for Science, E-48011,,
Bilbao, Spain
We show dynamic wave-front sensing as a temperature-induced index
of refraction changes for thermalization processes in liquids. Lightliquid interaction is analyzed withthe help of visible image changes ofa diffraction patterns response.

®

/Europe-EQEC 2023

Room Osterseen ICM

Room 1 Hall B1 (B11)

Bari, Italy; 5 Dipartimento di Scienza
e Alta Tecnologia, Universitá
dell’Insubria, Como, Italy; 6 Center
for Nano Science and Technology,
Fondazione Istituto Italiano diTecnologia, Milano, Italy
We demonstrate a new type of optical solitons in a free-running ringsemiconductor laser. The soliton
is predicted within the frameworkof complex Ginzburg-Landau equation and confirmed by both the experimental measurements and numerical simulations.

Institute of Science and Technology(KAIST), 34141 Daejeon, South
Korea; 4 Department of Physics,
Chungbuk National University,
28644 Cheongju, South Korea
Time-resolved magneto-optic measurements are performed to study
coherent light-spin interaction in
ferromagnetic Co/Pt and Co films.
We found out that laser-induced
nonequilibrium spin states play animportant role in ultrafast demagnetization of ferromagnetic materials.

EF-2.5 WED

CF-9.6 WED

17:15

Cavity soliton Raman selffrequency shift cancellation∙N. Englebert, C. Simon, C. Mas
Arabí, F. Leo, and S.-P. Gorza;
OPERA-Photonique, Université librede Bruxelles, Brussels, Belgium
We report theoretically and experimentally on the formation of temporal cavity solitons shorter than thefundamental limit imposed by thestimulated Raman scattering in afiber Kerr resonator that includes aphase modulator.

⋅ Wednesday 28 June 2023
Room 6 Hall B3 (B32)

17:15

Field-Resolved Infrared Spectroscopy using a Broadband
Achromatic Interferometer∙S. Maithani1,2 , A. Maity1,2,3 , W.
Schweinberger1,2,3 , A. Weigel1,2,3 , F.
Krausz1,2,3 , and I. Pupeza1,2,4 ; 1 Max
Planck Institute of Quantum Optics,
2
Garching,
Germany;
LudwigMaximilians-University
Munich,3
Garching,
Germany;
Centerfor
Molecular
Fingerprinting,
Molekuláris- Ujjlenyomat Kutató
Közhasznú Nonprofit Kft., Budapest,
Hungary; 4 Leibniz Institute of
Photonic Technology – Member of
research alliance “Leibniz HealthTechnologies”, Jena, Germany
We demonstrate a broadband
mid-infraredinterferometricsetup, cancelling source excitationnoise and extending the dynamic
range in molecular field-resolved
spectroscopy. First electro-opticsampling measurements at thedestructive port showed a tenfold
suppression of the excitation field.

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)short (<300mm) Fabry-Perot DBR
Raman-Brillouin lasers in highly
nonlinear fiber. Our aim is to better
understand their application tocompact cascading of Raman laser
DFBs.

CI-4.6 WED

17:15

THz-bandwidth passive logic
gates through noninstantaneous
nonlinearity∙N. Perron1 , M. Chemnitz2 , B.
Fischer1 , S. Junaid2 , M. Schmidt2 ,and R. Morandotti1 ; 1 Institut National de la Recherche Scientifique(INRS-EMT), Varennes, Canada;
2
Leibniz Institute of Photonic
Technology, Jena, Germany
We implement ultrafast, powerefficient, all-optical logic gates basedon a liquid-core optical fiber platform. We present, theoretically andexperimentally, the unique nonlinear interactions driving each logic
operation, implemented using only
standard telecom components.

135

CJ-5.6 WED

17:15

Influence of clad-to-core ratio on
the performance of Nd-doped
LMA fiber amplifiers at 915 nm∙R. Florentin1 , K. Le Corre1,2 , T.
Robin2 , B. Cadier2 , A. Barnini2 ,R. Prakash3 , G. Santarelli3 , H.
Gilles1 , S. Girard1 , and M. Laroche1 ;1
CIMAP, ENSICAEN-CNRS-CEA,
Normandie
Université,
Caen,France; 2 Exail (formerly iXblue),Lannion, France; 3 LP2N, IOGS,CNRS and Université de Bordeaux,Bordeaux, France
We report an analytical, numerical and experimental work abouthigh power emission at 915nm. It
investigates the impact of clad-tocore ratio and bending radius of
Neodymium doped large mode area
fibers on the output power.

EB-9.6 WED

17:15

Entanglement source for spaceground quantum communication∙T. TROISI, Y. PELET, G. SAUDER,
S. TANZILLI, and A. MARTIN; Institut de Physique de Nice, UMR
7010, NICE, France
We present a high rate entangledbased photon source working attelecom wavelength, com- patible
with existing fibre communication
networks, with hybrid encoding(energy-time and polarisation),with the aim of fulfilling spatialconstraints.

CLEO

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/Europe-EQEC 2023

⋅ Wednesday 28 June 2023

Hall B0
13:00 – 14:00
CH-P: CH Poster session
CH-P.1 WED

Two-photon lensless endoscopes with multicore
fibersF. El Moussawi1 , M. Hofer2 , ∙S. Sivankutty1 , A.
Bertoncini3 , D. Labat1 , A. Cassez1 , G. Bouwmans1 , R.
Cossart4 , O. Vanvincq1 , C. Liberale3 , H. Rigneault2 , and
E. Andresen1 ; 1 Univ. Lille, CNRS, UMR 8523 - PhLAM- Physique des Lasers Atomes et Molécules, Lille, France;
2
Aix-Marseille University, CNRS, Institut Fresnel, Marseille, France; 3 King Abdullah University of Science andTechnology, Thuwal, Saudi Arabia; 4 Aix-Marseille University, INSERM, INMED, Marseille, France
We present here two approaches to functionalizing abending-resilient multicore fiber for lensless endoscopesby tapering and 3D printing micro-optics at its tip. A
major improvement in the sensitivity (>10x) is experimentally demonstrated.
CH-P.2 WEDSingle-Molecule Microscopy in Ultrahigh Vacuum∙T. Fang, N. Vogeley, and D. Wang; Institute of Physics,
University of Kassel, 34132 Kassel, Germany
By adapting oil-immersion microscopy to a novel
vacuum window, we resolve the dynamics of single
molecules on a fused-silica surface under ultrahigh vacuum conditions with high spatial and temporal resolution.
CH-P.3 WEDWavelength Scanning Multimode Fiber Imaging
B. Lochocki1 , ∙A. Ivanina1 , A. Bandhoe1 , J.F. de Boer2 ,and L.V. Amitonova1,2 ; 1 Advanced Research Center for
Nanolithography (ARCNL), Amsterdam, Netherlands;
2
LaserLaB, VU Amsterdam, Amsterdam, Netherlands
Compressive imaging via a multimode fiber is demonstrated using a visible spectrum swept source and wavelength dependent speckle illumination. The highresolution image reconstruction is shown for narrow
sweeping bandwidth of < 27.5 nm.
CH-P.4 WED

Deeply Sub-wavelength 2D Optical Metrology with
Superoscillatory Light∙Y. Wang1 , J.-K. So2 , E.A. Chen2 , C. Rendón-Barraza2 ,B. Wang2 , G. Adamo2 , E. Plum1 , K. MacDonald1 , J.-Y.
Ou1 , and N. Zheludev1,2 ; 1 Optoelectronics Research Centre & Centre for Photonic Metamaterials, University ofSouthampton, Southampton, United Kingdom; 2 Centre
for Disruptive Photonic Technologies, Nanyang Technological University, Singapore, Singapore
We demonstrate optical metrology for two-dimensional

sub-wavelength objects with resolution beyond λ/50 via
deep learning-enabled analysis of light scattering fromtarget objects illuminated by the phase singularity of superoscillatory structured light.
CH-P.5 WED

Next Generation of Nonlinear Laser Microscopy
Based on High Energy Fs-Pulses: Widefield Mode up
to 2.2 microns∙L. Vittadello1,2 , F. Kodde1,2 , J. Klenen1,2 , and M.
Imlau1,2 ; 1 University of Osnabrueck, Department of
Physics, Osnabrueck, Germany; 2 Center of CellularNanoanalytics Osnabreuck, Osnabrueck, Germany
The use of lasers having energy per pulse in the μJ allows(i) to develop an easily reproducible nonlinear widefieldmicroscope and (ii) to image deeper with less photodamage up to 2.2 microns.
CH-P.6 WED

Cantilever-Enhanced Photoacoustic Detector forBlack and Brown Carbon∙J. Karhu1,2 , J. Kuula2,3 , T. Mikkonen2,4 , M. Ward2 , A.
Virkkula3 , E. Ikonen1,5 , T. Hieta6 , H. Timonen3 , and M.
Vainio2,4 ; 1 Aalto University, Espoo, Finland; 2 University
of Helsinki, Helsinki, Finland; 3 Finnish Meteorological Institute, Helsinki, Finland; 4 Tampere University, Tampere,
Finland; 5 VTT Technical Research Centre of Finland, Espoo, Finland; 6 Gasera Ltd., Turku, Finland
We present a photoacoustic instrument for multiwavelength measurement of aerosol light absorption. The
method uses cantilever-enhanced photoacoustics, which
improves sensitivity and is particularly suitable for measuring multiple modulation frequencies simultaneously.
CH-P.7 WEDInfluence of the non-thermally coupled three-photonband on the performance of Y2 O3 : Yb3+ /Er3+
single-particle nanothermometers
A.R. Pessoa1,2 , J.A.O. Galindo2 , L.F. dos Santos3 , R.R.
Gonçalves3 , S.A. Maier4,5,1 , ∙L.d.S. Menezes2,1 , and A.M.
Amaral2 ; 1 Chair in Hybrid Nanosystems, Faculty ofPhysics, Ludwig-Maximilians-University, Munich, Germany; 2 Physics Department, Universidade Federal de Pernambuco, Recife, Brazil; 3 Chemistry Department, Universidade de São Paulo, Ribeirão Preto, Brazil; 4 School ofPhysics and Astronomy, Monash University, Melbourne,,
Australia; 5 Department of Physics, Imperial College London, London, United Kingdom
Intruding overlapped non-thermally coupled emission
bands can lead to temperature readout errors in luminescence nanothermometry. We apply a new simple method
to correct it based on the different power dependenciesof the relevant emission bands.

CH-P.8 WEDOptical Localization of Nanoparticles in
Sub-Rayleigh Clusters∙B. Wang1 , Y. Li2 , E.A. Chan1 , G. Adamo1 , B. An2 ,Z. Shen1 , and N.I. Zheludev1,3 ; 1 Centre for Disruptive
Photonic Technologies, The Photonics Institute, School ofPhysical and Mathematical Sciences, Nanyang Technological University, Singapore, Singapore; 2 Artificial Intelligence Research Institute, School of Computer Science and Engineering, Nanyang Technological University,
Singapore, Singapore; 3 Optoelectronics Research Centre
and Centre for Photonic Metamaterials, University ofSouthampton, Southampton, United Kingdom
By deep learning analysis of diffraction patterns oflight scattered on sub-wavelength nano-holes clustered
within Rayleigh distance, we retrieve their positions withhigh accuracy breaking the diffraction limit of opticalresolution.

Laffont1 ; 1 Paris-Saclay University, CEA, List,, Palaiseau,
France; 2 Paris-Saclay University, CEA, Service d’Etudes
Mécaniques et Thermiques, Gif-Sur-Yvette, France; 3 CEACESTA, Le Barp, France; 4 CEA-DAM, Le Ripault, Monts,
FranceHigh temperature and strain measurements were
performed within a titanium plate, with pairs of
femtosecond-Point-by-Point Fiber Bragg Gratings arrayanchored with plasma projection of ceramic powder.
Numerical and experimental cartography of the plate
were investigated.
CH-P.12 WED

Nanometer-precision multimode fiber ruler∙K. Abrashitova1 and L.V. Amitonova1,2 ; 1 Advanced Research Center for Nanolithography (ARCNL), Amsterdam, Netherlands; 2 Vrije Universiteit Amsterdam, Amsterdam, Netherlands
We demonstrate single-nanometer-precision metrology
with a hair-thin multimode optical fiber. Our results
show the nanoscale optical ruler at the output fiber
facet and establish a new benchmark for compact opticalalignment sensors.

Spatially Encoded Compressive Microscope for
Ultrabroadband VIS/NIR/SWIR Hyperspectral
Imaging∙L. Klein1,2 , K. Žídek1 , and J. Touš3 ; 1 Regional Centre
for Special Optics and Optoelectronic Systems (TOPTEC)
Institute of Plasma Physics of the Czech Academy of Sciences, Za Slovankou 1782/3, 182 00, Prague, Czech Republic; 2 Technical University of Liberec, Faculty of Mechatronics, Informatics and Interdisciplinary Studies, Studentská 1402/2, 461 17, Liberec, Czech Republic; 3 Crytur,
spol. s.r.o., Na Lukách 2283, 51101, Turnov, Czech Republic
A broadband hyperspectral microscope is presented.
Thanks to the compressive imaging principle, the system
can create hyperspectral data in a wavelength range from400-2200 nm. Performance tests and potential applications of the setup are demonstrated.

CH-P.10 WED

CH-P.13 WED

Numerical Study on Multiplexing Scalability in
Ptychography∙D.S. Penagos Molina1,2,3 , W. Eschen1,2,3 , C. Liu1,2,3 , J.
Limpert1,2,3,4 , and J. Rothhardt1,2,3,4 ; 1 Institute of Applied Physics and Abbe Center of Photonics, FriedrichSchiller-University Jena, Jena, Germany; 2 HelmholtzInstitute Jena, Jena, Germany; 3 GSI Helmholtzzentrzum für Schwerionenforschung, Darmstadt, Germany;
4
Fraunhofer Institute for Applied Optics and Precision Engineering, Jena, Germany
We present a detailed numerical analysis on the multiplexing capabilities in ptychography for boosting scanning performance. By using 16 incoherent beams, a performance increase up to 15x was found.

High Temperature Performance of Femtosecond
Laser Written FBGs
∙R. Elliott, T. Lee, M. Beresna, M. Ibsen, and G. Brambilla;
Optoelectronics Research Centre, University of Southampton, Southampton, United Kingdom
We investigate thermal stability of Bragg gratings fabricated with different femtosecond laser writing parameters, reporting high stability up to 1200∘ C, and study
structural and spectral changes at the high temperature
failure regime including by tapering.

CH-P.9 WED

CH-P.11 WEDIn-Titanium Embedded multiplexed femtosecond
Fiber Bragg Gratings under intense heat flow –Comparison between experimental and numericalheat and strain cartography∙E. Deliancourt1 , A. Lerner1 , K. Achour2 , A. Jolly3 , J.C. Le Pallec2 , A. Quet4 , C. Guérin3 , S. Hulin1 , and G.

136

CH-P.14 WEDFano resonances in a Photonic Crystal side-coupled
Micro Ring Resonator for refractive index sensing
J.H. Mendoza Castro1,2 , ∙A.S. Vorobev1,3,4 , S. Iadanza3,4 ,B. Lendl2 , M. Grande1 , and L. O’Faolain3,4 ; 1 Department
of Electrical and Information Engineering, Politecnico diBari, Via E. Orabona, 4, 70126 , Bari, Italy; 2 Institute ofChemical Technologies and Analytics, TU Wien, Getreidemarkt 9/164,1060 , Vienna, Austria; 3 Centre for Advanced Photonics and Process Analysis, Munster Technological University, T12 T66T Bishopstown, Cork, Ireland;

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Hall B0
Tyndall National Institute, T12 PX46 , Cork, Ireland
We present a compact Si3 N4 Photonic Crystal (PhC) Micro Ring Resonator (MRR) structure able to support
Fano lineshapes with high-Q factor (104 ), and asymmetry, in the presence of air and water.
4CH-P.15 WED

Integrated ArUco Fiducial Markers in Resonant
Waveguide Gratings for Pose Estimation∙F.A. Kraft, M. Ahmadi, and M. Gerken; Chair for Integrated Systems and Photonics, Kiel University, Kiel, Germany
We show the integration of ArUco fiducial markers withresonant waveguide gratings via a lithographic process.
This enhances their capabilities in regards of pose estimation and angle-dependency compensation.
CH-P.16 WED

Improved optical inspection of lateral III-V-semiconductor oxidation afforded by a spectrally-shaped
illumination∙N. Monvoisin, E. Hemsley, L. Laplanche, G. Almuneau,
S. Calvez, and A. Monmayrant; LAAS-CNRS, Toulouse,
FranceWe report the implementation of a spectrally-shapedsource for an improved optical in-situ inspection of lateral III-V-semiconductor wet oxidation process that is
critical in Vertical-Cavity Surface-Emitting Laser (VCSEL) fabrication.
CH-P.17 WEDNeuromorphic Camera Assisted High-Flow Imaging
Cytometry for Particle Classification
I. Tsilikas1 , S. Deligiannidis2 , A. Tsirigotis3 , G.
Tsigaridas1 , A. Bogris2 , and ∙C. Mesaritakis3 ; 1 National
Technical University of Athens, Dept. Physics, Athens,
Greece; 2 University of West Attica, Dept. Informatics andComputer Engineering, Egaleo, Greece; 3 University of the
Aegean, Dept. Information and Communication Systems
Engineering, Samos, Greece
Here we experimentally combine high-flow imagingcytometer, an event-based 10 kframe/sec capable neuromorphic camera and lightweight machine learning, so
as to simultaneously image and classify different type ofparticles with an accuracy of 97.6%.
CH-P.18 WEDFourier Ptychography Microscopy for rapid
characterization of ultrafast irradiated surfaces
N. Del Carmen Lozano, N. Faure, X. Sedao, R. Stoian, C.
Fournier, T. Olivier, and ∙C. Mauclair; Laboratoire Hubert Curien, Saint-Etienne, France
Fourier Ptychography Microscopy (FPM) is used tocharacterize surfaces processed by ultrafast laser. We

analyse its reconstruction performance (amplitude andphase). The FPM constitutes a promising in-situ characterization mean for ultrafast laser machining systems.
CH-P.19 WEDDual-Comb Spectroscopy for Environmental Sensing∙A. Eber, L. Fürst, F. Siegrist, A. Kirchner, R. di Vora,and B. Bernhardt; Institute of Experimental Physics, Graz,
Austria
A mobile frequency-doubled dual-comb set-up wasdeveloped for the measurement of atmospheric trace
gasses. First results from field experiments are compared
to laboratory measurements of nitrogen dioxide and dependencies to traffic volume are discussed.
CH-P.20 WEDClassification Of Environmental Micro-Fibres Using
Stimulated Raman Microspectroscopy∙S. Laptenok1 , L. Genchi1 , C. Martin2,3 , F. Baalkhuyur2 ,C. Duarte2 , and C. Liberale1,4 ; 1 Biological and Environmental Science and Engineering Division, King Abdullah University of Science and Technology , Thuwal, Saudi
Arabia; 2 Red Sea Research Center and Computational
Bioscience Research Center, King Abdullah University of
Science and Technology, Thuwal, Sadi Arabia; 3 Red Sea
Global, SEZ Department of Environmental Sustainability,
AlRaidah Digital City, Riyadh , Sadi Arabia; 4 Computer,Electrical and Mathematical Sciences and Engineering,
King Abdullah University of Science and Technology ,Thuwal, Sadi Arabia
The analysis of the chemical composition of the microfibers collected from different environments using
a broadband stimulated Raman scattering microscopesuggests that most of the collected microfibers are of natural origin.
CH-P.21 WEDStudy of Beam Steering using LCoS for LiDAR
Applications∙S.-J. Son, T.S. Meetei, B. Park, D.-K. Ko, and N.E. Yu;
Gwangju Institute of Science and Technology, Gwangju,
South Korea
Optical beam steering at wavelength of 1550nm using
a LCoS device was investigated for LiDAR application.
The maximum steering angle of 15.6∘ was well matchedwith the short pixel period of 3.6 microns.
CH-P.22 WEDMiniaturization of a multi-gas sensor for environmental gases based on mid-infrared Quantum
Cascade Lasers (QCL) and Silicon integration of
Photoacoustic Cells
C. Constancias1 , B. Ben Bakir1 , ∙M. Doron1 , M. Dubois1 ,O. Lartigue1 , G. Lasfargues1 , J. Skubich1 , M. Volpert1 , G.

Magat1 , J. Marianne1 , P. Labazuy2,3 , S. Moune2,3 , andE. Régis2,3 ; 1 Univ. Grenoble Alpes, CEA, LETI, F-38000
Grenoble, France; 2 Université Clermont Auvergne, CNRS,
IRD, OPGC, Laboratoire Magmas et Volcans, F-63000
Clermont-Ferrand, France; 3 Observatoire de Physique duGlobe Clermont Ferrand (OPGC), Campus Universitairedes Cézeaux, 4 Avenue Blaise Pascal, F-63178 Aubière,
FranceFor environmental purposes, we design the miniaturization of a multi-gas sensor based on mid-infrared Quantum Cascade Lasers and Silicon integration of Photoacoustic Cells. For out-of-the-lab use, electronics downsizing is required without compromise on performance.
CH-P.23 WEDMulti-species Temperature Analysis in Methane
Plasmas using Supercontinuum-based Fourier
Transform Spectroscopy∙R. Krebbers1 , N. Liu1,2 , F.J.M. Harren1 , A.
Khodabakhsh1 , and S.M. Cristescu1 ; 1 Life Science Trace
Detection Laboratory, Institute for Molecules and Materials, Radboud University, Nijmegen, Netherlands; 2 Laser
Spectroscopy and Sensing Laboratory, Anhui University,
Hefei, China
In this presentation, results will be shown using
supercontinuum-based Fourier transform spectroscopy
for methane plasmas. Supercontinuum sources allow toprobe plasmas and observe full ro-vibrational bands ofmultiple molecular species to obtain the plasma temperature.
CH-P.24 WED

Surface Modification to Optimize Generation and
Detection of Light-Induced Acoustics∙M. Illienko1 , P. Sudera1 , M. Velsink1 , and S. Witte1,2 ;1Advanced Research Center for Nanolithography, Amsterdam, Netherlands; 2 Vrije Universiteit Amsterdam, Amsterdam, Netherlands
Weak strain-optic coupling in most materials limits theapplication of ultrafast photoacoustics. We show enhancement of light-induced ultrasound detection by applying transparent nanolayers. Further improvement
can be achieved by nanometre-scaled structuring of thesample surface.
CH-P.25 WEDUltra-sensitive micro-toroid resonator sensor capableof resolving the angular orientation of nanoscale
objects∙M. Jalali and D. Erni; Universität Duisburg-Essen, Duisburg, Germany
A nanoring is added to a micro-toroid, to achieve aplasmonic-photonic coupling between the ring and themicro-toroid. The ring will result in an electric field

137

enhancement around the micro-toroid and accordingly
improves the sensitivity.
CH-P.26 WEDHigh availability motion sensor with nonlinear
interferometry and AI∙R. Matha1,2 , S. Barland1 , and F. Gustave2 ; 1 Université
Côte d’azur – CNRS, Institut de Physique de Nice, Valbonne , France; 2 DOTA, ONERA, Université Paris-Saclay,
Plaiseau, France
We show that a hybrid sensor based on multiple channels of self-mixing interferometry and a neural network provides a high-availability displacement measurement, robust to signal noise and to channel loss for noncooperative targets.
CH-P.27 WED

Large-scale optical compression of free-space using
an experimental three-lens spaceplate∙N.J. Sorensen, M.T. Weil, and J.S. Lundeen; Physics Dept.
and Nexus for Quantum Technologies, University of Ottawa, Ottawa, Canada
We present a broadband three-lens spaceplate consisting of conventional optics in a 4-f arrangement. We experimentally measure compression ratios of 15.6, replacing 4.4 meters of free-space, three orders of magnitude
greater than current optical spaceplates.
CH-P.28 WEDHigh-speed TIRF and 3D super-resolution structured
illumination microscope with large field of view
based on fiber optic components∙H. Ortkrass1 , J. Schürstedt1 , G. Wiebusch1 , K.
Szafranska2 , P. McCourt2 , and T. Huser1 ; 1 Biomolecular
Photonics Research Group, Faculty of Physics, Bielefeld
University, Bielefeld, Germany; 2 Department of Medical
Biology, UiT - The Arctic University of Norway, Tromsø,
NorwayThe presented TIRF and 3D structured illumination microscope (SIM) overcomes present limitations of commercially available and custom-built setups and featuresa small size, different imaging modalities and a costefficient implementaion.
CH-P.29 WED

Sensing the position of a single scatterer in an opaquemedium by mutual scattering
M.D. Truong, A. Lagendijk, and ∙W.L. Vos; Complex Photonic Systems (COPS), MESA + Institute for Nanotechnology, University of Twente, P.O. Box 217, 7500 AE , Enschede, Netherlands
We investigate the potential of mutual scattering, lightscattering with multiple properly phased incident beams,
to study the metrology and extract structural informa-

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Hall B0
CH-P.31 WED

CH-P.33 WED

CH-P.35 WED

Ppb-level detection of methane using quartz
enhanced photoacoustic spectroscopy (QEPAS)
combined with bismuth-doped fiber amplifier∙M. Zatorska and M. Nikodem; Wroclaw University of
Science and Technology, Wroclaw, Poland
Quartz-enhanced photoacoustic spectroscopy ofmethane near 1651 nm is presented. With the useof a novel bismuth-doped fiber amplifier, the detection
limit down to 11 ppb is obtained for dry sample atambient pressure.

A novel Terahertz Microstructure Optical Fibre
Biosensor based on Surface Plasmon Resonance∙Y. Zhang1,2 , T. Miao2 , K. Li1 , N. Conper1 , and J. Xue2 ;1Faculty of Computing, Engineering and Science, University of South Wales, Pontypridd, United Kingdom;2
Department of Physics, School of Arts & Sciences, University of Science & Technology , Xi’an, China
Based on the SPR unique advantages, a D-type MOF
biosensor using graphene as the SPR excitation material
is designed, which presents the highest sensing sensitivity with 1300 GHz/RIU within the THz frequency range.

Electro-Optic Frequency Comb with Fourier-Limited
Pulses achieved with a Hyper-Dispersion Compressor∙E.M. Bayer1,2 , F. Bregolin2 , T. Puppe2 , R. Herda2 , T.
Hellerer1 , and R. Wilk2 ; 1 Hochschule München University of Applied Sciences, Munich, Germany; 2 TOPTICA
Photonics AG, Graefelfing, Germany
We present an EOM-frequency comb, with a repetition
rate of 7.8 GHz and a total spectral width of 132.6 GHz.
We achieve Fourier-limited pulses with a duration of 12
ps via a hyper-dispersion compressor.

Laser Induced Defects for 3D Fluorescence Imaging
of Optical Structures
G. Ong, M. Beresna, G. Brambilla, and ∙T. Lee; Universityof Southampton, Southampton, United Kingdom
We demonstrate a method to 3D image optical structures by exploiting femtosecond laser induced structuraldefects acting as fluorophores for fluorescence imaging.
Silica waveguides, multi-core fibre geometries and multiple cladding layers can be spatially resolved.

CH-P.34 WEDGround-based remote sensing of CO2 in the atmosheric column using a portable laser heterodyne
radiometer with a balanced photodetector
T. Wei, J. Wang, F. Shen, and ∙W. Chen; Université du Littoral Côte d’Opale, Dunkerque, France
All-fiber coupled portable laser heterodyne radiometer(LHR), using a wideband (1500–1640 nm) tunable external cavity diode laser as local oscillator, was developed
for ground-based remote sensing of CO2 in the atmospheric column.

13:00 – 14:00

EE-P.3 WED

EE-P.5 WED

EE-P.7 WED

EE-P: EE Poster session

Low-energy population inversion in graphene
evidenced in a three-pulse pump-probe experiment
K. Mavridou1,2 , A. Seidl1,2 , A. Pashkin1 , M. Helm1,2 , and∙S. Winnerl1 ; 1 Helmholtz-Zentrum Dresden-Rossendorf,
Dresden, Germany; 2 Technische Universität Dresden,
Dresden, Germany
We study the dynamics of mid-infrared population inversion in intrinsic graphene. The population inversion
is unambiguously evidenced by a sign change in the differential transient transmission in a three-pulse pumpprobe experiment.

Bright and ultrafast electron point source made of
LaB6 nanotip
O. Bhorade, I. Blum, J. Houard, B. Deconihout, S.
Moldovan, and ∙A. Vella; UNIROUEN, CNRS, Groupe dePhysique des Matériaux, Normandie Université, Rouen,
FranceWe study the electron emission properties of LaB6 nanotip under static electric field and under femtosecond
laser illumination using a 2.25m laser at 13 MHz. Multiphoton and strong-field emission regimes are reported.

EE-P.4 WED

Ab initio calculations for valley-selective dynamicalFranz-Keldysh effect in monolayer WSe2
∙S. Yamada1 , K. Yabana2 , and T. Otobe1,3 ; 1 Kansai Photon Science Institute, National Institutes for Quantum Science and Technology, Kizugawa, Kyoto, Japan; 2 Center for
Computational Sciences, University of Tsukuba, Tsukuba,
Ibaraki, Japan; 3 Photon Science Center, The University ofTokyo, Hongo, Bunkyoku, Tokyo, Japan
Valley selection control of the dynamical Franz-Keldysh
effect in TMD monolayer is achieved by ab initio calculations mimicking measurements of attosecond transientabsorption spectroscopy. A simplified two-band model
reveals the mechanism behind the phenomena.

Ultrafast nanoplasmonic photoelectron dynamics
between the multiphoton and strong-field regimes
with tunable IR excitation∙B. Bánhegyi1,2 , G. Ligeti1 , Z.G. Kiss1 , Z. Pápa1,3 , P.
Rácz1 , and P. Dombi1,3 ; 1 Wigner Research Centre forPhysics, Budapest, Hungary; 2 Budapest University ofTechnology and Economics, Budapest, Hungary; 3 ELIALPS Research Institute, Szeged, Hungary
We observed transition between multiphoton andstrong-field nanoplasmonic photoemission regimes.
Based on the photoelectron spectra, we identified cutoff electrons even for trinagular spectra (lacking typicalrescattering plateus) and we observed hybrid photoemission channels.

tion, especially the original depth of a moving scatterer,
inside an opaque sample.
CH-P.30 WEDPolarization Grating-Based Spectropolarimeter for
Circular Polarizer Inspections∙Y.-C. Liang1 , Y. Chen2 , C.-T. Wang1 , S.-C. Jeng3 , and C.K. Lee1 ; 1 Department of Photonics, National Sun Yat-sen
University, Kaohsiung, Taiwan; 2 College of Photonics, National Yang Ming Chiao Tung University, Tainan, Taiwan;
3
Institute of Imaging and Biomedical Photonics, Collegeof Photonics, National Yang Ming Chiao Tung University,
Tainan, Taiwan
Traditional inspections of polarizer films are timeconsuming or invasive, such as ellipsometry or crosssection imaging. We estimate the resolution validity by
matrix and construct a polarization grating-based spectropolarimeter to demonstrate efficient inspection of circular polarizers.

EE-P.1 WEDUltrafast, All-Optical, and Highly Efficient Imaging
of Molecular Chirality via Low-Order Nonlinear
Spectroscopy
J. Vogwell1 , L. Rego1 , O. Smirnova2,3 , and ∙D. Ayuso1,2 ;1Imperial College London, London, United Kingdom;2
Max Born Institute, Berlin, Germany; 3 Technische Universität, Berlin, Germany
We introduce an ultrafast chiro-optical method basedon sum-frequency generation. In contrast to traditional
implementations, the medium’s chirality is encoded in
the intensity of the nonlinear response, rather than in its
phase, with extreme efficiency.
EE-P.2 WEDVibrational Ladder Climbing of Liquid-Phase
Carbon Dioxide∙I. Morichika, H. Tsusaka, Q. Wan, and S. Ashihara; Institute of Industrial Science, The University of Tokyo, 4-6-1
Komaba, Meguro-ku, Tokyo 153-8505, Japan
We report on successful demonstration of multiquantum vibrational excitation in the anti-symmetricstretch of liquid-phase carbon dioxide up to the v = 9
state with mid-infrared femtosecond laser pulses.

CH-P.32 WEDNonlinear light stopping via self-action∙R. Arkhipov1,2 , M. Arkhipov1 , I. Babushkin3 , and N.
Rosanov1,2 ; 1 St. Petersburg State University, St. Petersburg, Russia; 2 Ioffe Institute, St. Petersburg, Russia;
3
Institute of Quantum Optics, Leibniz Universit¨at Hannover, Hannover, Germany
In this talk, we demonstrate theoretically recently predicted new phenomenon - the self-stopping of intense
single-cycle optical pulse in a homogeneous resonant
medium.

Optimizing Spacer Layer in Surface PlasmonCoupled Emission Substrates for Single-Molecule
Localization Microscopy∙J.-Z. Lai and F.-C. Chien; Department of Optics and Photonics, National Central University, Taoyuan, Taiwan
The fluorescence signals of blinking fluorophores in the
single-molecule localization microscopy were enhancedby the optimal spacer layer of the surface plasmoncoupled emission substrate for reducing the required excitation power density in live cell imaging.

EE-P.6 WED138

CH-P.36 WED

EE-P.8 WEDRobust generation of isolated attosecond pulses with
self-compressed sub-cycle drivers from negatively
pumped hollow capillary fibers∙M.F. Galán, J. Serrano, E. Conejero Jarque, C.
Hernández-García, and J. San Roman; Universidad
de Salamanca, Salamanca, SpainWe theoretically demonstrate the robust and tunablegeneration of isolated attosecond pulses from high-orderharmonics driven by sub-cycle waveforms generated bysoliton self-compression in a gas-filled hollow capillaryfiber with a decreasing pressure gradient

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Hall B0
Mid-infrared nonlinear response in the excitonic
insulator Ta2 NiSe5∙K. Morimoto, K. Uchida, and K. Tanaka; Department ofphysics, Kyoto university, Kyoto, Japan
We investigated the sideband generation in the excitonic insulator Ta2 NiSe5 with gap-resonant midinfrared pulses and observed enhancements of sideband
emissions with decreasing temperature.

mental Science and Technology, Keio University, Yokohama, Japan; 2 Center for Spintronics Research Network,
Keio University, Yokohama, Japan; 3 National Instituteof Information and Communications Technology, Tokyo,
Japan
We demonstrate ultrafast, uniform coherent populationtransfer of excitons via adiabatic rapid passage using
chirped pulses in InAs QDs with and without a FabryPerot resonator.

EE-P.10 WED

EE-P.12 WED

EE-P.9 WED

We investigated the nature of optical-to-electrical conversion of CEP-dependent ultrafast currents in dielectrics by studying the relationship between the current, laser beam and electrode geometry. We observed signatures of non-local, quasi-instantaneous current transfer.

We investigate influence of MAPbBr3 additives on
crystallinity and carrier dynamics in (FAPbI3)1x(MAPbBr3)x solar cell films and verify that 0.8 mol%
MAPbBr3 stabilizes crystal phase and enhances carrierlife time leading to highest photo-conversion efficiency.

EE-P.13 WED

Attosecond Transient Interferometry∙O. Kneller1 , C. Mor1 , N. Yaffe1 , D. Azoury3 , M. Krüger4 ,S. Patchkovskii2 , and N. Dudovich1 ; 1 Weizmann Instituteof Science, Rehovot, Israel; 2 Max-Born-Institute, Berlin,
Germany; 3 Massachusetts Institute of Technology, Cambridge, MA, USA; 4 Technion - Israel Institute of Technology, HAIFA, Israel
SPRINT resolves the transient phase of attosecond pulses
via XUV-XUV interferometry, revealing the quantum
evolution of strongly driven systems. This scheme
probes the complex , sub cycle dynamics, hidden in mosttransient absorption measurements.

EE-P.14 WED

Non-local transfer of ultrafast currents generated by
few-cycle laser pulses∙B. Fehér1 , V. Hanus1 , V. Csajbók1 , Z. Pápa1,2 , J. Budai2 ,P. Paul3,4 , A. Szeghalmi3,4 , and P. Dombi1,2 ; 1 Wigner
Research Centre for Physics, Budapest , Hungary; 2 ELIALPS Research Institute, Szeged, Hungary; 3 Institute ofApplied Physics, Friedrich Schiller University Jena, Jena,
Germany; 4 Fraunhofer Inst. for App. Opt. and Prec. Eng.,
Centre of Excellence in Photonics, Jena, Germany

Impact of MAPbBr3 Additives on Crystallinity andCharge Carrier Dynamics of Mixed Perovskite Films∙J. Park1 , B.J. Kang2 , T.G. Park1 , J.J. Yoo2 , Y.U. Jeong3 ,M. Park4 , S.S. Shin2 , and F. Rotermund1 ; 1 Departmentof Physics, Korea Advanced Institute of Science and Technology, Daejeon, South Korea; 2 Division of Advanced Materials, Korea Research Institute of Chemical Technology,
Daejeon, South Korea; 3 Radiation Center for Ultrafast
Science, Korea Atomic Energy Research Institute, Daejeon, South Korea; 4 Department of Chemistry, Collegeof Natural Science, Pukyong National University, Busan,
South Korea

13:00 – 14:00

EF-P.3 WED

EF-P.5 WED

EF-P.7 WED

EF-P: EF Poster session

Dark Temporal Cavity Soliton Pairs in Fabry-Pérot
Resonators with Normal Dispersion and Orthogonal
Polarizations∙G.N. Campbell1 , L. Hill1,2 , P. Del’Haye2,3 , and G.-L.
Oppo1 ; 1 University of Strathclyde, Glasgow, United Kingdom; 2 Max Planck Institute for the Science of Light, Erlangen, Germany; 3 Friedrich Alexander University ErlangenNuremberg, Erlangen, Germany
We present dark and dark-bright temporal cavity soliton
pairs for a Fabry-Pérot resonator with a Kerr medium,normal dispersion, and two polarizations. Spontaneous
symmetry breaking of dark soliton pairs results in modified frequency combs.

Bright and dark solitons in pure quartic Kerr
resonators∙P. Parra-Rivas1,4 , S. Hetzel2 , Y. Kartashov3 , P. Fernandez de Cordoba4 , J.A. Conejero4 , A. Aceves2 , and C.
Milian4 ; 1 Dipartimento di Ingegneria dell’Informazione,
Elettronica e Telecomunicazioni, Sapienza Universita diRoma, Roma, Italy; 2 Department of Mathematics, Southern Methodist University, Dallas, USA; 3 Institute of Spectroscopy, Russian Academy of Sciences, Troitsk, Moscow,
Russia; 4 Institut Universitari de Matematica Pura i Aplicada, Universitat Politecnica de Valencia, Valencia, Spain
We study the bifurcation structure and stability of temporal bright and dark dissipative solitons emerging inpure quartic Kerr resonators. We show that pure quartic
dispersion enhances the features of such states.

Femtosecond filaments and air waveguides generated
by TW vortex beams∙S. Fu, B. Mahieu, A. Mysyrowicz, and A. Houard ; Laboratoire d’Optique Appliquée, Palaiseau, France
We study the filamentation of femtosecond vortex beams
produced with different laser sources at 800 nm and 1030
nm and demonstrate the possibility to use these vortex
filaments as meter-scale air waveguide.

The contribution has been withdrawn.
EE-P.11 WEDUltrafast Uniformed Quantum Manipulation with
Chirped Pulses in InAs Quantum Dot Ensemble withResonator∙Y. Takahashi1,2 , K. Miyauchi1,2 , Y. Kinoshita1,2 , K.
Akahane3 , and J. Ishi-Hayase1,2 ; 1 School of Funda-

EF-P.1 WED

Zeno-Like Effect for Supercontinuum Generation by
Soliton Fission∙N. Bahr1,2 , S. Willms1,2 , I. Babushkin1,2 , U. Morgner1,2 ,O. Melchert1,2 , and A. Demircan1,2 ; 1 Institute of Quantum Optics, Leibniz University Hannover, Hannover, Germany; 2 Cluster of Excellence PhoenixD (Photonics, Optics, and Engineering – Innovation Across Disciplines),
Hannover, Germany
Soliton fission of perturbed higher order solitons is inhibited when introducing absorption in the range of frequencies of the resonantly generated dispersive wave.
This demonstrates a classical analog of the quantum mechanical Zeno-Effect.
EF-P.2 WEDObserving in single-shot the space-time dynamics ofsoliton collision with a recirculating fiber loop
∙F. Copie, P. Suret, and S. Randoux; Laboratoire PhLAM,
Université de Lille, Villeneuve d’Ascq, France
Several scenarios of soliton collision are experimentallyobserved in great details via single-shot recordings ofspatiotemporal diagrams. The remarkable impact of
the relative phase between solitons and the collisioninduced temporal shifts are quantitatively verified.

EF-P.4 WEDProgrammable THz-range comb multiplication using
a feedback-controlled multi-wavelength laser∙S. Abdollahi, P. Marin-Palomo, M. Ladouce, and M.
Virte; Brussels Photonics Team (B-PHOT), Vrije Universiteit Brussel, Brussels, Belgium
We demonstrate all-optical THz-range comb multiplication based on a feedback-controlled on-chip multiwavelength laser. Varying the phase of the signal fed
back to the laser we clone the injected comb to offset frequencies up to 1.3THz.

EF-P.6 WEDGeneralized thermodynamics of optical multimodesystems and the breach of the second law ofthermodynamics∙G. Steinmeyer; Max-Born-Institut, Berlin, Germany
Thermodynamic descriptions of optical multimode systems have recently obtained significant attention, despitea frequently observed decrease in entropy, which violates
the second law. Here, a generalized theory is presented
that overcomes shortcomings of previous approaches.

139

EF-P.8 WEDOptical solitons in Hatano-Nelson systems∙I. Komis1,3 , Z.H. Musslimani2 , and K.G. Makris1,3 ;
Institute of Electronic Structure and Laser, Foundation
for Research and Technology-Hellas (FORTH), 70013,
Heraklion, Greece; 2 Department of Mathematics, Florida
State University, Florida, 32306-4510, Tallahassee, USA;
3
ITCP, Department of Physics, University of Crete, 70013,
Heraklion, Greece
We investigate the interplay between Kerr nonlinearity
and non-Hermiticity in a Hatano-Nelson lattice. We
obtain lattice soliton solutions and study their stability,
along with their localization degree as a function of theasymmetric coupling strength.
1EF-P.9 WEDExploring nonlinear propagation with higher orderdispersion: Exact soliton solutions and the structureof their poles∙Y.L. Qiang1 , T.J. Alexander1 , and C.M. de Sterke1,2 ;1Institute of Photonics and Optical Science (IPOS), Schoolof Physics, The University of Sydney, Australia; 2 The Uni-

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versity of Sydney Nano Institute (Sydney Nano), The University of Sydney, Australia
We explore soliton solutions at high dispersion orders.
We present families of analytic bright soliton solutions
and a novel frequency-domain approach that may uncover the analytic form of solutions which are currently
only known numerically.
EF-P.10 WED

Numerical Prediction of Incoherent Modulation
Instability Dynamics through Deep Learning
Approaches∙Y. Boussafa, L. Sader, V.T. Hoang, B. Pessoa Chaves, A.
Tonello, and B. Wetzel; XLIM Research Institute, CNRSUMR 7252, University of Limoges, Limoges, France
We present a numerical study of modulation instability dynamics where optical coherent seeds compete withnoise amplification. We demonstrate that neural networks can efficiently predict these incoherent dynamics
and retrieve the optical seeds parameters.
EF-P.11 WEDPredatory Prey modes for a few moded laser system∙N.G.R. Broderick1 , P.G.R. Smith2 , R. Bannerman2 , A.I.
Flint2 , J.C. Gates2 , and C.B.E. Gawith2 ; 1 Dodd-Walls
Centre and Department of Physics, University of Auckland, Auckland, New Zealand; 2 Optoelectronics ResearchCentre, University of Southampton, Southampton, United
Kingdom
We discuss different models for a Raman-Brillouin Fabry
Perot laser system and compare them to experimental
results. We show that this behaviour can be explainedusing a simple Lotta-Volterra model with multiple preyspecies.
EF-P.12 WEDNoise correlations in phase-locked VECSEL arrays∙S. Karuseichyk1 , V. Pal2 , I. Sagnes3 , and F. Bretenaker1 ;1LuMIn, Université Paris-Saclay, ENS, CNRS, CentraleSupélec, Gif-sur-Yvette, France; 2 Department of Physics,
Indian Institute of Technology Ropar, Rupnagar, India;
3
C2N, CNRS, Université Paris Saclay, Université Paris
Sud, Palaiseau, France
Phase-locking of the VECSEL laser array in a degenerate cavity was investigated. The influence of phaselocking on the intensity noise correlation between neighboring lasers and spectral synchronization up to single
frequency operation was clearly identified.
EF-P.13 WEDEnabling coherent supercontinuum from picosecond
pulses∙D. Castelló-Lurbe; Institut Universitari de Ciències delsMaterials, Universitat de València, Catedrático Agustín

Escardino 9, 46980 Paterna, Spain; Departament deFísica Aplicada i Electromagnetisme, Universitat deValència, Dr. Moliner 50, 46100 Burjassot, Spain; Brussels Photonics, Department of Applied Physics and Photonics, Vrije Universiteit Brussel, Pleinlaan 2, 1050 Brussel, Belgium
Modulation instability of picosecond pulses underanomalous dispersion is canceled by exploiting a Kerrindex resonance in a silicon waveguide. This result opens
a new avenue for generating coherent supercontinuum
from on-chip pulsed lasers.
EF-P.14 WED

How time-distributed feedback impacts the laser
dynamics?
∙M. Skënderas1 , S.W. Jolly1,2 , and M. Virte1 ; 1 Brussels
Photonics (B-PHOT), Vrije Universiteit Brussel, Brussels,
Belgium; 2 OPERA-Photonique, Universite Libre de Bruxelles, Bruxelles, Belgium
We numerically investigate the impact of the timedistributed feedback on the laser dynamics by employing
fiber Bragg Gratings with different lengths but with similar reflectivity. We report stability alterations for gratings
longer than 7 cm.
EF-P.15 WED

Observation of Brillouin backscattering in a 50cmlong high-index doped silica chip waveguide
M. Zerbib1 , V.T. Hoang2 , J.C. Beugnot1 , K.P. Huy1 ,B. Little3 , S.T. Chu4 , D.J. Moss5 , R. Morandotti6 , B.
Wetzel2 , and ∙T. Sylvestre1 ; 1 Institut FEMTO-ST, CNRSUniversité de Franche-Comté, 25030 Besancon, France,
Besancon, France; 2 Université de Limoges, XLIM, UMR
CNRS 7252, 123 Avenue A. Thomas, 87060 Limoges,
France, Limoges, France; 3 QXP Technologies Inc., Xian,
China, Xian, China; 4 Department of Physics, City University of Hong Kong, Tat Chee Avenue, Hong Kong,
SAR, China, Hong Kong, China; 5 Optical Sciences Centre, Swinburne University of Technology, Hawthorn, VIC
3122, Victoria, Australia, Victoria, Australia; 6 INRSEMT, 1650 Boulevard Lionel-Boulet, Varennes, J3X 1S2,
Québec, Canada, Varennes, Canada
We report the observation of Brillouin backscattering in
a 50-cm long spiral high-index doped silica chip waveguide and show that the measured Brillouin frequency
shift at 16 GHz is in very good agreement with theory.
EF-P.16 WED

Bipartite-intensity-correlated comb emissions inquantum cascade lasers∙T. Gabbrielli1,2 , N. Bruno1,2 , N. Corrias3 , S. Borri1,2 ,L. Consolino1,2 , A. Zavatta1,2,3 , P. De Natale1,2 , and
F. Cappelli1,2 ; 1 Istituto Nazionale di Ottica (CNR-INO),
Florence, Italy; 2 European Laboratory for Non-linear

Spectroscopy (LENS), Sesto Fiorentino - Florence, Italy;
QTI srl, Florence, Italy
We demonstrate the presence of intensity correlations
in different comb-emission regimes in quantum cascadelasers, setting the basis for a deeper understanding of the
non-linear processes happening in their waveguide.
3

EF-P.17 WED

Temporal Fourier-Transform Phase Retrieval in
Photorefractive Optical Transient Detection∙J. García-Monreal, F. Silva, E. Roldán, G.J. de Valcárcel,
and A. Esteban-Martín; Departament d’Òptica i Optometria i Ciències de la Visió, Burjassot (Valencia), Spain
We report an experimental method that combines photorefractive optical transient detection with single-spottime-domain interferometric complex-field retrieval.
The system suppresses stationary background, providing
high-contrast detection and measurement of phase shiftsof a light beam.
EF-P.18 WEDSlow vector breathers
D. Stoliarov1 , ∙Q. Wang1 , S. Sergeyev1 , H. Kbashi1 , Z.
Huang2 , and C. Mou2 ; 1 Aston Institute of Photonic Technologies (AIPT), Aston University, Birmingham, United
Kingdom; 2 Key Laboratory of Specialty Fiber Optics andOptical Access Networks, Shanghai University, Shanghai,
China
The slow-scale polarization dynamics of breathers were
examined experimentally. The study showed that thebreather’s power spike emerges according to the periodic phase difference slip, thereby indicating orthogonalstates of polarization desynchronization.
EF-P.19 WEDAsymmetric Nonlinear Couplers: Benefits ofSkewness in Dual-Core Optical Fibers
M. Longobucco1,2 , N.V. Hung3 , L.X.T. Tai4 , R.
Buczynski1,2 , I. Astrauskas5 , A. Pugzlys5 , A. Baltuska5 ,B. Malomed6 , M. Trippenbach7 , and ∙I. Bugar5,8 ;1
Department of Glass, Lukasiewicz Research Network- Institute of Microelectronics & Photonics, Aleja, Lotników 32/46, Warsaw, Poland; 2 Department of Photonics, Faculty of Physics, University of Warsaw, Pasteura5, Warsaw, Poland; 3 International Training Institute forMaterials Science, Hanoi University of Science and Technology, No 1 - Dai Co Viet Str., Hanoi, Vietnam; 4 Facultyof Physics, Warsaw University of Technology, Koszykowa
75, Warsaw, Poland; 5 Photonics Institute, TU Wien,
Gußhausstraße 25-29, Vienna, Austria; 6 Departmentof Physical Electronics, School of Electrical Engineering,
Faculty of Engineering, Center for Light-Matter Interaction, Tel Aviv University, Tel Aviv, Israel; 7 Instituteof Theoretical Physics, Faculty of Physics, University of

140

Warsaw, Pasteura 5, Warsaw, Poland; 8 Department ofChemistry, University of Ss. Cyril and Methodius in
Trnava, Nám. J. Herdu 2, Trnava, Slovakia
High contrast nonlinear switching of sub-nanojoule
femtosecond pulses was achieved using high index difference soft glass dual-core fibers. The advantage of thedual-core asymmetry is studied experimentally and numerically in self-switching and cross switching configurations.
EF-P.20 WEDFundamental laser-cavity detuning underlying
dissipative soliton mode-locked lasers∙L. Dai, S. Sun, Z. Zha, C. Mou, and H. Guo; KeyLaboratory of Specialty Fiber Optics and Optical Access Networks, Joint International Research Laboratoryof Specialty Fiber Optics and Advanced Communication,
Shanghai Institute for Advanced Communication andData Science, Shanghai University, Shanghai, China
We demonstrate off-resonance behavior of optical dissipative solitons in decoherently driven laser cavities.
An external probing laser is introduced to the cavity,
which enables both the laser-cavity detuning measurement, and a soliton on-off switching dynamic.
EF-P.21 WEDExperimental study of the effects of optical feedbackon the spatial and temporal coherence of theradiation emitted by a semiconductor laser∙M. Duque Gijón1 , C. Masoller1 , and J. Tiana-Alsina2 ;1
Departament de Fisica, Universitat Politecnica deCatalunya, Terrassa, Spain; 2 Department de Fisica
Aplicada, Facultat de Fisica, Universitat de Barcelona,
Barcelona, Spain
We propose a simple experimental technique based on
speckle analysis to discriminate the effects of opticalfeedback on spatial and temporal coherence of the lightemitted by an edge-emitting laser in the coherence collapse regime.
EF-P.22 WEDEngineering nonlinear optical processes by arbitrarily manipulating phase relationships of the relevant
electromagnetic fields
C. Ohae1,2 , W. Liu2 , J. Zheng2 , and ∙M. Katsuragawa1,2 ;1Institute for Advanced Science, University of ElectroCommunications, Tokyo, Japan; 2 Graduate School ofInformatics and Engineering, University of ElectroCommunications, Tokyo, Japan
We discuss on engineering nonlinear optical processes
by arbitrarily manipulating phase relationships of therelevant electromagnetic fields and show some experimental results in which high-order Raman-resonant
four-wave-mixing process is used as a typical example.

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EF-P.23 WEDConical Diffraction Holography and Two-wave
Mixing∙M.W. Iqbal1,2 , Y. Shiposh3 , A. Kohutych3 , N. Marsal1,2 ,A. Grabar3 , and G. Montemezzani1,2 ; 1 Université de Lorraine, CentraleSupélec, LMOPS, Metz, France; 2 Chair in

13:00 – 14:00
JSI-P: JSI Poster session
JSI-P.1 WEDNanoscale structural dynamics by EUV transient
gratings∙F. Bencivenga, L. Foglia, C. Masciovecchio, and R. Mincigrucci; Elettra-Sincrotrone Trieste, Trieste, Italy
The use of EUV transient gratings to probe collective dynamics at sub-100 nm length-scales is presented, as wellas the exploitation of this approach in other contexts, including nonlinear spectroscopy in gas phase samples
JSI-P.2 WEDPhotonics, CentraleSupélec, LMOPS, Metz, France; Inst.
for Solid State Physics and Chemistry, Uzhhorod National
Univ., Uzhhorod, Ukraine
Polarization-sensitive holography and two-wave mixing
amplification of vector beams is achieved in optically biaxial photorefractive Sn2 P2 S6 . Under conical diffraction
3

Generation of ultrafast laser pulses at the SXP
instrument of the European XFEL
∙P. Grychtol1 , E. Tikhodeeva1 , M. Seidel2 , C.M. Heyl2 ,V. Vardanyan1 , D. Doblas-Jimenez1 , S. Molodtsov1 , and
M. Izquierdo1 ; 1 European XFEL, 22869 Schenefeld, Germany; 2 DESY, 22607 Hamburg, Germany
This contribution presents the pump-probe laser infrastructure in general and more specifically the laser pulse
compression scheme of the SXP instrument at the European XFEL.
JSI-P.4 WED

Ultrafast Laser Systems for High Repetition Rate
FELs
A. Ahmed, O. Akcaalan, S. Alisauskas, H. Cankaya, G.
Cirmi, J. Darvill, U. Große-Wortmann, V. Hariton, ∙I.
Hartl, S. Hartwell, C.M. Heyl, Y. Hua, Y. Jiang, T. Lang,
F. Pressacco, M. Seidel, A. Swiderski, H. Tavakol, A. Tajalli, H. Tünnermann, M. Kazemi, C. Li, C. Mahnke, C.
Mohr, and J. Zheng; Deutsches Elektronen Synchroton
DESY, Hamburg, Germany
We describe the ultrafast laser systems which are currently planned, under construction or installed to operate the high repetition rate free electron laser facilities
FLASH and European XFEL.

13:00 – 14:00

JSIV-P.2 WED

JSIV-P: JSIV Poster session

Photo-Electrochemical Imaging of Ultrathin
Single-Crystalline Gold Micro-Flakes∙M. Sabzehparvar, P. Feurstein, F. Kiani, and G. Tagliabue; École Polytechnique Fédérale de Lausanne, Lausanne, Switzerland
We study photo-induced activity of gold micro-flakes ofdifferent thicknesses using light-assisted scanning elec-

The contribution has been withdrawn.

EF-P.24 WEDSubharmonic locking and optical frequency combs inshort-cavity swept semiconductor lasers

JSI-P.5 WED

JSI-P.3 WEDTime-Resolved Experiments at the Small Quantum
Systems Beamline at European XFEL
∙T. Mullins, A. Alangattuthodi, T. Baumann, R. Boll, A.
De Fanis, S. Dold, T. Mazza, J. Montano, Y. Ovcharenko,
N. Rennhack, A. Roerig, S. Sasikumar, B. Senfftleben, M.
Togawa, S. Usenko, and M. Meyer; European XFEL, Schenefeld, Germany
We present the many pump-probe capabilities at the SQS
beamline. Experiments on ion spectroscopy, electron
spectroscopy or x-ray scattering, using either two x-ray
pulses or combining x-rays with optical laser pulses canbe carried out.

JSIV-P.1 WED

conditions the effect is possible with any polarization
combinations, including orthogonally polarized object
and reference waves.

High Repetition-Rate Photoinjector Laser System for
S3FEL
B. Zhang1 , X. Li2 , Q. Liu2 , Z. Zhu2 , J. Luo2 , Z. He1,2 ,W. Liu2,3 , ∙G. Wu1,2 , W. Zhang1,2 , and X. Yang1,2,4 ;1State Key Laboratory of Molecular Reaction Dynamics,
Dalian Institute of Chemical Physics, Chinese Academyof Sciences, Dalian, China; 2 Institute of Advanced Science Facilities, Shenzhen, China; 3 School of Physics
and Astronomy, Sun Yat-Sen University, Zhuhai, China;
4
Department of Chemistry and Shenzhen Key Laboratoryof Energy Chemistry, Southern University of Science andTechnology, Shenzhen, China
We present the 1 MHz photoinjector laser system for the
newly proposed Shenzhen superconducting soft X-ray
FEL facility. The current status, challenges, and plans forfurther improving the performance of this laser system
are discussed.
JSI-P.6 WEDEnabling Storage Ring FEL for lasing below 170 nm
and production of 120 MeV circularly polarized γ-ray
by VUV mirrors∙L. Kochanneck1 , H. Ehlers1,2 , S. Mikhailov3,4 , J. Yan3,4 ,V. Popov3,4 , P. Wallace3,4 , G. Swift3,4 , M. Ahmed3,4,5 , Y.K.
Wu3,4 , L.O. Jensen1,6 , and D. Ristau1,7,8 ; 1 Laser Zentrum Hannover e.V, Hollerithallee 8, Hannover 30419,

trochemical microscopy. Our work aims to reveal dependencies on thickness and wavelength for photocatalytic activity and stability, and the possible edge effects.
JSIV-P.3 WED

Optimizing the Nanostructures in Ultrathin
Cu(In,Ga)Se2 Solar Cells∙S. Sedaghat and M. Schmid; Faculty of Physics &141∙A. Stroganov, A. Kovalev, and E. Viktorov; ITMO University, St Petersburg, Russia
We numerically analyze a short-cavity frequency-swept
semiconductor laser model and report on existence ofsubharmonic locking phenomenon that generates sustainable periodic pulse trains with a radian frequency
being a unit fraction of the sweep rate.

Germany; 2 Laseroptik GmbH, Horster Str. 20, Garbsen
30826, Germany; 3 Department of Physics, Duke University, Horster Str. 20, Garbsen 30826, USA; 4 Triangle Universities Nuclear Laboratory, Horster Str. 20, Garbsen
30826, USA; 5 Department of Mathematics and Physics,
North Carolina Central University , Horster Str. 20, Garbsen 30826, USA; 6 Trumpf Lasersystems for Semiconductor Manufacturing GmbH, Johann-Maus-Str. 2, Ditzingen 71254, Germany; 7 Leibniz University Hannover, Institute of Quantum Optics, Welfengarten 1, 30167 Hannover, Germany; 8 Cluster of Excellence PhoenixD (Photonics, Optics and Engineering - Innovation Across Disciplines), Welfengarten 1a, 30167 Hannover, Germany
Storage-ring FEL was enabled for lasing below 170 nm
and 120 MeV gamma ray production by high-reflective
and stable hybride mirrors for the first time.
JSI-P.7 WED

Seed laser upgrade for EEHG operation of FERMI
FEL-1∙P. Cinquegrana, A. Demidovich, G. Kurdi, I. Nikolov, P.
Sigalotti, P. Susnjar, and M. Danailov; Elettra-Sincrotrone
Trieste S.C.p.A., Basovizza, Trieste, Italy
The FERMI FEL upgrade, which is designed to utilize
Echo Enabled Harmonic Generation is under commissioning. We present the details of the updates to the seedlaser system required by this upgrade.

CENIDE, University of Duisburg-Essen, Duisburg, Germany
Dielectric nanostructures assist in trapping the light
more efficiently inside the ultrathin Cu(In, Ga)Se2 absorber. In this work, we opto-electronically investigate the impact of two different dielectric nanostructures(nanoparticles and point contacts) on the photovoltaic
parameters.

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Room 4b ICM⋅ Thursday 29 June 2023
Room 13a ICM

Room 13b ICM

Room 14a ICM

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

EA-2: Nonlinear quantum
opticsCK-8: Advanced design
methods

EH-2: Quantum plasmonics

CA-10: Ytterbium lasers

Chair: Francesco Ceccarelli, Istituto
di Fotonica e Nanotecnologie - Consiglio Nazionale delle Ricerche (IFNCNR), Milano, Italy

Chair: Ivan Bucharov, Sofia University, Bulgaria

EF-3: Kerr solitons andfrequency combs II

Chair: Juergen Volz, Humboldt Universität, Berlin, Germany

Chair: Cristian Ciracì, Istituto italiano di tecnologia, Lecce, Italy

CB-8: Quantum cascade laser
frequency combs
Chair: Giacomo Scalari, ETH,
Zürich, Switzerland

Chair: Pedro Para-Rivas, Università
la Sapienza, Roma, Italy

EA-2.1 THU

CK-8.1 THU

EH-2.1 THU (Invited)

CA-10.1 THU

CB-8.1 THU

EF-3.1 THU

8:30

8:30

Interaction between heralded
non-classical light and a highly
non-linear cold Ryberg-blockaded
ensemble∙F. Hoffet, J. Lowinski, L. Heller, A.
Padron-Brito, K. Theophilo, and H.
de Riedmatten; ICFO - The Insituteof Photonics Science, Casteldefells,
Spain
Systems displaying strong nonlinear response at low light level
have recently drawn attention.
Here, we experimentally demonstrate the interaction between
an input heralded quantum stateof light and a highly non-linear
blockaded Rydberg ensemble.

Inverse Design of Microresonators Using Machine Learning∙A. Pal1,2 , A. Ghosh1,2 , S. Zhang1 ,T. Bi1,2 , and P. Del’Haye1,2 ; 1 Max
Planck Institute for the Science ofLight, 91058 Erlangen, Germany;
2
Friedrich-Alexander-Universität
Erlangen-Nürnberg, 91058 Erlangen,Germany
We apply a machine learning algorithm to inverse design integrated
microresonators with desired dispersion properties along with experimental verification. This method
can be used for tailoring broadband
Kerr soliton frequency combs.

EA-2.2 THU

CK-8.2 THU

8:45

Optical waveform engineering of
non-Gaussian states∙A. Kawasaki1 , K. Takase1,2 ,B.K. Jeong1 , T. Kashiwazaki3 ,T. Kazama3 , K. Enbutsu3 , K.
Watanabe3 , T. Umeki3 , S. Miki4,5 ,H. Terai4 , M. Yabuno4 , F. China4 ,W. Asavanant1,2 , M. Endo1,2 , J.-i.
Yoshikawa2 , and A. Furusawa1,2 ;1The University of Tokyo, Tokyo,
Japan; 2 RIKEN Center for Quantum
Computing, Saitama, Japan; 3 NTT
Device Technology Labs, Kanagawa,Japan; 4 Kobe University, Hyogo,
Japan; 5 National Institute of Information and Communications,Hyogo, Japan
We propose a method of arbitrary-

8:45

Demonstration of a low-depth
universal linear optical circuit∙T. Odagawa1 , K. Sakaino1 , S.
Kimura1 , T. Inagaki1 , H. Tang2 , K.
Tanizawa3 , K. Ikeda4 , M. Okano4 ,M. Takenaka2 , H. Yamada1 , and
N. Matsuda1 ; 1 Tohoku University,
Sendai, Japan; 2 The University ofTokyo, Tokyo, Japan; 3 Tamagawa
University, Tokyo, Japan; 4 National
Institute of Advanced Industrial
Science and Technology, Ibaraki,
Japan
Downsizing a universal linear optical circuit is crucial for scalable
implementation in the limited chiparea. We experimentally demonstrate the feasibility of a novel cir-

8:30

Ultrafast nanophotonics andopto-electronics: from all-opticalswitching based on metamaterialcavity electrodynamics to plasmondriven polaritonic chemistry∙N. Maccaferri; Department of
Physics, Umeå University, Umeå,SwedenHere, we will discuss different ways
to harness ultrafast phenomena
within the field of nanophotonics.
Our results can be applied ina broad range of applications,from all-optical switching-based
information processing to optoelectronics and photochemistry.

8:30

8:30

8:30

21.5 W 153 fs Kerr-lens Modelocked Yb:CALYO Bulk Oscillator∙X. Tian1 , W. Tian1 , Q. Li1 , G.
Wang1 , C. Bai1 , L. Zheng1 , Y. Yu1 , X.
Xu2 , Z. Wei3 , and J. Zhu1 ; 1 Xidian
University, Xi’an, China; 2 Jiangsu
Normal University, Xuzhou, China;
3
Chinese Academy of Science, Beijing, China
We reported on the demonstration of Kerr-lens mode-locked
Yb:CALYO laser, delivering 153-fs
pulses with an average power of
21.5 W.

Frequency modulated combs insemiconductor lasers∙B. Schwarz1,2 , N. Opačak1,2 , F.
Pilat1 , S. Dal Cin1 , J. Hillbrand1 ,M. Beiser1 , R. Weih3 , J. Koeth3 , S.
Höfling4 , M. Piccardo2,5 , and F.
Capasso2 ; 1 Institute of Solid StateElectronics, TU Wien, Vienna,
Austria; 2 John A. Paulson School ofEngineering and Applied Sciences,
Harvard University, Cambridge,
USA; 3 Nanoplus GmbH, Gerbrunn,
Germany; 4 Institute Technische
Physik,University
Würzburg,
Würzburg, Germany; 5 Center for
Nano Science and Technology,
Fondazione Istituto Italiano diTecnologia, Milan, Italy
Most comb research is focused on
the generation of pulses. However, frequency combs can also exhibit a very different behavior withnearly constant output intensity. An
overview on both theory and experiments will be presented.

Quiet point engineering for
low-noise microwave generation
with soliton microcombs
A. Triscari, A. Tusnin, ∙A. Tikan,
and T. Kippenberg; Institute ofPhysics, Swiss Federal Instituteof Technology Lausanne (EPFL),
Lausanne, Switzerland
In this work, we employ the avoided
mode crossing engineering in microresonators for the ultra-low noise
microwave generation with dissipative Kerr solitons.

CA-10.2 THU

CB-8.2 THU

EF-3.2 THU

8:45

Compact Single and Double Pass
Yb Amplifier Using a
High-Brightness Multi-Watt
Tapered Laser Diode∙S. Dabbene1 , R. Gotti1 , D.
Jedrzejczyk2 , A. Heinrich2 , M.
Messner2 , A. Agnesi1 , and F.
Pirzio1 ; 1 Dipartimento di Ingegneria
Industriale e dell’Informazione,
Università di Pavia, Pavia, Italy;2
Pantec Biosolutions AG, Ruggell,
Liechtenstein
We present a Yb:KYW amplifier
pumped by a M2 <1.5, 5-W tapered
diode. Seeding with a continuouswave or mode-locked (<270 fs)
tunable (1023-1035 nm) laser, we
obtained double-pass small-signal142

8:45

Hot-Cavity Linewith
Enhancement Factor of
Mid-Infrared Semiconductor
Lasers∙F. Pilat1 , N. Opačak1 , D.
Kazakov1,2 , S. Dal Cin1 , F.
Capasso2 , G. Strasser1 , and B.
Schwarz1,2 ; 1 Institute of Solid
State Electronics, TU Wien, Wien,
Austria; 2 John A. Paulson School ofEngineering and Applied Sciences,
Harvard University, Cambridge,
Massachusetts, USA
The linewidth enhancement factor
describes the coupling of the intensity and phase of the laser lightand is therefore an important property for frequency comb genera-

8:45

Dissipative coherent structuresand satellite comb generation indispersion-periodic Kerr
microresonators∙M. Anderson, A. Tikan, A. Tusnin,
A. Davydova, J. Riemensberger, andT. Kippenberg; Institute of Physics,
Swiss Federal Institute of Technology Lausanne (EPFL), Lausanne,
Switzerland
We generate broadband satellite
switching wave microcombs in asilicon nitride microresonator withlongitudinally varying dispersion.
We show in theory and experiment
how this variation enables quasiphase matching and the emergenceof Faraday Instability.

CLEO

Room 14b ICM

Room Osterseen ICM®

/Europe-EQEC 2023

⋅ Thursday 29 June 2023

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

CH-9: Quantum andsingle-photon sensing

JSI-5: Ultrafast molecular
dynamics

CF-10: New trends in postcompression II

CG-3: Taylored targets andfieldsCJ-6: Specialty fiber anddevicesEB-10: Quantum memories

Chair: Crina Cojocaru, Universitat
Politecnica de Catalunya, Barcelona,
Spain

Chair: Daniela Rupp, ETH Zürich,
Switzerland

Chair: Ondřej Hort, ELI Beamlines
Facility, Dolní Břežany, Czech Republic

Chair:
Lukas Gallmann,ETH,
Zürich, Switzerland

Chair: Federica PolI, University ofParma, Parma, Italy

CH-9.1 THU (Invited)

JSI-5.1 THU (Invited)

CF-10.1 THU

CG-3.1 THU

CJ-6.1 THU

8:30

Ultrasensitive Concentration andChirality Measurements Realized
by Sub-Shot-Noise Absorption
Spectroscopy Using Entangled
Photon Pairs∙K. Matsuzaki1,2 and T. Tahara2,1 ;1
RIKEN Center for Advanced
Photonics, RIKEN, Wako, Japan;
2
Molecular Spectroscopy Laboratory,
RIKEN, Wako, Japan
Based on sub-shot-noise absorption
spectroscopy that we realized using
entangled photon pairs as the lightsource, we performed concentrationand chirality measurements with asensitivity beyond the limit of theconventional method.

8:30

X-ray Induced Coulomb Explosion
Imaging of Complex Molecules∙R. Boll; European XFEL, Schenefeld,
Germany
Snapshot images of the complete
structure of a gas-phase moleculewith eleven atoms, including allhydrogens, can be recorded by
Coulomb explosion imaging using intense, femtosecond soft X-ray
pulses from the European XFEL.

8:30

Factor hundred compression ofmulti-mJ 1.2 ps pulses at 1030 nm
to few cycles using multi-pass cells∙E. Escoto1 , S. Rajhans1,2 , N.
Khodakovskiy1 , P.K. Velpula3 , B.
Farace1 , R. Shalloo1 , K. Põder1 , J.
Osterhoff1 , W.P. Leemans1 , I. Hartl1 ,and C.M. Heyl1,4,5 ; 1 Deutsches
Elektronen-Synchrotron
DESY,
Hamburg, Germany; 2 FriedrichSchiller-Universität Jena,
Jena,
Germany; 3 UGC-DAE Consortiumfor Scientific Research, Indore, India;
4
Helmholtz-Institute Jena, Jena,
Germany; 5 GSI Helmholtzzentrum
für Schwerionenforschung GmbH,
Darmstadt, Germany
We demonstrate a two orders ofmagnitude compression of 10-mJ,
1.2-ps pulses from a Yb:YAG Innoslab laser system using two gasfilled multi-pass cells, providing 7mJ, few-cycle pulses approaching
the terawatt regime at kHz repetition rate.
CF-10.2 THU

8:45

Factor 9 Compression Down to 31
fs in a High-Pressure
Krypton-Filled Multi-Pass Cell
∙M. Kadiwala1 , S. Goncharov1 , K.
Fritsch2 , and O. Pronin1 ; 1 Helmut
Schmidt University, Hamburg, Germany; 2 n2-Photonics GmbH, Hamburg, Germany
We demonstrate factor-9 compression down to 31 fs in a single
Krypton-filled multi-pass cell withan overall transmission of 95 % andwith 90 % of the energy in the central peak.

8:30

Complex Structures of Spatiallyand Spectrally Resolved SolidHigh Harmonics
K.M. Kowalczyk1 , H. Allegre1 , A.S.
Wyatt2 , E. Springate2 , J.W.G. Tisch1 ,J.P. Marangos1 , and ∙M. Matthews1 ;1Imperial College, London, United
Kingdom; 2 Central Laser Facility,
Harwell, United Kingdom
We present the complex structures of spatially-resolved highharmonics from MgO and Sapphire. The spectral interference
patterns changing with laser andsample parameters present insight
into the channels of strong-fieldrecombination in the crystal
structures.
CG-3.2 THU

EB-10.1 THU

8:30

Towards the development of
mid-infrared all-integrated fiber
laser systems for drone-based
remote sensing∙T. Gretzinger, T.T. Fernandez, andA. Fuerbach; Macquarie University,
Sydney, Australia
The development of a hybrid chipfiber mid-infrared laser system ispresented. It represents the basic building blocks for all-integrated
compact laser sources for dronebased molecular sensing in the spectral fingerprint region.

Simultaneous Trapping of Two
Optical Pulses in an Atomic
Ensemble as Stationary Light
Pulses∙U.-S. Kim and Y.-H. Kim; Department of Physics, Pohang Universityof Science and Technology, Pohang,South Korea
We show theoretically that stationary light pulse (SLP) supports multiple phase-matching conditions andthen experimentally demonstrate simultaneous SLP trapping of two optical pulses, resulting in an effective
Q-factor of 2.9×109 and N-atom cooperativity of 8 × 106 .

CJ-6.2 THU

EB-10.2 THU

8:45

High-order harmonic generation
in a sub-mm glass chip
∙A. Azzolin1,2 , G. Giovannetti2 ,G. Fan2,3,4 , M.S. Ahsan2,5 , S.
Rockenstein1 ,L. Colaizzi1,2,6 ,E. Maansson2 ,D. Faccialà5 ,F. Frassetto7 , D.W. Lodi6 , C.
Manzoni5 , R. Martínez Vàzquez5 ,M. Devetta5 , R. Osellame5 , L.
Poletto7 , S. Stagira5,6 , C. Vozzi5 ,V. Wanie2 , A. Trabattoni2,8 , and F.
Calegari1,2,3 ; 1 Physics Department,
University of Hamburg, Germany;
2
Centre for Free-Electron Laser
Science, DESY, Hamburg, Germany;
3
The Hamburg Centre for Ultrafast
Imaging, University of Hamburg,
Germany; 4 Shangai Key Lab ofModern Optical System, University of Shangai for Science andTechnology, China; 5 Institute for
Photonics and Nanotechnologies,
CNR, Milano, Italy; 6 Physics Department, Politecnico di Milano,
Italy; 7 Institute for Photonics and

143

8:30

Chair: Fabrizio Piacentini, INRIM,
Torino Italia

8:45

Dy3+- and Pr3+-doped phosphateglass optical fibres for laser
emission at visible wavelengths∙N.G. Boetti1 , D. Pugliese2 , M.
Segura3 , S. Slimi3 , P. Loiko4 , G.
Perrone2 , D. Janner2 , M. Ceballos3 ,F. Diaz3 , M. Aguilo3 , X. Mateos3 ,and J. Lousteau5 ; 1 Links foundation, Torino, Italy; 2 Politecnico di
Torino, Torino, Italy; 3 Universitat
Rovira i Virgili , Tarragona, Spain;
4
Université de Caen, Caen, France;
5
Politecnico di Milano, Milano, Italy
Dy3+- and Pr3+-doped phosphateglasses were investigated as gain material for visible laser emission. Optical fibres were manufactured fromthe developed glasses and a prelim-

8:45

Spectral superresolution using aquantum memory∙M. Mazelanik1 , A. Leszczyński1 ,and M. Parniak1,2 ; 1 Universityof Warsaw, Warsaw, Poland;
2
UniversityofCopenhagen,Copenhagen, Denmark
We demonstrate a quantum-optimalmeasurement of frequency separation between two narrow spectral
lines by utilizing optical quantum
memory with built-in processing capabilities.

CLEO

Room 1 ICM

Room 4a ICM

waveform engineering of optical
non-Gaussian states and demonstrate the generation of Schrödinger
cat states with waveforms useful forlarge-scale optical quantum computing.

cuit structure with about half a circuit depth of conventional ones.

EA-2.3 THU

CK-8.3 THU

9:00

®

/Europe-EQEC 2023

Room 4b ICM

9:00

EH-2.2 THU

9:00⋅ Thursday 29 June 2023
Room 13a ICM

Room 13b ICM

gain G0 ∼40, Pout ∼2.5 W, optical-tooptical efficiency ∼50%, M2 <1.1.

tion. Here we study different midinfrared lasers and operating conditions.

CA-10.3 THU

CB-8.3 THU

9:00

Room 14a ICM

9:00

Single photon routing using a
waveguide coupled atomic array∙T. Ray, J. Berroir, Z. Li, A. Urvoy, and J. Laurat; Laboratoire
Kastler Brossel, Sorbonne Université,
CNRS, ENS-Université PSL, Collegède France, Paris, France
We demonstrate the routing of a single photon by controlling the reflection and simultaneously creating an electromagnetically induced
transparency window in a waveguide coupled atomic array.

Machine Learning Techniques for
the Free-Form Inverse Design ofNanophotonic Devices∙T. Gahlmann and P. Tassin;
Chalmers University of Technology,
Gothenburg, Sweden
Free-form inverse design ofnanophotonic matasurfaces canbe solved with a modified CGAN
machine learning method thatbalances the accuracy of desired optical properties with experimental
feasibility.

Ultrasensitive Optical Probing of
Plasmonic Hot Electron
Occupancies
J. Budai1,2 , Z. Pápa1,3 , P. Petrik4 ,and ∙P. Dombi1,3 ; 1 ELI-ALPS, ELIHU Non-Profit Ltd., Szeged, Hungary; 2 Department of Optics andQuantum Electronics, University ofSzeged, Szeged, Hungary; 3 Wigner
Research Centre for Physics, Budapest, Hungary; 4 Institute of Technical Physics and Materials Science,Centre for Energy Research, Budapest, Hungary
We demonstrate with ellipsometry that upon the optical excitation of surface plasmon polaritons,
a non-thermal electron population
appears in the topmost domain of
the plasmonic film directly coupled
to the local fields

Diode-pumped Kerr-lens modelocked Yb:YAl3(BO3)4 laser
H.-J. Zeng1 , Z.-L. Lin1 , W.-Z. Xue1 ,G. Zhang1 , Y. Huang1 , Y. Chen1 , V.
Petrov2 , P. Loiko3 , X. Mateos4 , L.
Wang2 , and ∙W. Chen1,2 ; 1 Fujian
Institute of Research on the Structure of Matter, Chinese Academyof Sciences, Fuzhou, China; 2 Max
Born Institute for Nonlinear Optics
and Short Pulse Spectroscopy, Berlin,
Germany; 3 Université de Caen, Caen
Cedex, France; 4 Universitat Rovira i
Virgili, Tarragona, SpainWedemonstrateadiodepumped Kerr-lens mode-locked
Yb:YAl3(BO3)4 laser delivering
soliton pulses as short as 36 fs at
1059.7 nm with an average output
power of 156 mW at 66.7 MHz.

Sub-Bandwidth Limited TimeDomain Signal in Mid-Infrared
Quantum Cascade Lasers∙B. Schneider, A. Dikopoldsev, F.
Kapsalidis, P. Täschler, M. Beck, andJ. Faist; ETH, Zürich, Switzerland
We demonstrate the observationof ultrashort features below the
Fourier-limit in the time domain
signal of mid-infrared quantum cascade laser frequency combs under
RF-injection. Mean-field theory
based simulations confirm the potential occurrence of such features.

EA-2.4 THU

CK-8.4 THU

EH-2.3 THU

CA-10.4 THU

CB-8.4 THU

9:15

Multimode squeezing in dissipative Kerr solitons∙M.A. Guidry1 , D.M. Lukin1 , K.Y.
Yang1,2 , and J. Vuckovic1 ; 1 E. L.
Ginzton Laboratory, Stanford University, Stanford, CA, USA; 2 John A.
Paulson School of Engineering andApplied Sciences, Harvard University, Cambridge, MA, USA
We study broadband quadraturesqueezing in Kerr soliton crystal microcombs. We propose an integrated photonic architecture to efficiently squeeze light over many
modes, enabled by the phase-locked
soliton dynamics.

9:15

Spectral Control of Microlaser
Array Using Artificial Neural
Networks∙W.K. Ng1 , Z. Xuan1 , D. Saxena1 ,I. Tanghe2,3 , K. Molkens2,3 , T.V.
Raziman1 , P. Geiregat3,4 , D.V.
Thourhout2,3 , and R. Sapienza1 ;1
The Blackett Laboratory, Department of Physics, Imperial College
London, London, United Kingdom;
2
Photonics Research Group, Ghent
University - imec, Ghent, Belgium;
3
Center for Nano- and Biophotonics,
Ghent University, Ghent, Belgium;
4
Physics and Chemistry of Nanostructures (PCN), Ghent University,
Ghent, Belgium
We achieved control of the lasing
spectrum in a complex system using a tandem neural network. The

9:15

Electron-near-field couplingstrength in gold nanoparticles∙E. Akerboom1 , V. di Giulio2 , N.J.
Schilder1 , F.J. Garcia de Abajo2 ,and A. Polman1 ; 1 NWO-Institute
AMOLF, Amsterdam,
Netherlands; 2 ICFO-Institut de Ciencies
Fotoniques, Barcelona, Spain
We study the coupling strength
between electrons and the opticalnear fields of dipole modes in gold
nanoparticles using Cathodoluminescence spectroscopy. Our model
goes beyond the non-recoil approximation and matches the foundtrends in measurements.

9:15

Single crystalline and ceramic
Yb:Lu2O3 gain media in thin-disklaser operation∙S. Esser1 , X. Xu2 , T. Graf1 , and
M. Abdou Ahmed1 ; 1 Universityof Stuttgart, Institut für Strahlwerkzeuge(IFSW),
Stuttgart,
Germany; 2 Jiangsu Key Laboratoryof Advanced Laser Materials andDevices, School of Physics andElectronic Engineering, Jiangsu
normal University, Xuzhou, China
The sesquioxide crystal Yb:Lu2O3
has excellent properties for thindisk lasers of high average power. A
conventionally grown single-crystal
and a polycrystalline ceramic
Yb:Lu2O3 disk are compared withregard to their laser performance.

144

9:15

Near-Infrared Optical Illumination for Injection Locking in
Quantum Cascade Lasers∙M. Bertrand1 , A. Parriaux2 , K.
Komagata2 , T. Südmeyer2 , andJ. Faist1 ; 1 Institute for Quantum
Electronics, ETH Zürich, Zürich,
Switzerland; 2 Laboratoire TempsFréquence, Institut de Physique,
Université de Neuchâtel, Neuchâtel,Switzerland
We study the influence of a 1.55 μm
pulse laser illuminating a quantum cascade laser frequency comb.
We demonstrate optical injection
locking of the repetition rate andspectral modification of the midinfrared spectrum.

EF-3.3 THU

9:00

Optical frequency combs inducedby modulation instability in fiber
Fabry-Pérot resonators: impact ofthe pump pulse duration∙T. Bunel1 , M. Conforti1 , Z.
Ziani1 , J. Lumeau2 , A. Moreau2 , A.
Fernandez3 , O. Llopis3 , J. Roul3 , A.
Perego4 , K. Wong5 , and A. Mussot1 ;1
University of Lille, CNRS, UMR
8523-PhLAM Physique des Lasers,
Atomes et Molécules, Lille, France;
2
Aix Marseille University, CNRS,
Centrale Marseille, Institut Fresnel,
Marseille, France; 3 LAAS-CNRS,
Université de Toulouse, CNRS, 7
avenue de Colonel Roche, Toulouse,
France; 4 Aston Institute of Photonic
Technologies, Aston University,
Birmingham, United Kingdom;
5
Department of Electrical and Electronic Engineering, The Universityof Hong Kong, Pokfulam Road,
Hong-Kong, China
We investigate the modulation
instability (MI) process in a fiber
Fabry-Pérot resonator generating
MI Kerr frequency combs in an
all-fiber setup.
Also, we showthat the driving pulse duration
impacts the Fabry-Pérot nonlinear
dynamics.
EF-3.4 THU

9:15

Dual frequency Raman cavity
soliton comb in a mini fiber ringcavity∙Y. Xu1,2 , Z. Li1,2 , S. Coen1,2 , M.
Erkintalo1,2 , and S. Murdoch1,2 ;1The Dodd-Walls Centre for
Photonic and Quantum Technologies, Dunedin, New Zealand;
2
Department of Physics, University of Auckland, Auckland, New
Zealand
Recent development of Raman gain
Kerr cavity solitons has opened a
new approach for generating ultrabroad frequency combs.
Wedemonstrate experimentally a dualRaman cavity soliton comb generation in a mini fibre ring cavity.

CLEO

Room 14b ICM

CH-9.2 THU

Room Osterseen ICM

9:00

JSI-5.2 THU

9:00

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)

CF-10.3 THU

9:00

Sub-μm Axial Precision Depth
Imaging With Entangled TwoColour Hong-Ou-Mandel
Microscopy∙C. Torre, A. McMillan, J. MonroyRuz, and J.C.F. Matthews; Quantum Engineering Technology Labs,
University of Bristol, Bristol, United
Kingdom
Sub-μm axial precision for 3D imaging Hong-Ou-Mandel microscopy is
experimentally demonstrated using
confocal imaging and a wavelengthentangled photon pair source with ∼103 photon pairs per pixel for semitransparent sample with ∼ 5 μm
depth features.

All-XUV Transient-Absorption
Spectroscopy On the Ultrafast
Dissociation of Oxygen Molecules∙M. Rebholz, A. Magunia, G.D.
Borisova, H. Lindenblatt, F. Trost,
R. Moshammer, C. Ott, and T.
Pfeifer; Max-Planck Institute for Nuclear Physics, Heidelberg, Germany
We employ all-XUV pump—probetransient-absorption spectroscopy
to investigate the femtosecond
dissociation dynamics of oxygen.
The time-dependent absorption
signal allows us to extract time
constants of the dissociation process
for neutral and charged oxygenfragments.

High-energy pulse compression ina multi-pass cell at 2μm∙T. Nagy, F. Furch, M. Bock, andU. Griebner; Max Born Institute for
Nonlinear Optics and Short Pulse
Spectroscopy, Berlin, Germany
We present high-energy pulse compression at 2μm in a multi-passcell. 40mJ, 2.8ps pulses at 1kHz are
spectrally broadened in a 3-m longmulti-pass cell filled with 850mbar
air. Experiments are compared with
3D simulations.

CH-9.3 THU

JSI-5.3 THU

CF-10.4 THU

9:15

Time-Correlated Single-Photon
Counting Measurements: A New
Approach For High-Speed∙A. Bovolenta, S. Farina, G. Acconcia, and I. Rech; Politecnico di
Milano, Milan, Italy
Historically, Time-Correlated Single Photon Counting (TCSPC) technique was characterized by long acquisition time. A completely new
approach will be presented, whichremoves all limitations, opening theway to a high-speed and zero distortion TCSPC.

9:15

Creating Electronic MolecularMovies Using Time-Resolved
X-Ray Photoelectron Spectroscopy∙D. Mayer1 , F. Lever1 , D. Picconi2 ,S. Alisauskas1 , A. Azzolin3,4 ,F. Calegari3,4,5 , G. Cirmi1,4 , S.
Düsterer1 , U. Frühling1 , A. Green6,7 ,I. Hartl1 , M. Kuhlmann1 , T.
Mazza6 , S. Palutke1 , S. Schulz1 , A.
Trabattoni4,8 , A. Tul Noor1 , andM. Gühr1 ; 1 Deutsches ElektronenSynchrotron (DESY), Hamburg,
Germany; 2 Zernicke Institute forAdvanced Materials, Groningen,
Netherlands; 3 University of Hamburg, Hamburg, Germany; 4 Center
for Free-Electron Laser Science(CFEL), Hamburg, Germany; 5 The
Hamburg Centre for Ultrafast Imag-

9:15

High average power nonlinear
post-compression at 1.9 μm
wavelength employing a gas-filled
multi-pass cell
∙L. Eisenbach1,2 , T. Heuermann3,4,5 ,Z. Wang3 , J. Schulte1,2 , R. Meyer1 ,M. Lenski3 , P. Gierschke3,6 , M.
Sugiura7 , K. Tamura7 , P. Rußbüldt1 ,J. Limpert3,4,5,6 , and C. Häfner1,2 ;1Fraunhofer Institute for Laser Technology (ILT), Aachen, Germany;
2
Chair for Laser Technology LLT,RWTH Aachen University, Aachen,
Germany; 3 Institute of Applied
Physics, Abbe Center of Photonics,
Friedrich-Schiller-University
Jena, Jena, Germany; 4 HelmholtzInstitute Jena, Jena, Germany; 5 GSI
Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany;⋅ Thursday 29 June 2023
Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Nanotechnologies, CNR, Padova,
Italy; 8 Institute of Quantum Optics,
Leibniz Universitaet Hannover,Germany
In this work we present experimental results on High-order Harmonic
Generation in a sub-mm glass cell,showing a remarkable extension of
the cut-off. The results are fully supported by 3D propagation simulations.

inary assessment of their emission
under blue light pumping was conducted.

CG-3.3 THU

9:00

The dynamical Franz-Keldysh
effect in the deep ultraviolet
probed by transient absorption
and dispersion of diamond
J. Reislöhner1 , X. Chen2 , D. Kim1 , S.
Botti2 , and ∙A.N. Pfeiffer1 ; 1 Instituteof Optics and Quantum Electronics,
Friedrich Schiller University, Jena,
Germany; 2 Institute of Condensed
Matter Theory and Optics, Friedrich
Schiller University, Jena, Germany
A tailored deep ultraviolet field
is used for transient absorption
and dispersion spectroscopy of diamond.
The dynamical FranzKeldysh effect and the optical Kerr
effect coexist in the near-bandgap
region.
CG-3.4 THU

9:15

The secret recipe for passive CEP
stabilization∙G. Steinmeyer1 , L. Ehrentraut1 , M.
Schnürer1 , R. Maksimenka2 , and N.
Forget2 ; 1 Max-Born-Institut, Berlin,
Germany; 2 Fastlite, Antibes, France
While conceptually appealing, passive CEP stabilization schemes often
exhibit disappointing noise performance. Excessive phase jitters arise
due to Gordon-Haus jitter multiplication during nonlinear spectral
broadening, but can be mitigatedwith suitable seed lasers.

145

CJ-6.3 THU

9:00

Room 8 Hall A1 (A12)

EB-10.3 THU

9:00

Revisiting Pump Light Absorption in Structured Double Clad
Fibers∙B.
Yildiz1,2 ,D.
Häßner1 ,1
A. Grobecker , S. Kuhn1 , N.
Haarlammert1 , and T. Schreiber1 ;1Fraunhofer Institute for Applied
Optics and Precision Engineering,
Jena, Germany; 2 Institute of Applied
Physics, Jena, Germany
We present the influence of thenumerical aperture on multimodelights behavior in specialty, double clad amplifier fibers. It is observed that depending on the incoming fields numerical aperture afibers absorption characteristic canvary drasticallyMachine learning optimal control
pulses in an optical quantum
memory∙E. Robertson1,2 , L. Esguerra1 ,L. Messner3 , G. Gallego2 , and J.
Wolters1,2 ; 1 Institute für Optische
Sensorsysteme, Deutsches Zentrum
für Luft- und Raumfahrt, Berlin,
Germany; 2 Technische Universität
Berlin, Berlin, Germany; 3 Institut
für Physik, AG Theoretische Optik
Photonik, Humboldt-Universität zu
Berlin, Berlin, Germany
We present a genetic algorithm applied to the control pulses of an optical memory, achieving a memory
efficiency of 0.35, and demonstrating a reduction of the pulse powerby 50%, with a minimal efficiency
tradeoff.

CJ-6.4 THU

EB-10.4 THU

9:15

Bi-Pulse Fiber Laser Source
Concept for Integrated-Path
Differential Absorption Lidarfrom Space∙L. Lombard, N. Cézard, A. Durécu,
and F. Gustave; Onera - The French
Aerospace Lab, Palaiseau, France
We propose and demonstrate a new
all-fiber 1.5μm Master-OscillatorPower-Amplifier architecture basedon bi-pulse strategy to mitigate
Stimulated-Brillouin-Scattering.
The pulses are alternatively long,narrow-linewidth and short, largelinewidth to alternate gas sensing
and altimetry functions from space.

9:15

A Single-Photon-Compatible
Telecom-C-Band Quantum
Memory in a Hot Atomic Gas
S. Thomas1 , S. Sagona-Stophel1 ,Z. Schofield2 , I. Walmsley1 , and∙P. Ledingham2 ; 1 IQOLS, Department of Physics, Imperial
College London, London, United
Kingdom; 2 Department of Physics
and Astronomy, The University ofSouthampton, Southampton, United
KingdomThis work demonstrates a hotatom-based quantum memory
for telecommunication photons
with a signal-to-noise ratio of
1.9(1) × 104 for input coherent
states of μin = 0.084(10) photons
per pulse.

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Room 4b ICM⋅ Thursday 29 June 2023
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modes that share the same spatial gain profile were also identified
through the weights of the trainedneural network.

EA-2.5 THU

9:30

Generating Ultracold Atomic
Persistent Currents with
Structured Light
G.W. Henderson, G.R.M. Robb, ∙G.L. Oppo, and A.M. Yao; SUPA &Department of Physics, University ofStrathclyde, Glasgow, United Kingdom
We model the evolution of coupled
ultracold atomic and optical fields
within a driven optical cavity, realising dynamic atomic persistent currents. The current’s speed and direction is determined by the light’s orbital angular momentum.

CK-8.5 THU

9:30

Predicting the interplay between
second- and third-order nonlinear
interaction in periodically-poled
nanophotonic waveguides using
machine learning∙S. Lauria and M.F. Saleh; HeriotWatt University, Edinburgh, United
Kingdom
We have developed a recurrent neural network that efficiently simulates the unidirectional pulse propagation equation. The model isvalidated via predicting complex
nonlinear interactions in a periodically poled nanophotonic LiNbO3
waveguide.

EH-2.4 THU

9:30

Ultrafast Charge and Spin
Dynamics in Au-Ni
Nanostructures
T. Tapani1 , N. Henriksson1 , A.
Ciuciulkaite2 , T. Deckert3 , J.
Allerbeck4 , H. Lee5 , D. Garoli6 , P.
Vavassori7 , D. Brida3 , V. Kapaklis2 ,and ∙N. Maccaferri1 ; 1 Umeå University, Umeå, Sweden; 2 Uppsala
University,
Uppsala,Sweden;3
University of Luxembourg, Luxembourg, Luxembourg; 4 Empa, Swiss
Federal Laboratories for Materials
Science and Technology, Dübendorf,
Switzerland; 5 Korea University,
Seoul, South Korea; 6 Istituto Italiano
di Tecnologia, Genova, Italy; 7 CIC
nanoGUNE & IKERBASQUE, San
Sebastian, Spain
We study charge and spin dynamics in hybrid Au-Ni nanostructures.
Experimental results, verified by numerical modelling, reveal a modification of the ultrafast demagnetization and dynamics induced by thestrong plasmonic response in the Au
structure.

CA-10.5 THU

9:30

High Performance Ytterbium
Regenerative Amplifier Based on
Yb:CALYO with High Energy 100
fs Pulses∙L. Petrov1 , D. Velkov1 , K. Georgiev
1, A. Trifonov2 , X. Xu3 , T.
Popminchev4,5 , and I. Buchvarov1,6 ;1Physics Department, Sofia University, Sofia, Bulgaria; 2 IBPhotonics
Ltd., Sofiia, Bulgaria; 3 Jiangsu Key
Laboratory of Advanced Laser Materials and Devices, School of Physics
and Electronic Engineering, Jiangsu
Normal University, Xuzhou, China;
4
Department of Physics, Universityof California San Diego, La Jolla,
USA; 5 Photonics Institute, TU Wien,
Vienna, Austria; 6 John Atanasoff
Center for Bio and Nano Photonics(JAC BNP), Sofia, Bulgaria
We present a high-performance
chirped-pulse regenerative amplifier based on a single disordered
Yb:CaYAlO4 crystal, generatingrecord-short ultrafast pulses of 102
fs and 2.2 mJ energy at 1 kHz

146

CB-8.5 THU

9:30

Comb formation in ring
Quantum Cascade Lasers underradio-frequency injection∙I. Heckelmann, M. Bertrand,
A. Dikopoltsev, M. Montesinos
Ballester, M. Beck, G. Scalari, andJ. Faist; Swiss Federal Instituteof Technology (ETH), Zürich,
Switzerland
Broadband optical frequency combs
have become fundamental for spectroscopic applications. Here, we
demonstrate an egg-shaped ring
Quantum Cascade Laser underradio-frequency injection as acontinuously tunable source forboth single-mode and coherent
multimode operation.

EF-3.5 THU

9:30

Thermally stable initiation ofdissipative Kerr solitons inphotonic molecules∙Ó.B. Helgason, M. Girardi, Z. Ye,
F. Lei, J. Schröder, and V. TorresCompany; Chalmers University ofTechnology, Gothenburg, Sweden
We demonstrate coupled anomalous dispersion microcavities enabling blue-detuned operation andthermally stable initiation of a dissipative Kerr soliton.

CLEO

Room 14b ICM

CH-9.4 THU

Room Osterseen ICM

9:30

Single-photon detector based
long-distance Brillouin opticaltime domain reflectometry∙M. Romanet1 , E. Rochat2 , K. Phan
Huy3 , and J.-C. Beugnot1 ; 1 FemtoST institute, CNRS UMR 6174,
University of Franche-Comté, 15B
avenue des Montboucons, 25000,
Besançon, France; 2 Omnisens SA,
Riond-Bosson 3, 1110 Morges,
Switzerland; 3 Femto-ST institute,
CNRS UMR 6174, Supmicrotech ENSMM, 15B avenue des Montboucons,
25000, besançon, France
We present a novel distributed
Brillouin optical time domainreflectometer based on quantum
technologies, using a single-photon
avalanche diodes in gated mode,with a range of 120 km and 10 m
spatial resolution.

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)ing, Hamburg, Germany; 6 European
XFEL,
Hamburg,
Germany;7
Stanford PULSE Institute, Menlo
Park, USA; 8 Leibnitz Universität
Hannover, Hannover, Germany
We show that time-resolved XPS is a
useful tool to track transient charge
flows in molecules after UV excitation. This provides direct sensitivity
to electronic states invovled in themolecular relaxation.

6

JSI-5.4 THU

CF-10.5 THU

9:30

Probing the Population of Dark
States in Ultrafast Reactions of
Nucleobases with Time-Resolved
NEXAFS at Free-Electron Lasers
F. Lever1 , ∙D. Mayer1 , D. Picconi2 ,S. Alisauskas1 , F. Calegari3,4,5 , S.
Düsterer1 , C. Ehlert6 , R. Feifel7 ,M. Kuhlmann1 ,T. Mazza8 ,M. Robinson4 , R. Squibb7 , A.
Trabbatoni4,11 , M. Ware9 , P.
Saalfrank10 , T. Wolf9 , and M.
1
Gühr1 ;
Deutsches ElektronenSynchtrotron (DESY), Hamburg,
Germany; 2 Zernicke Institute forAdvanced Materials, Universtity ofGroningen, Groningen, Netherlands;
3
Institut für Experimentalphysik,
University of Hamburg, Hamburg,
Germany; 4 Center for Free-Electron
Laser Science (CFEL), Hamburg,
Germany; 5 The Hamburg Centre
for Ultrafast Imaging, Universityof Hamburg, Hamburg, Germany;
6
Heidelberg Institute for Theoretical Studies (HITS), Heidelberg,
Germany; 7 Department of Physics,
Gothenburg University, Gothenburg,
Sweden; 8 European XFEL, Schenefeld, Germany; 9 Stanford PULSE
Institute, SLAC National Accelerator
Laboratory, Menlo Park, USA;
10
Institut für Chemie, Universität
Potsdam,
Potsdam,Germany;
11
Leibnitz Universität Hannover,Hannover, Germany
UV absorption in nucleobases is amajor cause of genetic lesions. We
use time-resolved NEXAFS spectroscopy to probe ultrafast internalconversion in the dynamics of UVphotoexcited thionucleobases. We⋅ Thursday 29 June 2023
Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)

Fraunhofer Institute for Applied
Optics and Precision Engineering(IOF), Jena, Germany; 7 Tokai
Optical Co., Ltd., Okazaki, JapanWe demonstrate the highly efficientnonlinear temporal compression of
178 W average power at 1.9 μm
wavelength down to 30 fs employing
a gas-filled Herriott-type multi-pass
cell.
9:30

Thermodynamic and nonlinear
optical analysis of multipass-cellbased pulse compression in the 2μm range∙C. Mei1 , U. Griebner2 , and G.
steinmeyer2,3 ; 1 Research Center for
Convergence Networks and Ubiquitous Services, University of Scienceand Technology Beijing, 100083 Beijing, China, Beijing, China; 2 Max
Born Institute for Nonlinear Optics
and Short Pulse Spectroscopy, MaxBorn-Stra\ss e 2a, 12489 Berlin, Germany, Berlin, Germany; 3 Institut
für Physik, Humboldt Universität zu
Berlin, Berlin, Germany
We numerically investigate pulse
compressions in four different solidmaterials inside multipass cells. It
shows that thermodynamic property of materials is at least equallyimportant as optical properties. Ourfindings provide effective guidelines
for high-energy 2-μm pulse compressorion.

CG-3.5 THU

9:30

Attosecond soft X-ray
spectroscopy reveals energy flow
in a semimetal
T. Sidiropoulos1 , N. Di Palo1 ,D. Rivas1,2 , S. Severino1 , M.
Reduzzi1 , ∙H.-W. Sun1 , Y.-H.
Chien1 , B. Nandy1 , B. Bauerhenne3 ,S. Krylow3 , T. Vasileiadis4 , T.
Danz5 , P. Elliott6,7 , S. Sharma6 , J.K.
Dewhurst7 , C. Ropers5 , Y. Joly8 , M.
Garcia3 , M. Wolf4 , R. Ernstorfer4 ,and J. Biegert1,9 ; 1 ICFO - Institut deCiencies Fotoniques, The Barcelona
Institute of Science and Technology,
Castelldefels, Spain; 2 European
XFEL GmbH, Holzkoppel 4, Schenefeld, Germany; 3 Theoretische
Physik, FB-10, Universität Kassel,
Kassel, Germany; 4 Fritz Haber
Institute of the Max Planck Society,
Berlin, Germany; 5 4th PhysicalInstitute - Solids and Nanostructures, University of Göttingen,Göttingen, Germany; 6 Max-BornInstitut für Nichtlineare Optik
und Kurzzeitspektroskopie, Berlin,
7
Germany;
Max-Planck-Institut
für Mikrostrukturphysik, Weinberg
2, Halle, Germany; 8 Université
Grenoble Alpes, CNRS, Grenoble
INP, Institut Néel, Grenoble, France;
9
ICREA-Institució Catalana de Recerca i Estudis Avançats, Barcelona,
Spain
We show that core-level x-ray absorption near edge structure spectroscopy with attosecond soft x-ray
pulses can image the energy flow between electrons, holes, and phonons
inside a material in real time.

147

CJ-6.5 THU

9:30

Yellow Silica Fiber Laser
Delivering an Output Power of∼150 mW∙M.-P. Lord, L. Talbot, M. Bernier,and R. Vallée; Centre d’optique, photonique et laser (COPL), Université
Laval, Québec, Canada
We report a dysprosium-doped silica fiber laser yielding an output
power of 147 mW at 585 nm. To
the best of our knowledge, this is thefirst demonstration of a monolithic
visible silica fiber laser.

EB-10.5 THU

9:30

Scalable Quantum Memory Nodes
using nuclear spins in Silicon
Carbide∙S.K. Parthasarathy1,2 , B. Kallinger1 ,F. Kaiser3,4 , P. Berwian1 , D.B.R.
Dasari3,4 , J. Friedrich1 , and R.
Nagy2 ; 1 Fraunhofer Institute for
integrated Systems and Device
Technology (IISB), Erlangen, Germany; 2 Group of Applied Quantum
Technologies, Friedrich-AlexanderUniversität
Erlangen-Nürnberg(FAU), Erlangen, Germany; 3 3rdInstitute of Physics and Stuttgart
Research Center of Photonic Engineering (SCoPE), University of
Stuttgart,
Stuttgart,
Germany;
4Center for Integrated Quantum
Science and Technology (IQST),
Ulm, Germany
A distributed quantum network
would require quantum nodes
with high fidelity. We show herethat using the solid-state spins in
4H-Silicon Carbide (4H-SiC) such agoal of Scalable Quantum memory
node could be realized.

CLEO

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Room 4a ICM

EA-2.6 THU

9:45

CK-8.6 THU®

/Europe-EQEC 2023

Room 4b ICM

9:45

EH-2.5 THU⋅ Thursday 29 June 2023
Room 13a ICM

9:45

Room 13b ICM

CA-10.6 THU

9:45

CB-8.6 THU

Room 14a ICM

9:45

EF-3.6 THU

9:45

Generation of over-8-dB squeezed
light by a broadband waveguide
optical parametric amplifier
toward fault-tolerant quantum
computers∙T. Kashiwazaki1 , T. Yamashima2 ,K. Enbutsu1 , T. Kazama1 , A. Inoue1 ,K. Fukui2 , M. Endo2,3 , T. Umeki1 ,and A. Furusawa2,3 ; 1 NTT Corporation, Kanagawa, Japan; 2 The University of Tokyo, Tokyo, Japan; 3 RIKEN,
Saitama, Japan
We achieved continuous-wave
8.3-dB quadrature squeezing usinga THz-order-broadband waveguide
optical parametric amplifier (OPA)
without loss-correction. This is
the first achievement of exceeding
the fault-tolerant threshold ofcontinuous-variable optical quantum computing by using waveguide
OPAs.

On-Chip Inverse Designed
Fabry-Pérot Resonators∙T. Bi1,2 , S. Zhang1 , A. Ghosh1,2 , O.
Lohse1 , I. Harder1 , K.Y. Yang3 , and
P. Del’Haye1,2 ; 1 Max Planck Institute for the Science of Light, 91058
Erlangen, Germany; 2 Departmentof Physics, Friedrich-AlexanderUniversität
Erlangen-Nürnberg,
91058 Erlangen, Germany; 3 John
A. Paulson School of Engineeringand Applied Sciences, Harvard
University, Cambridge, MA, USA
Fabrication supported by inversedesign unlocks a diverse range ofapplications by traversing throughthe full parameter space. One such
example is highly-reflective mirrors.
We use inverse-design to demonstrate on-chip silicon nitride FabryPérot microresonators.

Large-Area Sub-5nm Plasmonic
Nanogap Arrays: Advanced Fabrication, Characterization andApplications∙J. Gour1 , S. Beer1 , P. Paul1 , A.
Alberucci1 , A. Szeghalmi1,2 , U.
Peschel3 , S. Nolte1,2 , and U.D.
1
Zeitner1,2,4 ;Friedrich Schiller
University Jena, Institute of Applied
Physics, Jena, Germany; 2 Fraunhofer
Institute for Applied Optics andPrecision Engineering IOF, Jena,
Germany; 3 Friedrich Schiller University Jena, Institute of Solid State
Theory and Optics, Jena, Germany;
4
Munich University of Applied
Sciences, Department of Applied
Sciences and Mechatronics, Munich,Germany
Our advanced fabrication technology creates large-scale, plasmonic
nanogap arrays down to singlenanometer widths, enabling new
insights in nanoscale physics andopening new possibilities for photonic devices based upon arrays ofinteracting nanogaps.

Sub-40 fs diode-pumped SESAM
mode-locked Yb:Sc2SiO5 laser
L. Dong1 , Z.-L. Lin2 , P. Loiko3 , Y.
Liu1 , G. Zhang2 , H.-J. Zeng2 , W.-Z.
Xue2 , S. Liu4 , L. Zheng5 , X. Mateos6 ,H. Lin7 , V. Petrov8 , L. Wang8 ,and ∙W. Chen2,8 ; 1 Qingdao University of Technology, Qingdao, China;
2
Fujian Institute of Research on the
Structure of Matter, Fuzhou, China;
3
Université de Caen, Caen Cedex,
France; 4 Shandong University of
Science and Technology, Qingdao,
China; 5 Yunnan University, Kunming, China; 6 Universitat Rovira i
Virgili, Tarragona, Spain; 7 Shenzhen
University, Shenzhen, China; 8 Max
Born Institute for Nonlinear Optics
and Short Pulse Spectroscopy, Berlin,
Germany
In this work, we demonstrate sub40 fs soliton pulse generation froma diode-pumped SESAM modelocked Yb:Sc2SiO5 laser near 1070
nm.

Two frequency-modulated comb
regimes in quantum cascade laserrings∙A. Dikopoltsev, I. Heckelmann, P.
Michelletti, G. Scalari, M. Beck,and J. Faist; ETH Zurich, Zurich,
Switzerland
Gain mechanisms of quantum cascade lasers (QCL) enable frequencycomb generation without external
nonlinear cavities. We study unidirectional lasing of radio-frequency
modulated QCL rings and find two
distinct frequency-comb regimes.
We develop a near-resonance analytical solution.

Direct temporal measurement ofswitching-waves in a normal
dispersion Kerr resonator
M. Macnaughtan1,2 , M. Erkintalo1,2 ,S. Coen1,2 , ∙S. Murdoch1,2 , andY. Xu1,2 ; 1 Dodd-Walls Centre for
Photonic and Quantum Technology,
Dunedin, New Zealand; 2 Physics
Dept, University of Auckland, Auckland, New ZealandNonlinear switching waves underpin the formation of frequency
combs in normal dispersion Kerr
resonators. We present direct measurements of the temporal profile ofswitching waves and compare theseresults to theoretical phasematching
predictions.

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

EA-3: Photonic quantum
technology

CK-9: Micro optical combs

EH-3: Nonlinear and active
metastructures

CA-11: New laser designs

CB-9: Quantum cascadelasers and frequency combs

EF-4: Spatiotemporal effects
in optical systems

Chair: Christian Jirauschek, Technical University of Munich, Germany

Chair: German de Valcarcel, University of Valencia, Burjassot, Spain

CB-9.1 THU

10:30

EF-4.1 THU (Keynote) 10:30

Picosecond pulses from a gainswitched quantum cascade laser∙P. Täschler, L. Miller, F. Kapsalidis, M. Beck, and J. Faist; Institutefor Quantum Electronics, Zurich,
Switzerland
We demonstrate short pulses (~ 30
ps) with Watt level peak power froma quantum cascade laser. Lasing on asingle longitudinal mode is achieved
via injection seeding. We interpretthe results using rate equations.

Physics and Application ofComplex Lasers∙H. Cao; Yale University, New
Haven, USA
A complex laser supports many
spatio-temporal modes that interact
nonlinearly with the gain material.
We have controlled spatio-temporal
dynamics of many-mode lasers andapplied them to speckle-free imaging, holography and parallel ultrafast random number generation.

Chair:
Martin Frimmer,
Zurich, Switzerland
EA-3.1 THU

ETH

10:30

Integrated microcavity optomechanics with a suspended
photonic crystal mirror∙A. Ciers1 , S. Kini Manjeshwar1 , J.
Monsel1 , C. Peralle2 , S.M. Wang1 ,P. Tassin2 , and W. Wieczorek1 ;1
Department of Microtechnology
and Nanoscience, Chalmers University of Technology, Gothenburg,
Sweden; 2 Department of Physics,
Chalmers University of Technology,
Gothenburg, Sweden
We realize a free-space microcavity from an AlGaAs heterostructure,

Chair: Minhao Pu, Technical University of Denmark, DTU Fotonik, Lyngby, Denmark
CK-9.1 THU (Invited)

10:30

Optical Combs for High-Capacity
Transmission and Energy-Optimization of Long-Haul Fiber Cables∙L. Oxenløwe ; Technical Universityof Denmark, Kgs. Lyngby, Denmark
Optical frequency combs have potential to replace many lasers in
optical transmitters, and support
Pbit/s-scale capacities for long andshort links. Long-haul links can reduce the number of amplifiers byspatial data-distribution.

Chair: Andrea Bragas, Universidad
de Buenos Aires, Argentina
EH-3.1 THU

10:30

Mid-infrared power limiters andsaturable-absorber mirrors basedon χ (3) GaAsSb/InGaAs intersubband polaritonic metasurfaces.
∙J. Krakofsky1 , M. Cotrufo2 , S.A.
Mann2 , G. Böhm1 , A. Alú2 , and
M.A. Belkin2 ; 1 Walter-Schottky Insitute (TU Munich), Munich, Germany; 2 City University of New York,New York, USA
We demonstrate a nonlinear polaritonic intersubband metasurface
wich can be used to create saturable absorbers and optical power

Chair: Richard Mildren, Macquarie
University, Australia

CA-11.1 THU

10:30

Laser cooling of an Yb3+-doped
KY3F10 crystal by 42 K
∙S. Püschel, C. Kränkel, and H.
Tanaka;Leibniz-Institute fürKristallzüchtung (IKZ), Berlin,
Germany
We grew a high-quality Yb:KY3F10
crystal and demonstrate laser cooling by 42 K from room temperature
under 4.1 W excitation. The coolingefficiency and power-dependent
performance of the Yb:KY3F10 arecomparable with state-of-the-art
Yb:YLF.

148

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Room 14b ICM

Room Osterseen ICM®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)⋅ Thursday 29 June 2023
Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)observe coherent oscillations in thephotoexcited population.
CH-9.5 THU

9:45

JSI-5.5 THU

9:45

CF-10.6 THU

9:45

CG-3.6 THU

9:45

CJ-6.6 THU

9:45

EB-10.6 THU

9:45

Development and Characterization of an EUV/soft X-ray SinglePhoton Sensitive sCMOS Camera∙N. Abdurakhimov1,2,3 and C.
Friedrich1 ; 1 greateyes GmbH, Berlin,
Germany; 2 Max Born Institute for
Nonlinear Optics and Short Pulse
Spectroscopy, Berlin, Germany;
3
Freie Universität, Berlin, Germany
We are developing a EUV/soft Xray sensitive sCMOS-sensor based
detector suitable for high repetition
rate imaging and spectroscopy aswell as single photon detection experiments

Free Electron Laser for theinvestigation of ultrafast chiraldynamics∙M. Bonanomi1,2 , D. Faccialà2 ,M. Devetta2 , Y. Mairesse3 , O.
Plekan5 , K.C. Prince5 , M. Di
Fraia5,7 , V. Blanchet3 , L. Nahon6 , I.
Powis4 , C. Callegari5 , and C. Vozzi2 ;1Politecnico di Milano, Milano, Italy;2
Istituto di Fotonica e Nanotecnologie, Milano, Italy; 3 Universitéde Bordeaux-CNRS_CEA, CELIA,
Talence, France; 4 School of Chemistry, University of Nottingham,
Nottingham,
United Kingdom;
5
Elettra-Sincrotrone Trieste, Basovizza - Trieste, Italy; 6 Synchrotron
Soleil, Gif sur Yvette, France;
7
CNR-IOM, Basovizza - Trieste,
Italy
Circular polarized XUV light froman FEL offers the possibility toinvestigate the ultrafast dynamic
in chiral molecules combining
the enantio-specificity of TRPECD with the chemical and site
specificity of TR-XPS.

Nonlinear Pulse Compression of a
Yb-Doped Thin-Disk Amplifier at
156 mJ and 5 kHz Using a
Gas-Filled Multipass Cell
∙Y. Pfaff1,2 , G. Barbiero1 , M.
Rampp1 , H. Wang1 , S. Klingebiel1 ,C.Y. Teisset1 , R. Jung1 , A.H.
Woldegeorgis1 , J. Brons3 , A.R.
Maier4 , C.J. Saraceno2 , and T.
1
Metzger1 ;TRUMPF Scientific
Lasers GmbH + Co.
KG, Unterföhring, Germany; 2 Photonics
and Ultrafast Laser Science,
Ruhr-University Bochum, Bochum,
Germany; 3 TRUMPF Laser GmbH,
Schramberg, Germany; 4 Deutsches
Elektronen-Synchrotron
DESY,
Hamburg, Germany
We present spectral broadening of
156 mJ pulses from a Yb-doped
thin-disk amplifier at 5 kHz repetition rate using a helium-filled
Herriott-type multipass cell andshow their compressibility from 461
fs to 39 fs.

Vacuum laser acceleration ofelectrons injected from nanotips∙A. De Andres1 , S. Bhadoria2 ,J. Marmolejo2 ,A. Muschet1 ,P. Fischer1 , A. Gonoskov2 , D.
Hanstorp2 , M. Marklund2 , and L.
Veisz1 ; 1 Department of Physics,Umeå University, Umeå, Sweden;
2
Department of Physics, University
of Gothenburg, Göteborg, Sweden
We accelerated high-charge (nC)electron bunches to relativistic energies by placing a nanotip in thewaist of a laser. The resulting electrons and the acceleration mechanism were studied against different focusing configurations (f#1 andf#3).

Suppressing Stimulated Brillouin
Scattering with High Beam
Quality by Selective Multimode
Excitation in Optical Fibers
C.-W. Chen1 , K. Wisal2 , S. WarrenSmith3 , P. Ahmadi4 , A.D. Stone1 ,and ∙H. Cao1 ; 1 Department ofApplied Physics, Yale University,
New Haven, USA; 2 Department of
Physics, Yale University, New Haven,
USA; 3 Future Industries Institute,
University of South Australia, Mawson Lakes, Australia; 4 Coherent,
1280 Blue Hills Ave., Bloomfield,
USA
We experimentally demonstrateefficient suppression of stimulated
Brillouin scattering in multimodefibers while maintaining highoutput-beam quality by shaping the input seed wavefront.
SBS threshold is enhanced tothree times the threshold for
fundamental-mode-only excitation.

Optical Fractional Fourier
Transform - experimental
implementation∙M. Jastrzȩbski1,2 , B. Niewelt1,2 , S.
Kurzyna1,2 , J. Nowosielski1,2 , W.
Wasilewski1,2 , M. Mazelanik1,2 , and
M. Parniak1,3 ; 1 Centre for Quantum Optical Technologies, Centreof New Technologies, University of
Warsaw, Warsaw, Poland; 2 Facultyof Physics, University of Warsaw,
Warsaw, Poland; 3 Niels Bohr Institute, University of Copenhagen,Copenhagen, Denmark
We present the experimental implementation of optical Fractional
Fourier Transform in quantum
memory.
It’s a promising tool
for superresolution and quantum
communication. We perform theoperations on Hermite-Gaussianmodes which are the eigenfunctionsof FrFT.

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

CH-10: Fiber sensors I

CL-2: Flow cytometry andultrasoundCC-1: Nonlinear THz phenomena

CG-4: Few-cycle drivers andharmonic sourcesCE-5: Sensor materials andstructures

EB-11: Single photon sourcesand detectors

Chair:
Xiaoming Wei, South
China University of Technology,
Guangzhou, China

Chair: Karl Unterrainer, Technicaluniversity of Vienna, Vienna, Austria

Chair: Mathieu Gisselbrecht, Lund
University, Lund, Sweden

Chair: Luca Vincetti, University of
Modena, Italy

Chair: Alexander Sergienko, Boston
University, USA

CL-2.1 THU

CC-1.1 THU (Invited)CG-4.1 THU

CE-5.1 THU

EB-11.1 THU

Chair: Laurent Bigot, CNRS, University of Lille, France

CH-10.1 THU

10:30

Computational fluorescenceimaging with multi-core fiber
bundles – Towards high-speed
imaging through bare opticalfibers.
∙S. Sivankutty1 , S. Guérit2 , O.
Leblanc2 , M. Hofer3 , G. Bouwmans1 ,E. Andresen1 , L. Jacques2 , and H.
Rigneault3 ; 1 Univ. Lille, CNRS,UMR 8523 - PhLAM - Physiquedes Lasers Atomes et Molécules,
Lille, France; 2 ICTEAM Institute,
UC Louvain, Louvain-la-Neuve,
Belgium; 3 Aix-Marseille University,

10:30

High-speed field-resolved infrared fingerprinting of particles inflow∙D. Gerz1,2,3 , M. Huber2,3 , H.
Mirkes2 ,F. Lindinger2,3 ,Y.
Münzenmaier2 ,A.
Weigel3,4 ,M. Kielpinski1 , T. Henkel1 , M.
Zigman2,3,4 , F. Krausz2,3,4 , J.
Popp1,5 , and I. Pupeza1,2,3 ; 1 Leibniz
Institute of Photonic Technology,
Jena, Germany; 2 Ludwig Maximilians University Munich, Garching,
Germany; 3 Max Planck Instituteof Quantum Optics, Garching,

10:30

THz Bandwidth Activation ofAnharmonic Coupling in CdWO4
M. Nielson, B. Knighton, L. Davis, A.
Alejandro, C. Rader, and ∙J. Johnson;
Brigham Young University, Provo,
USA
2D THz spectroscopy enables us
to isolate anharmonic coupling between phonon modes in CdWO4.
We show that the THz bandwidth
activates this coupling, when wewould not otherwise expect it to beefficient.

10:30

Multi-TW laser pulses in the
single-cycle regime by single thinplate compression
S. Tóth1 , ∙I. Seres1 , L. Lehotai1 , J.
Csontos1 , A. Farkas1 , Á. Mohácsi1 ,Á. Börzsönyi1 , K. Osvay2 , and
R.S. Nagymihály1 ; 1 ELI ALPS
Research
Institute,
Szatymaz,
Hungary; 2 National Laser InitiatedTransmutation Laboratory, Szeged,
Hungary
Single thin plate post-compressionof the SYLOS lasers of ELI ALPS
was experimentally demonstrated,

149

10:30

High numerical aperture opticalbundle for biological imaging∙R. Kasztelanic1,2 , D. Pysz2 , R.
Stepien2 , R. Czajkowski3 , and R.
Buczynski1,2 ; 1 Faculty of Physics,
Warsaw University, Warsaw, Poland;
2
Lukasiewicz Research Network, Institute of Microelectronics and Photonics, Warsaw, Poland; 3 Nencki Institute of Experimental Biology PAS,
Warsaw, Poland
Imaging bundles with a high numerical aperture have been fabricated, tested, and used for two-

10:30

Optically-Coherent Color Center
Ensembles Coupled to HighFinesse Silicon Carbide
Microresonators∙D. Lukin1 , D. Catanzaro1 , M.
Guidry1 , M. Ghezellou2 , J. Yang1 , H.
Abe3 , T. Ohshima3 , J. Ul-Hassan2 ,and J. Vuckovic1 ; 1 Stanford University, Stanford, USA; 2 Linkoping
University, Linkoping, Sweden;
3
National Institutes for Quantum
Science and Technology, Takasaki,
Japan
Small ensembles of silicon vacancy

CLEO

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/Europe-EQEC 2023

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formed by a DBR and a suspended
photonic crystal. We demonstrate
tunability of the cavity resonanceand observe optomechanical effects
that deviate from canonical optomechanics.

limiters in the mid-infrared regime
with record high contrast ratio anda χ (3) non-linearity of 10−12 m2 /V 2 .

EA-3.2 THU

EH-3.2 THU

10:45

Single-pass femtosecond parametric process towards continuous
variables quantum networks
T. Kouadou, ∙F. Sansavini, M. Ansquer, J. Henaff, N. Treps, and V.
Parigi; Laboratoire Kastler Brossel,
Sorbonne Université, CNRS, ENSPSL Research University, Collège deFrance , 75005 Paris, France
We demonstrate the generation of
21 squeezed spectral modes at 156
MHz, combining frequency- andtime- multiplexing in multimodesqueezing. This paves the way tothe implementation of scalable andfully reconfigurable multipartite entangled states.

EA-3.3 THU

11:00

A high-fidelity reconfigurable
photonic processor for NISQ
computing∙A. Cavaillès1 , P. Boucher1,2 , S.
Gigan1,3 , and K. Müller1 ; 1 LightOn,
3-5 Impasse Reille, Paris, France;
2
Quantonation, 58 rue d’Hauteville
75010, Paris, France; 3 Laboratoire
Kastler Brossel, ENS–Université PSL,
CNRS, Sorbonne Université, College
de France, 24 Rue Lhomond, F75005, Paris, France

CK-9.2 THU

11:00

A Photonic Integrated High-power Soliton Microcomb Generator∙X. Ji, Y. Liu, Z. Qiu, A. Voloshin, andT.J. Kippenberg; Institute of Physics,
Swiss Federal Institute of Technology
Lausanne , Lausanne, Switzerland
We demonstrate a compact soliton
microcomb light source, with an
output power of 7.9 mW, at a compact device footprint of 12.5 mm2 .

⋅ Thursday 29 June 2023

10:45

CA-11.2 THU

Room 13b ICM

10:45

CB-9.2 THU

Room 14a ICM

10:45

Novel High-Q Metasurface Design
for Second-Harmonic Generation∙G.Q. Moretti1 , B. Tilmann2 , A.
Tittil2 , E. Cortés2 , S.A. Maier2,3,4 ,A.V. Bragas1 , and G. Grinblat1 ;1
Departamento de Física, FCEN,IFIBA-CONICET,
Universidad
de Buenos Aires, Buenos Aires,
2
Argentina;
Chair in Hybrid
Nanosystems,
Nanoinstitute
Munich, Faculty of Physics, LudwigMaximilians-Universität, München,
Germany; 3 School of Physics andAstronomy, Monash University,
Melbourne, Australia; 4 Departmentof Physics, Imperial College London,
London, United Kingdom
We show numerically recordbreaking SHG efficiencies for anovel GaP metasurface design,
sustaining a very high-Q QBIC
resonance.
A coupler element
is added instead of traditional
approaches for the excitation of themode.

Efficient Tm:Lu2O3 laser at ~2250
nm∙K. Eremeev1 , P. Loiko1 , S.
Balabanov2 , L. Guillemot1 , P.
Camy1 , C. Kränkel3 , and A. Braud1 ;1
Centre de Recherche sur les Ions,
les Matériaux et la Photonique(CIMAP), UMR 6252 CEA-CNRSENSICAEN, Université de Caen
Normandie, Caen, France; 2 G. G.
Devyatykh Institute of Chemistryof High-Purity Substances of RAS,
Nizhny Novgorod, Russia; 3 LeibnizInstitut für Kristallzüchtung (IKZ),
Berlin, Germany
Spectroscopic properties of Tm3+doped sesquioxides A2O3 (A = Y,
Lu, Sc) relevant for laser operation on the 3H4→3H5 transition
were studied. A continuous-wave
Tm:Lu2O3 laser generated 654 mW
at 2238-2309 nm with 68.9% slope
efficiency.

Strongly modulated QCLs as
broadband Mid-IR sources∙A. Cargioli1 , M. Bertrand1 , S.
Hakobyan2 , R. Maulini2 , S. Blaser2 ,T. Gresch2 , A. Muller2 , and J. Faist1 ;1
Institute for Quantum Electronics,
ETH Zurich, Zurich, Switzerland;2
Alpes Lasers, St Blaise, Switzerland
Compact and stable broadband
Mid-IR sources are fundamental
for spectroscopy applications. Here,
we prove that we can stabilise andbroaden the emission of a QCL up
to 250cm^-1 by strongly injecting a
low-frequency RF signal.

EH-3.3 THU

CA-11.3 THU

CB-9.3 THU

11:00

Multiresonant Metasurfaces for
Broadband Quadratic Spectral
Phase Manipulations∙O. Tsilipakos1 and T. Koschny2 ;1National Hellenic Research Foundation, Athens, Greece; 2 Ames National
Laboratory, Ames, Iowa, USA
We propose multiresonant metasurfaces exhibiting a purely quadratic
spectral phase to be utilized for temporal pulse shaping of broadband
signals. This overcomes the funda-

11:00

LED pumped alexandrite
amplifier.
∙E. Thellier1 , H. Taleb1 , C. Le
Blanc1,2 , P. Pichon1 , F. Druon1 ,P. Georges1 , and F. Balembois1 ;1
Université Paris-Saclay,
Institut d’Optique Graduate School,
CNRS, Laboratoire Charles Fabry,
Palaiseau, France; 2 Laboratoire pourl’Utilisation des Lasers Intenses,
CNRS, Ecole polytechnique, CEA,
Palaiseau, France

150

11:00

Low dissipation quantum cascadesurface emitting lasers∙D. Stark1 , F. Kapsalidis1 , S.
Markmann1 , M. Bertrand1 , Z.
Wang1 , R. Wang1 , B. Meng1 , E.
Gini2 , M. Beck1 , and J. Faist1 ;1
Institute for Quantum Electronics,
ETH Zürich, Zürich, Switzerland;
2
FIRST Center for Micro- andNanoscience, ETH Zürich, Zürich,
Switzerland
We report on the design, fabri-CLEO

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CNRS, Institut Fresnel, Marseille,
FranceWe present a high-speed fluorescence imaging technique throughlensless endoscopes using a featuring a bending-resilient multicore
fiber and computational imaging
with a single pixel detector

CH-10.2 THU

10:45

Room 1 Hall B1 (B11)⋅ Thursday 29 June 2023
Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)

Germany; 4 Center for MolecularFingerprinting, Budapest, Hungary;
5Institute of Physical Chemistry
and Abbe Center of Photonics,
Friedrich-Schiller University, Jena,
Germany
We acquire infrared spectral fingerprints of a stream of 9-μm-sized particles flowing at ~20 μm/ms througha 30-μm-thick water channel, using
high-dynamic-range field-resolved
spectroscopy (FRS). This paves theway to high-throughput, label-free
FRS flow cytometry.

yielding sub-2-cycle pulses withmore than 3 TW peak power atthe output. Pulse characterizationshows high spatio-temporal quality
after compression.

photon imaging of the fluorescencesignal of latex beads, ex vivo hippocampal neurons, and in vivo cortical neurons.

color centers are integrated intohigh finesse whispering gallery
mode resonators, fabricated using
the Silicon Carbide-on-Insulator
quantum
photonic
platform,
towards realization of multi-emitter
spin-spin coupling in Silicon
Carbide.

CL-2.2 THU

CG-4.2 THU

CE-5.2 THU

EB-11.2 THU

10:45

Time-Stretched Imaging Flow
Cytometry and Photonic
Neuromorphic Processing for
Particle Classification
I. Tsilikas1 , A. Tsirigotis2 , S.
Deligiannidis3 ,G. Tsigaridas1 ,A. Bogris3 , and ∙C. Mesaritakis2 ;1
National Technical University ofAthens, Dept.
Physics, Athens,
Greece; 2 University of the Aegean,
Dept. Information and Communication Systems Engineering, Samos,
Greece; 3 University of West Attica,
Dept. Informatics and Computer
Engineering, Egaleo, Greece
We present experimental results
concerning particle classification
using a time-stretched imagingcytometer followed by a photonic
neuromorphic accelerator.
The
combined system offers an accuracy
increase of 5% alongside a compression of parameters by a factorof 2.5.

CH-10.3 THU

CL-2.3 THU

11:00/Europe-EQEC 2023

Room 6 Hall B3 (B32)

Coherent Beam Shaping with
Multicore Fiber Photonic
Lanterns∙A. Milne1 , H.E. Parker1 , T.A.
Wright2 , A. Benoît1 , K. Harrington2 ,J. Leach1 , D.B. Phillips3 , J.M. Stone2 ,T.A. Birks2 , and R.R. Thomson1 ;1Institute of Photonics and Quantum
Sciences, Heriot-Watt University,
Edinburgh, EH14 4AS, United
Kingdom; 2 Department of Physics,
University of Bath, Bath, BA2 7AY,
United Kingdom; 3 School of Physics
and Astronomy, University of Exeter,
Exeter, EX4 4QL, United Kingdom
We demonstrate that photonic
lanterns made from polarisation
maintaining multicore fibre enable
controlled coherent beam shaping
at their multimode end without
the requirement for access to themultimode end, opening up newopportunities in microendoscopy.

Improved Visible-guiding Antiresonant Hollow-Core Fiber for
Gas-phase Raman Spectroscopy∙T. Kelly1 , S. Rikimi1 , I. Davidson1 ,W. Brooks2 , M. Foster2 , F. Poletti1 ,S.A. Mousavi1 , P. Horak1 , and N.
Wheeler1 ; 1 University of Southampton, Southampton, United Kingdom;
2
IS-Instruments Ltd, Tonbridge,
United Kingdom
Here we report on the fabrication, characterization and testing

®

11:00

Ultrasound Modulated Optical
Tomography with Persistent
Spectral Hole Burning Filter for
In Vivo Deep Tissue Imaging∙Q.M. Thai1,2 , G. Kalot3 , C. Venet1 ,J. Seguin3 , M. Bocoum1 , N. Mignet3 ,J.-L. Gennisson4 , F. Ramaz1 , and1
A. Louchet-Chauvet1 ;InstitutLangevin, ESPCI Paris, Université
PSL, CNRS, Paris, France; 2 Clusterof Excellence Physics of Life (PoL),TU Dresden, Germany; 3 UniversitéCC-1.2 THU

11:00

Ultrafast and Low-Threshold THz
Mode Switching of Two-Dimensional Nonlinear Metamaterials∙B.J. Kang1,3 , D. Rohrbach1 , F.
Brunner1 , S. Bagiante1,2 , H. Sigg2 ,and T. Feurer1 ; 1 University of Bern,
Bern, Switzerland; 2 Paul Scherrer
Institute, Villigen, Switzerland;
3
Korea Research Institute of Chemical Technology, Daejeon, SouthKorea
We report ultrafast THz-field

10:45

10:45

10:45

High energy, monocycle,
CEP-stable IR pulse generation
based on advanced DC-OPA∙L. Xu1,2 and E.J. Takahashi1,3 ;1Ultrafast Coherent Soft X-ray
Photonics Research Team, RAP,
RIKEN, Wako, Saitama, Japan;
2
Attosecond Science Research Team,
RAP, RIKEN, Wako, Saitama, Japan;
3
Extreme Laser Science Laboratory,
CPR, RIKEN, Wako, Saitama, Japan
Based on the advanced DC-OPA
scheme and two kinds of nonlinear crystals, a 53 mJ, 8.58 fs (nearlymonocycle at 2.44 um), CEP-stable
MIR laser source was developed.

Lithium-Niobate-On-Insulatorbased electric field sensors∙N. Courjal1 , A. Hoblos1 , M.
Suarez1 , R. Salut1 , M. Amidullah2 ,V. Kemlin3 , J. Schiellein2 , A. Boutin4 ,A. Bouvier4 , V. Calero1 , B. Robert1 ,L. Grosjean1 , F. Baida1 , and M.-P.
Bernal1 ; 1 FEMTO-ST Institute,
25000 Besançon, France; 2 THALESLAS, 78990 Elancourt, France;
3
THALES Research & Technology,
91767 Palaiseau, France; 4 Exail Integrated Systems, 75003 Paris,
FranceWe report on the nanostructuring
and characterization of an LNOIbased electro-optical photonic crystal assembled at the tip of a fiber
for non-intrusive electric field sensing. These developments pave theway for ultra-compact sensors and3D photonic hybrid platforms.

Experimental Verification of
Photon Pair Indistinguishability
Enhancement via Heralded
Post-Selection∙R. Checchinato1 , J. Lee1 , F. Redivo
Cardoso2 , J.-H. Littmann1 , J.R.
Gonzales-Ureta1 , S. Höfling3 , C.
Schneider4 , C.J. Villas-Boas2 , and A.
Predojević1 ; 1 Department of Physics,
Stockholm University,
Sweden;2
Departamento de Física, Universidade Federal de São Carlos, Brazil;
3
Technische Physik, Physikalisches
Institut and Würzburg-Dresden
Cluster of Excellence ct.qmat,
Universität Würzburg, Germany;
4
Institute of Physics, University of
Oldenburg, Germany
We probe the indistinguishability ofphoton pairs generated in a cascadedecay using Hong-Ou-Mandel interference. We present a methodof enhancing the indistinguishability through heralded detection andpost-selection.

CG-4.3 THU

CE-5.3 THU

EB-11.3 THU

11:00

Waveform Synthesizer-based
Tunable Attosecond Beamline∙G.M. Rossi1,2 , R.E. Mainz1,2 , F.
Scheiba1,2 , M.A. Silva-Toledo1,2 , M.
Kubullek1,2 , and F.X. Kärtner1,2 ;1Center for Free-Electron Laser
Science,
Deutsches ElektronenSynchrotron
DESY,
Hamburg,2
Germany; Physics Department and
The Hamburg Centre for Ultrafast
Imaging, University of Hamburg,
Hamburg, Germany

151

11:00

Fabrication of Externally Microstructured Flat Optical Fibre for
In-process Monitoring of Laminated Composite Structures∙C. Holmes1 , S. Zahertar1 , B.
Moog1 , M. Godfrey1 , T. Lee1 , A.
Annunziato2 , F. Anelli2 , B. Shi1 ,M. Beresna1 , M. Whitaker1 , F.
Prudenzano2 , R. Day3 , and J.
Barton4 ; 1 University of Southampton, Bristol, United Kingdom;
2
Politecnico di Bari, Bari, Italy;

11:00

Singly resonant frequency conversion for manipulation of a frequency-multiplexed single photon∙R. Ikuta1,2 , M. Yokota1 , T.
Kobayashi1,2 , N. Imoto2 , and T.
Yamamoto1,2 ; 1 GSES, Osaka University, Toyonaka, Japan; 2 QIQB,
Osaka University, Toyonaka, Japan
Frequency-multiplexed entanglement distribution is important for
high-speed and multi-user quantum
network. In the situation, quantumCLEO

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We present a low-footprint reconfigurable linear optical network for
NISQ through complex mixing andwavefront shaping. We implementwith high fidelity circuits ranging up
to 8-inputs/38-outputs and present
avenues to minimize losses and increase scalability.

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mental limitations of conventional,
non-resonant approaches (bulky)
and modern, singly-resonant metasurfaces (narrowband).

We demonstrate a compact 28
passesalexandrite
amplifier,pumped by a Ce:YAG luminescentconcentrator at 2.5 kW peak power
leading to a significant gain of 14.9.

cation and characterization of low
dissipation quantum cascade surface emitting lasers (QCSEL) emitting at wavelengths of 4.5 μm or
8 μm. The results are an important step towards low-cost batterydriven QCLs.

EF-4.2 THU

11:15

Quantum-enhanced stimulated
Raman scattering spectroscopy indual-polarization scheme∙Z. Xu1 , K. Oguchi1 , S. Nitanai2 , Y.
Taguchi1 , Y. Sano1 , and Y. Ozeki1 ;1
Department of Electrical Engineering and Information Systems, The
University of Tokyo, Tokyo, Japan;
2
Department of Electrical and Electronic Engineering, The University ofTokyo, Tokyo, Japan
In this report, we introduce anovel strategy for high-power
quantum-enhanced
stimulated
Raman scattering spectroscopy
in a dual-polarization scheme. A
noise reduction level of 0.5 dB
was achieved in both polarization
modes.

3D Integration of Microcombs∙M. Girardi, O.B. Helgason, A.
Caut, M. Karlsson, A. Larsson, andV. Torres-Company; Department ofMicrotechnology and Nanoscience,
Chalmers University of Technology,
Göteborg, Sweden
We demonstrate the integration of
a power efficient frequency combwith a wavelength demultiplexer,
by three-dimensional integration of
two Si3N4 core geometries optimized for nonlinear and linear operations.

Heavily doped semiconductors for
integrated nonlinear plasmonics∙C. Ciraci1 , F. De Luca1,2 , and M.
Ortolani3 ; 1 Istituto Italiano di Tecnologia, Arnesano, Italy; 2 Universitàdel Salento, Lecce, Italy; 3 Sapienza
University of Rome, Roma, Italy
In this talk we numerically investigate heavily doped semiconductors as a platform for integrated nonlinear plasmonics at midinfrared frequencies. We study freeelectron nonlinearities and use surface charge density modulation tocontrol and enhance the nonlinear
response.

Spectrally combined diodespumped femtosecond Ti:sapphirelasers and its application to twophoton & coherent anti-Stokes
Raman scattering microscopy∙D.H. Song1,2 , C. Huh1 , and H.S. Seo1,2 ; 1 Electronics and Telecommunications Research Inst., Daejeon,South Korea; 2 BlueTileLab, Daejeon,South Korea
We present a simpler and costeffective technique to increase
mode-locked (ML) power andpulse energy by exploiting spectrally combined pump diodes.
These compact femtosecond Ti:S
lasers were successfully applied tohome-built video-rate two-photon& coherent anti-Stokes Raman
scattering microscopes.

Private free-space transmission
based on chaos synchronisation in
the 8-14 μm atmospheric transparency window∙P. Didier1,2 , S. Zaminga1 , O.
Spitz1,4 , E. Awwad1 , G. Maison2 , M.
Carras2 , and F. Grillot1,3 ; 1 Telecom
Paris, Institut Polytechnique deParis, Paris, France; 2 mirSense,
Paris, France; 3 Center for HighTechnology Materials, University of
New-Mexico, Albuquerque, USA;
4
College of Optics and Photonics,
University of Central Florida,
Orlando, USA
We demonstrate a 5 Mbit/s chaosbased free-space private transmission system at 9.3 μm, in one of thetransparency windows of the atmosphere. This system is relevant for
FSOC applications where security isof paramount importance.

Hexagonal patches and modes indegenerated nonlinear cavities:
the role of aberrations
S.V. Gurevich1 , F. Maucher2 , N.
Vigne3 , A. Garnache3 , I. Sagnes4 ,A. Bartolo5 , M. Marconi5 , M.
Guidici5 ,and ∙J. Javaloyes2 ;1Institute for Theoretical Physics,
University of Münster, Münster,Germany; 2 Departament de Física
& IAC-3, Universitat de les Illes
Balears, Palma, Spain; 3 Institutd’Electronique et des Systèmes,CNRS UMR5214,
Montpellier,France; 4 Centre de Nanosciences etde Nanotechnologies, CNRS UMR
9001, Université Paris-Saclay, Paris,
France; 5 Université Côte d’Azur,
CNRS, Institut de Physique de Nice,
Valbonne, France
We consider the transverse nonlinear dynamics of a nonlinear opticalsystem in presence of spherical aberrations close to the degenerate selfimaging condition. Off axis emission and Turing patterns are observed in good agreement with theexperiment.

EA-3.5 THU

CK-9.4 THU

EH-3.5 THU

CA-11.5 THU

CB-9.5 THU

EF-4.3 THU

EA-3.4 THU

11:15

11:30

A simulation framework for feedforward in quantum photonic
systems∙J.C. Adcock1 , D.A. Quintero
Dominguez1 , Q. Palmer1,2 , S.G.
Currie1,2 , W.J. Munro3 , and J.W.
Silverstone1 ; 1 Big Photon Lab,
University of Bristol, Bristol, United
Kingdom; 2 Quantum Engineering
Center for Doctoral Training,
University of Bristol, Bristol, United
Kingdom; 3 NTT Basic ResearchLaboratories & Research Center
for Theoretical Quantum Physics,

CK-9.3 THU

11:15

11:30

Self-Injection-Locked Microcombs via Synthetic Reflection∙A. Ulanov1 , T. Wildi1 , N. Pavlov2 ,J. Jost2 , M. Karpov2 , and T.
Herr1,3 ; 1 Deutsches ElektronenSynchrotron
DESY,
Hamburg,
Germany; 2 Enlightra Sarl, Renens,
3
Switzerland;
Physics Department, Universität Hamburg UHH,
Hamburg, Germany
Self-injection locking to a photonic
crystal ring-microresonator withsynthetic reflection is demonstrated for the first time.
The

EH-3.4 THU

11:15

11:30

Strong nonlinear efficiency enhancement in the visible and UV
ranges from plasmonic gold
nanogratings∙S. Mukhopadhyay1 , L. RodriguezSuné1 ,C. Cojocaru1 ,M.A.
Vincenti2 , K. Hallman3 , G. Leo4 ,M. Belchovski2 , D. de Ceglia2 , M.
Scalora5 , and J. Trull1 ; 1 Departmentof Physics, Universitat Politècnica
de Catalunya, Terrassa (Barcelona),
Spain; 2 Department of Information
Engineering – University of Brescia,
Brescia, Italy; 3 PeopleTec, Inc. ,CA-11.4 THU

11:15

11:30

Progress in Blue Diode-Pumped
Titanium:Sapphire Regenerative
Amplifier at Room Temperature∙D. Hug1 , A. Dax2 , A. Trisorio2 ,R. Carreto3 , T. Südmeyer4 , and B.
Resan1 ; 1 Institute of Product andProduction Engineering, Universityof Applied Sciences and Arts Northwestern Switzerland, 5210 Windisch,
Switzerland; 2 Laboratory for Nonlinear Optics, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland;
3
TLD Photonics AG, 5430 Wettingen, Switzerland; 4 Time and Fre-

152

CB-9.4 THU

11:15

11:30

High-Power Quantum Cascade
Lasers for 8 μm spectral range
E. Cherotchenko1 , V. Dudelev1 ,D. Mikhailov1 , G. Savchenko1 ,D. Chistyakov1 , S. Losev1 , A.
Babichev1 ,A.
Gladyshev2,3 ,I. Novikov2,3 ,A. Lutetskiy1 ,D. Veselov1 ,S. Slipchenko1 ,D. Denisov2 , A. Andreev4 , I.
Yarotskaya4 , K. Podgaetskiy4 , M.
Ladugin4 , A. Marmalyuk4 , N.
Pikhtin1 , L. Karachinsky2,3 , V.
Kuchinskii1 , A. Egorov5 , and ∙G.
Sokolovskii1 ; 1 Ioffe Institute, Saint-

11:30

Spatially localized structures in aself-imaging semiconductor laser
cavity: diffraction and complex
non-linearity management.
∙N. Vigne1 , A. Bartolo1,2 , M.
Marconi2 , G. Beaudoin5 , K.
Pantzas5 ,J. Javaloyes3 ,S.V.
Gurevich4 , I. Sagnes5 , M. Giudici2 ,1and A. Garnache1 ;Institutd’Electronique et des Systèmes,Montpellier, France; 2 Institut dePhysique de Nice, Nice, France;
3
Departament de Física , Universitat de les Illes Balears, Palma

CLEO

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of a low-loss, large core visible
guiding 10-element single-cladding
ring anti-resonant hollow core fiber
for spontaneous gas-phase Raman
spectroscopy measurements.

de Paris Cité, INSERM, CNRS,UTCBS, Faculté de Pharmacie, Paris, France; 4 Laboratoired’imagerie
biomédicale
multimodale, Université Paris-Saclay,
CEA, CNRS, INSERM, Orsay,
FranceWe report the first in vivo ultrasound modulated optical tomography (UOT) images on mice, using
extremely selective persistent spectral hole burning filter. It demonstrates the potential of UOT for
deep-tissue imaging for medical applications.

induced mode switching of
two-dimensional nonlinear metamaterials
onsemiconductor
substrates with different band gaps.
We establish the dominant carrier
generation mechanism and present
detailed system dynamics.

The development of an attosecond transient absorption beamline
featuring tailored sub-cycle pumpwaveforms with spectrum spanning700-2200 nm and tunable isolated
attosecond probe pulses with photon energies in the 30-400 eV range
is presented.

3CH-10.4 THU

CL-2.4 THU

CC-1.3 THU

CG-4.4 THU

11:15

11:15

11:15

11:15

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)

Wrexham Glyndwr University,
Wrexham,UnitedKingdom;
4
University of Bristol, Bristol, United
Kingdom
Using a stack-and-draw approachand physical micromachining externally microstructured flat optical fibre is fabricated and used for new
monitoring capability in high-value
composite materials, including carbon and glass fibre reinforced polymer.

frequency conversion applicableto frequency-multiplexed photons
is required.
For this purpose,
we developed optical frequency
tweezers.

CE-5.4 THU

EB-11.4 THU

11:15

11:15

Hollow-Core-Fibre-Delivered
Attenuated Total Internal Reflection Heterodyne Spectroscopy∙P. Castro-Marin1 , K. Johnson2 ,C. Farrel2 , I.A. Davidson3 , G.T.
Jaison3 , N.V. Wheeler3 , F. Poletti3 ,D.J. Richardson3 , and D.T. Reid1 ;1
Heriot Watt University, Edinburgh,2
United Kingdom;
Chromacity
LTD, Edinburgh, United Kingdom; 3 University of Southampton,
Southampton, United Kingdom
We report the first example of attenuated total internal reflection
Fourier-transform infrared heterodyne spectroscopy, delivered by ahollow-core fibre. Using broadband
OPO illumination from 2600–3400
cm-1, we present an example measurement using LDPE plastic.

Cavitation Bubbles Generated In
Water By A 2.9μm Laser For
Sacrificial Layer-Free Bioprinting
Applications
S. Mohajan1 , J.-C. Delagnes1 , B.
Allisy1 , A. Iazzolino2 , B. Viellerobe2 ,and ∙S. Petit1 ; 1 CELIA Centre Lasers
Intenses et Applications UMR 5107
Université Bordeaux-CNRS-CEA,
Talence, France; 2 POIETIS, Bioparc
Bordeaux Métropole, 27 alléeCharles Darwin, Pessac, France
We investigated, experimentally andtheoretically, the bubble cavitation
ruling the microjet generation forbioprinting applications during 2.9
μm laser–water interaction. Novel
LAB system utilizing vibrational absorption of water in the middleinfrared has been investigated.

Terahertz driven electron
emission from designed metal
structures and structured
graphene∙T.O. Buchmann1 , M. Sebek1 ,A. Shivayogimath2 , P. Bøggild2 ,S. Lange1 , and P.U. Jepsen1 ;1
Department of Electrical andPhotonics Engineering, Kongens
Lyngby, Denmark; 2 Department of
Physics, Kongens Lyngby, Denmark
We demonstrate cold field electron
emission from graphene and metallic surfaces driven by the electricfield of lightwaves at terahertz frequencies. Electron energy, emission
threshold, and field dependency for
different structures are investigated.

High Harmonic Generation in
Neon Inside a Thin-Disk Laser
Oscillator: Towards a CoherentSingle-Stage 100-eV Source∙J. Drs1 , J. Fischer1 , M. Müller1 ,N. Modsching1 , F. Trawi1 , T.
Ullsperger2 , V.J. Wittwer1 , and T.
Südmeyer1 ; 1 Laboratoire TempsFréquence (LTF), Institut dePhysique, Université de Neuchâtel,Neuchâtel, Switzerland; 2 Institute ofApplied Physics, (Friedrich Schiller
University Jena), Jena, Germany
We show an ultrafast TDL oscillator capable of driving HHG in neon
directly inside its cavity. The result paves the way toward a compact
single-stage 100-eV coherent XUVsource.

Optical Sensing of Various Environmental Parameters Using
Molecular Switches
A. Günther1,2,4 , ∙Y. Deja1 , P. Kotra1 ,M. Kilic3 , K. Tran3 , F. Renz3,4 ,W. Kowalsky2,4 , and B. Roth1,4 ;1Hannover Centre for Optical
Technologies, Hannover, Germany;
2
Institute for High Frequency Technology, Braunschweig, Germany;3
Institute of Inorganic Chemistry,
Hannover, Germany; 4 Cluster of
Excellence - PhoenixD, Hannover,Germany
We use Fe(II)-triazole complexes as
optical switches and show their potential to detect changings in temperature, humidity or electric andmagnetic fields, respectively. First
results by embedding particles into
optical waveguides will also be presented.

Efficient converted single-photon
source at telecom band forquantum communication∙M. Cohen1 , R. Dalidet1 , M.
Billard2 , F. Pastier2 , V. Giesz2 , A.
Martin1 , S. Tanzilli1 , P. Senellart3 ,N. Somaschi2 , and L. Labonté1 ;1Universite Côte d’Azur, CNRS,
Institut de Physique de Nice (INPHYNI), Nice, France; 2 Quandela
SAS, Palaiseau, France; 3 Universite
Paris-Saclay, CNRS, Centre deNanosciences et de Nanotechnologies(C2N), Palaiseau, France
We achieve a frequency conversion
interface to convert single photons
emitted by a single photon source
toward telecommunication C-band.
We demonstrate near 50 % of endto-end efficiency and single photon
properties conservation.

CH-10.5 THU

CL-2.5 THU

CC-1.4 THU

CG-4.5 THU

CE-5.5 THU

EB-11.5 THU

11:30

Optimized microstructure designof hollow-core photonic crystal
fibres for ultra-sensitive optofluidic sensing∙C. Helfrich and F. Tani; Max Planck
Institute for the Science of Light, Erlangen, Germany
We study the design of single-ringhollow-core fibres for optofluidic
applications. We identify a routeto maximise the polarisation purityof the guided light and derive ananalytical expression for the loss ofhigher-order modes.

11:30

Hot-wire fibre optic flowmeterbased on single mode-multimodesingle mode structure as a sensing
respiratory device
M. Cavagnetto, ∙M. Olivero, A. Vallan, and G. Perrone; Politecnico di
Torino, dept. of Electronics andTelecommunications, Torino, Italy
A novel fibre optic flowmeter ispresented, which relies on a single mode-multimode-single mode
structure optically heated by a pumplaser, acting as a hot-wire sensor forthe monitoring of breath.

11:30

Optical Rectification and Second
Harmonic Generation of Intense
Terahertz Pulses∙D.J.H. Ludlow, C. Rader, N.K.
Green, and J.A. Johnson; Brigham
Young University, PROVO, USA
Nonlinear optical processes with(terahertz) THz frequency lighthave rarely been measured andcharacterized.
Using 2D THz
spectroscopy, we clearly observeTHz-optical rectification and THzsecond harmonic generation in avariety of materials.

11:30

Compact, intense extreme-ultraviolet sources for attosecond science and absorption spectroscopy∙B. Major1,2 , K. Kovács3 , E.
Svirplys4 , M. Anus4 , O. Ghafur4 ,K. Varjú1,2 , M.J.J. Vrakking4 , V.
Tosa3 , and B. Schütte4 ; 1 ELI ALPS,ELI-HU Non-profit Ltd.,, Szeged,
Hungary; 2 Department of Optics
and Quantum Electronics, University of Szeged, Szeged, Hungary;3
National Institute for Research andDevelopment of Isotopic and Molecular Technologies, Cluj-Napoca,

153

11:30

Fully Printed GaTe Based Photodetector on PET Substrate∙C. Odaci1,2 , M.S. Khan2 , D. Corzo2 ,M. Jose2 , A. Roshanghias2 , and U.
Aydemir1 ; 1 Bursa Uludag University,
Bursa, Turkey; 2 Silicon Austria Labs
GmbH, Villach, Austria
We report on a methodology forcost-effective fabrication of photodetector on flexible substrates.
The fabrication is done using
printing of solution processed IIIVI monochalcogenide materials
on PET sheets. The sensor is char-

11:30

Autler-Townes effect and composite pulses based methods for
single-shot measurements ofphonon number states∙N. Kuk1 , M. Mallweger1 , M.H.
Oliveira1,2 , R. Thomm1 , H. Parke1 ,G. Higgins1,3 , R. Bachelard2,4 ,C.J. Villas-Boas2 , B.T. Torosov5 ,N.V. Vitanov6 , and M. Hennrich1 ;1
Department of Physics, Stockholm
University, Stockholm, Sweden;
2
Universidade Federal de São
Carlos, Departamento de Física,São Carlos, Brazil; 3 Department of

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Room 1 ICM

Room 4a ICM

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Room 14a ICM

Tokyo, Japan
Quantum measurement and feedforward is the only viable path tobuild scalable quantum technology
with linear optics. Here, we develop
a multi-physics simulation framework to model quantum feedforward in the time domain.

chip-integrated system does notrely on random imperfection-based
backscattering and permits deterministic and robust generation of
single-soliton microcombs.

Huntsville, USA; 4 Lab. Matériaux etPhénomènes Quantiques, Université
Paris Cité&CNRS, Paris, France;
5
Aviation and Missile Center, US
Army CCDC, Redstone Arsenal,
Huntsville, USA
We report a combined experimental/theoretical observation of dramatic enhancement (over three orders of magnitude) in second andthird harmonic efficiencies from aplasmonic gold nanograting resonant at 800nm, relative to the flat
metal layer.

quency Laboratory, Université deNeuchâtel, 2000 Neuchâtel, Switzerland
We present progress in directly blue
diode-pumped Titanium:Sapphire
regenerative amplifier for ultrashort pulse amplification at room
temperature. An optimized pumpconfiguration is studied experimentally and theoretically to reach asmall signal gain > 30 %.

Petersburg, Russia; 2 Connector
Optics LLC, Saint Petersburg,
Russia; 3 ITMO University, Saint Petersburg, Russia; 4 JSC MF Stelmakh
Polyus Research Institute, Moscow,
Russia; 5 Alferov University, SaintPetersburg, Russia
With two-step MBE-MOCVD epitaxy, we fabricated different highpower QCL structures for 8μm
wavelength range. Under shortpulsed pumping, we demonstrated
record-high peak power >16W, as aresult of improved thermal conductivity of the upper contact layer.

de Mallorca, Spain; 4 Institutefor Theoretical Physics, Münster,Germany; 5 Centre for Nanosciences
and Nanotechnology, Palaiseau,
FranceWe demonstrate the existence of
spatially localized structure inside
a self-imaging semiconductor laser
cavity with the help of a thin
chromium metasurface. This system
is also suitable for the multiplexingof exotic light state.

EA-3.6 THU

CK-9.5 THU

EH-3.6 THU

CA-11.6 THU

CB-9.6 THU

EF-4.4 THU

11:45

Detection-loss tolerant real-time
amplitude measurement for ultrafast optical quantum processors:
5-dB squeezing from DC to 43
GHz∙A. Inoue1 , T. Kashiwazaki1 , T.
Yamashima2 ,N.
Takanashi2 ,T. Kazama1 , K. Enbutsu1 , K.
Watanabe1 , T. Umeki1 , M. Endo2,3 ,and A. Furusawa2,3 ; 1 NTT Corporation, Kanagawa, Japan; 2 The
University of Tokyo, Tokyo, Japan;
3
RIKEN, Saitama, Japan
A broadband real-time amplitude
measurement using an opticalphase-sensitive amplifier and ahigh-speed optical communication
detector has been proposed. In
this study, 5 dB squeezing was
successfully measured in real-timefrom DC to 43 GHz.

11:45

Soliton Microcomb RepetitionRate locking via CW Laser
Injection∙T. Wildi1 , A. Ulanov1 , T. Voumard1 ,M. Ludwig1 , and T. Herr1,2 ;1Deutsches Elektronen-Synchrotron
DESY, Hamburg, Germany; 2 Physics
Department, Universität Hamburg
UHH, Hamburg, Germany
Repetition-rate locking of soliton
microcombs through the injectionof an auxiliary continuous-wave
laser in the spectral wing of the soliton is studied, resulting in significant phase-noise reduction and alloptical control.

11:45

Asymmetric Dielectric Metasurfaces for Upconversion Lasers∙N. Sefidmooye Azar1 , M. Parry2,3 ,W.S.L. Lee4,5 , D.-Y. Choi6 , D.N.
Neshev2,3 , and K.B. Crozier1,4,5 ;1School of Physics, University of
Melbourne, Victoria, Australia;
2
Australia National University, Research School of Physics, Canberra,
Australia; 3 Australian ResearchCouncil (ARC) Centre of Excellence
for Transformative Meta-Optical
Systems, Research School of Physics,
The Australian National University,
Canberra,
Australian
CapitalTerritory, Australia; 4 Department
of Electrical and Electronic Engineering, University of Melbourne,
Victoria, Australia; 5 Australian
Research Council (ARC) Centreof Excellence for Transformative
Meta-Optical Systems, Universityof Melbourne, Victoria, Australia;
6Laser Physics Centre, Research
School of Physics, Australia National
University, Canberra, Australia
Previous work has demonstrated
upconversion lasers that use latticeplasmons to provide a resonance atthe lasing wavelength. Here, we experimentally demonstrate an asymmetric dielectric metasurface withhigh-Q resonances at both pumpand lasing wavelengths.

11:45

10 mJ, 100 W, 10 kHz Hybrid
Laser System Based on Rod-Type
End-Pumped Yb:YAG Amplifiers
Featuring Depolarization Compensation∙A. Kazakevičius1,2 , R. Danilevičius2 ,and A. Michailovas1,2 ;1National Center for Physical Sciences and Technology, Vilnius,
Lithuania; 2 Ekspla ltd., Vilnius,
Lithuania
We present a high energy and average power hybrid laser system featuring amplification in end-pumped
rod-type Yb:YAG and a novel depolarization loss reduction techniquethat is based on a spatially variable
waveplate.

154

11:45

Phase-locked and phase-tuned
resonant-MOEMS external cavity
QCLs and their application forfast and broadband mid-infrared
reflectometry∙Y.V. Flores1 , M. Schwarzenberg2 ,A. Merten2 , B. Srocka3 , and M.
Haertelt1 ; 1 Fraunhofer Institute forApplied Solid State Physics, Freiburg,
Germany; 2 Fraunhofer Institute for
Photonic Microsystems, Dresden,
Germany; 3 Sentronics Metrology
GmbH, Mannheim, Germany
We present a multiplexed MOEMSEC-QCL module that combines
three
individual
broadband
resonant-MOEMS EC-QCLs withthe goal of scaling up the broadband
coverage without compromising
the scanning time. We further
discuss applications for wafer-based
IC-manufacturing.

11:45

Localization of spatiotemporalchaos in driven dissipative
systems with parabolic potential∙Y. Sun1 , P. Parra-Rivas1 , M.
Ferraro1 , F. Mangini1 , M. Zitelli1 ,and S. Wabnitz1,2 ; 1 Sapienza
University of Rome, Rome, Italy;2
Istituto Nazionale di Ottica,
Pozzuoli, Italy
We analyze the spatiotemporal dynamics arising in driven dissipative
systems with parabolic potential andpredict the existence of chaoticons,i.e., confined spatiotemporal chaos.

CLEO

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Room 6 Hall B3 (B32)

4Romania;
Max-Born-Institut,
Berlin, Germany
We present a new high-harmonic
generation (HHG) scheme – termed
as strongly overdriven regime – providing continuum radiation ranging
from 18 to 140 eV albeit using long
driving laser pulses, giving a flexible
and compact HHG concept.

CH-10.6 THU

11:45

High-Resolution Distributed
Acoustic Sensor and its
Applications in MechanicalEngineering∙A. Masoudi1 , T. Furness2 , J.
Williamson2 , T. Lee1 , M. Beresna1 ,S. Fletcher2 , X.J. Jiang2 , and
1
G. Brambilla1 ;University ofSouthampton,
Southampton,
United Kingdom; 2 University of
Huddersfield, Huddersfield, United
Kingdom
In this study, the application of highresolution distributed acoustic sensors (H-DAS) in mechanical engineering is studied. It is explained
how such system can act as an artificial nervous system of mechanicalstructures.

CL-2.6 THU

11:45

A Smart Optofluidic Sensing
Platform Ensuring Patients’
Safety during Parenteral
Nutrition Administration∙V. Bello, E. Bodo, and S. Merlo;
Department of Electrical, Computerand Biomedical Engineering, University of Pavia, Pavia, Italy
We present an optofluidic sensing
platform for monitoring the correctness of fluid nutritive drugs administered intravenously during parenteral nutrition, by measuring thedisplacement of a laser beam induced by the liquid refractive index.

CC-1.5 THU

11:45

Subcycle Surface Electron
Emission by Strong-Field THz
Waveforms
S. Li1,2 , A. Sharma3 , P.S. Nugraha1,4 ,Z. Márton3,5 , C. Lombosi1 , Z.
Ollmann1,5 , I. Márton6,7 , P.
Dombi3,6 , J. Hebling1,4,5 , and ∙J.A.
Fülöp1,3 ; 1 Szentágothai ResearchCentre, University of Pécs, Pécs,
2
Hungary;
Tianjin University,
Tianjin, China; 3 ELI-ALPS ResearchInstitute, Szeged, Hungary; 4 MTAPTE High-Field Terahertz ResearchGroup, Pécs, Hungary; 5 Instituteof Physics, University of Pécs, Pécs,
Hungary; 6 Wigner Research Centre
for Physics, Budapest, Hungary;
7
Institute for Nuclear Research(Atomki), Debrecen, Hungary
The confinement of single-cycle
THz-waveform-driven
surfaceelectron emission to one of the two
half cycles and the control of theactive half cycle by changing thefield polarity is demonstrated.

CG-4.6 THU

11:45

High order harmonic generation
with spatially shaped flat top
driver to control XUV chromaticaberrations
K. Veyrinas1 , M. Plach2 , J. Peschel2 ,M. Hoflund2 , F. Catoire1 , C.
Valentin1 , P. Smorenburg3 , H.
Dacasa2 , S. Maclot2 , C. Guo2 , H.
Wikmark2 , A. Zair4 , V. Strelkov5,6 ,C. Picot7 , C. Arnold2 , P. EngJohnsson2 , A. L’Huillier2 , E. Mevel1 ,and ∙E. Constant7 ; 1 Universityof Bordeaux, CNRS, CEA, Celia,
Talence , France; 2 Lund University,
Dept of Physics, Lund, Sweden;
3
ASML
Research,
Veldhoven,
Netherlands; 4 King’s college, London, United Kingdom; 5 Prokhorov
institute Russian academy of sciences , Moscow, Russia; 6 Moscow
institute of physics and technology,
Dolgoprudny, Russia; 7 Univ. Lyon,
CNRS, iLM, Villeurbanne, France
Generation of high order harmonics
in gas with a spatially shaped flattop beam allows us to control the
XUV chromatic aberrations. Flattop driver reduces the XUV chromatic aberrations as compared to a
Gaussian driver.

155

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)acterized by four-probe measurements.

Microtechnology and Nanoscience(MC2), Chalmers University ofTechnology, Gothenburg, Sweden;
4
Université Côte d’Azur, CNRS, Institut de Physique de Nice, Valbonne,
France; 5 Institute of Solid State
Physics, Bulgarian Academy of Sciences, Sofia, Bulgaria; 6 Departmentof Physics, St. Kliment Ohridski
University of Sofia, Sofia, Bulgaria
We introduce two methods for detecting the motional state of a single trapped ion using the AutlerTownes effect and the composite
pulses. They can be used for detection of a Fock or a thermal state.

CE-5.6 THU

EB-11.6 THU

11:45

ZnO based, piezotronic opticalfiber sensors for tracing volatileorganic compounds
D. Lopez-Torres1,3 , C. Elosua
Aguado1 ,G.A. Pappas2 ,M.
Konstantaki3 , A. Klini3 , A. Lappas3 ,F.J. Arregui1 , and ∙S. Pissadakis3 ;1
Electric, Electronic and Communication Department, Public
University of Navarre, Pamplona,
Spain; 2 Composite Materials andAdaptive Structures, ETH Zurich,
3
Institute
Zurich, Switzerland;of Electronic Structure and Laser(IESL), Foundation for Research
and Technology-Hellas, Heraklion,
GreeceZnO films are used as piezotronictransductors overlaid onto tilted
optical fiber Bragg gratings for
tracing volatile organic compounds
vapours down to 10ppm. The ZnO
piezotronic transduction is investigated using optical, structural andnumerical methods.

11:45

Resolving photon numbers using
ultra-high-resolution timing
single-channel electronic readoutof a conventional superconducting nanowire single-photon
detector∙G. Sauer1,2 , M. Kolarczik3 , R.
Gomez1,2 , H. Fedder3 , and F.
Steinlechner1,2 ; 1 Institute of Applied
Physics, Abbe Center of Photonics,
Friedrich Schiller University, Jena,
Germany; 2 Fraunhofer Institutefor Applied Optics and Precision
Engineering IOF, Jena, Germany;
3
SwabianInstruments
GmbH,
Stuttgart, Germany
We show how ultra-high-resolution
timing measurements of the rising and falling edges of electrical pulses generated from superconducting nanowire single-photon detectors enable to distinguish photon
numbers of up to 5 in a single-shotmeasurement.

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Foyer, 1st oor ICM

NOTES

12:00 – 13:00
CLS-1: Career and diversity lunch for early
postdocs
Chair: Rachel Grange, ETH Zurich, Switzerland
Postdocs looking for the next steps in their career will
have the opportunity to share the challenges they are facing with their peers and more advanced researchers. Preregistration is mandatory.

Room 1 ICM

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14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

EA-4: Quantum light sources I

CK-10: Metasurface technologies and applications

EH-4: Tunable and holographic metasurfaces
Chair: Victor Pacheco-Peña, University of Newcastle, United Kingdom

CB-10: Single mode and narrow linewidth semiconductor
lasersEF-5: Dissipative solitonsand mode-locking I

Chair: Leif Oxenløw, DTU Fotonik,
Kgs. Lyngby, Denmark

JSIII-1: Photonic reservoir
computing, extreme learningand ising machines I
Chair: Kathy Lüdge, Ilmenau University of Technology, Germany

Chair: Andrea Knigge, Ferdinand
Braun Institute, Berlin, Germany

Chair: Katarzyna Krupa, Instituteof Physical Chemistry PAS, Warsaw,
PolandCK-10.1 THU

EH-4.1 THU

JSIII-1.1 THU

CB-10.1 THU

EF-5.1 THU

Chair: Vindhiya Prakash, Centre forQuantum Technologies, NUS, Singapore
EA-4.1 THU

14:00

Quantum interference with single
molecules: steps towards a competitive single-photon source∙R. Duquennoy1,2,3 , M. Colautti2,3 ,P. Lombardi2,3 , C. Toninelli2,3 , and
R. Emadi2,3 ; 1 University of Naples
Federico II, Naples, Italy; 2 CNRINO, Sesto Fiorentino, Italy; 3 LENS,
Sesto Fiorentino, Italy
Single molecules are good single
photon source (SPS) candidates
thanks to their good photonic
proper- ties. We here report on
quantum interference in a HongOu-Mandel (HOM) experiment:a fundamental process in bothquantum computation and boson
sampling protocols.

14:00

Multiple Stimuli-Responsive
Polymer Coated Metasurfaces∙S.L. Walden1,2 ,C. Zou1,2,3 ,4,5
P. Poudel , K. Tanaka1,2 , A.
Minovich1,2 , T. Pertsch2,6 , F.H.
Schacher4,5 , and I. Staude1,2 ;1Institute of Solid State Physics,
Abbe Center of Photonics, Friedrich
Schiller University Jena, Jena,
Germany; 2 Institute of Applied
Physics, Abbe Center of Photonics,
Friedrich Schiller University Jena,
Jena, Germany; 3 Institute of Microelectronics, Chinese Academy of
Sciences, Beijing, China; 4 Instituteof Organic Chemistry and Macromolecular Chemistry, Friedrich
Schiller University Jena, Jena,
Germany; 5 Jena Centre for Soft
Matter (JCSM), Friedrich Schiller
University Jena, Jena, Germany;
6
6Fraunhofer Institute of Applied
Optics and Precision Engineering,
Jena, Germany
Tuneable optical metasurfaces, employing an external stimulus, arepromising platforms to achieve tailored, dynamic manipulation ofelectromagnetic fields. We showthat combinations of stimuli can
produce dynamic tuning over a wide
transmission range.

14:00

Sol-gel metasurfaces in barium
titanate for electro-optic tuning∙H. Weigand1 , Ü.-L. Talts1 , V.V.
Vogler-Neuling1 , A. Karvounis1 , J.
Winiger2 , P. Benedek3 , V. Wood3 , J.
Leuthold2 , and R. Grange1 ; 1 ETH
Zurich, Department of Physics, Institute for Quantum Electronics HPT
H3, Auguste-Piccard-Hof 1, 8093
Zurich, Switzerland; 2 ETH Zurich,Department of Information Technology and Electrical Engineering,ETZ K82, Gloriastrasse 35, 8092
Zurich, Switzerland; 3 ETH Zurich,Department of Information Technology and Electrical Engineering, ETZ
H96, Gloriastrasse 35, 8092 Zurich,
Switzerland
Nanofabrication of electro-optic devices is challenging in terms ofmaterial availability and scalability. We design and fabricate softnanoimprinted metasurfaces fromlow-cost, scalable sol-gel barium titanate, enabling fast electro-optic
tuning in the visible and NIR.

14:00

Unconventional Computing basedon Four Wave Mixing in Highly
Nonlinear Media∙K. Sozos1 , S. Deligiannidis1 , C.
Mesaritakis2 , and A. Bogris1 ;1
University of West Attica, Dept.
of Informatics and Computer
Engineering.
Aghiou Spiridonos,
12243, Egaleo, Athens, Greece;
2
University of the Aegean, Dept. ofInformation and Communication
Systems Engineering, Palama 2,
Karlovassi, 83200, Samos, Greece
We propose a novel nonlinear processor for unconventional computing based on the nonlinear properties of four-wave mixing products inhighly nonlinear media. The processor outperforms strong digital nonlinear algorithms in the mitigationof Kerr nonlinearities.

156

14:00

Sub-kHz linewidth, high power,
frequency agile photonic integrated E-DBR laser∙A. Siddharth, G. Lihachev, R. Ning
Wang, X. Ji, Z. Qiu, J. Riemensberger, and T. Kippenberg; Swiss Federal Institute of Technology Lausanne(EPFL), Lausanne, Switzerland
We demonstrate an E-DBR laser
based on hybrid integration of
RSOA and Si3 N4 chip with microheaters, reaching sub-kHz laser
linewidth with more than 30 mW
output power and mode-hop freetuning range upto 62.4 GHz.

14:00

A Reliable Master Equation For
Passively Mode-Locked Lasers
F. Prati1 , A.M. Perego2 , J. Redondo3 ,and ∙G.J. de Valcárcel4 ; 1 Università
dell’Insubria, Como, Italy; 2 Aston
University, Birmingham, United
3
Kingdom;
Universitat Politècnica de València, Gandia, Spain;
4
Universitat de València, Valencia,
Spain
We present a universal masterequation for modelling passively
mode-locked lasers, valid forarbitrary time scales of gain andabsorption dynamics, and describing Q-switching, Q-switchedmode-locking, fundamental andharmonic mode-locking,andlocalised structures.

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Room 14b ICM

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Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

CH-11: Fiber sensors II

CL-3: Lightmatter interaction
Chair: Johann Danzl, Institute of
Science and Technology Austria,
Klosterneuburg, Austria

CG-5: Ultrafast quantum
physics and correlated
systems

CE-6: Optical materials:
Measurements

EB-12: Quantum optics II

Chair:
Costache,Fraunhoffer
Dresden, Germany

CC-2: High power THz
sourcesCH-11.1 THU

Florenta
IPMS

14:00

Distributed Rayleigh Fiber
Sensing Enabling Quantitative
Monitoring in Real Time of the
Refractive Index with a Sub-cm
Resolution∙L. Alliot de Borggraef1,2 and H.
Guillet de Chatellus1,2 ; 1 Laboratoire
InterdisciplinairedePhysique,
UGA/CNRS,
38000
Grenoble,
France; 2 Univ Rennes, CNRS,
Institut FOTON - UMR 6082, 35000
Rennes, France
We report a system based onRayleighscattering
enabling
quantitative monitoring of therefractive index variations along acommercial single-mode fiber witha sub-cm spatial resolution and aninterrogation rate of 20 kHz.

CL-3.1 THU

Chair: Juliette Mangeney, ENS, Paris

Chair: Adrian Pfeiffer, University
Jena, Germany

14:00

CC-2.1 THU (Keynote) 14:00

CG-5.1 THU

On-chip nanotweezers for ultrafast antibacterial susceptibility
testing at the single-cell scale: thecase of bacteriophages∙E. Tartari1 , S. Glicenstein2 , N.
Villa1 , E. Picard2 , E. Hadji2 , P.
Marcoux3 , M. Zelsmann4 , G.
Resch5 , and R. Houdré1 ; 1 Institut
de Physique, Ecole Polytechnique
Federale de Lausanne, Lausanne,
Switzerland; 2 Université Grenoble
Alpes, CEA Grenoble, Grenoble INP,
IRIG, PHELIQS, SiNaPS, Grenoble,
France; 3 Université Grenoble Alpes,
CEA,
LETI,
Minatec-Campus,
4
Grenoble,
France;Université
Grenoble Alpes, CNRS, CEA/LETI
Minatec, Grenoble INP, LTM,
Grenoble, France; 5 Laboratory ofbacteriophages and phage therapy,
Center for Research and Innovationin Clinical Pharmaceutical Sciences(CRISP),
Lausanne
University
Hospital(CHUV),
Lausanne,
Switzerland
In phage therapy, rapid and accurate selection of therapeutic phages
is crucial. We report the use ofphotonic crystal cavities as on-chipnanotweezers for ultrafast analysisof phage susceptibility at the singlebacterium level.

High power ultrafast moves into
the Terahertz domain∙C. Saraceno, S. Mansourzadeh, T.
Vogel, C. Millon, and M. Khalili;
Ruhr University Bochum, Bochum,
Germany
We discuss latest advances in highaverage power laser driven THz
sources, discuss limitations andpresent future applications.

Attosecond Chronoscopy of
Many-Body Correlations between
Bloch Electrons∙J. Freudenstein1 , M. Borsch2 , M.
Meierhofer1 , D. Afanasiev1 , C.P.
Schmid1 , F. Sandner1 , M. Liebich1 ,A. Girnghuber1 , M. Knorr1 , M.
Kira2 , and R. Huber1 ; 1 Departmentof Physics, University of Regensburg,
Regensburg, Germany; 2 Department
of Electrical Engineering and Computer Science, University of Michigan, Ann Arbor, Michigan, USA
Multi-terahertz
fieldsforce
electron-hole pairs in semiconductors onto closed recollision paths.
Precisely clocking these trajectories reveals first-ever attosecond
signatures of many-body correlations between delocalized Blochelectrons, opening unprecedented
views of quantum dynamics andphase transitions.

157

14:00

Chair: Martina Gerken, Kiel University, GermanyCE-6.1 THU

14:00

High-Accuracy Measurement ofRefractive Indices in
GaAs/AlGaAs Thin-Film
Heterostructures∙L.W. Perner1,2 , G.-W. Truong3 , D.
Follman3 , M. Prinz1 , G. Winkler1 ,S. Puchegger4 , G.D. Cole3 , and O.H.
Heckl1 ; 1 Christian Doppler Laboratory for Mid-IR Spectroscopy and
Semiconductor Optics, Faculty Center for Nano Structure Research, Faculty of Physics, University of Vienna,
Vienna, Austria; 2 Vienna Doctoral
School in Physics, University of Vienna, Vienna, Austria; 3 Thorlabs
Crystalline Solutions, Santa Barbara, CA, USA; 4 Faculty Center for
Nano Structure Research, Faculty ofPhysics, University of Vienna, Vienna, Austria
We report a method to simultaneously measure the refractive index
of two materials in as-depositedheterostructures by analysis of
FTIR spectra and extraction oflayer thicknesses via SEM, yielding
excellent results for a GaAs/AlGaAs
DBR.

Chair: Alexander Sergienko, Boston
University, USA

EB-12.1 THU

14:00

Observation of the quantum Gouy
phase
∙M. Hiekkamäki, R.F. Barros, M.
Ornigotti, and R. Fickler; Tampere
University, Tampere, Finland
Using the N00N state phase sensitivity, in conjunction with the intrinsic properties of transverse-spatial
modes, allowed us to investigate
the Gouy phase of Fock-states, inaddition to highlighting importantfeatures and applications of spatial
mode Fock-states.

CLEO

Room 1 ICM
EA-4.2 THU

Room 4a ICM
14:15

Tunable Single-Photon Generation in a Scanning Electron
Microscope based on Silicon
Photonics∙M. Sirotin, T. Chlouba, R.
Shiloh,and P. Hommelhoff;Friedrich-Alexander-Universität
Erlangen-Nürnberg,
Erlangen,Germany
We report a method for generating quantum states of light inside
the silicon-on-insulator microcavities with free electrons in a scanning electron microscope, resulting in tunable over the whole telecom range heralded single-photon
source.

EA-4.3 THU

14:30

High-Brightness Narrowband
Tunable Fiber Laser for Quantum
Dot Excitation∙N.M. Lüpken, M. Brinkmann, S.
Dobner, and T. Hellwig; Refined
Laser Systems GmbH, Münster, Germany
We present a novel turn-key
portable fiber laser for efficientquantum dot excitation to generate
single photons. The laser combinesa mode-hop-free and alignmentfree tunability between 770 nm to980 nm with a high pulse-to-pulse
coherence and excellent stability.

CK-10.2 THU®

/Europe-EQEC 2023

Room 4b ICM
14:15

EH-4.2 THU⋅ Thursday 29 June 2023
Room 13a ICM

14:15

JSIII-1.2 THU

Room 13b ICM
14:15

CB-10.2 THU

Room 14a ICM
14:15

Tuneable Spatially Entangled
Photon-Pair Emission from a
Nonlinear Metasurface∙M.A. Weissflog1 , J. Ma2 , J. Zhang2 ,S. Saravi1 , T. Pertsch1,3 , D.N.
Neshev2 , F. Setzpfandt1,3 , and A.A.
Sukhorukov2 ; 1 Institute of Applied
Physics, Abbe Center of Photonics,
Friedrich Schiller University Jena,
Jena, Germany; 2 ARC Centreof Excellence for Transformative
Meta-Optical Systems (TMOS),
Department of Electronic Materials
Engineering, Research School ofPhysics, The Australian National
University, Canberra, Australia;
3
Fraunhofer Institute for Applied
Optics and Precision Engineering,
Jena, Germany
We experimentally demonstrateentangled photon-pair generationfrom a nonlinear metasurface with
optically tuneable emission angles
facilitated by nonlocal guidedmode resonances.
We observe
orders-of-magnitudeenhancedemission compared to unpatterned
films in transmission, reflection andcounter-propagating geometries.

Mechanically Tunable Conformable Holographic Metasurfaces∙J. Xiao1 , R.I. Hunter1 , D.A.
Robertson1 , G.M. Smith1 , S.
Horsley2 , S.A. Schulz1 , and A.D.
Falco1 ; 1 School of Physics andAstronomy, University of St Andrews, North Haugh, St Andrews,
United Kingdom; 2 Department of
Physics and Astronomy, Universityof Exeter, Stocker Road, Exeter,
United Kingdom
We design, fabricate, and characterize shape-dependent flexible andconformable holographic metasurfaces which produce different images depending on the curvature of
the substrate.

Ultrafast Boltzmann Sampling
using Photonic Ising Machines for
Machine Learning∙G. Van der Sande, F. Böhm, D.
Alonso-Urquijo, and G. Verschaffelt; Applied Physics Research Group,
Vrije Universiteit Brussel, Brussels,
Belgium
Ising machines are a promisingcomputational concept for solving
resource intensive optimization
problems.
We experimentallydemonstrate Boltzmann samplingon an optoelectronic Ising machine
and apply it to the unsupervised
training of stochastic generative
neural networks.

Threshold with photon recycling
in nanolasers with extreme
dielectric confinement∙M. Saldutti1,2 , Y. Yu1,2 , and J.
Mørk1,2 ; 1 DTU Electro, Technical
University of Denmark, Kongens
Lyngby, Denmark; 2 NanoPhoton Center for Nanophotonics, Technical University of Denmark, Kongens
Lyngby, Denmark
We propose a new lasing threshold definition, valid all the way
from the macro to the nanoscaleand reflecting the recycling processthat photons experience in emerging nanolasers with deep subwavelength optical confinement.

EH-4.3 THU

JSIII-1.3 THU

CB-10.3 THU

CK-10.3 THU

Nonlocal metasurfaces with giant
tunability enabled by kirigami∙F. van Gorp, C. Coulais, and J. van
de Groep; Van der Waals-Zeeman
Institute, Institute of Physics, University of Amsterdam, Amsterdam,
Netherlands
We demonstrate reconfigurable
optical metasurfaces using flexible
kirigami substrates to mechanicallytune non-local resonances ofsilicon nanoparticle arrays. Using
numerical simulations we show anear unity reflection with 45 times
larger than the resonance linewidth.

14:30

Large Area Plasmonic Metasurface for Augmented Reality
G. Cardoso, F. Hamouda, V.
Yam, and ∙B. Dagens; Université
Paris-Saclay, CNRS, Centre deNanosciences et de Nanotechnologies, Palaiseau, France
We evaluate the impact of spatial arrangement of plasmonic nanostructures composing metasurfaces on
their global optical characteristics inthe visible spectrum. Considering
two fabrication methods we discuss
their relevance for Augmented Reality application.

14:30

14:30

Exploiting Kerr Nonlinearity for
Photonic Extreme Learning
Machines∙A. Lupo, M. Zajnulina, and S.
Massar; Laboratoire d’Information
Quantique, Université libre de Bruxelles, Bruxelles, Belgium
A fiber-based Extreme Learning
Machine (ELM) is introduced.
It exploits Kerr nonlinearity toprocesses information encoded in
the input frequency-comb lines.
We experimentally show that the
Kerr-enhanced ELM outperforms
its computer-based counterpart
network.

158

14:30

Sub-MHz linewidth UV laser
diode for metrologicalapplications
R. Kervazo1 , A. Congar2 , G.
Perin1 , L. Lablonde3 , R. Butté4 ,N. Grandjean4 , L. Bodiou1 , J.
Charrier1 , and ∙S. Trebaol1 ; 1 Univ
Rennes, CNRS, Institut FOTON- UMR 6082, Lannion, France;2
Oxxius, 4 rue Louis de Broglie,
Lannion, France; 3 Exail, rue Paul
Sabatier, Lannion, France; 4 Instituteof Physics, Ecole PolytechniqueFédérale de Lausanne (EPFL),
Lausanne, Switzerland
We report a compact sub-MHz
linewidth UV laser diode laser basedon a fiber bragg grating external cavity. The laser emits a single modeemission at 399.6 nm with a 40 dB
side mode suppression ratio.

EF-5.2 THU

14:15

Influence of time-delayed feedback on the dynamics of temporal
localized structures in passively
mode-locked semiconductor
lasers∙T. Seidel1 , A. Bartolo3 , N. Vigne4 ,A. Garnache4 , G. Beaudoin5 , I.
Sagnes5 , M. Giudici3 , J. Javaloyes2 ,S. Gurevich1 , and M. Marconi3 ;1
Institute for Theoretical Physics& Center for Nonlinear Science(CeNoS), University of Münster,Germany; 2 Dpt. de Física, Universitat de les Illes Balears & IAC-3,
Campus UIB, Palma de Mallorca,
Spain; 3 Université Côte d’Azur,
Centre National de La Recherche
Scientifique, Institut de Physique deNice, Valbonne, France; 4 Institutd’Electronique et des Systèmes,UMR5214, University of Montpellier, France; 5 Centre de Nanosciences
et de Nanotechnologies, CNRS,
Université Paris-Saclay, UMR 9001,
Palaiseau, France
We analyze the effect of optical feedback on the dynamics of modelocked semiconductor lasers operated in the regime of temporal localized structures. Depending on the
feedback delay harmonic solutions
can be either reinforced or hindered.
EF-5.3 THU

14:30

Simple scheme for generation of
two-color photonic molecules
S. Willms1,2 , ∙S. Bose2,3 , O.
Melchert1,2 , U. Morgner1,2 , I.
Babushkin1,2 , and A. Demircan1,2 ;1Institute of Quantum Optics,
Hannover, Germany; 2 Cluster of
Excellence PhoenixD, Hannover,Germany; 3 Institute of Photonics,
Hannover, Germany
The generation of two-color photonic molecules is challenging,
due to the requirement of two incommensurable yet group-velocity
matched frequencies. We propose
a spectral tunneling based selfgeneration scheme from a single
input pulse.

CLEO

Room 14b ICM
CH-11.2 THU

Room Osterseen ICM
14:15

Fibre optic distributed temperature sensing with a CMOS SPAD
array
∙C. Tye, K. Ehrlich, A. Green, and
M. Tanner; Institute of Photonics
and Quantum Sciences, Heriot-Watt
University, Edinburgh, United Kingdom
Improvements to distributed temperature sensing measurements aredemonstrated using a CMOS SPAD
array offering multiplexed photon
counting and therefore rapid measurement (10 s) with ∼1 ∘ C accuracy,
and the ability to measure over >100m.

CH-11.3 THU

14:30

Whispering-gallery modes toinvestigate opto-mechanicalinteractions in optical fibers∙L.A. Sánchez1 , M. DelgadoPinar1,2 , A. Díez1,2 , and M.V.
Andrés1,2 ; 1 Laboratory of Fiber
Optics,ICMUV,
Universidad
de Valencia, Burjassot, Spain;2
Departamento de Física Aplicada yElectromagnetismo, Universidad de
Valencia, Burjassot, Spain
A novel optical method toinvestigate
opto-mechanicalresonances in optical fibers isdemonstrated.
Based on the
excitation of whispering-gallery
modes, transverse acoustic mode
resonances, which are responsible
for the forward Brillouin scattering
effect, are characterized.

CL-3.2 THU

14:15

Cellular Level Resolution
Ambient Mass Spectrometry
Imaging using 3 μm Laser
Ablation∙R.A. Battle1 , D. Simon2,3 , Y.
Xiang2 , K. Robinson2,3 , T.H.
Runcorn1 , R.T. Murray1 , and Z.
1
Takats2,3 ;Femtosecond Optics
Group, Department of Physics,
Imperial College London, London,
2
United Kingdom;
Department
of Systems Medicine, Faculty of
Medicine, Imperial College London,
London, United Kingdom; 3 The
Rosalind Franklin Institute, Didcot,
United Kingdom
We report a parametric 3 μm laserbased ambient mass spectrometry
imaging platform. Single-cell level
pixel size (10 μm) images of mousebrain samples acquired using ourplatform are presented.

CL-3.3 THU

14:30

Steering stable light fields throughdynamic scattering media∙C. Sharp1 , C. Mididoddi1 , P. delHougne2 , S. Horsley1 , and D.B.
Phillips1 ; 1 Department of Physics
and Astronomy, University of Exeter, Exeter, United Kingdom; 2 Univ.
Rennes, CNRS, IETR, Rennes, France
We study light control through partially moving scattering systems. We
present a suite of new methods toguide light around hidden moving
regions, relying only on external
camera measurements.

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)⋅ Thursday 29 June 2023
Room 6 Hall B3 (B32)

CG-5.2 THU

14:15

Quantum Beat Spectroscopy ofHelium Photoelectrons∙D. Hoff, S. Mikaelsson, S. Carlström,
P.K. Maroju, N. Ouahioune, C. Guo,
C.L. Arnold, A. L’Huillier, and M.
Gisselbrecht; Department of Physics,
Lund University, Lund, Sweden
Quantum beat spectroscopy is a versatile method for studying excitedstates in matter. We apply it to Helium and study the interference pattern in the low kinetic energy region
near ionization threshold.

CG-5.3 THU

CE-6.2 THU

14:15

Room 8 Hall A1 (A12)
EB-12.2 THU

14:15

Mid-Infrared Dual-Comb Spectroscopy and FTIR Microscopy to
Study Transparent Glasses Modified In-Bulk with Femtosecond
Lasers∙M. Singleton; Empa, Dübendorf,
Switzerland
We investigate in the mid-IR
absorbance and refractive index
changes of transparent glass samples, which have been irradiatedwith focused fs-laser pulses. The
aim is to enable fast closed-loop
control of the machining process.

Certification of Non-GaussianStates using Double Homodyne
Detection∙G.
Roeland1 ,N.
TripierMondancin1 ,D. Barral1 ,U.
Chabaud2,3 , F. Grosshans3 , D.
Markham3,4 , M. Walschaers1 , V.
Parigi1 , and N. Treps1 ; 1 Laboratoire
Kastler Brossel, Sorbonne Université,
ENS-PSL Université, Collège deFrance, Centre National de laRecherche Scientifique, 4 place
Jussieu, Paris, France; 2 Universitéde Paris, IRIF, CNRS, Paris, France;
3
Sorbonne Université, LIP6, CNRS,
4 place Jussieu, Paris, France;
4
JFLI, CNRS, National Institute ofInformatics, University of Tokyo,
Tokyo, Japan
In this work, we report on the use of
double homodyne detection on optical frequency comb pulses for thecertification of non-Gaussian features of quantum states, without theneed for full tomography.

CE-6.3 THU

EB-12.3 THU

14:30

Few-femtosecond Limit of the
Floquet Theory∙M. Lucchini1,2 , F. Medeghini1 , Y.
Wu1,2 , F. Vismarra1,2 , R. BorregoVarillas2 , A. Crego2 , F. Frassetto3 , L.
Poletto3 , S.A. Sato4,5 , H. Hübener5 ,U. De Giovannini5,6 , Á. Rubio5,7 ,and M. Nisoli1,2 ; 1 Department of
Physics, Politecnico di Milano, Milano, Italy; 2 Institute for Photonics and Nanotechnologies, IFN-CNR,
Milano, Italy; 3 Institute for Photonics and Nanotechnologies, IFNCNR, Padova, Italy; 4 Center for
Computational Sciences, Universityof Tsukuba, Tsukuba, Japan; 5 Max
Planck Institute for the Structure
and Dynamics of Matter, Hamburg,
Germany; 6 Università degli Studi
di Palermo, Dipartimento di Fisica
e Chimica-Emilio Segrè, Palermo,
Italy; 7 Center for Computational
Quantum Physics (CCQ), The Flatiron Institute, New York, USA
Few-fs pulses of controlled time duration and intensity are used to create a Floquet state of a free electron. Comparison with an analytical model proves that the Floquet
theory surprisingly holds in the fewcycle limit.
159

Room 7 Hall A1 (A11)

14:30

Inverse calculation of liquid
crystal parameters using scientificmachine learning∙C.P. Jisha1 , A. Alberucci1 , and S.
Nolte1,2 ; 1 Friedrich Schiller University, Jena, Germany; 2 Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany
A novel method based on scientificmachine learning to characterize aliquid crystal cell is developed.

14:30

Quantum Control and Coherenceof Orbital Levels of a Tin-Vacancy
Color Center in a Diamond
Nanopillar∙C.G. Torun1 , J.H.D. Munns1 ,F.M. Herrmann1 ,M. IsazaMonsalve1 , V. Villafane2 , A. Thies3 ,T. Pregnolato1,3 , G. Pieplow1 , and T.
Schröder1,3 ; 1 Humboldt-Universität
zu Berlin, Department of Physics,
Berlin, Germany; 2 Walter Schottky
Institut and Physik Department,
Technische Universität München,
Münich, Germany; 3 FerdinandBraun-Institut, Berlin, Germany
We control two different qubits configurations selected from the orbital
levels of a tin-vacancy center in diamond and measure their coherence. We implement experimentswith coherent population trapping,ultrashort optical pulses, and quasicontinuous driving.

CLEO

Room 1 ICM
EA-4.4 THU

Room 4a ICM
14:45

CK-10.4 THU®

/Europe-EQEC 2023

Room 4b ICM
14:45

EH-4.4 THU⋅ Thursday 29 June 2023
Room 13a ICM

14:45

JSIII-1.4 THU

Room 13b ICM
14:45

CB-10.4 THU

Room 14a ICM
14:45

EF-5.4 THU

14:45

GaAs Site-controlled Pyramidal
Quantum Dots as Spin Qubit
Sources for a Photonic Cluster
State Construction: the Role ofLight-hole-like Excited States∙F. Mattana1 , I. Ranjbar Jahromi1 ,G. Ronco2 , M. Rota2 , F.B. Basset2 , R.
Trotta2 , E. Pelucchi1 , and G. Juska1 ;1
Tyndall National Institute, Cork,
Ireland; 2 Sapienza University, Rome,
Italy
We present a comprehensive spectroscopic study of highly uniform
energetic structure of Pyramidalsite-controlled GaAs quantum dots
specifically directing our interest to
their applicability to the photonic
cluster state generation.

Halide perovskite metasurfaces
with tunable exciton-polariton
electroluminescence∙Y. Wang1,2 , J. Tian1,3 , M. Klein1,3 ,G. Adamo1,3 , H. Son Tung4 , and C.
Soci1,3 ; 1 Centre for Disruptive Photonic Technologies, TPI, Nanyang
Technological University, Singapore;
2
Interdisciplinary Graduate School,
Energy Research Institute @NTU
(ERI@N), Nanyang Technological
University, Singapore; 3 School ofPhysical and Mathematical Sciences,
Nanyang Technological University,
Singapore; 4 Institute of Materials
Research and Engineering, Agency
for Science Technology and Research(A*STAR), Singapore
We report strong coupling between
excitons and photonic bound statesin the continuum in electricallydriven perovskite metatransistors.
We show tunability of electroluminescence directivity by drainsource voltage and polarization control through metasurface design.

Tunable Chiral Electro-Optic
Metasurfaces∙L. Wang and I. Shadrivov; Australian National University, Canberra, Australia
We numerically study polarisation
conversion achieved by anisotropic
metasurfaces made of electro-optic
material on silica substrates and findthe tunable cross-polarisation transmission coefficient is 0.5, while thetunability of circular dichroism isclose to 0.8.

Phase vs. Intensity Encoding in an
Experimental Time Delay Reservoir Computing Scheme∙I. Estébanez, L. Talandier, I. Fischer,and A. Argyris; Instituto de Física Interdisciplinar y Sistemas Complejos
IFISC (CSIC-UIB), Palma de Mallorca, Spain
We compare information encoding
schemes in phase and intensity in atime delay RC with external opticalinformation injection. We experimentally demonstrate smaller errors
in a time series prediction task when
encoding in phase.

Red-Emitting Distributed Bragg
Reflector Lasers for StrontiumBased Optical Atomic Clocks∙N. Goossen-Schmidt1 , C. Pyrlik1,2 ,B. Arar1 , M.T. Hassan1 , A.
Bawamia1 , J. Fricke1 , A. Knigge1 ,A. Maaßdorf1 , M. Schiemangk1 ,H. Wenzel1 , and A. Wicht1 ;1
Ferdinand-Braun-Institut, LeibnizInstitut für Höchstfrequenztechnik,
Berlin, Germany; 2 Institut für
Physik, Humboldt-Universität zu
Berlin, Berlin, Germany
We developed compact, monolithic
distributed Bragg reflector lasers at
689 nm and 707 nm for strontium
optical clocks. At more than 40 mW
output power, they provide a record
spectral linewidth of only 0.4 MHz.

Switching dynamics of soliton
molecular complexes in a 2 μm
ultrafast fiber laser∙Y. Zhou1 , J. Shi1 , G. Hu1 , and K. K.
Y. Wong1,2 ; 1 Department of Electrical and Electronic Engineering, The
University of Hong Kong, Hong kong,
China; 2 Advanced Biomedical Instrumentation Centre, Hong Kong
Science Park, Hong kong, China
We report the switching dynamics of soliton molecular complexes
around 2 μm that can be triggeredby the collision of drifting soliton,
simultaneously opening an emerging window in the longer wavelength.

EA-4.5 THU

CK-10.5 THU

EH-4.5 THU

JSIII-1.5 THU

CB-10.5 THU

EF-5.5 THU

15:00

An ultra-broadband, integrated
mid-infrared photon-pair source∙F. Roeder, R. Pollmann, A.
Gnanavel, O. Brecht, C. Eigner, L.
Padberg, M. Stefszky, B. Brecht, and
C. Silberhorn; Paderborn University,
Integrated Quantum Optics, Institute for Photonic Quantum Systems(PhoQS), Warburger Straße 100,
33098, Paderborn, Germany
We demonstrate a broadband,
mid-infrared PDC source basedon a periodically poled Ti:LiNbO3
waveguide exceeding a bandwidthof 23 THz achieved via optimizationof group velocity and group velocity
dispersion for signal and idler
photons.

15:00

Addressable Metasurfaces byElectrically Driven Transparent
Conducting Oxide Micro-Heaters∙K. Zangeneh Kamali1 , L. Xu2 ,N. Gagrani1 , H.H. Hoe Tan1 , C.
Jagadish1 , A. Miroshnichenko3 , D.
Neshev1 , and M. Rahmani2 ; 1 ARC
Centre of Excellence for Transformative Meta-Optical Systems, Research
School of Physics, The Australian
National University, Canberra, Australia; 2 Advanced Optics and Photonics Laboratory, Department ofEngineering, School of Science andTechnology, Nottingham Trent University, Nottingham , United Kingdom; 3 School of Engineering and Information Technology, University of
New South Wales, Canberra, Australia
We demonstrate a rapid and programmable amplitude modulator
based on the thermo-optical effectby integrating transparent conducting oxide micro-heaters with

15:00

Security applications of laser-empowered plasmonic metamaterials
V.D. Le, H. Ma, N. Dalloz, F. Vocanson, and ∙N. Destouches; University Jean Monney, Laboratory Hubert
Curien, Saint-Etienne, France
Image multiplexing enables a surface to display different images depending on the conditions of observation. Here laser processingof random plasmonic metasurfaces
enables the encryption of up to
four images observable under whitelight.

15:00

Programming optical learning
machines with spatial-spectral
optimization∙L.J.-L. Hsieh1,2 , Y. Zhou1,2,3 ,I. Oguz1,2 , M. Yildirim1,2 , N.U.
Dinc1,2 , C. Gigli2 , K.K.Y. Wong3 , C.
Moser1 , and D. Psaltis2 ; 1 Laboratoryof Applied Photonics Devices,
École Polytechnique Fédérale deLausanne, Switzerland; 2 Optics
Laboratory, École PolytechniqueFédérale de Lausanne, Switzerland;
3
Department of Electrical and Electronic Engineering, The University ofHong Kong, China
A multi-mode fiber-based opticalprocessor is programmed with 99%
fewer parameters compared to a digital counterpart.

160

15:00

25-layer stacked 1.55 um-band
Quantum Dot DFB Laser∙A. Matsumoto, T. Umezawa,
S. Nakajima, and K. Akahane;
National Institute of Information
and Communications Technology(NICT), Koganei, Japan
In this paper, we report we fabricated a 1.55 μm-band QD-DFBLD with a possibly unprecedented
multi-stacked structure, such as 25
layers, and the obtained characteristics were much better than the results we reported previously.

15:00

Pump depletion limits the existence of Kerr solitons in singlyresonant optical parametricoscillators∙C. Mas Arabí1 , N. Englebert1 , P.
Parra-Rivas2 , S.-P. Gorza1 , and F.
Leo1 ; 1 OPERA-photonics, Université
libre de Bruxelles, Brussels, Belgium;
2
Dipartimento di Ingegneria dell’ Informazione, Elettronica e Telecomunicazioni, Sapienza Università diRoma, Rome, Italy
We analyze Kerr dissipative solitons
in a parametrically driven resonator.
We employ variational methods toanalytically calculate the soliton existence region and use this result toobtain the pump-to-soliton power
conversion.

CLEO

Room 14b ICM
CH-11.4 THU

Room Osterseen ICM
14:45

CL-3.4 THU

14:45

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)CC-2.2 THU⋅ Thursday 29 June 2023
Room 6 Hall B3 (B32)

14:45

CG-5.4 THU

14:45

Room 7 Hall A1 (A11)
CE-6.4 THU

14:45

Room 8 Hall A1 (A12)
EB-12.4 THU

14:45

A Fibre Optic Force Sensing
Method Based on the S2 Imaging
TechniqueA. Srikanthan1 , ∙N. Vukovic1 ,C. Codemard2 , and M. Zervas1 ;1
Optoelectronics Research Centre, University of Southampton,
Southampton SO17 1BJ, U.K.,
Southampton, United Kingdom;
2
TRUMPF Lasers UK Ltd, Wellington Park, Tollbar Way, Hedge End,Southampton SO30 2QU, U.K.,
Southampton, United Kingdom
We report an implementation of alarge-mode-area optical fibre combined with a self-interferometricspatial and spectral (S2) imaging
technique for force sensing. The advantages of the method include thedesign simplicity and low temperature sensitivity.

On-chip optical nanotweezers forphage trapping and identification∙S. Glicenstein1 , N. Villa2 , E.
Tartari2 , E. Picard1 , P.R. Marcoux3 ,M. Zelsmann4 , G. Resch5 , R.
Houdré2 , and E. Hadji1 ; 1 Univ.
Grenoble Alpes, CEA Grenoble,
Grenoble INP, IRIG, PHELIQS,
SiNaPS, Grenoble, France; 2 Institut
de Physique, École PolytechniqueFédérale de Lausanne, Switzerland;
3
University Grenoble Alpes, CEA,
LETI-DTBS-SBSC-LCMI/LBAM,
4
Grenoble,
France;University
Grenoble Alpes, CNRS, CEA/LETI
Minatec, Grenoble INP, LTM,
Grenoble, France; 5 Laboratory ofbacteriophages and phage therapy,
CRISP, Lausanne University Hospital(CHUV), Lausanne, Switzerland
For phage therapy the developmentof a fast phagogram to identify the
optimal phages to administer is essential. We report the use of onchip nanotweezers for phage trapping and distinguish them according to their family

THz time-domain spectroscopy
with a GHz single-cavity dualcomb laser∙B. Willenberg1 , C.R. Phillips1 , J.
Pupeikis1 , S.L. Camenzind1 , L.
Liebermeister2 , R.B. Kohlhaas2 ,B. Globisch2 , and U. Keller1 ;1Department of Physics, ETH
Zurich,Zurich,Switzerland;2
Fraunhofer Institute for Telecommunications, HHI, Berlin, Germany
We present rapid THz-TDS witha free-running single-cavity dualcomb. Combined with efficient photoconductive antennas the system
has competitive performance: 55 dB
dynamic range in the THz spectrumat 2 GHz resolution and 2 s measurement time.

A look under the tunnelingbarrier via attosecond-gatedinterferometry∙O. Kneller1 , D. Azoury1 , Y.
Federman1 , M. Krueger1 , A.J.
Uzan1 , G. Orenstein1 , B.D. Bruner1 ,O. Smirnova2 , S. Patchkovski2 ,M. Ivanov2 , and N. Dudovich1 ;1
Weizmann institute of science , Rehovot, Israel; 2 Max-Born Institute,
Berlin, Germany
Attosecond-gated interferometry
integrates subcycle gating with alloptical attosecond interferometry.
It perturbs the tunneling dynamics
and maps it into the phase of theemitted harmonics, probing theevolution of the wavefunction in
the classically forbidden region.

Temperature dependence ofemission cross section andfluorescence lifetime of Tm:YLF
in the 78-300 K range∙M. Pergament1 , U. Demirbas 1,2 ,J. Thesinga1 , M. Kellert1 , and F.
Kärtner1,3 ; 1 Deutsches ElektronenSynchrotron
DESY,CenterforFree-Electron Laser Science, Hamburg, Germany; 2 Antalya Bilim
University,Laser Technology Laboratory , Antalya , Turkey; 3 Universityof Hamburg,Physics Department,
Hamburg, Germany
We present a detailed study of thespectroscopic properties of Tm:YLF
to understand its amplification performance at cryogenic temperatures. Fluorescence lifetime andemission measurements suggest thatcryogenic amplifiers on Tm:YLF canreach kW power levels.

Quantum State Tomography of
Qudits via Hong-Ou-MandelInterference∙Y. Tsujimoto1 , R. Ikuta2,3 , K.
Wakui1 , T. Kobayashi2,3 , and M.
Fujiwara1 ; 1 National Institute ofInformation and Communications
Technology (NICT), Koganei, Tokyo,
Japan; 2 Graduate School of Engineering Science, Osaka University,
Toyonaka, Osaka, Japan; 3 Centerfor Quantum Information and
Quantum Biology, Osaka University,
Toyonaka, Osaka, Japan
We propose and experimentallydemonstrate a method to performthe quantum state tomography ofan n-partite qudit state embedded
in single photons based on the
Hong-Ou-Mandelinterference
between the target photon andancillary probe light.

CH-11.5 THU

CL-3.5 THU

CC-2.3 THU

CG-5.5 THU (Invited)CE-6.5 THU

EB-12.5 THU

15:00

X-ray profiling with an enhanced
backscattering optical fibre in
single mode-multimode-single
mode configuration∙M.
Olivero1 ,A.
Bellone1 ,1
A. Vallan , W. Blanc2 , M.
Benabdesselam2 , F. Mady2 , and
G. Perrone1 ; 1 Politecnico di Torino,
dept. of Electronics and Telecommunications, Torino, Italy; 2 Université
Côte d’Azur, CNRS, Institut dePhysique de Nice, Nice, France
A novel optical fibre sensor for commissioning in X –ray radiotherapy ispresented. It relies on an enhanced
backscattering fibre used in a single mode-multimode-single mode
configuration that converts the dose
into a wavelength shift.

15:00

Photo-activated Phosphate
Minerals and Femto-second
pulsed near-IR Lasers for the
Restoration of Damaged Dental
Enamels∙A. Jha1 , N. Iqbal1 , S. Strafford1 ,S.K. Lognathan1 , E.K. Barimah1 ,A.D. Anastasiou3 , J. Wu2 , M.
Malinowski2 , A. Nielson2 , S. Pavitt2 ,B. Nattress2 , and T. Brown4 ; 1 Schoolof Chemical & Process Engineering,
University of Leeds, UK; 2 Schoolof Dentistry and Leeds Dental
Hospital, University of Leeds,
UK; 3 Department of Chemicalengineering & Analytical Sciences,
Manchester, UK; 4 School of Physics
and Astronomy, University of St.
Andrews, UK
We demonstrate a novel methodology for restoring acid-eroded
enamel with photo-active minerals
and a 100femto-second pulsedlaser, operating at 1040nm with
100MHz repetition rate.
The

15:00

Broadband THz emission from
LT-GaAs photoconductive
antenna driven by Yb-doped fiber
amplifier at 200 kHz repetition
rate∙N. Nilforoushan1 , C. Kidd2 , A.
Fournier1 , S. Dhillon1 , J. Freeman2 ,and J. Mangeney1 ; 1 Laboratoirede Physique de l’Ecole Normale
Supérieure, ENS, Université PSL,
CNRS, Sorbonne Université, Université de Paris, Paris, France;
2
School of Electronic and ElectricalEngineering, University of Leeds,
Woodhouse Lane, Leeds, United
Kingdom
We report on the broadband THz
emission with peak electric fieldexceeding 10 kV/cm using conventional LT-GaAs photoconductive antenna driven by optical pulses
at 1030 nm wavelength at a repetition rate of 200 kHz.

15:00

Engineering optical Schrödinger”cat” and entangled states using
intense laser-atom interactions∙P. Tzallas; Foundation for Research
and Technology-Hellas, Institute ofElectronic Structure & Laser, GR70013 Heraklion (Crete), Greece.,
Heraklion (Crete), Greece
I will present our recently developed fully quantized approach, withwhich, optical Schrödinger ”cat”
and entangled states have been produced by implementing quantum
operations in the high harmonic
generation process induced by intense laser-atom interactions.

161

15:00

Revelation and analysis of opticalphase delay exhibited by Al-doped
4H-SiC due to current induction∙H. Du1 , H. Takeda1 , T. Kadowaki2 ,N. Tate1 , T. Kawazoe2 , Y. Oki1 ,M. Ohtsu3 , and K. Hayashi1 ;1Depertment of Electronics, Kyushu
University, 744 Motooka, Nishi-ku,
Fukuoka, 819-0395, Japan; 2 Nichia
Corporation, 3-13-19 Moriya-cho,
Kanagawa-ku, Yokohama, Kanagawa, 221-0022, Japan; 3 Research
Origin for Dressed Photon, 3-1319 Moriya-cho,
Kanagawa-ku,
Yokohama, Kanagawa, 221-0022,
Japan
This article discusses a SiC-SLM
that exhibited an extremely large
magneto-optical effect in the visible range, and examined the photophysical properties of this device,especifically the phase delay.

15:00

Phase-noise-insensitive orthogonality verification of singlephoton-level temporal modes∙J. Szuniewicz1 , S. Sagona-Stophel2 ,S. Thomas2 , I. Walmsley2 , and M.
Karpiński1 ; 1 Faculty of Physics,
University of Warsaw, Warszawa,
Poland; 2 Quantum Optics andLaser Science, Blackett Laboratory,
Imperial College London, London,
United Kingdom
A second-order interference technique for measuring the orthogonality of temporal modes at the single photon level is presented. It is
resistant to phase fluctuations andallows for an infinite measurement
length without loss of visibility.

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metasurfaces. The system exhibits
sub-millisecond rise-time and ninefolds of amplitude modulation.
EA-4.6 THU

15:15

CK-10.6 THU

15:15

EH-4.6 THU

15:15

JSIII-1.6 THU

15:15

CB-10.6 THU

15:15

EF-5.6 THU

15:15

Purcell enhanced single-photon
emission from a QD coupled to a
Gaussian-shaped microcavity∙L. Engel, S. Kolatschek, T. Herzog,
S. Vollmer, M. Jetter, S.L. Portalupi,
and P. Michler; Institut für Halbleiteroptik und Funktionelle Grenzflächen, University of Stuttgart,
Stuttgart, Germany
Gaussian-shaped microcavities are
realized by epitaxial overgrowth of
DBRs on wet-chemically etched microlenses. The mode structure isanalysed and a quantum dot is tuned
on resonance with the cavity mode
showing Purcell-enhanced singlephoton emission.

Second Harmonic Generation in
Monolithic Gallium Phosphide
Metasurfaces∙M. Yang1,2 , M. Weissflog2 , D.
Arslan1,2 , T. Pertsch2 , and I.
Staude1,2 ; 1 Institute of Solid State
Physics, Friedrich Schiller University
Jena, Jena, Germany; 2 Instituteof Applied Physics, Abbe Centerof Photonics, Friedrich Schiller
University Jena, Jena, Germany
We numerically investigate second
harmonic generation in resonantmonolithic GaP metasurfaces with<110> crystal orientation, reachinga conversion efficiency of 5.5×10^(4). The potential of the metasurfaces
for nonlinear wavefront shaping applications is also explored.

Environment-Dependent Holographic Metasurfaces In The
Visible Range∙J. Xiao, L. Yan, T. Plaskocinski, M.
Biabanifard, S. Persheyev, M. Askari,
and A.D. Falco; School of Physics andAstronomy, University of St Andrews,
North Haugh, St Andrews, United
Kingdom
We discuss the properties of tunable holographic metasurfaces that
encode different images on both therefractive index of the surrounding
medium and the wavelength used toreveal them.

Optical Computing for Machine
Learning with Integrated Waveguides∙M. Yildirim1 , I. Oguz1 , F.
Kaufmann2 , M.R. Escale2 , R.
Grange2 , D. Psaltis1 , and C. Moser1 ;1Ecole Polytechnique Federal deLausanne - EPFL, Lausanne,
Switzerland; 2 Eidgenössische Technische Hochschule Zurich -ETHZ,
Zurich, Switzerland
We present a data transformation
approach with nonlinear wave
propagation inside lithium niobate waveguides to improve theperformance of machine learning
applications. The results indicate
10% accuracy increase compared todigital models on several datasets.

Non-linear broad spectral tuningof a semiconductor laser andapplication to coherent dual
frequency source∙B. Chomet1 , S. Blin2 , A. Bartolo2 ,G. Beaudoin3 , I. Sagnes3 , and
A. Garnache2 ; 1 Laboratoire dePhysique de l’École Normale
Supérieure, Paris, France; 2 IES, Univ
Montpellier, CNRS, Montpellier,France; 3 C2N, CNRS UMR 9001,
Université Paris-Saclay, Palaiseau,
FranceWe report on non-linear broad spectral tuning of a low-noise single frequency laser based on III-V semiconductor technology. A fundamental study of non-linear multimode laser dynamics showed theroute to red-shifted single-mode operation.

Implications of tristability indissipative Kerr soliton formation∙E.K. Akakpo1 , M. Haelterman
1, F. Leo1 , and P. Parra-Rivas1,2 ;1
OPERA-photonics, Universit librede Bruxelles, Bruxelles, Belgium;
2
Dipartimento
diIngegneriadell’Informazione,
Elettronica
e Telecomunicazioni,
Sapienza
Universitá di Roma, Roma, Italy
We study the implications oftristability in dissipative soliton
formation in dispersive Kerr
optical cavities when secondandfourth-orderchromatic
dispersion are considered, unveiling the transition between
standard-homoclinic-snaking- andcollapsed-homoclinic-snakingrelated states.

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

EA-5: Quantum light sources II

CK-11: Photonic crystals andperiodic structures

EH-5: Concepts and applications in plasmonics andmetastructures

JSIII-2: Photonic reservoir
computing, extreme learningand ising machines II

CB-11: High-performance
diode lasers

EF-6: Dissipative solitonsand mode-locking II

Chair: Andrea Bragas, Universidad
de Buenos Aires, Argentina

Chair: Daniel Brunner, Université deFranche-Comté, FEMTO, Besançon,FranceChair: Karl Häusler, Ferdinand
Braun Institute, Berlin, Germany

Chair: Julien Javaloyes, University ofBalearic Islands, Palma de Mallorca,
Spain

EH-5.1 THU

JSIII-2.1 THU

CB-11.1 THU

EF-6.1 THU

Chair: Alexei Ourjoumtsev, College
de France, Paris, France

EA-5.1 THU

16:00

Novel unipolar quantum dot
diode structures for advanced
sources of quantum light∙S.L. Portalupi1 , T. Strobel1 , J.H.
Weber1 , M. Schmidt2 , L. Wagner1 ,L. Engel1 , M. Jetter1 , A.D. Wieck2 , A.
Ludwig2 , and P. Michler1 ; 1 Institut
für Halbleiteroptik und Funktionelle
Grenzflächen, Center for Integrated

Chair: Mukundakumar Balasubrahmaniyam, Tel Aviv University, Israel

CK-11.1 THU

16:00

Wide-bandwidth and LowReflection High-efficiency
Grating Couplers∙X. Zhou and H.K. Tsang; The Chinese University of Hong Kong, Hong
Kong, China
We proposed photolithographybased grating coupler that has -0.95
dB coupling efficiency with 1 dB

16:00

Inverse-designed opticalmetagratings for free-space
integral equations solving∙A. Cordaro1 , B. Edwards2 , V.
Nikkhah2 , A. Alù3 , N. Engheta2 , and
A. Polman1 ; 1 AMOLF, Amsterdam,
Netherlands; 2 University of Pennsylvania, Philadelphia, USA; 3 City
University of New York, New York,

16:00

Scalable Delay Line-Free
All-Optical Reservoir∙I. Boikov1 , D. Brunner2 , and A. De
Rossi1 ; 1 Thales Research and Technology, Palaiseau, France; 2 FEMTOST, Besançon, FranceAhighlycompact(104
neurons/mm2 ) reservoir computer composed of directly coupled

162

16:00

GaAs-based wide-aperture single
emitters with 68 W output power
at 69% efficiency realized using aperiodic buried-regrown-implantstructure
B. King, S. Arslan, A. Boni, P.S.
Basler, C. Zink, P. Della Casa,
D. Martin, A. Thies, A. Knigge,and ∙P. Crump; Ferdinand-Braun-

16:00

Comb-driven cavity solitons – amultidimensional study in freespace enhancement cavities∙M. Högner1,2 , A. Hertlein1,2 , P.
Sulzer3,4 , J. Schmuck1,2 , C. Hofer3,4 ,A.K. Mills3,4 , D.J. Jones3,4 , and I.
Pupeza1,2,5 ; 1 Max Planck Instituteof Quantum Optics, Garching,
Germany; 2 Ludwig-Maximilians-

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Room 8 Hall A1 (A12)enamel wear rates were investigatedfrom in vitro studies using healthy
volunteers.
CH-11.6 THU

15:15

CL-3.6 THU

15:15

CC-2.4 THU

15:15

Integrated photonic interrogatorsfor fiber-optic sensing systems∙S. Stopiński1,2,3 , K. Anders1,2,3 ,A. Jusza1,3 , M. Słowikowski4 , A.
Bieniek1 , and R. Piramidowicz1,2,3 ;1Warsaw University of Technology,
Institute of Microelectronics andOptoelectronics, Warsaw, Poland;
2
LightHouse Sp.
z o.o., Lublin,
Poland; 3 VIGO Photonics S.A.,Ożarów
Mazowiecki,
Poland;4
Warsaw University of Technology,
Centre for Advanced Materials andTechnologies CEZAMAT, Warsaw,
PolandWe present and discuss photonic
integrated interrogators of fiber
Bragg gratings, based on an arrayed waveguide grating (AWG)
demultiplexer and asymmetric
Mach-Zehnderinterferometers(AMZI).

Femtosecond laser crosslinking ofcollagen for local increase of
corneal stiffness∙A. Stoecker1,2 , T.J. Glandorf2 ,T. Koch3 , R. Ackermann3 , S.
Nolte3,4 , J. Missbach-Guentner5 ,and C. Russmann1,6 ; 1 University ofApplied Science and Arts, Facultyof Engineering and Health, Goettingen, Germany; 2 Georg-AugustUniversity, Faculty of Chemistry,
Goettingen, Germany; 3 Institute ofApplied Physics, Abbe Center of Photonics, Friedrich-Schiller-University,
4
Jena,
Germany;
Fraunhofer
Institute for Applied Optics andPrecision Engineering, Jena, Germany; 5 University Medical Center,
Department of Diagnostic and Interventional Radiology, Goettingen,Germany; 6 Molecular-BiomarkersNanoimaging Laboratory, Brigham&
Women’s
hostpital/Harvard
Medical School, Boston, USA
Due to the rising demand for myopia correction, we introduce alaser application for vision correction without ablation. For that, we
directly crosslink corneal collagento increase the local stiffness and individually form the cornea.

High-intensity single-cycle THz
source driven by a high-power
fiber laser
R. Becheker1 , L. Guiramand2 ,∙A. Martinez3,4 , S. Idlahcen1 , J.
Houard5 , T. Godin1 , X. Ropagnol2 ,D. Paparo4 , F. Blanchard2 , A. Vella5 ,and A. Hideur1 ; 1 CORIA, UMR6614
CNRS, INSA Université de Rouen
Normandie, Saint Etienne duRouvray, France; 2 Département degénie électrique, École de technologie
supérieure, Montréal, Québec H3C
1K3, Canada; 3 CNR-ISASI, Instituteof Applied Sciences and Intelligent
Systems ‘E. Caianiello’, 80078
Pozzuoli, Italy; 4 Scuola Superiore
Meridionale, Largo S. Marcellino,
10, 80138 Napoli, Italy; 5 GPM
UMR6634 CNRS, INSA Universitéde Rouen Normandie, Saint Etienne
du Rouvray, France
We report on the generation of intense THz pulses by optical rectification in lithium niobate using ahigh-power ultrafast fibre laser. THz
pulses with 800 fs duration and 114
mW average power are produced.

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

CH-12: Super-resolution
imaging

CL-4: Photonic technology
for biomedical applications

CC-3: Novel approach THz
sources

Chair: Cristian Focsa, University ofLille, France

Chair: Thomas Huser, University ofBielefeld, Germany

CH-12.1 THU

CL-4.1 THU

16:00

Lensless scanning super-resolved
imaging of arbitrary shaped
objects∙S. Kurdiumov1 , T. Grant1 , J.-Y.
Ou1 , E. Plum1 , N. Papasimakis1 , K.
MacDonald1 , and N.I. Zheludev1,2 ;1University of SouthamptonOptoelectronics Research Centre &Centre for Photonics Metamate-

16:00

Interferometric Gated Off-Axis
Reflectometry (iGOR) - A Label
Free Method to Measure Lipid
Membrane Dynamics and Deduce
Biophysical Properties∙F. Turley1 , D. Regan2 , P. Borri2 ,and W. Langbein1 ; 1 School of Physics
and Astronomy, Cardiff University,
Cardiff, United Kingdom; 2 School

CE-6.6 THU

15:15

EB-12.6 THU

15:15

Illuminating Hidden Symmetries
in Topological Insulator Thin
Films
∙B.C. Connelly, P.J. Taylor, and G.J.
de Coster; DEVCOM Army ResearchLaboratory, Adelphi, Maryland, USA
Topological photocurrents in lowtwinned Bi2Se3 are studied using
THz spectroscopy and symmetry
analysis of nonlinear optical photoresponses.
We find emergent
threefold symmetric responses of
the intrinsic crystal are induced by
the circular photon drag effect.

Experimental Demonstration ofHigh-dimensional Hyperentangled Quantum States∙L.J. Gonzalez Martin del Campo1,2 ,N.E.
Tangarife
Villamizar1,2 ,S.
Sharma1,2 ,C.
Spiess1,2 ,R. Sondenheimer1,2 ,and F.
Steinlechner1,2 ; 1 Fraunhofer IOF,
Jena, Germany; 2 Friedrich Schiller
University, Jena, Germany
We present the experimental
demonstration of high-dimensional
hyperentangled quantum states of
up to an eight-dimensional Hilbert
space in the time-energy andpolarization degrees of freedom.

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

CG-6: Attosecond methods
and fundamentals

CE-7: Nonlinear opticalmaterials

EB-13: Quantum simulationand computation

Chair: Hartmut Roskos, University
of Frankfurt, Germany

Chair: Balasz Major, ELI ALPS,
Szeged, Hungary

Chair: Virginie Nazabal, Universityof Rennes, Institute of Chemical Sciences, France

Chair: Fabrizio Piacentini, Istituto
Nazionale di Ricerca Metrologica,
Torino,CC-3.1 THU

CG-6.1 THU

CE-7.1 THU (Invited)

EB-13.1 THU

16:00

Single-Cycle THz Generation
Inside a Modelocked Thin-Disk
Laser∙Y. Wang, S. Mansourzadeh, T.
Vogel, and C.J. Saraceno; RuhrUniversität-Bochum, Bochum, Germany
We demonstrate the generation of
single-cycle THz pulses intracavity

16:00

Breakdown of the Single-Collision
Condition in Gas-Phase HighHarmonic Generation
P.-A. Chevreuil1 , F. Brunner1 ,U. Thumm2 , U. Keller1 , and ∙L.
Gallmann1 ; 1 ETH Zurich, Department of Physics, Zurich, Switzerland;
2
Kansas State University, Department of Physics, Manhattan, Kansas,

163

16:00

Post-2000 nonlinear optical materials and their characterization:
data tables and best practices∙N. Vermeulen1 , D. Espinosa2 , A.
Ball3 , J. Ballato4 , P. Boucaud5 , G.
Boudebs6 , C. Campos7 , P. Dragic8 ,A. Gomes7 , M. Huttunen9 , N.
Kinsey3 , R. Mildren10 , D. Neshev11 ,L. Padilha12 , M. Pu13 , R. Secondo3 ,16:00

Experimental Demonstration of
Entangled Photonic Qubits in aContinuous-Time Quantum Walk
∙R.J. Chapman1 , S. Häusler2 , G.
Finco1 , F. Kaufmann1 , and R.
Grange1 ; 1 Optical NanomaterialGroup, Institute for Quantum
Electronics, Department of Physics,
ETH Zurich, Zurich, Switzerland;

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Quantum Science and Technology(IQST) and SCoPE, Universityof Stuttgart, Stuttgart, Germany;
2
Lehrstuhl für Angewandte Festkörperphysik,
Ruhr-Universität
Bochum, Bochum, Germany
A novel n-i-n diode structure embedding semiconductor quantum
dots is demonstrated. Very low
photon decoherence over timescales
covering 6 orders of magnitude isproven combining three complementary spectroscopy techniques.
Spectral and charge tuneability isshown.

bandwidth 76 nm, and low reflection one with -0.73 dB coupling
efficiency with minimum reflection
low as -44 dB.

USA
Inverse-designed metasurfaces cansolve prescribed Fredholm integral
equations at optical wavelengths. To
this end, a mirror is included to provide the feedback required to perform the Neumann series that solves
the equation.

nonlinear integrated microcavities
is proposed, allowing real-time autonomous processing of high-speed
optical signals in optical domain.

Institut gGmbH, Leibniz-Institut für
Höchstfrequenztechnik, Berlin, Germany
915nm BRIS diode lasers using
laterally periodic buried-regrownimplant-structuring deliver 68W
pulsed power with 69% efficiency(500μs) from a single 1.2mm
aperture in a miniaturized package
and sustain a lateral super-mode to
30W continuous wave power.

Universität München, Garching,
Germany; 3 Quantum Matter Institute, University of British Columbia,
Vancouver, Canada; 4 Department of
Physics and Astronomy, Universityof British Columbia, Vancouver,
Canada; 5 Leibniz Institute of Photonic Technology—Member of the
Research Alliance ‘Leibniz HealthTechnologies’, Jena, Germany
Free-space cavities enable highpeak-power,
250-nm-bandwidth
dissipative solitons generated fromatemporally-inhomogeneous
pulse seed of 25 nm bandwidth.
Seed parameters determine theformation of single solitons versus
soliton molecules.
Systematic
variation yields a map of possible(multi-)soliton states.

EA-5.2 THU

CK-11.2 THU

EH-5.2 THU

JSIII-2.2 THU

CB-11.2 THU

EF-6.2 THU

16:15

Squeezed Light for Future
Gravitational Wave Detectors∙F. Meylahn1,2 , B. Willke1,2 , and H.
Vahlbruch1,2 ; 1 Max Planck Institutefor Gravitational Physics, Hannover,Germany; 2 Leibniz Universität Hannover, Hannover, Germany
The application of squeezed lightenables to reach sensitivities beyond the standard quantum limit
in laser interferometry. We present
today’s highest squeezing level at1550 nm wavelength covering thecomplete detection band of future
gravitational-wave detectors.

16:15

Scaling Theory of Wave Confinement in Classical and Quantum
Periodic Systems∙M. Kozon1,2 , A. Lagendijk1 , M.
Schlottbom2 , J.J.W. van der Vegt2 ,and W.L. Vos1 ; 1 Complex Photonic Systems (COPS), MESA+ Institute for Nanotechnology, University of Twente, Enschede, Netherlands; 2 Mathematics of Computational Science (MACS), MESA+ Institute for Nanotechnology, University of Twente,, Enschede, Netherlands
We present a rigorous method toclassify the dimensionality of wave
confinement in periodic superlattices, applicable to any type of physical system: acoustic, electromagnetic, electronic, spin, etc.

16:15

Mode-independent resonances incascaded-mode resonators∙V. Ginis, I.-C. Benea-Chelmus, J. Lu,
M. Piccardo, and F. Capasso; John
A. Paulson School of Engineering andApplied Sciences, Harvard University, Cambridge, MA 02138, USA
We introduce a new class of optical resonators that uses transverse
mode coupling in a cascade process,established by mode-converting reflectors. The resonator characteristics differ from Fabry-Perot resonators and can be modified overwide ranges.

16:15

Speeding up a time-delay
photonic reservoir∙M. Goldmann1 , I. Estebanez1 , E.A.
Vlieg2 , C.R. Mirasso1 , I. Fischer1 ,A. Argyris1 , and M.C. Soriano1 ;1Instituto de Física Interdisciplinar
y Sistemas Complejos (IFISC, UIBCSIC), Palma de Mallorca, Spain;2
IBM Research, Zürich, Switzerland
We demonstrate numerically andexperimentally significant accelerations of a photonic delay-based
reservoir used for time series forecasting. Even for a constant long delay, we achieve near GHz data processing rates with high prediction
accuracy.

164

16:15

High power, internally wavelengthstabilized diode lasers withepitaxially-stacked multiple active
regions for LiDAR applications∙A. Knigge, N. Ammouri, H. Christopher, M. Beier, J. Fricke, A. Maaßdorf, A. Ginolas, J. Glaab, A. Liero,and H. Wenzel; Ferdinand-BraunInstitut, Berlin, Germany
905nm-lasers with 3 active regions
in common waveguides stabilized
by Bragg gratings are reported with
<0.5nm linewidth, 0.07nm/K thermal shift, 2.2kW ns-pulse-powerfrom bars and 100W from single
emitters. 5-active-zone lasers show
further increased performance.

16:15

Real-time evolution of passive
free-space cavity solitons∙P. Sulzer1,2 ,M. Högner3,4 ,A. Hertlein3,4 , J. Schmuck3,4 , C.
Hofer1,2 , A.K. Mills1,2 , I. Pupeza3,4,5 ,and D. Jones1,2 ; 1 Quantum Matter
Institute, University of British
Columbia, Vancouver, Canada;
2
Department of Physics and Astronomy, University of British Columbia,
Vancouver, Canada; 3 Max-PlanckInstitut für Quantenoptik, Garching,
Germany; 4 Ludwig-MaximiliansUniversität München, Garching,
Germany; 5 Leibniz Institute of Photonic Technology - Member of the
Research Alliance ’Leibniz HealthTechnologies”, Jena, Germany
We use shot-to-shot spectroscopy
and interferometry to investigate
the dynamics of dissipative highpeak-power temporal solitons in afree-space passive resonator driven
by a mode-locked laser frequency
comb. We discuss soliton generation, collision, and noise suppression.

CLEO

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/Europe-EQEC 2023

⋅ Thursday 29 June 2023

Room 14b ICM

Room Osterseen ICM

Room 1 Hall B1 (B11)

Room 6 Hall B3 (B32)

Room 7 Hall A1 (A11)

Room 8 Hall A1 (A12)rials, University of Southampton,
Southampton, United Kingdom;2
Centre for Disruptive Photonics
Technologies, Nanyang Technological
University,
Singapore,
Singapore
We build super-resolution images ofarbitrary shaped and sized objects
pixel-by-pixel via deep learningenabled analysis of their light scattering patterns.
First proof-ofprinciple experiments show resolution better that λ/4.

of Biosciences, Cardiff University,
Cardiff, United Kingdom
Interferometric Off-axis reflectometry is a novel label-free microscopy
technique that allows observation at
327Hz of both the thickness and axial position of suspended lipid membrane. We have optimised methods
for creating and observing model
membranes.

of a modelocked thin-disk laser using a simple and cost-efficient 50μm thin LiNbO3 plate, reaching 1.2
mW THz average power from acompact and efficient setup.

USA
When producing soft x-ray highharmonics, interactions of photoelectrons with neighboring atoms
may become important. We study
this regime experimentally and theoretically and provide guidelines on
how to mitigate those collisions.

Institute for Sensors and Electronics, University of Applied Sciences
and Arts Northwestern Switzerland,Windisch, Switzerland
We experimentally demonstrate
the quantum CNOT gate in acontinuous-time quantum walk,realized in a lithium niobate-oninsulator waveguide array.
We
verify the two-qubit operation with
82.3 ± 4 % fidelity and prepare entangled Bell states with 88.9 ± 0.4 %fidelity.

CH-12.2 THU

CL-4.2 THU

CC-3.2 THU

CG-6.2 THU

E. Tokunaga14 , D. Turchinovich15 ,J. Yan11 , K. Yvind13 , K. Dolgaleva2 ,and E. Van Stryland16 ; 1 Vrije Universiteit Brussel, Brussels, Belgium;
2
University of Ottawa, Ottawa,
3
Canada;Virginia Commonwealth University, Richmond, USA;
4
Clemson University, Clemson, USA;
5
Université Côte d’Azur, SophiaAntipolis, France; 6 Univ Angers,
7
Angers, France;
Universidade
Federal de Pernambuco, Recife,
Brazil; 8 University of Illinois at
Urbana-Champaign, Urbana, USA;
9
Tampere University, Tampere,
Finland; 10 Macquarie University,
Sydney, Australia; 11 Australian
National University,
Canberra,
Australia; 12 Universidade Estadualde Campinas, Sao Paulo, Brazil;
13
Technical University of Denmark,Lyngby, Denmark; 14 Tokyo University of Science, Tokyo, Japan;
15
Universität Bielefeld, Bielefeld,
Germany; 16 University of Central
Florida, Orlando, USA
On the occasion of 60 years of
nonlinear-optical research,wepresent new data tables listing
nonlinear-optical properties fordifferent material categories asreported in the literature since
2000, and provide best practices fortheir characterization.

16:15

Flexible multicore-multimodefiber endoscope for superresolution imaging∙Z. Lyu1,2 , K. Abrashitova1 , J.F.
de Boer2 , E.R. Andresen3 , H.
Rigneault4 , and L.V. Amitonova1,2 ;1Advanced Research Center for
Nanolithography,
Amsterdam,
2
Netherlands;
Department of
Physics and Astronomy, and LaserLaB, Vrije Universiteit, Amsterdam,
Netherlands; 3 Univ. Lille, CNRS,UMR 8523 - PhLAM - Physique desLasers, Lille, France; 4 Aix-Marseille
Universit’e, CNRS, Centrale Marseille, Institut Fresnel, Marseille,
FranceA novel concept of super-resolution
imaging through a flexible hairthin fiber probe is demonstrated.
The long-standing problem of multimode fiber imaging is solved by using a unique multicore-multimodeprobe and computational compressive sensing algorithms.

16:15

Phase contrast imaging methods
using laser based Kα X-ray source
A. Ferré1 ,∙R. Clady1 ,G.
Giakoumakis2 ,D. Gutz1 ,J.
Primot3 , O. Utéza1 , and A.
Stolidi4 ; 1 Aix-Marseille University/CNRS,
Marseille,
France;2
Université
Paris-Saclay/ONERA
DMAS, Paris, France; 3 Université
Paris-Saclay/ONERADOTA,Paris, France; 4 Université ParisSaclay/CEA, , Paris, France
We present the first adaptation ofmulti-lateral shearing interferometry (MLSI) technique on laser-based
K alpha X-ray source operating at ahigh repetition rate (100 Hz) withinteresting potential for time resolved phase contrast imaging.

16:15

New Standards in Intense,
Broadband Terahertz Generation
via Optical Rectification∙N.K. Green, C. Rader, D.J.H. Ludlow, B.W. Palmer, S.-H.(.
Ho,
Z. Zaccardi, M.J. Lutz, A. Alejandro, M.F. Nielson, G.A. ValdiviaBerroeta, C. Chartrand, P. Peterson, D.J. Michaelis, and J.A. Johnson;
Brigham Young University, Provo,USA
We present the nonlinear opticalcrystals PNPA and MNA and provide an analysis of their opticaland THz properties. These crystals
outperform industry standards inbroadband THz generation throughoptical rectification.

16:15

Adjustable polarisation gate forHigh Order Harmonic Generation∙C. Picot1 , T. Nemec2 , F. Catoire2 ,J. Vabek2,3,4 , and E. Constant1 ;1
Institut Lumière Matière, UMR
5306 Université Lyon 1 - CNRS,
Université de Lyon, Villeurbanne,
France; 2 Centre des Lasers Intenses
et Applications, Université deBordeaux-CNRS-CEA,,
Talence,
France; 3 ELI Beamlines Centre,
FZU- Institute of Physics of the Czech
Academy of Sciences, Na Slovance2, 182 21, Prague, Czech Republic;
4
Czech Technical University in
Prague, FNSPE, Brehov´a 7, 115 19,
Prague, Czech Republic
We generate high order harmonics with polarisation gating. We
show that we can displace our narrow gate temporally without distorting it, which continuously shifts thecentral frequency of the harmonics, without changing the spectral
width.

165

2

EB-13.2 THU

16:15

Efficient photon conversion in ascalable microwave-to-optics
transducer
M. Weaver, P. Duivestein, A.
Bernasconi, S. Scharmer, M.
Lemang, T. van Thiel, F. Hijazi,
B. Hensen, S. Gröblacher, and∙R. Stockill; QphoX B.V., Delft,
Netherlands
We present a high-bandwidth,
ultra-low noise microwave-tooptical transducer based on
Lithium
Niobate-on-SOI.
We
realise efficient transduction in
the quantum ground state, adding
6.2±1.8 photons of input-referrednoise.

CLEO

Room 1 ICM
EA-5.3 THU

Room 4a ICM
16:30

CK-11.3 THU®

/Europe-EQEC 2023

Room 4b ICM
16:30

EH-5.3 THU⋅ Thursday 29 June 2023
Room 13a ICM

16:30

JSIII-2.3 THU

Room 13b ICM
16:30

CB-11.3 THU

Room 14a ICM
16:30

EF-6.3 THU

16:30

Two-photon emission and correlations from a superlattice-based
superconducting light-emitting
structure∙S. Bouscher1 , D. Panna1 , K.
Balasubramanian2 , R. Jacovi1 , A.
Kumar1 , C. Schneider3 , S. Höfling3 ,and A. Hayat1 ; 1 Department ofElectrical Engineering, Technion,
Haifa, Israel; 2 Electrical Engineering
Faculty, Indian institute of technology, Kanpur, India; 3 Technische
Physik, Physikalisches Institut andWilhelm Conrad Röntgen ResearchCenter for Complex Material
Systems, Universität Würzburg,
Würzburg, Germany
We demonstrate evidence of
two-photon emission and photon pair correlations, resulting
from injected Cooper-pairs insuperconductor-semiconductor
structures. Such structures can beutilized for multiple applications
including enhanced two-photon
gain, electrically-driven entangledphoton generation and Bell-state
analyzers.

Propagation-Invariant TwoPhoton Suppression Induced by
Polarization-Mediated Artificial
Gauge Fields∙M. Ehrhardt1 , C. Dittel2,3,4 ,M. Heinrich1 , and A. Szameit1 ;1Institute for Physics, Universityof Rostock, Rostock, Germany;2
Physikalisches Institut, AlbertLudwigs-Universität
Freiburg,
Freiburg, Germany; 3 EUCOR Centre
for Quantum Science and Quantum
Computing,Albert-LudwigsUniversität Freiburg,
Freiburg,Germany; 4 Freiburg Institute forAdvanced Studies, Albert-LudwigsUniversität Freiburg,
Freiburg,Germany
We construct artificial gauge
fields in waveguide lattices withcustomized birefringence and experimentally demonstrate that, fora net phase of π, two-photon statesremain steadily suppressed during
propagation in square lattices.

Surface Roughness effects on ENZ
media IR spectra∙D. Navajas, J.M. Pérez-Escudero,
and I. Liberal; Department of Electrical, Electronic and Comunnications
Engineering, Insitute of Smart Cities(ISC), Public University of Navarre(UPNA), Pamplona, Spain
We experimentally investigate theeffect of surface roughness on ENZ
media using SiC substrates. The
ENZ band is found to be morerobust than dielectric and SPhP
bands across different roughness
size-scales.

Delay-based reservoir computing
with spin-VCSELs: Interplay
between internal dynamics andperformance
L. Mühlnickel, L. Jaurigue, and ∙K.
Lüdge; Institut für Physik, Technische
Universität Ilmenau, Ilmenau, Germany
We numerically investigate thetime-series prediction performanceof a delay-based reservoir computer
based on a spin-VCSEL with
optically-injected phase-modulated
data. A strong dependence on theinternal charge-carrier timescales isfound which enables speed-up andoptimization.

High power CW 780 nm diodelasers for use in additive manufacturing∙S. Arslan, P.S. Basler, B. King, J.
Glaab, A. Maaßdorf, D. Martin, A.
Knigge, A. Ginolas, S. Kreutzmann,and P. Crump; Ferdinand-BraunInstitut gGmbH, Leibniz-Institut
für Höchstfrequenztechnik GustavKirchhoff-Straße 4, 12489, Berlin,
Germany
780nm TM-polarized diode lasers
for additive manufacturing application are demonstrated with
25W continuous wave power from
1200μm stripes and beam quality
suitable for coupling into 1mm-core
fiber, exploiting efficient epitaxial
designs and low thermal-resistance
mounting.

Long-Range “Talking” of Vector
Solitons and their Synchronization in Fabry-Pérot Resonators∙L. Hill1,2 , E.-M. Hirmer1,3 , G.
Campbell2 , T. Bi1,3 , A. Ghosh1,3 ,G.-L. Oppo2 , and P. Del’Haye1,3 ;1Max Planck Institute for the
Science of Light, Erlangen, Germany; 2 University of Strathclyde,
Glasgow,
UnitedKingdom;
3Friedrich-Alexander-Universität
Erlangen-Nürnberg,
Erlangen,Germany
We study Kerr interactions of differently polarized solitons in highQ Fabry-Pérot cavities. With otherresults, we show how the maximum
number of soliton pairs can be limited – useful for vectorial frequency
comb generation and telecommunications.

EA-5.4 THU

CK-11.4 THU

EH-5.4 THU

JSIII-2.4 THU

CB-11.4 THU

EF-6.4 THU

16:45

Theory of Spontaneous Parametric Down-Conversion in Thin
Etalons∙E.A. Santos1 , F. Setzpfandt1,2 , and
S. Saravi1 ; 1 Institute of Applied
Physics, Abbe Center of Photonics,
Friedrich Schiller University Jena,
Jena, Germany; 2 Fraunhofer Institute for Applied Optics and Precision
Engineering, Jena, Germany
We develop a theoretical descriptionof photon-pair generation in nonlinear etalons that can naturally treat
internal Fabry-Pérot interference effects and study angular propertiesof pairs generated in forward andcounter-propagating configurations
in subwavelength thin etalons.

16:45

Permanent Tailoring of BIC
Resonances Using Temperature∙A. Kuppadakkath1 , A. Barreda1 ,L. Ghazaryan1 ,T. Bucher1 ,2
K. Koshelev , Y. Kivshar2 , T.
Pertsch1,3,4 , D. Choi2 , I. Staude1,4 ,and F. Eilenberger1,3,4 ; 1 Friedrich
Schiller University Jena, Jena,
Germany; 2 Australian National
University, Canberra, Australia;
3
Fraunhofer-Institute for Applied
Optics and Precision Engineering
IOF, Jena, Germany; 4 Max Planck
School of Photonics, Jena, Germany
All-dielectric metasurfaces can support Quasi-Bound states in the continuum (BIC) resonances. We showthat gradual and short-term heating can be utilized for thermal
postprocessing-assisted permanent
tailoring of BIC resonance in the visible and near-infrared range.

16:45

Ultrafast Dynamics of Gigahertz
Nano-optomechanical Metasurface Array∙I. Ajia1 , J.-Y. Ou2 , N. Zeludev2 ,and O. Muskens1 ; 1 Physics andAstronomy, Faculty of PhysicalSciences and Engineering, Universityof Southampton, Southampton,
United Kingdom; 2 Optoelectronics
Research Centre and Centre for
Photonic Metamaterials, Universityof Southampton, Southampton,
United Kingdom
Using ultrafast transient spectroscopy, we investigate optomechanical modes in dielectricmetasurface array.
Here, weleverage the tunability of the pumpwavelength to demonstrate precise
control of the vibrational modes ina SiC based metasurface array.

16:45

An autonomous semiconductor
laser neural network∙A. Skalli1 , X. Porte1 , N. Haghighi2 ,S. Reitzenstein2 , J. Lott2 , and D.
Brunner2 ; 1 UBFC - FEMTO-ST
Institute, Besançon, France; 2 Institut
für Festkörperphysik, Technische
Universität Berlin, Berlin, Germany
We implemented a fully autonomous and parallel neuralnetwork of 350+ nodes using offthe-shelf componenets. Our systemshows excellent performance inheader recognition tasks.
Our
approach is highly relevant andscalable in size and bandwidth.

166

16:45

Monolithic MMI-coupler-based
Dual-Wavelength MOPA at 830
nm for Spectroscopic Applications∙A. Müller, J.-P. Koester, L.S.
Theurer, J. Fricke, H. Wenzel, A.
Knigge, and B. Sumpf; FerdinandBraun-Institut(FBH),
Berlin,Germany
A monolithic, multi-mode interference coupler-based master oscillator
power amplifier at 830 nm is presented. It provides 500 mW narrowband, dual-wavelength laser emission in alternating or parallel operation, suitable for Raman and THz
spectroscopy.

16:45

Kerr cavity solitons in active
PT -symmetric dimers∙J. Yelo-Sarrión1 , C. Mas Arabí1 ,P. Parra-Rivas2 , F. Leo1 , and S.-P.
Gorza1 ; 1 OPERA-photonics, Université libre de Bruxelles, Bruxelles, Belgium; 2 Dipartimento di Ingegneriadell’Informazione, Elettronica e Telecomunicazioni, Sapienza Università
di Roma, Roma, Italy
We study the existence and stabilityof Kerr cavity solitons in coherently
driven coupled ring resonators withgain and loss, for non-identical ring
resonance frequencies and close to
the PT -symmetric regime.

CLEO

Room 14b ICM
CH-12.3 THU

Room Osterseen ICM
16:30

CL-4.3 THU

16:30

®

/Europe-EQEC 2023

Room 1 Hall B1 (B11)CC-3.3 THU

Room 6 Hall B3 (B32)

16:30

Surpassing the diffraction limit
via Hermite-Gaussian Imaging forincoherent two-dimensional
objects∙J. Frank, A. Duplinskiy, K. Bearne,
and A.I. Lvovsky; University of Oxford, Oxford, United Kingdom
We present Hermite-Gaussian
Imaging, a generally applicable
super-resolution imaging scheme in
the far field using linear optics andinnovative passive measurements.
We surpass the diffraction limit
and achieve a resolution limited byphoton shot noise.

Preservation of orbital angularmomentum of light alongpropagation through a turbid
tissue-like scattering medium∙A. Sdobnov1 , I. Lopushenko1 , A.
Bykov1 , and I. Meglinski1,2 ; 1 OptoElectronics and Measurement Techniques, University of Oulu, Oulu,
Finland; 2 College of Engineering andPhysical Sciences, Aston University,
Birmingham, United Kingdom
We show that upon propagation
through a turbid tissue-like scattering medium the orbital angular momentum of light is preserved witha noticeably different phase shift –twist of light, providing a high potential for tissue diagnosis.

Multicycle Terahertz Generation
Using High-energy Pulse Trains∙C. Rentschler1,2 , Z. Zhang1 ,U. Demirbas1 , K. Ravi1 , M.
Pergament1 , N.H. Matlis1 , and1
F.X. Kärtner1,2,3 ;Center for
Free-Electron Laser Science CFEL,
Deutsches Elektronen-Synchrotron
DESY,
Hamburg,
Germany;2
Department of Physics, Universityof Hamburg, Hamburg, Germany;
3
The Hamburg Centre for Ultrafast
Imaging, University of Hamburg,
Hamburg, Germany
We report on precise parameter
control of multicycle terahertz generation by nonlinear optical conversion using a new approach basedon tunable high-energy pulse trains
and demonstrate its potential toboost current sub-percent conversion efficiencies.

CH-12.4 THU

CL-4.4 THU

CC-3.4 THU

16:45

Fabrication of a 3D-printed
device for super-resolution lightmicroscopy using two-photon
polymerization∙G. Zyla1 , G. Maconi2 , A. Nolvi2 , D.
Ladika3 , V. Melissinaki1 , J. Marx4 ,I. Kassamakov2 , and M. Farsari1 ;1
IESL/FORTH, Heraklion, Greece;
2
University of Helsinki, Helsinki,
Finland; 3 Department of Materials
Science and Technology, University ofCrete, Heraklion, Greece; 4 Ruhr University Bochum, Bochum, Germany
This work presents a novel approachto developing a flexible device forachieving spatial super-resolution
in conventional light microscopes
and scanning white light interferometers. The super-resolution wasachieved using a microstructure
printed by two-photon polymerization.

16:45

Adaptive Metasurfaces for Smart
Standalone Histopathology with
Polarized Light using adaptive
metasurfaces∙C. Dirdal1 , P. Thrane1 , C. Meng2 , O.
Sieryi3 , A. Bykov3 , S. Bozhevolnyi2 ,and I. Meglinski3 ; 1 SINTEF Smart
Sensors and Microsystems, Oslo,
Norway; 2 Centre for Nano Optics,
University of Southern Denmark,Odense, Denmark; 3 Optoelectronics
and Measurement Techniques Unit,
University of Oulu, Oulu, Finland
We present a novel polarization sensitive histophatology modality for
detection of cancer in tissue, and ourambition to further develop it towards a smart, standalone system byuse of adaptive metasurfaces.

⋅ Thursday 29 June 2023

CG-6.3 THU (Invited)

16:30

Attosecond Interferometry∙N. Dudovich; Weizmann Institute of
Science, Rehovot, Israel
Attosecond science encodes the subcycle dynamics of a quantum system in the coherent properties ofattosecond pulses. Advanced interferometric schemes resolves such
coherence and retrieves fundamental phenomena, from tunneling inatoms and molecules to ultrafast dynamics in solids.

16:45

Efficient Photoconductive Terahertz Generation with Tunable
Pulse Compression and Highfrequency Modulation∙Y. Lampert, A. Tomasino, S. Rajabali, and I.-C. Benea-Chelmus; Ecole
Polytechnique Federale de Lausanne(EPFL), Lausanne, Switzerland
We demonstrate a substantial improvement in generated Terahertz
shape and intensity from photoconductive antenna in 7.5-meter telecom fiber link using a tunable prism
pair. We achieve modulation frequencies up to 75 MHz with electrooptic modulation.

167

Room 7 Hall A1 (A11)
CE-7.2 THU

16:30

Room 8 Hall A1 (A12)
EB-13.3 THU

16:30

Surface Second-Harmonic Generation in Molecularly Bonded
InGaP Waveguides on Si Thermal
Oxide∙A. Peralta Amores and M. Swillo;
School of Engineering Sciences, RoyalInstitute of Technology (KTH), Stockholm, Sweden
Heterogeneous integration of 2 mmlong and 235 nm thick double
inverse-tapered InGaP waveguides
on thermally grown SiO2 via nativeoxide molecular bonding is demonstrated. Second-harmonic generation from the surface optical nonlinearity is verified experimentally.

Higher-Dimensional Hong-OuMandel Effect with Linear-Optical
Grover Multiports∙A. Sergienko1 , D. Simon2 , S.
Osawa1 , and C. Schwarze1 ; 1 Boston
University, Boston, USA; 2 Stonehill
College, Easton, USA
We expand traditional two-photon
Hong-Ou-Mandel (HOM) effectonto a higher-dimensional set of
spatial modes and introduce aquantum network switch providing
controllable
redistributionofentangled states over four modes
using
directionallyunbiasedlinear-optical Grover four-ports.

CE-7.3 THU

EB-13.4 THU

16:45

Z-scan Measurements on nonlinear absorption and refractionof physical vapor depositiongrown Cr2 Te3 at a wavelength of1560 nm∙K. Lee1 , I.H. Lee2,3 , Y.G. Kim2,3 ,S.-y. Kwon1 , G. Lim1 , J. Jung1 ,Y.J. Chang2,3 , and J.H. Lee1 ;1School of Electrical and Computer
Engineering, Seoul, South Korea;
2
Department of Physics, Seoul,
South Korea; 3 Department of Smart
Cities, Seoul, South Korea
Z-scan measurements were conducted to investigate the nonlinear optical responses of nanoscalelayered Cr2 Te3 grown by physical vapor deposition. Nonlinear
absorption coefficient and nonlinear refractive index were −(1.91 ±0.08) × 105 cm/GW and −1.63 ± 0.06
cm2 /GW at 1560 nm, respectively..

16:45

Spectrally multimode squeezed
states of light in the telecom bandusing waveguides
V.R. Rodriguez1,2 , ∙D. Fainsin1 , G.L.
Zanin1 , N. Treps1 , E. Diamanti2 ,and V. Parigi1 ; 1 Laboratoire Kastler
Brossel, Sorbonne Université, ENSUniversité PSL, CNRS, Collège deFrance, 4 place Jussieu, Paris, France;
2
Sorbonne Université, LIP6, CNRS, 4
place Jussieu, Paris, France
We present and characterize asource of spectrally multimodesqueezed state of light at telecom
wavelength. The state is made outof a periodically-poled waveguide(PPKTP) pumped by a femtosecond
laser.

CLEO

Room 1 ICM
EA-5.5 THU

Room 4a ICM
17:00

CK-11.5 THU®

/Europe-EQEC 2023

Room 4b ICM
17:00

EH-5.5 THU⋅ Thursday 29 June 2023
Room 13a ICM

17:00

JSIII-2.5 THU

Room 13b ICM
17:00

CB-11.5 THU

Room 14a ICM
17:00

EF-6.5 THU

17:00

An integrated waveguide resonator squeezer for optical networks∙M. Stefszky, M. Santandrea, F. vom
Bruch, V. Quiring, R. Ricken, C.
Eigner, H. Herrmann, and C. Silberhorn; Integrated Quantum Optics,
Institute for Photonic Quantum Systems (PhoQs), Paderborn University,
Paderborn, Germany
In this paper we demonstrate a titanium indiffused lithium niobate
waveguide resonator squeezer using that includes an on-chip electrooptic-modulator for cavity lengthstabilisation. This device is therefore suitable for use in many quantum networks.

Photonic nanostructures for efficient coupling and light enhancement in semiconductor quantum
technologies∙S. Bauer1 , S. Kolatschek1 , F.
Hornung1 , C. Nawrath1 , N. Hoppe2 ,R. Sittig1 , R. Joos1 , P. Vijayan1 , D.
Wang1 , J. Fischer1 , C. Schweikert2 ,N. Witz1,3 , M. Berroth2 , S.L.
Portalupi1 , M. Jetter1 , and P.
Michler1 ; 1 Institut fur Halbleiteroptik und Funktionelle Grenzflächen
(IHFG), Center for Integrated
Quantum Science and Technology(IQST) and SCoPE, 70569 Stuttgart,
Germany; 2 Institute of Electricaland Optical Communications Engineering, 70569 Stuttgart, Germany;
3
Twenty-One
Semiconductors,
72654 Neckartenzlingen, Germany
This work will focus on several photonic nanostructures to enhance theemission properties of semiconductor quantum dots.

The contribution has been withdrawn.

Function enhancement of spatial
photonic Ising machine by parallel processing using space-division multiplexing∙S. Shimomura, K.-i. Okubo, H. Yamashita, Y. Ogura, H. Suzuki, and
J. Tanida; Osaka University, Osaka,Japan
We propose a method for expanding
functions of a spatial photonic Isingmachine by parallel processing using space-division multiplexing.

Design strategies to optimize
660 nm DBR tapered laser performance∙G. Blume, O. Matalla, H. Wenzel, A. Maaßdorf, D. Feise, J. Fricke,
P. Ressel, S. Kreutzmann, A. Ginolas, A. Sahm, A. Knigge, and K.
Paschke; Ferdinand-Braun-Institut(FBH), Berlin, Germany
Tapered diode lasers with internal DBR gratings were developed
for a single mode emission at 660
nm. Their intended use is as pumpsource for SPDC in a miniaturized
quantum OCT scanner system.

Conservative Solitons andReversibility in Time-Delayedmodels for Optical Micro-Cavities
T. Seidel1 , J. Javaloyes2 , and ∙S.
Gurevich1 ; 1 Institute for Theoretical Physics, University of Münster,
Münster, Germany; 2 Departamentde Fisica, Universitat de les Illes
Balears, Palma de Mallorca, Spain
We discuss the existence of reversible conservative time-delayed
systems in a dispersive micro-cavity
with a Kerr medium coupled to an
external mirror. At low energies,
the equivalence with the nonlinear Schrödinger equation is demonstrated.

EA-5.6 THU

CK-11.6 THU

EH-5.6 THU

JSIII-2.6 THU

CB-11.6 THU

EF-6.6 THU

17:15

Atom-mediated Nonlinear
Sources of Quantum Light∙A. Krstić1 ,P. Tiwari1 ,F.
1,2
Setzpfandt , U. Peschel3 , and
S. Saravi1 ; 1 Institute of Applied
Physics, Abbe Center of Photonics, Friedrich-Schiller University
Jena, Jena, Germany; 2 Fraunhofer
Institute for Applied Optics and Precision Engineering, Jena, Germany;3
Institute of Condensed Matter
Theory and Solid State Optics,
Friedrich-Schiller University Jena,
Jena, Germany
We propose a scheme for a hybrid
source of quantum light, consistingof a 2-level emitter embedded ina nonlinear cavity, that can generate multiple-pair number states withsignificantly enhanced probability
compared to conventional sources.

17:15

Extreme Ultraviolet Metaoptics∙M. Ossiander1 , H.K. Hampel2 , M.L.
Meretska1 , S.W.D. Lim1 , N. Knefz2 ,T. Jauk2 , M. Schultze2 , and F.
Capasso1 ; 1 John A. Paulson Schoolof Engineering and Applied Sciences, Harvard University, Cambridge, USA; 2 Institute of Experimental Physics, Graz University ofTechnology, Graz, Austria
We demonstrate the first dielectric
metalens for light with 50 nm wavelength by exploiting that holes in Silicon guide extreme ultraviolet radiation. We experimentally achieve
focusing of high-harmonic radiation down to 1.6 times the diffraction limit.

17:15

Design, Fabrication and Characterization of Double Helical Plasmonic Antennas∙A. Tsarapkin1 , S. Jürgensen2 ,T. Feichtner3 , K. Mackosz4 , V.
Deinhart1 , I. Utke4 , S. Reich2 , andK. Höflich1 ; 1 Ferdinand-BraunInstitut (FBH), Berlin, Germany;
2
Freie Universitat Berlin, Berlin,
Germany; 3 University of Würzburg,
Würzburg, Germany; 4 Empa-Swiss
Federal Laboratories for Materials
Science and Technology, Thun,
Switzerland
A plasmonic double nano-helix canact as a sensitive antenna for circularly polarised light. In this work weanalyse its excitation mechanism,
fabrication by direct electron beam
writing, and optical characterisation.

17:15

Time-Multiplexed Photonic
Reservoir Computer for Recognition of Human Actions in Videos∙E. Picco1 , P. Antonik2 , and S.
Massar1 ; 1 Laboratoire d’Information
Quantique, CP 224, Université Libre de Bruxelles, Brussels, Belgium;
2
MICS EA-4037 Laboratory, CentraleSupélec, F-91192 Gif-sur-Yvette,
France, Gif-sur-Yvette, France
We demonstrate the use of a photonic reservoir computer based ontime-multiplexing for the classification of human actions in videos.
Our fast and low complexity system
has classification error comparable
to state-of-the-art Machine Learning algorithms.

168

17:15

High optical confinement green
SLEDs and LDs with InAlN
claddings∙M. Malinverni, A. Castiglia, M.
Rossetti, A. Ferhatovic, D. Martin,
M. Duelk, and C. Velez; Exalos AG,
Schlieren, Switzerland
AlInGaN-based SLEDs and LDs
emitting above 510nm with a bottom n-type InAlN cladding aredemonstrated with increased opticalconfinement and improved performance with respect to conventional
AlGaN cladding based devices.

17:15

Frequency Combs and Photonic
SnakesS.
Benadouda
Ivars1,2 ,Y.
3,4
Kartashov ,P.
Fernández
de Córdoba1 , J.A. Conejero1 ,L. Torner3,5 , and ∙C. Milián
Enrique1 ; 1 Institut Universitaryde Matemàtica Pura i Aplicada,2
València,
Spain;
Universitat
Politècnica de Catalunya, Terrassa,
3
Spain;
ICFO, The Barcelona
Institute of Science and Technology,
Barcelona, Spain; 4 Institute ofSpectroscopy, Russian Academyof Sciences, Troitsk, Moscow,
Russia; 5 Universitat Politècnica deCatalunya, Bareclona, Spain
We present a new type of stable nonlinear wave featuring twodimensional zigzags, which we term
Photonic Snakes.
These represent the unprecedented arrest of thesnake instability and naturally form
two-dimensional frequency combs
in cylindrical microresonators.

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Room 14b ICM
CH-12.5 THU

Room Osterseen ICM
17:00

CL-4.5 THU

17:00

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/Europe-EQEC 2023

Room 1 Hall B1 (B11)CC-3.5 THU⋅ Thursday 29 June 2023
Room 6 Hall B3 (B32)

17:00

CG-6.4 THU

17:00

Plasmonic Nano-aperture Labelfree Imaging for Nano-Biosensing
S. Mallick and ∙W.-C. Shih; University of Houston, Houston, USA
We demonstrate ultra near-field
index
modulated
PlAsmonic
NanO-apeRture lAbel-free iMAging (PANORAMA) that addresses
existing issues for both SPR and
LSPR imaging techniques, andshow its applicability for transparent nanoparticles and extracellular
vesicles, e.g., exosomes.

Design of an optical bench forpolychromatic characterisation ofadvanced intraocular lens designs
with spatial light modulator∙V.
Gonzalez-Fernandez1 ,S.
Fernandez-Nuñez1 , N. Garzon2 ,M. García-Montero2 , C. AlbarránDiego3 , and J.A. Gomez-Pedrero1 ;1
Dpto.de Optica,
Universidad
Complutense de Madrid, Madrid,2
Spain; Dpto. de Optometría yVisión, Universidad Complutense de
Madrid, Madrid, Spain; 3 Dpto. deÓptica y Optometría y Ciencias dela Visión, Universitat de València,
Burjassot, Spain
We propose the design of an optical bench system to measure thepoint spread function of advanced
designs of intraocular diffractive
lenses through focus, to characterize
the extended focus and its chromaticaberration

Giant Core-Shell Plasmonic
Enhancement of Spintronic
Terahertz Emission∙V. Cecconi1,2 , Y. Tian1 , L. Peters1,2 ,L. Olivieri1,2 , A. Cutrona1,2 , J.S.
Totero Gongora1,2 , A. Pasquazi1,2 ,and M. Peccianti1,2 ; 1 University of
Sussex, Brighton, United Kingdom;2
Loughborough University, Loughborough, United Kingdom
Wedemonstrateorders-ofmagnitude local enhancement ofterahertz emission from a spintronic stack driven by plasmonicenhanced optical coupling andultrafast heating supported by asparse core-shell nanoparticle layer.

Attosecond-pump attosecondprobe spectroscopy at kHz
repetition rate
M. Kretschmar, E. Svirplys, T. Nagy,
M.J.J. Vrakking, and ∙B. Schütte;Max-Born-Institut, Berlin, Germany
Attosecond-pumpattosecondprobe spectroscopy is demonstrated
for the first time at kHz repetition
rates. Using a commercial laser anda compact setup, sequential twophoton absorption is demonstrated
in a two-color pump-probe scheme.

CH-12.6 THU

CL-4.6 THU

CC-3.6 THU

CG-6.5 THU

17:15

Super-Resolution Multipole
Decomposition Tomographic
Microscopy∙T. Chang1 , J.-K. So1 , E.A. Chan1 ,G. Adamo1 , N. Papasimakis2 , Y.
Shen2 , and N.I. Zheludev1,2 ; 1 Centre
for Disruptive Photonic Technologies,
SPMS and TPI, Nanyang Technological University, Singapore, Singapore; 2 Optoelectronics Research Centre and Centre for Photonic Metamaterials, University of Southampton,
Southampton, United Kingdom
Super-resolution imaging techniquethat overcomes the quantitative lightdetection accuracy limit is proposed. The spatial separation ofa weaker multipole radiation mode
from stronger modes followed bysuccessive measurements of thosecoefficients is the key.

17:15

High Numerical Aperture ZrO2
Holographic Metasurfaces for
Biophotonics Applications∙M. Biabanifard, T. Plaskocinski, J.
Xiao, and A. Di Falco; Universityof St Andrews, St Andrews, United
Kingdom
We present the realization of ZrO2
holographic metasurfaces. We discuss critically the advantages andlimitations of the platform anddemonstrate its use as a replacement
for high numerical aperture objectives for integrated optical trapping
applications.

17:15

0.8 mW of 10 – 39 THz mid-IR
radiation generated in GaSe with
an amplified Kerr-lens modelocked Cr:ZnS oscillator∙J.G. Meyer and O. Pronin; HelmutSchmidt-University, Hamburg, Germany
With an amplified Cr:ZnS oscillator
we generate via IDFG 0.8 mW of radiation from 10 to 39 THz (7.7 – 30μm). It represents a coherent lightsource for broadband spectroscopy
deep in the mid-IR region.

17:15

A Polarization Insensitive Femtosecond Enhancement Cavity for
Photoelectron Tomography at
100 MHz Repetition Rate
∙J.-H. Oelmann1,2 , T. Heldt1,2 ,L. Guth1,2 , N. Lackmann1 , V.
Wössner1 , S. Kokh1 , J. Nauta1,3 ,T. Pfeifer1 , and J.R. Crespo LópezUrrutia1 ; 1 Max-Planck-Institut fürKernphysik, Heidelberg, Germany;2
Heidelberg Graduate School for
Physics, Heidelberg, Germany;3
Current address:
Departmentof Physics, College of Science,
Swansea University,
Swansea,
United Kingdom
We present a novel polarization
insensitive enhancement cavity
for multi-photon ionization experiments at high laser intensity.
Combined with a compact intracavity velocity-map imaging (VMI)
spectrometer, the setup enables
photoelectron
tomography
at
100 MHz repetition rate.

169

Room 7 Hall A1 (A11)
CE-7.4 THU

17:00

Shaping the nonlinear response ofsilica single-mode fibers withnanodiamonds volumetricallyintegrated in the core
G. Stȩpniewski1,2 , P. Hänzi3 ,T. Kardaś4 , S. Łukasik1 , Y.
Stepanenko5 , M. Głowacki6 , V.
Romano3 , R. Buczyński1,2 , R.
Bogdanowicz6 , A.M. Heidt3 , and∙M. Klimczak1 ; 1 University of
Warsaw, Faculty of Physics, Warsaw,
Poland; 2 Łukasiewicz Research Network, Institute of Microelectronics
and Photonics, Warsaw, Poland;
3
University of Bern, Institute ofApplied Physics, Bern, Switzerland;
4
Fluence Sp. z o.o., Warsaw, Poland;5Institute of Physical Chemistry,
Polish Academy of Sciences, Warsaw, Poland; 6 Gdańsk Universityof Technology, Faculty of Electronics, Telecommunications andInformatics, Gdańsk, Poland
Negative nonlinearity fibers could
open currently inaccessible regimes
in ultrafast optics. Nonlinearity
shaping in silica fibers is investigated by introducing nanodiamonds
into the fiber core using tetraethyl
orthosilicate hydrolysis, followed byz-scan and XFROG measurements.
CE-7.5 THU

17:15

ICP-CVD Silicon-rich silicon
nitride for supercontinuum
generation∙A. Jayantha, A. Andrieux, I. Gallet,
C. Finot, and K. Hammani; Laboratoire ICB, CNRS/uB, Dijon 21000,
FranceWe report the fabrication of ICPCVD silicon-rich silicon nitride
having a refractive index of 2.44 attelecommunications wavelength.
The nonlinear properties of thematerial allow the demonstration ofa supercontinuum.

Room 8 Hall A1 (A12)
EB-13.5 THU

17:00

Universal Photonic Quantum
Gate by Cooper-pair-based
Optical Nonlinearity∙S. Bouscher and A. Hayat; Department of Electrical Engineering, Technion, Haifa, Israel
We propose a new concept of
Cooper-pair-nonlinearity-based
photonic
universal
SWAP(ϕ)quantum gates. Phase is added
only to the Ψ+ Bell-state throughtwo-photon nonlinearity inducedby the superconducting state.

EB-13.6 THU

17:15

Pulsed approach to reservoir
computing towards quantum
protocols∙J. Henaff, M. Ansquer, F. Sansavini,
N. Treps, and V. Parigi; Sorbonne
Université, Paris, France
Our work aims at the implementation of quantum enhanced machinelearning protocols in a Continuous
Variables photonics platform. It focuses on the implementation of protocols based on network structures,
like quantum reservoir computing,
via multimode quantum optics.

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/Europe-EQEC 2023

Room 13a ICM
17:45 – 19:15
PD-1: Postdeadline session I: Beam and pulse
control and quantum physics
Chair: Daniele Brida, Université du Luxembourg, LuxembourgPD-1.1 THU

17:45

Gigawatt-Scale Acousto-Optic Modulation in
Ambient Air∙Y. Schrödel1 , C. Hartmann2 , T. Lang1 , J. Zheng1 , M.
Steudel3 , M. Rutsch2 , S.H. Salman1,4,5 , M. Kellert6 , M.
Pergament6 , T. Hahn-Jose7 , S. Suppelt2 , J.H. Dörsam2 ,A. Harth3 , W.P. Leemans1,8 , F.X. Kärtner6,8,9 , I. Hartl1 ,M. Kupnik2 , and C.M. Heyl1,4,5 ; 1 Deutsches ElektronenSynchrotron DESY, Hamburg, Germany; 2 Technische
Universitat Darmstadt, Measurement and Sensor Technology, Darmstadt, Germany; 3 Hochschule Aalen, Department of Optics and Mechatronics, Aalen, Germany; 4 Helmholtz-Institute Jena, Jena, Germany; 5 GSI
Helmholtzzentrum fur Schwerionenforschung GmbH,
Darmstadt, Germany; 6 Center for Free-Electron Laser
Science CFELL, Deutsches Elektronen-Synchrotron DESY,
Hamburg, Germany; 7 INOSON GmbH, St. Ingbert, Germany; 8 University of Hamburg, Department of Physics,
Hamburg, Germany; 9 The Hamburg Centre for Ultrafast
Imaging, Hamburg, Germany
We employ intense ultrasound fields in gases enabling
us to control laser light in extreme parameter ranges,
acousto-optically modulating 1030 nm ultrashort pulses
with peak power of 20 GW efficiently (> 50%) in ambientair.
PD-1.2 THU

Quantum Optics, Garching, Germany; Institute of Applied Physics, Friedrich Schiller University Jena, Jena, Germany; 6 Fraunhofer Inst. for App. Opt. and Prec. Eng.,
Centre of Excellence in Photonics, Jena, Germany
We present an on-chip scanning CEP probe for on-air,single-beam measuring of 3D CEP maps of nJ-class fewcycle laser beam focus. We achieved a proof-of-concept
sculpting of CEP distributions using an SLM-feedback
loop.
5

17:55

On-Chip, On-Air Carrier-Envelope Phase Detector ofnJ-Level Laser Pulses and Spatial CEP Sculpting∙V. Hanus1 , B. Fehér1 , V. Csajbók1 , P. Sándor1 , Z. Pápa1,2 ,J. Budai2 , Z. Wang3,4 , P. Paul5,6 , A. Szeghalmi5,6 , and
P. Dombi1,2 ; 1 Wigner Research Centre for Physics, Budapest, Hungary; 2 ELI-ALPS Research Institute, Szeged,
Hungary; 3 Physics Department, Ludwig-MaximiliansUniversität, Munich, Germany; 4 Max Planck Institute of

We present a dual-oscillator-based field-resolved midinfrared spectrometer with individual-scan referencing.
The system acquires electro-optic sampling traces at4200 scans/s with octave-spanning mid-infrared coverage and can correct the mid-infrared excitation-pulse
fluctuations on the individual-scan level.
PD-1.5 THU

18:25

Single-Shot, High-Repetition Rate Carrier-EnvelopePhase Detection via optical Fourier transform∙C. Guo1 , M. Miranda2,3 , A.-K. Raab1 , A.-L. Viotti1 , P.T.
Guerreiro2,3 , R. Romero2,3 , H. Crespo2,3 , A. L’Huillier2,3 ,and C.L. Arnold2,3 ; 1 Department of Physics, Lund University, Lund, Sweden; 2 IFIMUP-IN and Departamentode Física e Astronomia, Universidade do Porto, Porto, Portugal; 3 Sphere Ultrafast Photonics, Porto, Portugal
We propose a single-shot Carrier-Envelope Phase measurement scheme, based on detecting f-2f fringes using
optical Fourier transform. This method is capable forhigh-repetition rate (>200 kHz) and low pulse energy
lasers.

Surprise in Highly Correlated Two-Electron System:
Extended Secondary Plateau in X-ray High Harmonic
Generation from Helium Due to Double Electron
Recombination
S. Wang1 , J. Yan1 , A. de las Heras2 , S. Song1 , A.
Prodanov1 , Z. Wu1 , C. Hernández-García2 , L. Plaja2 , D.
Popmintchev3 , and ∙T. Popmintchev1,3 ; 1 Department of
Physics, Center for Advanced Nanoscience, University ofCalifornia San Diego, La Jolla, USA; 2 Departamento deFísica Aplicada, Universidad de Salamanca, Salamanca,
Spain; 3 Photonic Institute, TU Wien, Vienna, Austria
We observe experimentally a secondary plateau in UVdriven high-harmonic generation in the X-ray regime
extending up to 300 eV, due to emission of a single X-ray
photon at double-recombination of highly-correlated
electrons of helium atoms.

PD-1.4 THU

PD-1.6 THU

PD-1.3 THU

18:05

18:15

Dual-Oscillator Field-Resolved Infrared Spectroscopy with Individual-Scan Referencing∙A. Maity1,2,3 , W. Schweinberger1,2,3 , C. Hofer1,2,3 ,S. Hutter4 , S. Gröbmeyer2 , D. Potamianos1,2,3 ,M. Trubetskov1 , H. Heydarian1 , M. Huber1,2 , M.
Kowalczyk1,2,3 , P. Steinleitner1 , Z. Wei 1,2 , A.
Leitenstorfer4 , I. Pupeza1,2,5 , F. Krausz1,2,3 , and A.
Weigel1,2,3 ; 1 Max-Planck-Institut of Quantum Optics,
Garching, Germany; 2 Ludwig-Maximilians-Universität
München, Garching, Germany; 3 Center for MolecularFingerprinting, Budapest, Hungary; 4 Department of
Physics and Center for Applied Photonics, University ofKonstanz, Germany; 5 Leibniz Institute of Photonic Technology – Member of research alliance “Leibniz HealthTechnologies”, Jena, Germany

18:35

Watt-class CMOS-compatible power amplifier∙N. Singh1 , J. Lorenzen1 , M. Sinobad1 , K. Wang2 ,M. Gaafar1 , H. Francis3 , M. Geiselmann3 , T. Herr1 ,S. Garcia-Blanco2 , and F. Kaertner1 ; 1 Deutsches
Elektronen-Synchrotron DESY, Hamburg, Germany;
2
University of Twente, Twente, Netherlands; 3 Ligentec,
Ecublens, Switzerland
We demonstrate in silicon photonics watt-class large
mode area power amplifier in a compact 3.6mm2 footprint. The output average power reached >0.9 W with
14.5 dB net gain around the signal wavelength of 1.85um.
PD-1.7 THU

18:45

Nanophotonic on-chip electron acceleration∙R. Shiloh, T. Chlouba, S. Kraus, L. Brückner, J. Litzel,

and P. Hommelhoff ; Physics Department, FriedrichAlexander-Universität
Erlangen-Nürnberg(FAU),
Staudtstraße 1, Erlangen, Germany
We experimentally demonstrate electron energy gainof 12.3keV on-chip using a 2μm femtosecond laserand 500μm-long silicon structure. Combined with ananophotonic nearfield confinement scheme, this represents a milestone in the miniaturization of electron accelerators.
PD-1.8 THU

18:55

Bose-Einstein Condensation of Photons in a FourSite Lattice Potential∙A. Redmann, N. Wolf, F. Vewinger, J. Schmitt, and M.
Weitz; Institute of Applied Physics, University of Bonn,
Wegelerstr.8, D-53115 Bonn, Germany
We have demonstrated Bose-Einstein condensation ofphotons into the ground state of a coupled four-site lattice potential. Both Bose-Einstein distributed spectra as
well as fringe signals upon recombination, showing thecoherence between wells, are observed.
PD-1.9 THU

19:05

Continuously Sustained Bose-Einstein Photon
Condensate in a Semiconductor Quantum Well OpenMicrocavity∙R.C. Schofield1 , M. Fu1 , E. Clarke2 , I. Farrer2 , H. Dhar3 ,R. Mukherjee4 , J. Heffernan2 , F. Mintert1 , R.A. Nyman1 ,and R.F. Oulton1 ; 1 Blackett Laboratory, Imperial College London, London, United Kingdom; 2 EPSRC National
Centre for III-V Technologies, University of Sheffield,
Sheffield, United Kingdom; 3 Department of Physics, Indian Institute of Technology, Bombay, India; 4 Zentrum
fur Optische Quantentechnologien, Universitat Hamburg,
Hambury, Germany
We present the observation of photon Bose-Einsteincondensation in a microcavity using thermalisation in asingle semiconductor quantum well. This enables a continuous condensate to be sustained for the first time withstrong photon-photon interactions.

Room 13b ICM
17:45 – 19:15

PD-2.1 THU

PD-2: Postdeadline session II: Nonlinear effects and electron physics

Ultra-low repetition rate frequency comb for
precision spectroscopy
F. Canella1,2,3 , J. Weitenberg2,4 , P. Dwivedi2,5 , F. Schmid2 ,G. Galzerano3 , T.W. Hänsch2,5 , T. Udem2,5 , and ∙A.
Ozawa2 ; 1 Dipartimento di Fisica, Politecnico di Milano, Milan, Italy; 2 Max-Planck-Institut für Quantenoptik, Garching, Germany; 3 Istituto di Fotonica e Nanotecnologie, Consiglio Nazionale delle Ricerche, Milan,

Chair: Crina Cojocaru, Universitat Politecnica deCatalunya, Barcelona, Spain

17:45

Italy; 4 Fraunhofer-Institut für Lasertechnik ILT, Aachen,
Germany; 5 Fakultät für Physik, Ludwig-MaximiliansUniversität München, München, Germany
We demonstrated a low-noise optical frequency combwith a 40 kHz repetition rate. Low repetition rate opticalfrequency combs are suitable for driving non-linear frequency conversion processes to perform precision spectroscopy at extreme ultraviolet wavelengths.

170PD-2.2 THU

17:55

Unexpected phase-locked Brillouin Kerr Frequency
comb in fiber Fabry Perot resonators∙T. Bunel1 , M. Conforti1 , J. Lumeau2 , A. Moreau2 , A.
Fernandez3 , O. Llopis3 , J. Roul3 , A. Perego4 , and A.
Mussot1 ; 1 Universite de Lille, CNRS, UMR 8523-PhLAM,
Villeneuve d’Ascq, France; 2 LAAS-CNRS, Universite deToulouse, CNRS, Toulouse, France; 3 Aix Marseille Univ,
CNRS, Centrale Marseille, Institut Fresnel, Marseille,

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/Europe-EQEC 2023

Room 13b ICM
France; Aston Institute of Photonic Technologies, Aston
University,, Birmingham, United Kingdom
We report the observation of a stable and broadband optical frequency comb in a high-Q fiber Fabry Perot resonator. We evidence it arises from an unexpected modelocking phenomena.
4PD-2.3 THU

18:05

Modifying the speed of light in vacuum with intenselaser pulses: The DeLLight Experiment∙A.E. Kraych1 , M. Mailliet1 , S. Robertson1,2 , F.
Couchot1,2 , and X. Sarazin1 ; 1 Université Paris-Saclay,
CNRS/IN2P3, IJCLab, Orsay, France; 2 Université ParisSaclay, Institut d’Optique Graduate School, CNRS,
Laboratoire Charles Fabry, Palaiseau, France
The DeLLight (deflection of light by light) experiment
aims to observe the optically induced index change ofvacuum, a nonlinear effect predicts by the Quantum
electrodynamics theory which has never been explored.
PD-2.4 THU

18:15

Quantum Optical Tomography using a TimeResolved and Mode-Selective Frequency-UpConversion Detector∙N. Namekata1 , N. Kobayashi2 , K. Nomura3 , T. Sako3 , N.

Takata , and S. Inoue ; Institute of Quantum Science,
Nihon University, Tokyo, Japan; 2 Department of Precision Machinery Engineering, College of Science and Technology, Nihon University, Chiba, Japan; 3 Laboratory ofPhysics, College of Science and Technology, Nihon University, Chiba, Japan; 4 Division of Brain Science, Institutefor Advanced Medical Research, Keio University School of
Medicine, Tokyo, JapanA 111-dB-sensitivity time-of-flight measurement system was developed to acquire a tomographic image ofa mouse brain using an mode-selective frequency upconversion single-photon detector.
4

1 1

PD-2.5 THU

18:25

The contribution has been withdrawn.
PD-2.6 THU

18:35

Co-levitation of an ultra-high-Q nanomechanicaloscillator and an atomic qubit∙D.S. Bykov1 , L. Dania1 , F. Goschin1 , M. Teller1,2 , andT.E. Northup1 ; 1 Institut für Experimentalphysik, Universität Innsbruck, Technikerstraße 25, 6020, Innsbruck,
Austria; 2 ICFO-Institut de Ciencies Fotoniques, The
Barcelona Institute of Science and Technology, 08860,
Castelldefels (Barcelona), Spain

We co-trap a nanoparticle and a calcium ion in the same
Paul trap. We use a dual-frequency trap drive to achieve
stable confinement of the particles, whose charge-tomass ratios differ by six orders of magnitude.
PD-2.7 THU

18:45

Observation of polarization Faticons in a fibre Kerr
resonator∙J. Fatome1,4 , E. Lucas1 , B. Kibler1 , L. Hill2,3 , G.-L.
Oppo2 , G. Xu4 , S.G. Murdoch4 , M. Erkintalo4 , and
S. Coen4 ; 1 Université de Bourgogne, Dijon, France;
2
University of Strathclyde, Glasgow, United Kingdom;3
Max Planck Institute for the Science of Light, Erlangen,Germany; 4 The University of Auckland, Auckland, New
Zealand
We report on the first experimental observation of a new
type of localized vectorial structure in normal dispersion, coherently-driven, fiber Kerr resonators, namely,
the temporal polarization faticon
PD-2.8 THU

18:55

Spontaneous Parametric Down-Conversion Beamingfrom a Lithium Niobate Nanostructured Resonator∙M. Celebrano1 , A. Zilli1 , V. Sultanov2,3 , M. Poloczek1,3 ,M. Ferrera4 , Y. Luan1 , E. Kokkinakis2 , T. SantiagoCruz2,3 , L. Carletti5 , A. Toma4 , M. Finazzi1 , and

M. Chekhova2,3 ; 1 Dipartimento di Fisica, Politecnico
di Milano, Milano, Italy; 2 Max Planck Institute for
the Science of Light, Erlangen, Germany; 3 FriedrichAlexander Universitat Erlangen-Nurnberg, Erlangen,Germany; 4 Istituto Italiano di Tecnologia, Genova, Italy;
5
Department of Information Engineering, Università di
Brescia and INO-CNR, Brescia, Italy
We report the design and fabrication of lithium niobate nanostructured resonators for directional beamingof spontaneous parametric down-conversion. Preliminary measurements achieved photon-pair production
rates exceeding 100 Hz/W at telecom wavelengths
PD-2.9 THU

19:05

Coherent Nonlinear Up-Conversion Imaging with
High-Q Metasurfaces∙L.D. Valencia Molina1,2 , R. Camacho Morales 1 , J.
Zhang1 , I. Staude2 , A.A. Sukhorukov1 , and D. Neshev1 ;1Australian National University, Canberra, Australia;
2
Friedrich Schiller University Jena, Jena, Germany
We demonstrate efficient upconversion imaging enabled
by high-Q bound-state-in-the-continuum resonances inlithium niobate metasurfaces. We demonstrate coherent
wavefront conversion in the Fourier plane of the opticalsystem despite the nonlocal character of the metasurface.

Hall B0
13:00 – 14:00
CE-P: CE Poster session
CE-P.1 THU

Plasmon-driven Photochemistry for Metallic Nanopore Arrays Fabrication
G. Lanzavecchia1 , J. Kuttruff2 , A. Doricchi1 , A. Viejo
Rodríguez3 , R. Krahne1 , ∙N. Maccaferri4 , and D. Garoli1 ;1Istituto Italiano di Tecnologia, Genova, Italy; 2 Universityof Konstanz, Konstanz, Germany; 3 University of Luxembourg, Luxembourg, Luxembourg; 4 Umeå University &Umeå Centre for Microbial Research, Umeå, Sweden
We show a process for the fabrication of nanopores
arrays via photocatalysis triggered by electromagnetic
field enhancement in plasmonic structures immersed inmetallic salt solutions and generating hotspots causing
pore diameter reduction below 5 nm.
CE-P.2 THU

Low-temperature and hydrogen-free silicon dioxidecladding for next-generation integrated photonics
Z. Li1,2 , ∙Z. Qiu1,2 , R.N. Wang1,2 , M. Divall1,2 , and T.
Kippenberg1,2 ; 1 Swiss Federal Institute of Technology Lausanne (EPFL), Lausanne, Switzerland; 2 Center for Quan-tum Science and Engineering, EPFL, Lausanne, Switzerland
We demonstrate a hydrogen-free low-loss silicon dioxide
film deposited with SiCl4 for cladding of photonic integrated circuits. A very wide low-loss window of 1260 nm
to 1625 nm is achieved at deposition temperature as low
as 300 ∘ C.
CE-P.3 THU

Laser-Assisted Bonding Prototype Equipment for
Hybrid Integration of Silicon Photonic Circuits∙A. Vlasov, T. Uusitalo, E. Lepukhov, H. Virtanen, S.-P.
Ojanen, J. Viheriälä, and M. Guina; Tampere University,
Physics Unit, Optoelectronic Research Centre, Korkeakoulunkatu 3, Tampere, FI-33720, Finland, Tampere, FinlandHybrid integration on silicon substrate is promising way
towards increased density and enhanced functionality.
We introduce the self-developed laser-assisted bonding setup with bottom coaxial irradiation architecture,
which combines the bonding beam delivery and microscopy channels.

CE-P.4 THU

CE-P.6 THU

Hybrid strip-loaded silicon rich nitride-thin filmlithium niobate waveguides for PIC applications∙T.S. Meetei1 , S.-J. Son1 , B. Park1 , Y.-T. Lee1 , andN.E. Yu1,2 ; 1 Advanced Photonics Research Institute,Gwangju Institute of Science and Technology, South Korea; 2 Research Centre for Photon Science and Technology,
Gwangju Institute of Science and Technology, South Korea
We investigate the mode properties of a strip-loaded
silicon-rich nitride and thin-film lithium-niobate hybrid waveguides at 1550 nm. The mode profiles of
TE0 and TM0 satisfying simultaneous single-modecondition and zero-birefringence are discussed for PIC
applications.

Three-photon and Four-photon Absorption in
Lithium Niobate and Lithium Tantalate by Z-scan
Technique∙I. Benabdelghani1,2 , G. Tóth1,2,3 , G. Krizsán1,2,3 , N.
Mbithi1,2,4 , G. Bazsó5 , P. Rácz5 , P. Dombi5 , J. Hebling1,2,3 ,and G. Polónyi1,3 ; 1 Szentágothai Research Centre, Pécs,
Hungary; 2 University of Pécs, Pécs, Hungary; 3 ELKHPTE High Intensity Terahertz Research Group, Pécs, Hungary; 4 Garissa University, Garissa, Kenya; 5 Wigner Research Centre for Physics, Budapest, Hungary
Intensity dependent three-photon and four-photon absorption of stoichiometric and congruent lithium niobate and lithium tantalate have been determined by zscan technique for ordinary and extraordinary polarization states.

CE-P.5 THU

Spectroscopic investigation of Tm3+-Dy3+ co-doped
KY3F10 crystals for 3 μm laser applications∙F. Canbaz1 and A. Butkus2 ; 1 University of Basel, Basel,
Switzerland; 2 Optogama UAB, Vilnius, Lithuania
Emission characteristics of Tm3+-Dy3+:KY3F10 withvarious concentration combinations are investigated at
the excitation wavelength of 1645nm. 3-μm emission
is obtained when Tm3+ is present in the crystal matrix,
suggesting successful energy transfer between the ions.

171

CE-P.7 THU

Estimation of photo-elastic coefficients in ionexchanged borosilicate glass cavities throughwhispering gallery mode resonation∙N. Kokkinidis1,2 , N. Korakas1,2 , and S. Pissadakis2 ;1
University of Crete, Heraklion, Greece; 2 Institute ofElectronic Structure and Laser (IESL), Foundation for

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Research and Technology-Hellas (FORTH), Heraklion,
GreeceWhispering gallery mode resonation is used for estimating the Pockels’ coefficients in pristine and potassium
ion-exchanged borosilicate glass cylindrical cavities, incorrelation with Young modulus measurements; the ionexchange process glass significantly affects borosilicate
glass photoelasticity.
CE-P.8 THU

Polarization Characteristics of Raman Scattering in
KGW Raman Laser Crystals by Polarized Incident
Light∙J.-C. Tung, S.-C. Chen, and M.-H. Hou; Department ofElectro-Optical Engineering, National Taipei University ofTechnology, Taipei, Taiwan
Np-cut potassium gadolinium tungstate (KGW) crystals
were demonstrated to excite scattered light under polarized incident light, exhibiting the unique properties ofangle-resolved polarized Raman spectroscopy and Raman intensity polar plots.
CE-P.9 THU

Extensive study of magneto-optical and optical properties of Cd1–xMnxTe between 675 nm and 1025 nm∙C. Tyborski, M.T. Hassan, M. Schiemangk, T. Flisgen,and A. Wicht; Ferdinand-Braun-Institut gGmbH, Berlin,
Germany
We show wavelength-dependent measurements of Faraday rotations and reflection/transmission values for various stoichiometric ratios of Cd1−x Mnx Te. From the data
we derive Verdet constants and absorption coefficients
helping to design miniaturized optical isolators.
CE-P.10 THU

Effects of Low-Temperature Annealing on CsPbBr3
Thin-Films by Ultrafast THz Spectroscopy∙L. Gatto1,2 , A. Treglia1,3 , G. Crippa1,2 , M. Devetta2 , G.
Folpini3 , A. Petrozza3 , S. Stagira1,2 , C. Vozzi2 , and E.
Cinquanta2 ; 1 Dipartimento di Fisica, Politecnico di Milano, Milano, Italy; 2 Istituto di Fotonica e Nanotecnologie,
CNR, Milano, Italy; 3 Center for NanoScience and Technology, IIT, Milano, Italy
We employed ultrafast terahertz spectroscopy to assess
the effects of low-temperature annealing on CsPbBr3
perovskite thin-films. We found counterintuitively faster
dynamics and lower photoluminescence after the annealing, suggesting the unexpected formation of nonradiative recombination channels.
CE-P.11 THU

Au nanoparticle doped metal-free perovskites∙A. Adappattu Ramachandran1 , H.C. Leo Tsui1 , P.
Docampo2 , and N. Healy1 ; 1 School of Mathematics,

Statistics and Physics, Newcastle University, United Kingdom, Newcastle Upon Tyne, NE1 7RU, United Kingdom;
2
School of Chemistry, University of Glasgow, Glasgow,
G12 8QQ, United Kingdom
We present the influence of gold nanoparticles (Au NPs)on the photoluminescence and non-linear optical properties of metal-free perovskites. The surface plasmon
resonance effect results in the enhancement of photoluminescence and second harmonic generation.
CE-P.12 THU

Nonlinear Optical Characterization of LiNb1−x Tax O3
Solid Solution Nanoparticles: The Influence of Zero
Birefringence∙J. Klenen1,2 , L. Vittadello1,2 , F. Kodde1,2 , V. Hreb3 ,V. Sydorchuk5 , U. Yakhnevych3 , D. Sugak3,4 , and M.
Imlau1,2 ; 1 Department of Physics, Osnabrueck University, 49076 Osnabrueck, Germany; 2 Research Centerfor Cellular Nanoanalytics, Osnabrueck (CellNanOs),
Osnabrueck University, 49076 Osnabrueck, Germany;
3
Department of Semiconductor Electronics, Lviv Polytechnic National University, 79013 Lviv, Ukraine; 4 Scientific
Research Company ‘Electron-Carat’, 79031 Lviv, Ukraine;
5
Institute for Sorption and Problems of Endoecology,
NASU, 03164 Kyiv, Ukraine
We present a comprehensive study of the nonlinear optical properties of nanocrystalline LiNb1−x Tax O3 solid
solutions with the goal to inspect the influence of zero
birefringence on the mechanisms of second and third
harmonic generation.
CE-P.13 THU

Potassium tantalate-niobate for electro-opticallydriven adiabatic frequency conversion∙A. Mrokon1 , L. Kirste2 , K. Buse1,3 , and I. Breunig1,3 ;1Laboratory for Optical Systems, Department of Microsystems Engineering - IMTEK, University of Freiburg,
Georges-Koehler-Allee 102, 79110 Freiburg, Germany;
2
Fraunhofer Institute for Applied Solid State Physics(IAF), Tullastrasse 72, 79108 Freiburg, Germany;
3
Fraunhofer Institute for Physical Measurement Techniques IPM, Georges-Koehler-Allee 301,, 79110 Freiburg,
Germany
We show how potassium tantalate-niobate crystals pave
the way for more than 100 GHz of mode-hop-free tuning within nanoseconds via electro-optically driven adiabatic frequency conversion. This might outperform
lithium-niobate based devices by orders of magnitude.
CE-P.14 THU

A saturable absorber of ternary low-dimensional
material heterojunction and its application in fiber
lasers∙W. Zhu, Q. Wu, and X. Liu; College of Automation, Nan-jing University of Information Science and Technology,
Nanjing , China
This contribution refers to a saturable absorber preparedby mixing three low-dimensional nanomaterials, and applies it to the fiber laser to check the characteristics of theoutput laser pulse.
CE-P.15 THU

Determination of the Inner Surface Area of 3D Wavelength Scale Structures by Using Angle-resolved
Fourier Image Spectroscopy∙N. Meethale Palakkool1 , M. Taverne1 , D. Rezaie1 , H.
Awachi1 , Y.-S. Chen2 , J.G. Rarity2 , C.-C.K. Huang3 ,and Y.-L.D. Ho1 ; 1 Northumbria University, Newcastle upon Tyne, United Kingdom; 2 University of Bristol,
Bristol, United Kingdom; 3 University of Southampton,
Southampton, United Kingdom
This paper involves optical characterization using
Fourier Image Spectroscopy to determine the inner surface area of 3D wavelength scale structures, with the aimof fabricating 3D electrodes with a large active surfacearea.
CE-P.16 THU

Material characterisation of LPCVD SiN and understanding loss behavior∙C. Cummins1 , B. Pan2,3 , G. Roelkens2,3 , M. Dahlem1 ,S. Saseendran1 , and P. Helin 1 ; 1 imec, Leuven, Belgium,
Belgium; 2 Photonics Research Group, INTEC, Ghent University - imec, Ghent, Ghent, Belgium; 3 Center for Nanoand Biophotonics, Ghent University - imec, Ghent, Ghent,
Belgium
The processing impact on LPCVD SiN waveguide loss
(C-band) is discussed. TOF-SIMS identifies impurities(H, Cl) in the fabricated devices, and we discuss the rationale for the optical losses exhibited from a materials
standpoint.
CE-P.17 THU

Improved photosensitive response of doped silica to a
213 nm pulsed laser using a multi-pass writing
approach∙Q.S. Ahmed, J.W. Field, P.C. Gow, C. Holmes, R.H.S.
Bannerman, P.L. Mennea, C.B.E. Gawith, P.G.R. Smith,and J.C. Gates; Optoelectronics Research Centre, University of Southampton, Southampton, SO17 1BJ, UK,
Southampton, United Kingdom
We report a refractive index change increase of 1.4×10−3
in Ge-doped silica with a 1.6 times higher grating’s
strength when depositing the same total fluence overmultiple passes using a 213 nm laser.

172

CE-P.18 THU

Second and third harmonic generation of millimetersized Zn(3-ptz)2 metal-organic framework crystals∙D. Hidalgo-Rojas2,5 , R. Rojas3 , R. Wheatley1,2 , J.
Enriquez2,4 , J. Garcia-Garfido2,4 , F. Herrera2,4 , D.P.
Singh2,4 , and B. Seifert1,2 ; 1 Facultad de Física, Pontificia Universidad Católica de Chile, Santiago de Chile;
2
Millenium Institute for Research in Optics (MIRO),
ANID, Santiago de Chile; 3 Department of Physics andMaterials Science, University of Luxembourg, Luxembourg; 4 Departamento de Física, Universidad de Santiago
de Chile, Chile; 5 Institute for Biological and Medical Engineering, Pontificia Universidad Católica de Chile, Santiago de Chile
In this work we present for the first time the second andthird harmonic generation of large, i.e., millimeter-sized
non-centrosymmetric Zn(3-ptz)2 MOF crystals, whichhave recently been successfully produced and opticallycharacterized in Chile.
CE-P.19 THU

The period chirp of optical gratings - Theory,
Modeling and Measurement∙F. Bienert, T. Graf, and M. Abdou Ahmed; IFSW - Universität Stuttgart, Stuttgart, Germany
We present the theory, modelling, and measurement of
the period chirp, a detrimental effect emerging from thefabrication of optical gratings when using laser interference lithography (LIL) and scanning beam interference
lithography (SBIL).
CE-P.20 THU

Stochiometric engineering of reconfigurable
photo-ionic chalcogenides for nanophotonic
applications∙A. Elfarash, A. Mandal, and B. Gholipour; University ofAlberta, Edmonton, Canada
We show, using high throughput physical vapor deposition techniques, that photo-ionic amorphous metaldoped chalcogenide semiconductors exhibit a stoichiometrically tunable optical response exhibiting both dielectric and plasmonic stoichiometries with precisely
controllable modulation contrasts.
CE-P.21 THU

Multi-parameter fitting of quantum dot spectroscopy
data using Markov Chain Monte Carlo methods∙P.R. Ramesh1 , A.S. Kulkarni1 , W. Liu1 , J.I. Climente2 ,H.Y. Ramirez3 , A.S. Bracker4 , D. Gammon4 , R.
Zurakowski1 , and M.F. Doty1 ; 1 University of Delaware,
Newark, USA; 2 Universitat Jaume I, Castello, Spain;
3
Universidad Pedagogica y Tecnologica de Colombia,
Boyaca, Colombia; 4 U.S. Naval Research Laboratory,
Washington, USA

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We present a Markov Chain Monte Carlo statisticalmethod for fitting quantum dot spectroscopy data andextracting information about individual energetic parameters, such as the energies of confined quantum
states and the many-body Coulomb interactions.
CE-P.22 THUCharacterisation of NIR Photoluminescenceemission (1250-1450nm) in Nd3+-Sm3+ withfluorotellurite Glasses for Biophotonic Applications∙E. Kumi-Barimah, X. Wang, and A. Jha; School of Chemical and Process Engineering, University of Leeds, Woodhouse Lane, Leeds, LS2 9JT, UK, Leeds, United Kingdom
We report for the first time ultra-broadband NIR photoluminescence emission properties and energy transfer mechanism between Nd3+- Sm3+ ions codoped fluorotellurite glasses under 405 nm and 800 nm excitation
sources
CE-P.23 THU

Dye Integrated Planar Guided Mode Resonators for
Miniature On-chip High-Brightness Source∙S. Gali, D. Rout, V. P, and S.K. Selvaraja; Indian Instituteof Science, Bangalore, India
A 200% amplified-emission and wavelength selective
spectral narrowing from fluorophores integrated engineered silicon nitride metasurface-based on-chip guided
mode resonator. This opens up avenues for efficient control of spontaneous emission towards realizing miniature
CMOS-compatible high-brightness sources.
CE-P.24 THU

Fabry-Pérot Type Thin-Film Electro-Optical Modulator in the λ= 900 nm to 1000 nm Spectral Region∙A.K. Rüsseler1,2 , L. Zhao1,3 , F. Kurth1,3 , J. Matthes2 ,13:00 – 14:00
CG-P: CG Poster session
CG-P.1 THU

Attosecond Optical Spectroscopy of Monocrystalline
Diamond∙G.L. Dolso1 , S.A. Sato2 , N. Di Palo1 , G. Inzani1 ,R. Borrego-Varillas3 , M. Nisoli1,3 , and M. Lucchini1,3 ;1Department of Physics, Politecnico di Milano, Milano,
Italy, Italy; 2 Center for Computational Sciences, University of Tsukuba, Tsukuba, Japan, Japan; 3 Institute for
Photonics and Nanotechnologies, IFN-CNR, Milano, Italy,
Italy
We measured attosecond electron dynamics in singlecrystalline diamond induced by few-femtosecond optical light pulses. Our results, supported by TDDFT sim-

G.-A. Hoffmann , M. Jupé , H.-H. Johannes , W.
Kowalsky1,3 , T. Schwenke1,4 , H. Menzel1,4 , A. Wienke1,2 ,and D. Ristau1,2,5 ; 1 Cluster of Excellence PhoenixD, Leibniz University Hannover, Hannover, Germany; 2 Laser
Zentrum Hannover e.V., Hannover, Germany; 3 Institut
für Hochfrequenztechnik, Technische Universität Braunschweig, Braunschweig, Germany; 4 Institut für Technische Chemie, Technische Universität Braunschweig, Braunschweig, Germany; 5 Institute of Quantum Optics, Leibniz
University Hannover, Hannover, Germany
Integrating a Fabry-Pérot interferometer structure inthin-film optical coatings enables shifting the resonanttransmission peak via refractive index changes of an active spacer layer. Our concept addresses wavelengths below 1000 nm and compact design requirements.
1,2

1,2

1,3

CE-P.25 THU

Sputtered PZT-on-SOI Acousto-Optic Modulator
Using Remote Buffer crystallisation∙S. Suraj, D. Yumnam, and S.K. Selvaraja; Indian Institute of Science, Bangalore, India
We demonstrate remote buffered sputter deposited thinfilm PZT-on-SOI acousto-optic phase modulation at
1550 nm. The measurement shows acousto-optic response up to 1 GHz supported by the simulation.
CE-P.26 THU

Semi-continuous Metal Films with Inhomogeneous
Broadening: Experiment-based Statistical Convoluted Models for Plasmonic Colours
L.J. Prokopeva1 , S. Chowdhury1 , ∙P. Nyga2 , K. Pagadala1 ,J. Simon1 , M.P. Nowak2 , C. Fruhling1 , S. Maćkowski3 , and
A.V. Kildishev1 ; 1 Elmore Family School of Electrical andComputer Engineering and Birck Nanotechnology Center,ulations, validate macroscopic models and identify thecontribution of individual sub-bands to the total opticalresponse.
CG-P.2 THU

Optical levitation of reflective shells using an LG01
vortex beam
∙A.-H. Munj, R. Smith, and W. Kerridge-Johns; Imperial
College, London, United Kingdom
We present optical levitation of reflective silver-coatedglass shells ranging from 53-93μm in diameter, at large
working distances (40-100mm) using a LG01 vortex
laser. Minimum levitation powers ranged from 50mW
to 100mW.

Purdue University, West Lafayette, USA; 2 Institute of Optoelectronics, Military University of Technology, Warsaw,
Poland; 3 Institute of Physics, Nicolaus Copernicus University, Torun, Poland
A new experiment-based model employing convolutionof statistical absorption is used to characterize the optical dispersion of semi-continuous metal films and simulate the nano-structured plasmonic colour coatings in
the time domain.

versité Paris-Saclay, Institut d’Optique Graduate School,
CNRS, Laboratoire Charles Fabry, 91127, Palaiseau,
France, Palaiseau, France
We demonstrate the first laser operation of a LEDpumped Er:Cr:YSGG at 2.79 μm. This luminescent concentrator is also a bright, broadband, incoherent source
at 1.6 μm, overcoming the performance of classicalsources in the SWIR.

CE-P.27 THU

FBGs in PCF for Four-Wave Mixing Sources for
Quantum Optics∙A.I. Flint1 , W.A.M. Smith2 , A.C. Davis2 , R.H.S.
Bannerman1 , P.C. Gow1 , J.C. Gates1 , D.H. Smith3 , P.J.
Mosley2 , and P.G.R. Smith1 ; 1 Optoelectronics ResearchCentre, University of Southampton, Southampton, United
Kingdom; 2 Centre for Photonics and Photonic Materials,
Department of Physics, University of Bath, Bath, United
Kingdom; 3 Quix BV, Enschede, Netherlands
We present the fabrication of fibre Bragg gratings insolid-core photonic crystal fiber using small-spot direct
213nm UV writing. The use of these gratings, as applied
to four-wave mixing sources for quantum optics, is discussed.

The contribution has been withdrawn.
CE-P.28 THU

Method for Separating the Relative Contributions to
the Emission Spectrum of Overlapping Luminescence Bands Presenting Different Dependencies on
the Excitation Power∙L.d.S. Menezes1,2 , J.A.O. Galindo2 , A.R. Pessoa1,2 , Y.E.
Serge-Correales3 , S.J.L. Ribeiro3 , and A.M. Amaral2 ;1Chair in Hybrid Nanosystems, Faculty of Physics,
Ludwig-Maximilians-University Munich, Munich, Germany; 2 Departamento de Física, Universidade Federal
de Pernambuco, Recife-PE, Brazil; 3 Instituto de Química,
Universidade Estadual Paulista, Araraquara-SP, Brazil
In spectroscopy, one often needs to distinguish overlapping luminescent bands. Rather complex procedures arecommonly used. A method is proposed based on different dependencies of luminescent lines with the excitation power at single excitation wavelength.
CE-P.29 THU

LED-pumped Er:Cr:YSGG
L. Lopez, F. Druon, P. Georges, and ∙F. Balembois; Uni-

CG-P.3 THU

First operation phase of the 10 Hz 2 PW laser of ELI
ALPS∙R.S. Nagymihály1 , J. Bohus1 , V. Pajer1 , A. Malakzadeh1 ,L. Lehotai1 , B. Bussiere2 , F. Falcoz2 , M. Ravet-Senkans2 ,O. Roy2 , P.-M. Paul2 , Á. Börzsönyi1 , K. Varjú1 , G. Szabó1 ,and M. Kalashnikov1 ; 1 ELI ALPS Research Institute,
Szeged, Hungary; 2 Amplitude , Evry, France
Performance and operation experiences of the novel 2
PW laser of ELI ALPS are presented in its first ramping
up phase at the >400 TW peak power level at 2.5 and 10
Hz repetition rates.
CG-P.4 THU

Comparison of two spatial characterisation methodsof XUV high-order harmonics for spatio-temporalcontrol of attosecond pulses
173

CE-P.30 THU

CE-P.31 THU

Doped Carbon Quantum Dots-Assisted Two-Photon
Lithography: A Facile Technique for Fabricating
Functional Micro/nanostructures∙S. RANI; IITB-Monash Research Academy, Mumbai, India
We report the application of doped carbon quantum dots
for fabrication of threedimensional, highly fluorescent,and functional micro/nanostructures using femtosecond
laserassisted two-photon lithography.

∙S. Prawdziak1 , C. Valentin1 , C. Péjot1 , F. Burgy1 , F.
Catoire1 , E. Constant2 , and E. Mével1 ; 1 Centre Lasers Intenses et Applications (CELIA), Talence, France; 2 Institut
Laser-Matière (ILM), Lyon, France
The spatial properties of XUV beams are measured andcompared in two different ways: the SWORD method
and a direct measurement using a Hartmann XUV wavefront sensor for further control of attosecond pulses.
CG-P.5 THU

Sub-atomic-unit Absolute Delay Calibration by the
Analytical Fitting of Attosecond Streaking
Measurements∙G. Inzani1 , N. Di Palo1 , G.L. Dolso1 , M. Nisoli1,2 , and
M. Lucchini1,2 ; 1 Department of Physics, Politecnico di Milano, Milano, Italy; 2 Institute for Photonics and Nanotechnologies, IFN - CNR, Milano, Italy

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Crucial prerequisites for measuring absolute timings in
attosecond experiments are a proper characterization of
the radiation and an absolute calibration of the delayaxis. A novel analytical fit makes it possible with a sub5-as accuracy.
CG-P.6 THU

Threshold Target Thickness in PW Laser Driven Ion
Acceleration∙S. Ter-Avetisyan ; University of Szeged, Szeged, Hungary
A “threshold” target thickness for proton acceleration isobserved. Above “threshold” proton energy almost independent on target thickness, below “threshold” it decreases. This observation, attributed to the pre-plasma,is confirmed analytically and by simulations.
CG-P.7 THU

Phase-Controlled Two-Color High-Order Harmonic
Generation in Laser-Produced Plasmas∙J. Mathijssen1,2 , K.S.E. Eikema1,2 , and S. Witte1,2 ;1Advanced Research Center for Nanolithography, Amsterdam, Netherlands; 2 Laserlab, Vrije Universiteit Amsterdam, Amsterdam, Netherlands
We have developed a setup for phase-controlled twocolor high-order harmonic generation in laser-produced
plasmas (LPP). This approach allows investigation of
LPP dynamics, and determining HHG ionization and recombination times for atoms with complex level structures.
CG-P.8 THU

Backward Photoelectron Emission In Ionization∙M.C. Suster, J. Derlikiewicz, F. Cajiao Vèlez, J.Z.
Kamiński, and K. Krajewska; Institute of Theoretical
Physics, Faculty of Physics, University of Warsaw, Warsaw, Poland
We proved that the mechanisms of the ionization process for low- and high-frequency laser pulses are differ-

13:00 – 14:00
EA-P: EA Poster session
EA-P.1 THU

Measurements of Bohmian Trajectories∙F. Huber1,2,3 , C. Versmold1,2,3 , J. Dziewior1,2,3 , L.
Knips1,2,3 , E. Meyer4 , A. Szameit4 , H. Weinfurter1,2,3 ,and J.D.A. Meinecke1,2,3 ; 1 Max-Planck-Institut für
Quantenoptik, Garching, Germany; 2 Department für
Physik, Ludwig-Maximilians-Universität, München,
Germany; 3 Munich Center for Quantum Science andTechnology (MCQST), München, Germany; 4 Institut für
Physik, Universität Rostock, Rostock, Germany

ent and, contrary to the status quo, the backward photoelectron emission in ionization is an inherently quantum
effect.

sampling, where strong-field ionization of atoms serves
as a temporal gate for petahertz-scale measurements of
optical fields.

CG-P.9 THU

CG-P.12 THUCharacterisation of a 200 nm Thick Liquid Jet Sheetfor Ion Acceleration∙A.P. Kovács1,2 , M. Karnok1 , T. Gilinger1 , M. Füle1,3 ,and K. Osvay1,2 ; 1 National Laser-Initiated Transmutation Laboratory, University of Szeged, Szeged, Hungary;2
Dept. of Optics and Quantum Electronics, University ofSzeged, Szeged, Hungary; 3 Dept. of Experimental Physics,
University of Szeged, Szeged, Hungary
A system has been developed for measuring the thickness of ultrathin liquid jets in vacuum and on-line operation. The method is demonstrated with the characterisation of a 200 nm thick water liquid jet.

Implementation of new frontend for PW-classPEARL laser facility∙I. Mukhin, K. Glushkov, A. Soloviev, A. Shaykin, V.
Ginzburg, I. Kuzmin, M. Martyanov, S. Stukachev, S.
Mironov, I. Yakovlev, and E. Khazanov; Institute of Applied Physics RAS, Nizhny Novgorod, Russia
The frontend laser with optical synchronization of
OPCPA amplification stages, a broader femtosecond
pulse spectrum, temporal shaping of pump pulse and asignificant increase in the stability has been developedfor PW-class PEARL laser

CG-P.10 THU

Second harmonic generation in a 140 fs Petawatt
laser system∙P. Fischer1 , B. Gonzalez-Izquierdo1 , V. Scutelnic1 , J.
Hartmann1 , M. Speicher1 , S. Bruce2 , A. Helal2 , M.
Spinks2 , E. Medina2 , H. Quevedo2 , M. Schollmeier1 , S.
Steinke1 , G. Korn1 , and E. Gaul1 ; 1 Marvel Fusion GmbH,
Munich, Germany; 2 Department of Physics, University ofTexas, Austin, USA
We reported on implementing efficient second harmonic
generation of 140fs laser pulse from the Texas Petawatt
system and the resulting ultra-clean temporal contrast.
Experimental and simulation results are presented.

The Effect of Multi-Filamentation on Shock-Wave
Generation inWater∙S. Eardley, J. Marangos, M. Matthews, R. Smith, and J.
Tisch; Imperial College London, London, United Kingdom
In a study of laser-water filamentation an inverse relationship between pulse duration and shockwave energy
was found. This relationship is attributed to the formation or lack of filament bundles and so-called superfilaments.
CG-P.11 THU

Moments Following Strong Field Ionization- Effect of
the Coulomb Potential on Free-Electron’s Trajectoryin Atomic Gases∙M. Agarwal1 and V. Yakovlev2 ; 1 Max Planck Institute of
Quantum Optics, Garching, Germany; 2 Ludwig Maximilian University of Munich, Munich, Germany
We have found that the electron-ion Coulomb interaction plays an essential role in nonlinear photoconductive

CG-P.13 THU

CG-P.14 THU

LED-pumped Ce:YAG luminescent concentrator for
absolute calibration of streaks cameras at nanosecond sweep durations
M. Nourry-Martin1,2 , A. Denoeud1 , C. Chollet1 , M.
Bonneau1 , T. Vinci3 , A. Ravasio3 , S. Brygoo1 , S. Darbon1 ,and ∙F. Balembois2 ; 1 CEA, DAM, DIF, Arpajon, France;

Université Paris-Saclay, Institut d’Optique Graduate
School, Centre National de la Recherche Scientifique, Laboratoire Charles Fabry, Palaiseau, France; 3 LULI, CNRS,
CEA, Sorbonne Université, Ecole Polytechnique–Institut
Polytechnique de Paris, Palaiseau, France
We demonstrate that a LED-pumped Ce:YAG luminescent concentrator is adapted to calibrate a streak opticalpyrometer at the ns scale. Its properties helps also to reduce the uncertainty of temperature measurements by afactor 2.5.
2CG-P.15 THU

Impact of electron-hole attraction on tunneling ratein crystalline solids based on quasi-Hartree-Fockequation∙Y. Shinohara, H. Sanada, and K. Oguri; NTT Basic Research Laboratories, NTT Corporation, Atsugi, Japan
We performed simulations to evaluate the influence ofelectron-hole interaction on tunneling ionization rate.
The simulation results show the enhancement of the ionization rate depends on applied field strength, indicating
field-dependent gap renormalization.
CG-P.16 THU

High-average Power, Soft X-ray Generation Driver at
2.1 μm∙R. Maksimenka1 , T. Pinoteau1 , N. Forget1 , D. Walke2 ,F. Gores2 , and I. Wilkinson2 ; 1 Fastlite, Antibes, France;2
Helmholtz-Zentrum Berlin für Materialien und Energie,
Berlin, Germany
We present a high-average power OPCPA system that
produces CEP-stable, few-cycle pulses centered at 2.1
μm. The system was built at the Helmholtz-Zentrum
Berlin and serves as a driver for a table-top, coherent,
ultrashort-pulse soft X-ray source.

In contrast to standard quantum mechanics, Bohmianmechanics, allows definite trajectories, while being fullycompatible with the standard theory in all empirical predictions. Using weak measurements we reconstruct trajectories in a double-slit and waveguide setup.

Active optical frequency standards provide interestingalternatives to their passive counterparts. Particularly,
such a clock alone continuously generates highly stablenarrow-line laser radiation. We report our study towards
the realization of such a clock.

atom at different excitation intensities. The preferred
time-ordering of the emitted photons from opposite
sidebands could be useful as a heralded narrowband single photon source.

EA-P.2 THU

EA-P.3 THU

Theoretical investigation of superradiant laser on atransition in neutral Sr and design of active opticalclock∙S. Dubey1 , S. Zhou2 , S. Bennetts 2 , F. Famà 2 , C.B.S.
Silva2 , B. Heizenreder2 , F. Schreck2 , G. Kazakov1 , and
S.A. Schäffer2 ; 1 Atominstitut, Vienna University of Technology, Austria; 2 University of Amsterdam, Netherlands

Observation of the Mollow Triplet from an opticallyconfined single atom
∙B.L. Ng1 , C.H. Chow1 , and C. Kurtsiefer1,2 ; 1 Centerfor Quantum Technologies, Kent Ridge, Singapore;2
Department of Physics, National University of Singapore,
Kent Ridge, Singapore
We characterize the atomic spectrum of a single 87 Rb

The Squeeze Laser∙A. Schönbeck, J. Südbeck, J. Zander, D. Berz-Vöge, and
R. Schnabel; Universität Hamburg, Hamburg, Germany
Photon shot noise imposes limits on high-precisionlaser-based measurements, which is often the case today
even at the highest light output. Quantum squeezing is atechnology that can circumvent the need for even higher
powers.

174

EA-P.4 THU

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EA-P.5 THU

Spin Noise Spectroscopy of Optical Light Shifts∙J. Delpy; ENS Paris-Saclay, Centrale Supélec, Université
Paris-Saclay, CNRS, Orsay, France
A light-induced nonequilibrium regime is introduced instandard spin noise spectroscopy, which results in a splitting of the spin noise spectrum. This splitting is theoretically shown to originate from and to allow for the measurement of light shifts.
EA-P.6 THU

Measurement based CV parametrized quantum
circuits.
∙A. Verma; Technical University of Denmark, Kongens
Lyngby, Denmark
In this submission, we show a deterministic and highfidelity generation of a large Haar random unitaryparametrized by Homodyne measurement angles. Suchan approach may promise scalable as well as high fidelity
unitary design.
EA-P.7 THU

Single-mode Quantum Non-Gaussian Light from
Warm Atoms∙J. Mika, L. Lachman, T. Lamich, R. Filip, and L. Slodička;
Palacky University Olomouc, Olomouc, Czech Republic
We present the source of a single-mode quantum nonGaussian light generated by the spontaneous four wave
mixing in a warm atomic vapor.
EA-P.8 THU

Nonclassical light generation from laser-driven
semiconductor intraband excitations∙R. Sondenheimer1,2 , I. Gonoskov3 , C. Hünecke3 , D.
Kartashov4 , U. Peschel1 , and S. Gräfe2,3 ; 1 Institute ofSolid State Theory and Optics, Friedrich Schiller University Jena, Jena, Germany; 2 Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany; 3 Institute of Physical Chemistry, Friedrich Schiller
University Jena, Jena, Germany; 4 Institute of Optics andQuantum Electronics, Friedrich Schiller University Jena,
Jena, Germany
We investigate the generation of higher-order harmonics from a quantum optics perspective via lasersemiconductor interactions. All field modes are entangled, allowing for novel quantum information processing protocols with high photon numbers over large frequency ranges.
EA-P.9 THU

automatic relocking ecdl in optical tweezer machinefor quantum computing and simulation∙m. zarei1,2 , i. knottnerus2 , a. urech2 , f. schreck2 , m.
zawada1 , and p. morzyński1 ; 1 institute of physics, facultyof physics, astronomy and informatics, nicolaus copernicus university, torun, Poland; 2 institute of physics, university of amsterdam, amsterdam, Netherlands
we present a web application dedicated to redpitaya
board for automatic and real-time relocking of theexternal-cavity diode lasers (ecdls) by cavity transmission and/or wavemeter signals in optical tweezer machine for quantum computing and simulation.
EA-P.10 THU

Towards the Development of an Optical Lattice Clock
Testbed Setup for the iqClock Project∙A. Jha1 , A. Singh1,2 , Y. Kale1 , J. Wayland1 , Y. Huyan1 , Q.
Sun1,2 , J. Jones1,3 , M. Gellesch1 , K. Bongs1 , and Y. Singh1 ;1
University of Birmingham, Birmingham, United Kingdom; 2 British Telecommunications, Ipswich, United Kingdom; 3 ColdQuanta UK limited, Oxford, United Kingdom
We report the progress of the development of the optical lattice clock testbed system (lab-based) which aims
at benchmarking another robust, field-deployable integrated optical lattice clock being developed under the iqClock project.
EA-P.11 THU

An Open-Access Optical Microcavity with UltraHigh Mechanical Stability∙M. Fisicaro, M. Witlox, H. van der Meer, M. Rost, andW. Löffler; Leiden University, Leiden, Netherlands
We have developed an open-cavity device with ultrahigh stability of 6 pm rms at 4 K, allowing the operation of an optical cavity with Finesse 1800 in closed-cycle
table-top cryostats without a mechanical low-pass filter.
EA-P.12 THU

Highly Pure and Bright Emission of Telecom C-Band
Quantum Dots in Circular Bragg Grating Cavities∙R. Joos, C. Nawrath, S. Kolatschek, S. Bauer, P. Pruy, R.
Sittig, P. Vijayan, J. Huang, M. Jetter, S.L. Portalupi, and
P. Michler; Institut für Halbleiteroptik und Funktionelle
Grenzflächen, Stuttgart, Germany
This work shows the first implementation of telecom Cband quantum dots coupled to circular Bragg gratings
cavities. Excellent single-photon purity and ultra-highemission rate can be achieved paving the way towards
complex quantum technology applications.
EA-P.13 THU

Spin-orbit coupling of light and cross-polarization
extinction for single-photon sources∙P. Steindl and W. Löffler; Leiden University, Leiden,
Netherlands
We show when and how mirror reflection Fresnel birefringence in combination with spin-orbit coupling can
improve the cross-polarized extinction ratio for sin-gle quantum dot–cavity resonance fluorescence experiments and single-photon production.
EA-P.14 THU

Compact ULE reference cavity for stabilization of 2.6
μm DFB diode laser to study long-range interactions
in ultracold Strontium atoms∙S. Ganesh, S. Zhang, B. Tiwari, K. Bongs, and Y. Singh;
University of Birmingham, Birmingham, United Kingdom
We present a compact ULE reference cavity for stabilizing DFB laser at 2.6um which is employed as a probe
for studying long-range induced electric dipolar interactions in ultracold Sr atoms trapped in deep optical lattice.
EA-P.15 THU

Dynamic Brillouin cooling for continuous optomechanical systems∙C. Zhu1,2 and B. Stiller1,2 ; 1 Max Planck Institute for
the Science of Light, Erlangen, Germany; 2 University
Erlangen-Nuremberg, Erlangen, Germany
We demonstrate that by periodically modulating a backward Brillouin process with a pulsed pump, a phonon
cooling rate of several orders of magnitude can beachieved.
EA-P.16 THU

Photon subtraction from two-mode squeezed
vacuum states using a waveguide trimer∙A.M. Datta1 , K. Tschernig2 , A. Perez-Leija2 , and K.
Busch1,3 ; 1 Institut für Physik, Humboldt-Universität zu
Berlin, Berlin, Germany; 2 CREOL, The College of Optics
and Photonics, University of Central Florida, Orlando,
USA; 3 Max-Born-Institut, Berlin, Germany
Recently, generating multiphoton quantum states using
photon subtraction from a two-mode squeezed vacuum
states was experimentally demonstrated. Here, we propose a new protocol where we reduce the number ofphoton-number-resolving detectors.
EA-P.17 THU

The contribution has been withdrawn.
EA-P.18 THU

Chiral Atomic Rydberg States∙S. Aull1 , S. Giesen2 , P. Zahariev1,3 , M. Debatin1 ,R. Berger2 , and K. Singer1 ; 1 Experimentalphysik 1,
Universität Kassel, Kassel, Germany; 2 Theoretische
Chemie, Philipps-Universität Marburg, Marburg, Germany; 3 Institute of Solid State Physics, Bulgarian
Academy of Sciences, Sofia, Bulgaria
It has been shown theoretically hat by combining Hydrogenic wavefunctions in superposition, the resulting
electronic state can show chiral properties. We propose
a protocol for experimentally creating those states in Rubidium.

175

EA-P.19 THU

Photon-Pair Recombination via Sum-Frequency
Generation by Chirped, Aperiodically Poled LiNb
Waveguide∙P. Hendra1,2 , J.R. León-Torres1,2 , and M. Gräfe1,2,3 ;1Fraunhofer Institute of Applied Optics and Precision Engineering IOF, Jena, Germany; 2 Abbe Center of Photonics, Friedrich-Schiller-Universität Jena, Jena, Germany;3
Institute of Applied Physics, Technical University ofDarmstadt, Darmstadt, Germany
Application of chirped, aperiodically poled Lithium Niobate waveguide in upconversion of entangled photon
pairs.
EA-P.20 THU

Resonant Scattering and Quantum Modulation of a
Coherent State with the Spin of a Quantum Dot
P. Androvitsaneas1,2 , A.B. Young2 , T. Nutz2 , J.M.
Lennon2 , ∙S.T. Mister2 , C. Schneider3 , M. Kamp4 , S.
Höfling4 , D.P.S. McCutcheon2 , E. Harbord2 , J.G. Rarity2 ,and R. Oulton2 ; 1 Cardiff University, Cardiff, United
Kingdom; 2 University of Bristol, Bristol, United Kingdom; 3 University of Oldenburg, Oldenburg, Germany;
4
Universität of Würzburg, Würzburg, Germany
We experimentally explore and theoretically model a dynamic QD spin-photon interaction. New scattered lightproperties and a discrete(quantised) phase modulationof the field are observed. These results have potential applications to quantum information processing tasks.
EA-P.21 THU

Fractional Fourier transform - Experimental
implementation for spectro-temporal cat state∙S. Kurzyna1,2 , B. Niewelt1,2 , M. Jastrzȩbski1,2 , J.
Nowosielski1,2 , W. Wasilewski1 , M. Mazelanik1 , and
M. Parniak1,3 ; 1 Centre for Quantum Optical Technologies,Centre of New Technologies, University of Warsaw,
Warsaw, Poland; 2 Faculty of Physics, University of Warsaw, Warsaw, Poland; 3 Niels Bohr Institute, University of
Copenhagen, Copenhagen, Denmark
By applying temporal and spectral modulation in gradient echo memory, we have performed experimental
implementation of fractional Fourier transform in time
frequency-domain. The results we have obtained may allow for spectro-temporal mode decomposition.
EA-P.22 THU

Hong-Ou-Mandel Effect between a Thermal Field anda Heralded Single-photon State: Improved visibility
by Multiphoton Components∙A. Khodadad Kashi1,2 , L. Caspani3 , and M. Kues1,2 ;1Institue of Photonics, Leibniz University, Hannover, Germany; 2 Cluster of Excellence, Leibniz University, Hannover, Germany; 3 Institute of Photonics, Department of

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Physics, University of Strathclyde, Glasgow, United Kingdom
Through the first experimental implementation of thespectral Hong-Ou-Mandel effect between a thermal field
and a heralded state, we demonstrate that under certain statistical conditions, multiphoton components in
the heralded state partially contribute to the HOM visibility.

EA-P.23 THU

EA-P.24 THU

Amplification and storage of orbital angular momentum of light via magnetically assisted optical gain
∙J.W.R. Tabosa, R.S.N. Moreira, and J.C.A. Carvalho;
Universidade Federal de Pernambuco, Recife, Brazil
We report on the amplification and storage of light carrying orbital angular momentum via magnetically assisted
optical gain in a sample of cold atoms. This amplification mechanism allows to enhance the efficiency of thememory.

Quantum Self-Sustained Oscillator Arrays Towards
Dissipative Time Crystals: Taming Phase Diffusion
via Coherent Delayed Feedback
M. Li1 , ∙G.J. de Valcárcel2 , and C. Navarrete-Benlloch2 ;1
Wilczek Quantum Center, Shanghai Jiao Tong University, Shanghai, China; 2 Departament d’Òptica i Optometria i Ciencies de la Visió, Universitat de València, Valencia, Spain

13:00 – 14:00

ing. Multiple quantum channels are derived from a common laser source. The approach is verified over a 70-kmlong deployed fiber link.

EB-P.7 THU

EB-P: EB Poster session
EB-P.1 THU

Deep Learning Based TEMPEST Attacks on a
Quantum Key Distribution Sender∙A. Baliuka1,2 , M. Stöcker1 , M. Auer1,2,3 , P. Freiwang1,2 ,H. Weinfurter1,2,4 , and L. Knips1,2,4 ; 1 LudwigMaximilian-University (LMU), Munich, Germany;2
Munich Center for Quantum Science and Technology(MCQST), Munich, Germany; 3 Universität der Bundeswehr München, Neubiberg, Germany; 4 Max Planck
Institute of Quantum Optics (MPQ), Garching, Germany
A side-channel attack on the electronics of a quantum
key distribution sender is demonstrated analyzing radiofrequency emissions using neural networks. It can extract almost all secret key at a few centimeters from thedevice.
EB-P.2 THU

Real field clock synchronization for quantum key
distribution using correlated photon pairs∙Y. Pelet, G. Sauder, O. Alibart, S. Tanzilli, and A. Martin;
INPHYNI, université cote d’azur, Nice, France
We present the implementation of a time synchronization protocol on a real field quantum key distribution
link spanning over 50km, managing to continuously
keep the relative drift between two distant clocks below
12 ps.
EB-P.3 THU

Multi-Channel Time-Bin Quantum Key Distribution
over a 70-km-long deployed Fiber Link
∙N. Pavlovic Tucakovic1 , K. Paciorek1 , M. Cabrejo
Ponce1,2 , C. Spiess1,2 , and F. Steinlechner1,3 ; 1 Fraunhofer
Institute for Applied Optics and Precision Engineering,
Jena, Germany; 2 Friedrich Schiller University Jena, Jena,
Germany; 3 Abbe Center of Photonics, Friedrich Schiller
University Jena, Jena, Germany
We demonstrate a weak coherent pulse source scheme
for time-bin encoded QKD with wavelength multiplex-

EB-P.4 THU

Countering detector manipulation attacks in quantum communication through detector self-testing∙L. Shen1 and C. Kurtsiefer1,2 ; 1 Center for Quantum Technologies, Singapore, Singapore; 2 Department of
Physics, National University of Singapore, Singapore, Singapore
We demonstrate a simple countermeasure to detect
detector manipulation attacks using an auxiliary lightsource. This addresses a significant hardware vulnerability in practical quantum key distribution and is suitable
for retrofitting onto existing systems.
EB-P.5 THU

Generative Adversarial Learning boosted by a
Photonic Quantum Frequency Coprocessor∙P. Rübeling1 , T. Bækkegaard1,2 , N.T. Zinner2 , and M.
Kues1 ; 1 Institute of Photonics, Hannover, Germany;
2
Department of Physics and Astronomy, Aarhus, Denmark
The potential of quantum Generative Adversarial Networks (qGANs) via Quantum Frequency Combs is explored numerically. Our results indicate that compared
to a conventional GAN the qGAN needs fewer epochs toconverge to the Nash equilibrium.

Controlling the Recovery Time of the Superconducting Nanowire Single Photon Detector using a
Tunable Resistor∙H. Wang1 , N. Noordzij2 , J.W.N. Los2 , and I.E. Zadeh1 ;1Department of Imaging Physics, Faculty of Applied Sciences, Delft University of Technology, Delft, Netherlands;
2
Single Quantum B.V., Delft, Netherlands
We outline a method using a tunable resistor in series
with the superconducting nanowire detector to adjust its
recovery time inside the cryostat. The resistance is determined by the heating effect on a superconducting wire.
EB-P.8 THU

Characterizing Polarization Switching in GainSwitched Vertical-Cavity Surface-Emitting Lasers for
Quantum Random-Number Generation
A. Quirce1 , ∙A. Valle1 , M. Valle-Miñon1 , and J.
Gutierrez2 ; 1 Instituto de Fisica de Cantabria (IFCA),
Universidad de Cantabria-CSIC, Santander, Spain;2
Departamento de Matemática Aplicada y Ciencias dela Computación, Universidad de Cantabria, Santander,Spain
We characterize a quantum-random number-generator
based on the excitation of the linearly polarized modesof a gain-switched VCSEL. We find good agreement between experiments and simulations incorporating themeasured device intrinsic parameters.
EB-P.9 THU

EB-P.6 THU

Novel Scheme for Clock Synchronisation inContinuous-Variable Quantum Key Distribution
Systems with Discrete Modulation∙C. Schaeffer and S. Kleis; Helmut Schmidt University,
Hamburg, Germany
At the distant locations of a CV-QKD system the timescales of free running electronics and lasers are synchronized with GPS stabilized oscillators. The software receiver operates reliable with a SNR = -26 dB.

DWDM-compatible entanglement distribution using
a biphoton frequency comb
∙T. Kobayashi1,2 , T. Yamazaki1,2 , R. Fujimoto2 , S. Miki3,4 ,F. China3 , H. Terai3 , R. Ikuta1,2 , and T. Yamamoto1,2 ;1Center for Quantum Information and Quantum Biology, Osaka University, Osaka, Japan; 2 Graduate Schoolof Engineering Science, Osaka University, Osaka, Japan;
3
Advanced ICT Research Institute, National Institute ofInformation and Communications Technology (NICT),
Hyogo, Japan; 4 Graduate School of Engineering, Kobe
University, Hyogo, Japan176

We analyze the possibility to dissipatively engineer timecrystalline states in arrays of self-sustained quantum oscillators. We find that this is feasible in 2D, 3D and meanfield geometries, with delayed coherent feedback helping
towards this goal.

We demonstrate a frequency-multiplexed polarizationentangled photon-pair distribution using 16-channel
DWDM compatible filter with 25 GHz spacing. The
photon pairs is generated by a singly resonant periodically poled lithium niobate waveguide resonator inside a
Sagnac-type interferometer.
EB-P.10 THU

Long-distance entanglement distribution withultra-bright polarization-entangled photon source
and frequency division multiplexing
S. Sharma1,2 , K. Lozano-Mendez1,2 , R. Gomez1,2 , A.
Kržič 1,2 , C. Spiess1,2 , L. Gonzalez1,2 , C.A. Melo
Luna1 , M. Gräfe1 , E. Beckert1 , and ∙F. Steinlechner1,3 ;1Fraunhofer Institute for Applied Optics and Precision
Engineering, Jena, Germany; 2 Friedrich Schiller University Jena, Jena, Germany; 3 Abbe Center of Photonics,
Friedrich Schiller University Jena, , Jena, Germany
An ultra-bright polarization-entangled photon source
based on SPDC, demonstrating high entanglement fidelity, presents a generation rate of ~1e8 Million
pairs/s/mW/nm. We experimentally investigate the performance of the source in simulated attenuation scenarios upto 60 dB.
EB-P.11 THU

Distributing High Rate of Polarization-Entangled
Photon Pairs over Long Distance through Standard
Telecommunication Fiber
L. Shen1 , C.H. Chow1 , ∙J.Y.X. Peh1 , X.J. Yeo1 , P.K. Tan1 ,and C. Kurtsiefer1,2 ; 1 Center for Quantum Technologies,
Singapore, Singapore; 2 Department of Physics, National
University of Singapore, Singapore, Singapore
We demonstrate entanglement distribution over 50kmof standard telecommunication fiber with >10,000/s pairrate using a non-degenerate photon source. The modest hardware requirements make it practical for quantum key distribution deployment in existing metropolitan networks.

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EB-P.12 THU

GaSb-based 1.5 μm quantum dot emitters forquantum photonic integration and communication
T. Hakkarainen1 , J. Hilska1 , ∙A. Chellu1 , L. Leguay2 , E.
Luna3 , A. Schliwa2 , and M. Guina1 ; 1 Optoelectronics Research Centre, Physics Unit, Tampere University, Tampere, Finland; 2 Institute for Solid State Physics, Technical University of Berlin, Berlin, Germany; 3 PaulDrude-Institut für Festkörperelektronik Leibniz-Institut
im Forschungsverbund Berlin e.V, Berlin, Germany
Epitaxial fabrication, energy structure, and emission
properties of GaSb quantum dots formed by filling droplet-etched nanoholes are presented. These
quantum-photonics building blocks emit at 1.5 μm enabling wavelength compatibility with fiber optics and Siphotonics.
EB-P.13 THU

Adaptive optics enabled entanglement distribution
over atmospheric turbulence channels.
∙V. Nafria and I.B. Djordjevic; University of Arizona,
TUCSON, USA
We present results from our experiment of an entangled distributed system over a 1.5km long retroreflectorbased free-space optical communication link. Our results demonstrate significant improvement in coincidence counts with the help of adaptive optics in a strong
turbulence regime.
EB-P.14 THU

Resilience of Quantum Key Distribution Source
against Laser-Damage Attack by a Variety of Lasers
D. Ruzhitskaya1,2 , I. Zhluktova3,4 , A. Ponosova1,2,3 , ∙D.
Trefilov1,2,5 , P. Chaiwongkhot6 , A. Huang7 , V. Kamynin3 ,and V. Makarov1,2,8 ; 1 Russian Quantum Center, Moscow,
Russia; 2 NTI Center for Quantum Communications,
National University of Science and Technology MISiS,
Moscow, Russia; 3 Prokhorov General Physics Institute of
Russian Academy of Sciences, Moscow, Russia; 4 MIREA– Russian Technological University, Moscow, Russia;
5
University of Vigo,, Vigo, Spain; 6 Mahidol University,
Bangkok, Thailand; 7 College of Computer Science andTechnology, National University of Defense Technology,
Changsha, China; 8 University of Science and Technology
of China, Shanghai, China
We show an overview of our progress in investigation of
the laser-damage attack on QKD sources. Harm to thesecurity of QKD systems caused by exposure to 1550-nm
CW and 1061-nm pulsed lasers is analyzed.
EB-P.15 THU

Second-order duality of light and its nonclassicalcomplementarity∙R. Ikuta; GSES, Osaka University, Toyonaka, Japan;

QIQB, Osaka University, Toyonaka, Japan
We introduce a concept of wave-particle duality in thecontext of second-order interference based on intensity correlation measurement known as the Hong-OuMandel interference and show the nontrivial property of
its complementarity.

Photonics, Friedrich Schiller University, Jena, Germany
We analyze in a modular approach the proper selectionof the wavelength involving all the relevant input parameters for the Entangled Photon Sources and the Optical
Ground Stations features in satellite QKD protocols.

independent entanglement verification of a two-mode
squeezed entangled state using a protocol found in [1].
With -1.5 dB of squeezing we are able to demonstrate theeffectiveness of the protocol.

EB-P.20 THU

EB-P.16 THU

Hybrid Integrated Photonic/Electronic Homodyne
Detector for GHz Baud Rate Continuous Variable
Quantum Key Distribution.
∙A. Boubriak1 , R. Kumar2 , J. Frazer1 , J. Matthews1 , and
E. Allen3 ; 1 University of Bristol, Bristol, United Kingdom;
2
University of York, York, United Kingdom; 3 University ofBath, Bath, United Kingdom
Making use of integrated photonics and integrated electronics allows for the possibility of GHz bandwidth homodyne detectors. In this work we demonstrate such a
device and its prospective use in a CV-QKD system.

Spectral purity characterization of telecom wavelength photons generated in aperiodically poled KTP∙J. Conrad1,2 , R. Gómez1,2 , M. Leipe1,2 , M. Cabrejo
Ponce1 , G. Sauer1,2 , and F. Steinlechner1,2 ; 1 Fraunhofer
Institute for Applied Optics and Precision Engineering
IOF, Jena, Germany; 2 Abbe Center of Photonics, Friedrich
Schiller University Jena, Jena, Germany
We characterize parametric down conversion emission
from periodically- and aperiodically poled KTP crystals
for spectral purity, heralding efficiencies, and Hong-OuMandel interference visibility and study the influence ofthe pump spectrum.

Characterization Method for Excitation Efficiency of
Semiconductor Quantum Dots
∙J.-H. Littmann1 , J. Lee1 , J.R. Gonzales-Ureta1 , R.
Checchinato1 , S. Höfling2 , C. Schneider3 , and A.
Predojević1 ; 1 Department of Physics, Stockholm University, 10691 Stockholm, Sweden; 2 Technische Physik,
Physikalisches Institut and Würzburg-Dresden Clusterof Excellence ct.qmat, Universität Würzburg, 97074
Würzburg, Germany; 3 Institute of Physics, University of
Oldenburg, 26129 Oldenburg, Germany
We present our measurements performed on quantum
dots emitting photon pairs where we establish a method
for accurate characterization of the excitation efficiency.

EB-P.17 THU

EB-P.21 THU

EB-P.25 THU

Coherent Raman spin control for the generation ofhigh fidelity entangled photonic states with group-IV
vacancies∙G. Pieplow1 , J.H.D. Munss2 , M.I. Monsalve1 , and T.
Schröder1,3 ; 1 Humboldt Universit ät Berlin, Berlin, Germany; 2 PsiQuantum, Palo Alto, USA; 3 FerdinandBraun-Institut, Berlin, Germany
We analyze the potential of group-IV vacancies for thegeneration of highly entangled photonic states. The work
focuses on the Raman spin gates, which can be, in principle, ultrafast and produce ultra-high-fidelity spin gates.

Phase-only temporal mode transformations withcomplex spectral and temporal phases
J. Szuniewicz, F. Sośnicki, and ∙M. Karpiński; Faculty ofPhysics, University of Warsaw, Warsaw, Poland
We show that an arbitrary phase-only transformation between temporal modes can be performed using only two
arbitrary phase patterns: one temporal and one spectral.
The phases can be found using a standard phase retrieval
algorithm.

Long Time-Delay Quantum Interference of Single
Photons Produced by a Quantum Dot - Cavity System∙K. Kanneworff1 , P. Steindl1 , J. Bowers3 , D.
Bouwmeester1,2 , and W. Löffler1 ; 1 Huygens-Kamerlingh
Onnes Laboratory, Leiden University, Leiden, Netherlands; 2 Dept. of Physics, University of California, Santa
Barbara, USA; 3 Dept. of Electrical & Computer Engineering, University of California, Santa Barbara, USA
Quantum interference of photons is essential for many
beyond-QKD applications of quantum networks – here
we investigate the interference of single photons createdmore than a thousand lifetimes apart.

EB-P.18 THU

Robust Time Transfer with Single Photons on Hybrid
Quantum Communication Scenarios in Fiber andFree-Space∙C. Spiess1,2 , K. Paciorek2 , N.L. Döll2 , A. Kržič1,2 , and F.
Steinlechner1,2 ; 1 Friedrich Schiller University Jena, Jena,
Germany; 2 Fraunhofer Institute for Applied Optics andPrecision Engineering IOF, Jena, Germany
Single photons are great timing carriers to synchronize
communicating parties. We show robust time transfer
on a 1.7 km free-space link. The time deviation is 100 ps
at 1-second integration time with only unstable crystal
oscillators.
EB-P.19 THU

Entangled photon source for satellite communications: Arguments in wavelength selections∙C.A. Melo-Luna1 , A. Kržič1 , S. Sharma1,2 , R. Mouchel1 ,D. Heinig1 , and F. Steinlechner1,2 ; 1 Fraunhofer Institutefor Applied Optics and Precision Engineering, IOF, Jena,
Germany; 2 Institute of Applied Physics, Abbe Center of

EB-P.22 THU

Efficient Implementation of Time-Bin BB84-QKD
Protocol with Phase-Randomized Weak Coherent
States∙S. Francesconi1 , N. Biagi1 , I. Vagniluca1 , D. Ribezzo2,3 ,T. Occhipinti1 , A. Zavatta1,2 , and D. Bacco1,4 ; 1 QTI s.r.l.,
Florence, Italy; 2 National Institute of Optics (CNR-INO),
Florence, Italy; 3 University Federico II, Naples, Italy;
4
University of Florence, Florence, Italy
In this work we propose a novel scheme for implementing the time-bin QKD BB84 protocol with onedecoy method employing phase-randomized weak coherent states and we test the setup performances over a
20 dB-attenuation channel.
EB-P.23 THU

Measurement device independent entanglement
witness of continuous variable states∙B.L. Larsen1 , S. Izumi2 , J.S. Neergaard-Nielsen1 , andU.L. Andersen1 ; 1 Technical university of Denmark , Kongens Lyngby, Denmark; 2 Xanadu Quantum Technologies
Inc, Ontario, Canada
We experimentally demonstrate measurement device

177

EB-P.24 THU

EB-P.26 THU

Single-Pixel Imaging LiDAR with Random-Modulated CW Laser for Application to 3D LiDAR∙D. Lim, D. Kim, K. Park, and Y.-s. Ihn; Emerging Scienceand Technology Directorate, Agency for Defense Development, Daejeon, South Korea
We present a single-pixel LiDAR system using randommodulated CW laser. Our work will be useful for 3D
single-pixel imaging for long unambiguous range.
EB-P.27 THU

Atomic Frequency Comb Memory in Warm
Rubidium Vapour∙Z. Schofield, A. Christan-Edwards, O. Mor , V. Laurindo Jr, and P.M. Ledingham; University of Southampton, Southampton, United Kingdom
The Atomic Frequency Comb quantum memory basedin warm Rubidium vapour allows for the storage and on
demand retrieval of quantum photonic information by
tailoring the spectra into equally spaced combs.

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EB-P.28 THU

Underwater transmission of mesoscopic twin-beamstates for applications in Quantum Communication
A. Allevi1 , ∙M. Lamperti1 , and M. Bondani2 ; 1 Universityof Insubria and IFN-CNR, Como, Italy; 2 Institute for Photonics and Nanotechnologies, IFN-CNR, Como, Italy
We demonstrate that mesoscopic twin-beam states exhibit good robustness against any kind of external degradation, such as losses and noise sources. In particular, we
experimentally investigate the possibility of using themfor underwater Quantum Communication.
EB-P.29 THU

Noise types in correlation-based target detection∙V. Kornienko and I. Tittonen; Aalto University, Helsinki,
Finland
We demonstrate analytically and with a model experiment that target detection protocols based on entangledstates are vulnerable towards the correlated noise froma partially reflecting jamming object, in contrast to thethermal background noise.
EB-P.30 THU

Quantum Randomness Certification Through Threestate Discrimination∙L. Nunes Faria, C. Rock i Carceller, Z. Liu, U. Andersen, J.
Neegaard-Nielsen, and J. Brask; Danmarks Tekniske Uni-

13:00 – 14:00
EH-P: EH Poster session
EH-P.1 THU

Holographic Optical Metasurfaces with High Trap
Stiffness∙T. Plaskocinski, J. Xiao, M. Biabanifard, S. Persheyev,
and A. Di Falco; University of St Andrews, St Andrews, United Kingdom
Photonic metasurfaces have been proposed to create
on-chip solutions for optical trapping applications. We
present a metasurface-enabled on-chip system, capableof trapping extended objects, with performance comparable to a system using high numerical aperture objectives.
EH-P.2 THU

The contribution has been withdrawn.
EH-P.3 THU

Parametric Metadevices for Electromagnetic Wave
Amplification∙F. Kovalev and I. Shadrivov; ARC Centre of Excellence
for Transformative Meta-Optical Systems (TMOS), Re-versitet, Kongens Lyngby, Denmark
Randomness is extracted by sending to a single-photon
detector three possible time bin encoding of coherent
states. Considering measurement outcomes which may
discriminate only two of the inputs, randomness is extracted from the other one.
EB-P.31 THU

Modulated Entangled Photon Source for Quantum
Secret Sharing∙P. Ancsin, M. Cabrejo Ponce, and F. Steinlechner; Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany
Quantum secret sharing is a multi-party quantum key
distribution scheme, which can be implemented by using
two-photon states only. Its feasablity has been demonstrated by the use of an actively modulated polarizationentangled photon source.
EB-P.32 THU

Towards Single-Photon Emitters (SPE) Integration
with Optical Fibers∙J.P. Berti Ligabô1 , T. Heindel2 , S. Reitzenstein2 ,J.N. Donges2 , C. Schneider3 , M.A. Schmidt4 , and F.
Eilenberger5 ; 1 Institute of Applied Physics, Friedrich
Schiller University, Jena, Germany; 2 Technische Universität Berlin, Berlin, Germany; 3 Carl von Ossietzky Univer-search School of Physics, The Australian National University, Canberra, Australia
We propose and study a parametric metadevice for amplification of electromagnetic waves. We found that our
subwavelength thin metadevices can provide amplification of up to 10 dB and analysed its stability.
EH-P.4 THU

Giant circular dichroic SHG behaviors of doubly SP
resonant asymmetric Al nanorod dimer structures∙A. Sugita and S. Tamotsu; Shizuoka University, Hamamatsu, Japan
Nonlinear chiroptics are reported about doubly SP resonant asymmetric aluminum nanodimers. SHG circulardichroism as large as ~0.6 was observed from artificial,chiral plasmonic systems. The value and sign were tunable by changing geometric parameters.
EH-P.5 THU

Deterministic nanoantenna array design for stable
plasmon-enhanced harmonic generation∙T.-I. Jeong1 , S. Kim1 , S. Kim1 , and S. Kim1,2 ;1Department of Cogno-Mechatronics Engineering, PUSAN, South Korea; 2 Department of Optics and Mechatronics Engineering, PUSAN, South Korea

sity of Oldenburg, Oldenburg, Germany; 4 Leibniz Institute of Photonic Technology, Jena, Germany; 5 Fraunhofer
IOF, Jena, Germany
A complete framework using custom design mechanics and metalenses for coupling strain engineered TMD(Transition-Metal Dichalcogenide) monolayers containing SPE (Single-Photon Emitters) into optical fibers is
described.
EB-P.33 THU

Photoluminescence (PL) imaging of QDs for deterministic fabrication of on-demand single-photon
sources∙A. A. Madigawa, B. Gaal, N. Gregersen, and B.
Munkhbat; Technical University Of Denmark, Lyngby,
DenmarkIn this study, we aim to investigate the photoluminescence imaging (PL) technique to determine the best approach to extract and position with high accuracy the
randomly positioned quantum dots (QD) in photonic
nanostructures.
EB-P.34 THU

Experimental Classification of Samples with Few
Coincidence Measurements Using PolarizationEntangled Photon Pairs∙V.R. Besaga1 , L. Zhang1 , A. Vega1 , P.S. Chauhan1,2 ,Deterministic design for stable plasmon-enhanced harmonic generation by analysis of the beam positiondependent THG yield with the density of a nanoantenna
array.
EH-P.6 THUHyper Rayleigh Scattering on Gold Nanoparticles :Insights into the Origin of the Response from a
Polarization Analysis∙M. Slemp1 , E. Salmon1 , C. Jonin2 , and P.-F. Brevet1 ;1
Non-Linear Optical Equipment and Interfaces Group(ONLI), Institut Lumière Matière ILM, UMR CNRS 5306,
Université Claude Bernard Lyon 1, Villeurbanne, France;
2
Laboratoire Charles Coulomb, UMR CNRS 5221, Université Montpellier, Montpellier, France
We present a polarization-resolved analysis of theHyper-Rayleigh Scattering Response for spherical gold
nanoparticles differing in size (200 down to 2 nm) to reveal the contributions to this response.
EH-P.7 THU

Topology for the classification and design ofdisordered metasurfaces∙T. Madeleine, N. Podoliak, O. Buchnev, G. D’Alessandro,
J. Brodzki, and M. Kaczmarek; University of Southamp-

178

T. Pertsch1,2 , A. Sukhorukov3 , and F. Setzpfandt1,2 ;Institute of Applied Physics, Abbe Center of Photonics, Friedrich Schiller University Jena, Jena, Germany;
2
Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Jena, Germany; 3 ARC Centre of Excellence
for Transformative Meta-Optical Systems (TMOS), Department of Electronic Materials Engineering, Research
School of Physics, The Australian National University,
Canberra, Australia
We demonstrate experimental non-local identificationof different polarization objects regardless of their orientation by performing only few coincidence measurements using the polarization-entangled photon pairs andonly one fixed polarization analyzed in the sample arm.
1

EB-P.35 THU

Control of Ion Motion using Rydberg Excitation∙M. Mallweger1 , A. Cidrim1,2 , H. Parke1 , S. Salim1 , N.
Kuk1 , R. Thomm1 , A. Santos1,2 , C. Zhang1 , and M.
Hennrich1 ; 1 Stockholm University, Stockholm, Sweden;
2
Universidade Federal de Sao Carlos, Sao Carlos, Brazil
The properties of trapped Rydberg ions, such as thepolarizability, scale drastically with increasing quantum
number. We can therefore employ a shifted trapping potential to perform coherent phase operations with the ion
motion.

ton, Southampton, United Kingdom
We built topological tools to characterise positional correlated disorder in metasurfaces. These tools can be used
for the fast design of complex physical systems and tonumerically investigate fundamental phenomena such as
Anderson localisation.
EH-P.8 THU

FaSST: a Frequency-agile Spintronic Superlattice
Terahertz Metasurface for non-contact detection ofmagnetic fields
S. Karmakar1 , ∙R.K. Varshney2 , and D. Roy Chowdhury3 ;1
Department of Electrical and Computer Engineering, Princeton University, New Jersey, 08544, USA;2
Department of Physics, Indian Institute of Technology Delhi, Hauz Khas, New Delhi, 110016, India;
3
Department of Physics, Ecole Centrale School of Engineering - Mahindra University, Hyderabad, Telangana,500043, India
We propose novel spintronic superlattice (FaSST) metasurface operating by terahertz magneto-transport mechanism. We detect presence of low-intensity magnetic
field (~ 30 mT) with capability of both frequency (~ 20
GHz) and intensity modulation of resonances.

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/Europe-EQEC 2023

Hall B0
EH-P.9 THU

Modulating the Temporal Dynamics of Nonlinear
Ultrafast Plasmon Resonances∙H. Asif and R. Sahin; Akdeniz University , Antalya,
TurkeyWe propose the lifetime enhancement of the second harmonic (SH) plasmon mode exclusively after the natural
decay time of the fundamental mode (FM), which distinguishes SH mode irrespective of its spatial convolution
with elementary modes.
EH-P.10 THU

Efficiency Characterization of Optical Vortex
Generation with Nanoplasmonic Media∙E.I. Albar1 , F. Bonafe1 , V. Kosheleva1 , A. Rubio1,2 , and
H. Appel1 ; 1 Max Planck Institute for Structure and Dynamics of Matter, Hamburg, Germany; 2 Center for Computational Quantum Physics (CCQ), New York, USA
We perform numerical simulations where we employ
Archimedean spirals and other gold nanoplasmonic
structures in order to generate optical vortices . We characterize efficiencies of such structures and address thegeneration mechanism of orbital angular momentum inelectromagnetic fields.
EH-P.11 THU

Minimizing the Focal Shift Effect on 2D Metalenses∙S. Aksu; Koç University, Istanbul, Turkey
We show that the numerical aperture is fundamentally
critical to minimize the focal shift effect on 2D metalenses to obtain symmetric focal intensity distribution,
which leads to better performing dielectric metalenses
in near and mid-IR.
EH-P.12 THU

Hydrodynamic Model of Plasmonic Crystal in
Magnetic Field∙I. Gorbenko and V. Kachorovskii; Ioffe Institute, St. Petersburg, Russia

EH-P.16 THU

EH-P.19 THUHigh entropy alloy for midinfrared metasurfaces∙Y. Nishijima and T. Sudo; Yokohama National University, Yokohama, Japan
We have evaluated the optical permittivity of High entropy alloys and their components for mid-infrared plasmon applications

Self-Assembled Deep Ultraviolet Rhodium nanogap
antenna to enhance single protein autofluorescence∙P. Roy1 , S. Zhu2 , J.B. Claude1 , J. Liu2 , and J.
Wenger1 ; 1 Aix Marseille Univ, CNRS, Centrale Marseille, Institut Fresnel, AMUTech,13013, Marseille,
France; 2 Department of Chemistry, Duke University,
Durham,27708, North Carolina, USA
Self-assembled label-free detection platform for single
proteins in DUV range using natural autofluorescenceand Rh Dimer gap antenna design, showing 2 orders
higher enhancement than confocal methods and 1 orderhigher than current state-of-the-art techniques.

EH-P.14 THU

EH-P.17 THUGraphene enhanced absorption entailed by theelectromagnetic field localization in a photonic
structure∙E. Otero1 , M. Grande2,3 , J. Trull1 , N. Akozbek4 , A.
D’Orazio2 , G.V. Bianco3 , G. Bruno3 , M. Scalora4 , and C.
Cojocaru1 ; 1 Department of Physics, Universitat Politècnica de Catalunya, Terrassa, Spain; 2 Department of Electrical and Information Engineering, Politecnico di Bari,
Bari, Italy; 3 CNR-NANOTEC, Bari, Italy; 4 Aviation andMissile Center, US Army CCDC, Redstone Arsenal, USA
We measure a 3.6-fold optical absorbance enhancementin graphene monolayers when placed onto a photonic
structure designed to localize the electromagnetic field
at its surface, with respect to the same layers without thestructure.

We discuss terahertz excitation of plasmonic crystal(multigated structure with periodic modulation of electron density) placed in magnetic field. We demonstratethat transmission spectrum of such a structure can becontrolled by the magnetic field.
EH-P.13 THU

Plasmon-Mediated Singlet Fission Dynamics in
TIPS-PEN near Silver-Organic interface∙P. Kolesnichenko1,2 , M. Hertzog1 , F. Hainer1,2 , F.
Deschler1,2 , J. Zaumseil1 , and T. Buckup1,2 ; 1 Instituteof Physical Chemistry, Heidelberg, Germany; 2 Centre forAdvanced Materials, Heidelberg, Germany
Plasmon-mediated singlet fission dynamics near silverorganic interface was observed. Changing the local electric field energy in the organic layer allows for tuning
the singlet fission yield in the broad range from ~70% to~180%.
EH-P.15 THU

Magnetoelectric coupling in partial double-slotted
all-dielectric resonator∙M. Pradhan, S. Sharma, S.B.N. Bhaktha, and S.K. Varshney; Indian Institute Of Technology Kharagpur, Kharagpur, India
Magnetoelectric coupling parameters in conjunction
with the anapole state are obtained in a partial doubleslotted all-dielectric silicon nanodisk resonator to enhance the bianisotropy for applications in nonreciprocity
and metachirality in the near-infrared region.

Excitation wavelength-dependent study to investigate
the mechanism of light-induced spectral redshift of asingle gold nanorod∙P. Ghosh1 , A.L. Chakraborty1 , and S. Khatua2 ;1
Department of Electrical Engineering, Indian Institute of Technology Gandhinagar, Gandhinagar, India;
2
Department of Chemistry, Indian Institute of Technology Gandhinagar, Gandhinagar, India
We report experimental observations of a lightinduced wavelength-dependent reaction on a single
gold nanorod and demonstrate the possible mechanism
behind by study of spectral redshift in the photoluminescence spectrum of gold nanorods.
EH-P.18 THUGraphene-based optically transparent metasurfaces
for smart windows∙G. Magno1 , L. Caramia1 , G.V. Bianco2 , G. Bruno2 , A.
D’Orazio1 , and M. Grande1,2 ; 1 Polytechnic University ofBari, Bari, Italy; 2 CNR-NANOTEC, Bari, Italy
We investigate optically transparent programmable digital mmWaves metasurfaces for smart windows and urban surfaces, using CVD graphene elements. Electromagnetic response depending on the specific encodingshows beam splitting and RCS reduction capabilities.

NOTES

179

EH-P.20 THU

Graphene plasmonics: a comprehensive atomistic
modeling∙L. Nicoli, P. Lafiosca, T. Giovannini, and C. Cappelli;
Scuola Normale Superiore, Pisa, Italy
We present a novel atomistic model, namely ωFQ, capable of predicting the optical properties of graphenebased substrates in a colloidal dispersion with application to plasmonics and plamson-mediated surface enhanced spectroscopies.

CLEO

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/Europe-EQEC 2023

⋅ Friday 30 June 2023

Room 1 ICM

Room 2 ICM

Room 3 ICM

Room 4a ICM

Room 4b ICM

Room 5 ICM

Room 11 ICM

Room 12a ICM

Room 12b ICM

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

CM-8: Laserbased surfacefunctionalizationand sensors

CJ-7: Mid-IR
fiber sources

EA-6: Quantum
optics in imaging

CK-12: Photonic
crystalsCC-4: THz QCL

ED-5: Precision
metrology

Chair:
Olivier
Dulieu,Université
Paris-Saclay, Paris

Chair: Marcus Ossiander, Graz University ofTechnology / Harvard
University, Austria

CI-5: Quantum
and free-spacecommunications

CE-8: Photonic
integrated circuits

Chair: Jesper Laegsgaard,
Technical
University of Denmark,Lyngby,Denmark

EI-1: 2D van der
Waals materials:
fundamentals andapplications

Chair:
Christopher
Holmes, University ofSouthampton, United
Kingdom

Chair:
LucileRukowski,Instituteof Physics of Rennes,
Rennes, France

8:30

CJ-7.1 FRI (Invited) 8:30

EA-6.1 FRI (Keynote) 8:30

CK-12.1 FRI

8:30

EI-1.1 FRI (Invited) 8:30

CC-4.1 FRI

CE-8.1 FRI

8:30

ED-5.1 FRI (Invited) 8:30

GlassHarp - A Micromechanical Device
for Direct Measurement of Momentum
Transfer and Mass
Removal During
Laser Ablation∙B. Hermann and
Y. Bellouard; Ecole
PolytechniqueFédérale de Lausanne(EPFL),
Neuchâtel,Switzerland
Understanding laser
ablation is not only offundamental interest
but also relevant formaterial processing
and novel concepts
for
space
debrisremoval. We use amicro-mechanicaloscillator made ofglass to directly detect
momentum transfer
and mass removal
during ablation.

All soft glass fiber
components andsources∙M. Rochette; McGIll
University, Montreal,
CanadaThis
presentation
highlights the latest
progress at McGill
University
towards
the fabrication of
optical fiber components and opticalfiber sources made ofsoft glasses. Opticalfiber couplers and allfiber sources will bepresented.

Imaging at the singlephoton limit using
homodyne detection
O.
Wolley1 ,S.
Mekhail1 ,P.-A.
Moreau2,3 ,T.
Gregory1 , G. Gibson1 ,4,5
G. Leuchs , and ∙M.
Padgett1 ; 1 Universityof Glasgow, Glasgow,
UnitedKingdom;2
National Cheng Kung
University,
Tainan,Taiwan; 3 Center for
Quantum Frontiers of
Research and Technology, Tainan, Taiwan;
4
Max Planck Institutefor the Science ofLight,
Erlangen,Germany; 5 FriedrichAlexander-Universität, Erlangen-, Germany
Using homodyne detection we obtain images in the short-wave
infrared region of thespectrum with an illumination flux of order
one photon per image pixel despite thecamera having a noise
floor one to two orderof magnitude higher.

Direct Determinationof OptomechanicalPhotonic Crystal
Mechanical Mode
Profile via Quasi
Near-Field
Perturbation∙T. Martel1 and R.
1
Braive1,2,3 ;Centrede Nanosciences etde Nanotechnologies,
Palaiseau,
France;2
Université Paris Cité,
Paris, France; 3 Institut
UniversitairedeFrance, Paris, France
We describe preliminary results of a novel
method allowing thedirectmeasurmentof mechanical mode
spatial repartition in
optomechanical photonic crystals throughthe local pertubationof the optical andmechanical modes.

Top down exfoliationof 2D materials andcreation of theirartificial structures∙F. Liu; Stanford University, Stanford, USA
We have developed
scalable and controllable
top-down
techniques to exfoliate
van der Waals crystals
and create 2D flakes,
nanoribbons,andartificial stacks, which
are used for studies
of static and dynamic
properties.

THz optical solitonsin planarized
quantum cascade
double ring lasers∙P. Micheletti1 , U.
Senica1 , A. Forrer1 , S.
Cibella2 , G. Torrioli2 ,M. Beck1 , J. Faist1 ,andG.
Scalari1 ;1
ETH Zurich, Zurich,
Switzerland; 2 CNRIstituto di FotonicaeNanotecnologie,
Rome, Italy
We report THz opticalsoliton formation in
double-waveguidering QCL featuring
anomalous
dispersion.
Free-runningspectra with sech2
envelopes are presented together with
SWIFT measurement
showing 12 ps pulses
in the reconstructedemission time-profile.

High-Speed Interband Cascade Infrared Photodetectors
for Free-Space
Communication∙R. Szedlak1 ,A.
Lardschneider1 ,H.
12
Knötig , R. Weih , P.
Didier3 , O. Spitz3 , J.
Koeth2 , F. Grillot3 ,and B. Schwarz1 ;1Institute of Solid StateElectronics, TU Wien,
Vienna,Austria;2
nanoplus Nanosystems and TechnologyGmbH,
Gerbrunn,
3
Germany;
Institut
Polytechnique, LTCI
Telecom, Paris, France
We analyze the highspeed
performanceand electrical bandwidth of interband
cascadeinfrared
photodetectors.
Limitationsareinvestigatedandan application in afree-space communication system isdemonstrated.

Low-loss lithium
tantalate photonic
integrated circuits
C.
Wang1,2 ,∙Z.
Li1 , Y. Chen2 , K.
Huang2 , X. Ke2 , J.
Riemensberger1 , R.N.
Wang1 , X. Ou2 , andT.J.
Kippenberg2 ;1
Institute of Physics,
Swiss Federal Institute of Technology
Lausanne(EPFL),
Lausanne,
Switzer2
land;State Key
Laboratory of Functional Materials for
Informatics, Shanghai
Institute of Microsystem and Information
Technology, Chinese
Academy of Sciences,
Shanghai, China
We show the first
LiTaO3 photonic integrated circuits (PICs)
fabricated on a 4-inch
LiTaO3-on-insulator(LTOI) wafer with
optical loss as low
as 5.5 dB m-1 andhigh-yields at thewafer scale.

Entanglementenhanced frequency
comparison of two
optical atomic clocks
B.C. Nichol, R. Srinivas, D.P. Nadlinger,
P. Drmota, D. Main,
G. Araneda,
C.J.
Ballance, and ∙D.M.
Lucas; Oxford University, Oxford, United
KingdomWedemonstrateentanglementenhanced frequency
comparison of two
trapped-ion opticalatomic clocks, which
are connected via
a 4m optical fibre
quantum
network
link. We approach
the ultimate precision
allowed by quantum
mechanics – theHeisenberg limit.

CC-4.2 FRI

CI-5.2 FRI

CE-8.2 FRIChair:Nathalie
Destouches,
HubertCurien Laboratory, St.
Etienne, France
CM-8.1 FRI

CM-8.2 FRI

8:45

Textile Strain Sensor
by FemtosecondLaser-Induced
Graphene Formation
on Kevlar∙D. Yang, H.K. Nam,
T.-S.D. Le, Y. Lee, Y.R. Kim, S.-W. Kim,

CK-12.2 FRIChair:
ChiaraTrovatello, Columbia
University, New York,
USA

8:45

SupersymmetricCompactificationand Higher-Dimensional Rearrangement of Photonic
Lattices∙T.A.W. Wolterink, M.
Heinrich, and A. Sza-

Chair: Ileana-Cristina
Benea-Chelmus,
EPFL,
Lausanne,
Switzerland

8:30

8:45

Heterogeneous
Terahertz Quantum
Cascade Laser For
Ultra-Broadband
Emission∙M. Jaidl1,2 , M. Beiser2,3 , M. Giparakis2,3 ,M.A. Kainz1,2 , D.
180

Chair:
Peter Horak,
UniversityofSouthampton,
Soutampton, United
Kingdom
CI-5.1 FRI

8:30

8:45

Mapping relations
between the polarization, the higherorder and the orbital
angular momentum
Poincaré spheres forinner points∙D. Marco1,2 , M.d.M.

8:45

Wafer-scale Manufacturing of Ultralow Loss, High-density Si3 N4 Photonic
Integrated Circuits∙X. Ji, R.N. Wang,
Z. Qiu, and T.J. Kippenberg; Institute of

CLEO

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⋅ Friday 30 June 2023

Room 13a ICM

Room 13b ICM

Room 14a ICM

Room 14b ICM

Room 14c ICM

Room Osterseen ICM

Room 21 ICM

Room 22a ICM

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

8:30 – 10:00

JSIII-3: Photonic
accelerators I

CD-11: Nonlinear
metasurfaces

EF-7: Complex
fiber dynamics II

CH-13: IR &Raman sensing

CL-5:
Spectroscopy

Chair: Volker Sorger,
GeorgeWashington
University, Washington and Optelligence,
Upper Marlboro, USA

Chair: Thomas Zentgraf, Paderborn University, Germany

Chair: A. Pasquazi,
University of Loughborough, United Kingdom

Chair:
Christoph
Haisch,Technical
University of Munich,Germany

EE-2: Ultrafast
processes inionised media

EJ-3: Nonlinear
optics modeling &artificial intelligence

EC-1: Non-linear
and non-hermitian topologicalphotonics

Chair: Stefan Skupin,
Université de Lyon,
Lyon, France

Chair:
Daria
Smirnova, Australian
National University,
Canberra, Australia

JSIII-3.1 FRI (Invited) 8:30

CD-11.1 FRI (Invited) 8:30

EF-7.1 FRI

CH-13.1 FRI

Motivation and challenges for applying
photonic neuromorphic computing
technologies∙B. Offrein, E. Vlieg,
F.
Hermann,
L.
Carraria Martinotti,
and F. Horst; IBM
Research Europe Zurich, Rueschlikon,
Switzerland
New concepts are
required to improve
the power efficiencyof neural networks.
Analog in-memorycomputingsignalprocessing can improve the efficiency
by several ordersof magnitude. The
prospects of photonic
conceptswillbediscussed.

Localized States in
Nonlinear Topological Photonics∙D. Smirnova; Australian National University, Canberra, Australia; RIKEN, Wakoshi, Japan
We discuss nonlinear
effects in topologicalphotonic
lattices.
This covers nonlinear dynamics ofedge
wavepackets
propagatingalong
the domain walls
and scenarios ofmodulational instability development,
linked to topologicalproperties of energy
bands.

Experimental observation of phasemode-locking in
multimode gradedindex optical fiber∙F. Mangini1 ,M.
Ferraro1 , Y. Sun1 ,1
M. Zitelli , P. ParraRivas1 , T. Hansson2 ,V. Couderd3 , andS.
Wabnitz1 ;1
Sapienza
University of Rome, Rome,
2
Italy;
Linköping
University, Linköping
, Sweden; 3 Universitéde Limoges, Limoges,
FranceIn this work, wehave experimentallydemonstrated,using a holographic
mode decomposition
technique, that thebeam self-cleaning is
associated with both awell-defined thermodynamic distributionof the intensities and a
spatial phase-locking
among the modes.

EF-7.2 FRI

8:30

8:45

Phase conjugationand focusing in nonHermitian fibers∙K. Makris1,2 andD. Psaltis3 ; 1 ITCPPhysics Department,
University of Crete,
Heraklion,
Greece;Chair: Francesco Tani,
MPI for the Science ofLight, Erlangen, Germany

Chair: Dario Polli,
Politecnico di Milano,
Milano, Italy

8:30

EE-2.1 FRI (Keynote) 8:30

CL-5.1 FRI (Invited) 8:30

EJ-3.1 FRI (Invited) 8:30

EC-1.1 FRI (Invited) 8:30

Standardising
electric-fieldresolved molecularfingerprints∙M. Huber1,2 , M.
Trubetskov1,2 ,W.
Schweinberger1,2,3 ,1,2P.
Jacob ,
M.
Zigman1,2,3 ,F.
Krausz1,2,3 , and I.
1,2,4
1
Pupeza;Max
Planck Institute of
Quantum
Optics,Garching, Germany;
2
Ludwig Maximilian
University
Munich,Garching, Germany;
3
Center for Molecular Fingerprinting,
Budapest, Hungary;4
Leibniz Institute of
Photonic Technology,
Jena, Germany
Electric-field-resolved
spectroscopy (FRS) of
impulsively-excitedmolecular vibrations
enables backgroundfree detection ofsample-specificinformation.
Here,
we present a dataprocessing procedurethat preserves theconsequent sensitivity
advantage
while
removing instrumentspecificexcitation
information, thereby
standardizing
FRS
fingerprints.

Air Photonics∙S. Skupin; Institut Lumière Matière, UMR
5306 Université Lyon
1 - CNRS, Universitéde Lyon, 69622 Villeurbanne, France
Interacions of ionizing
ultrashort laser pulses
in ambient air are
frequenly exploited in
nonlinear photonics.
We review major
applications ranging
fromfemtosecond
filamentationandpulse compression tobroadband THz generation and describe
challenges and trends.

Unconventional
SERS: from metal/
plasmon-free towearable/flexible
SERS∙K. Goda; The University of Tokyo, Tokyo,
Japan
I present two types
ofunconventionalsurface-enhanced
Raman spectroscopy(SERS) with highmeasurement reproducibility,
namelyporouscarbonnanowires
andgold nanomesh as
SERS substrates formetal/plasmon-free
and wearable/flexible
SERS applications.

Complete computation of macroscopic
high harmonic
generation using
artificial intelligence∙J.M. Pablos-Marín,
J. Serrano, and C.
Hernández-García;
Universidad de Salamanca, Salamanca,
Spain
Artificial intelligence
allows us to perform
full
macroscopic
calculations of highharmonic generation
based on the TDSE.
We apply our method
to retrieve complex
topologicalEUV
harmonic structures,
revealing
characteristics that usualapproximations don’t
resolve.

Topological photonics with cavity
polaritons∙J. Bloch; Center for
NanoscienceandNanotechnology,
Palaiseau, FranceThis talk will address
the exploration of
topological photonics
using cavity polaritons.
The generalproperties of thisdrivendissipative
non-linear platform
will be discussed
together with the newooportunities
they
offer.

181

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Room 1 ICM

Room 2 ICM

9:00

Full control of surface roughness whenengraving transparent materials using
femtosecond laser
ablation∙E. Kažukauskas1 , S.
Butkus1,2 , V. Jukna1 ,D. Paipulas1 , and V.
1
Sirutkaitis1 ;Laser
ResearchCenter,Faculty of Physics,
Vilnius
University,
Vilnius,
Lithuania;
2
Light
Conversion,
Vilnius, Lithuania
In this study, weinvestigate the surface
roughness of laserengraved fused silica
samples and search
for ways to control it.

/Europe-EQEC 2023

Room 4a ICM
meit; University of Rostock, Rostock, Germany
Self-imaging photonic
lattices enable perfecttransfer of quantum
and classical states,
yet are challenging to
implement at scale.
We harness supersymmetry to engineer
compacted
twodimensional systems
exhibiting
equivalentcharacteristics
and experimentallyinvestigate
theirdynamics.

and Y.-J. Kim; KAIST(Korea Advanced Institute of Science andTechnology), Daejeon,South Korea
Strain sensors areused in the field ofadvanced healthcare,structural monitoring,and human-machineinterface. Here, we
introduce the directlaser conversion of
Kevlar textile to laserinduced graphene byfemtosecond laser for
implementing a strain
sensor.

CM-8.3 FRIRoom 3 ICM®

CJ-7.2 FRI

9:00

FBG-stabilized Dysprosium:fluoroindate mid-infraredfiber laser
Y. Ososkov, J. Lee,
T. Fernandez, ∙A.
Fuerbach,and S.
Jackson; MQ Photonics(Macquarie
University), Sydney,
Australia
We report a narrowlinewidth
laser
operation with afirst-reported highreflectivity
FBG
inscribed in the Dydoped
fluoroindate
glass.
The result
suggests significant
improvements
influoroindate
fiber
quality and implies
future developmentof high-power wavelength stabilized MIR
laser sources.

CK-12.3 FRI

9:00

Spectral topologicaledge state transfer indiamond photonic
latticesG.
CáceresAravena1,2 ,B.
Real1,2 , D. GuzmánSilva1,2 , ∙P. Vildoso1,2 ,I.
Salinas1,2 ,A.
Amo3 , T. Ozawa4 ,and R.A. Vicencio1,2 ;1DepartamentodeFísica, Facultad deCiencias Físicas y
Matemáticas,
Universidad de Chile,
Santiago,
Chile;
2
Millenium Institutefor Research in Optics- MIRO, Santiago,
Chile; 3 Univ. Lille,
CNRS, UMR 8523PhLAM-Physiquedes Lasers Atomes etMolécules,
F-59000
Lille, France, Lille,
4
France;Advanced⋅ Friday 30 June 2023

Room 4b ICM

EI-1.2 FRI

9:00

Control of electron
density in WSe2
monolayers via
photochlorination∙E.
Katsipoulaki1,2 ,I.
Demeridou1 ,G.
Vailakis1,3 ,P.
Patsalas4 ,G.
Kopidakis1,3 ,G.
Kioseoglou1,3 , and E.
Stratakis1,2 ; 1 Instituteof Electronic Structureand Laser,
Foundation for ResearchandTechnology,
Heraklion,
Crete,
Greece; 2 Departmentof Physics, Universityof Crete,
Heraklion, Crete, Greece;
3
Department
ofMaterials
ScienceandTechnology,
University of Crete,
Heraklion,
Crete,
Greece; 4 Departmentof Physics, Aristotle
University of Thessaloniki, Thessaloniki,
GreeceThis work is focusedon the study of the effect of photochemical
doping and thus theelectron/hole density
on the optoelectronic
properties of single
layers transition metal
dichalcogenides andtheir heterostructures.
182

Room 5 ICM

Room 11 ICM

Room 12a ICM

Theiner1,2 , B. Limbacher1,2 , M.C. Ertl1,2 ,A.M. Andrews2,3 , G.
Strasser2,3 , J. Darmo1,2 , and K. Unterrainer1,2 ; 1 Photonics
Institute, TU Wien,
Vienna,Austria;2
Center for Microand Nanostructures,
TU Wien, Vienna,
Austria; 3 Institute ofSolid State Electronics,
TU Wien, Vienna,
Austria
We present a heterogeneous
terahertz
quantum
cascadelaser consisting offive individual active
regions. The devices
emit in a spectral
range from 1.9 to
4.5 THz, covering a
bandwidth of 1.37
octaves.

Sánchez-López1,3 , C.
Hernández-García4 ,and I. Moreno1,5 ;1Instituto de Bioingeniería,
Universidad
Miguel Hernández deElche, E-03202 , Elche,
Spain; 2 Aix Marseille
Université,
CNRS,
Centrale
Marseille,
Institut Fresnel, UMR
7249, 13397, Marseille
Cedex 20, France;
3
DepartamentodeFísicaAplicada,
Universidad MiguelHernández de Elche,
E-03202, Elche, Spain;
4
Grupo de Investigación en Aplicacionesdel Láser y Fotónica,
DepartamentodeFísicaAplicada,
Universidad
deSalamanca, E-37008,
Salamanca,
Spain;
5
DepartamentodeCiencia de Materiales,Óptica y Tecnología
Electrónica,
Universidad
MiguelHernández de Elche,
03202, Elche, Spain
We study theoreticallyand experimentallythe mapping between
the points inside thePoincaré sphere (PS),the orbital angularmomentum PS, andthe higher-order PS
for vector beams
and present a newpartiallypolarized
light generator.

Physics, Swiss Federal
Institute of Technology
Lausanne, Lausanne,
SwitzerlandWedemonstrate
Si3 N4photonic
integrated
circuitsfeaturingultra-low
propagation loss andtight optical confinement, fabricated witha subtractive process.
We show an intrinsic
quality factor as highas 20×106 at 1.55
μm across a 100 mm
wafer.

CC-4.3 FRI

9:00

Surface-Emitting
Broadband THz
Quantum Cascade
Laser Frequency
Combs with InverseDesigned Waveguide
Facets∙S. Gloor, U. Senica, P.
Micheletti, M. Beck, J.
Faist, and G. Scalari;
ETH Zürich, Zürich,
Switzerland
We present a surface emitting THz
Quantum
CascadeLaser with inverse
designed facet showing frequency comb
emission over 800
GHz with 13mW ofpeak power and anantenna with beam
divergence below 20∘
at 20K.

CI-5.3 FRI (Invited) 9:00

High-rate quantum
key distribution overfree-space links∙T. Roger, R. Singh,
C. Perumangatt, D.
Marangon, P.R. Smith,
M. Sanzaro, and A.
Shields; Toshiba Eu-

CE-8.3 FRI

9:00

High-Efficiency
Grating Fiber-Chip
Couplers at Telecom
Wavelength inGallium Nitride-onSapphire Waveguide
Platform∙S. Kaniyar Prasanna
Kumar, S. Raghavan,
and S.K. Selvaraja;
IISc, Bengaluru, India
Abstract: Fiber-chip
grating couplers in
GaN-on-Sapphireplatform with Coupling efficiency of-4.1 dB/coupler isdemonstrated,
best
reported so far. This
enables developmentof possible strategies
to harness nonlinear
photonics with GaN
platform

Room 12b ICM

ED-5.2 FRI

9:00

Ultrafast and Subnanometer-Precision
Time-of-Flight
Detection of >1000
Space-to-WavelengthEncoded Optical
Pulses∙Y. Na and J. Kim;
KAIST,
Daejeon,South Korea
We
demonstrate
ultrafasttime-offlight detection with
sub-nm-precisionand ~6-mm nonambiguity-range
byelectro-optic
sampling of opticalfrequency
combs.
When combined withspace-to-wavelength
encoding, massively
parallel time-of-flightdetection of >1000
pulses can be realizedwith 260-megapixels/s
pixel-rate.

CLEO

Room 13a ICM

Room 13b ICM

CD-11.2 FRI

Impact of Photonic
Integration Platforms on the Performance of Neuromorphic Accelerators∙L. De Marinis1 , N.
Andriolli2 , S. Gupta3 ,and G. Contestabile1 ;1ScuolaSuperiore
Sant’Anna, Pisa, Italy;
2
CNR-IEIIT,
Pisa,
Italy; 3 Indian Instituteof Technology Patna,
Bihta, India
We
discusshowdifferent
photonic
integration
technologies affect theperformance of photonic neuromorphic
processors in termsof resolution, power
consumption
andfootprint efficiency.
The
investigation
highlights trade-offs
between the technolo-

Ultra-Fast HighContrast Optical
Modulation in Si
Metasurfaces
A. Trifonov1 ,K.
Zangeneh
Kamali2 ,K. Georgiev1 , L. Xu3 ,G. Crotti4 , U. Arregui
Leon4 , M. Rahmani3 ,G. Della Valle4 , ∙I.
Buchvarov1 , and D.
1
Neshev1,2 ;Sofia
University , Sofia,
Bulgaria; 2 Australian
National University,
Canberra, Australia;
3
Nottingham
Trent
University, Nottingham, United Kingdom;
4
Politecnico di Milano,
Milano, Italy
We demonstrate ultrafast
high-contrast
opticalmodulationof high-quality factor
crystalline
siliconmetasurfaces,
ex-

9:00

/Europe-EQEC 2023

Room 14a ICM

Room 14b ICM

Institute of Electronic
Structure and Laser(IESL)-FORTH,
Heraklion,
Greece;3
Optics Laboratory,
Ecole Polytechnique
Federale de Lausanne(EPFL),
Lausanne,
Switzerland
Phase
conjugation
and reverse propagation in media that
contain gain or loss
is impossible.
By
introducing the concept of Parity-Phase
conjugation (PPC),
we achieve perfectphase
conjugationand focusing in nonHermitian multimodeoptical fibers.

CH-13.2 FRI

EF-7.3 FRI

CH-13.3 FRI

2JSIII-3.2 FRI 9:00

®

9:00

Optoacoustic active
cooling in waveguides∙L.
Blázquez
Martínez1,2 ,P.
Wiedemann1,2 ,A.
Geilen1,2 , C. Zhu1 ,and B. Stiller1,2 ; 1 Max
Planck Institute for
the Science of Light,
Erlangen, Germany;
2
DepartmentofPhysics,
FriedrichAlexander Universität
Erlangen-Nürnberg,
Erlangen, Germany
We report the experimental realization ofactive cooling of GHz
acoustic phonons via
backward Brillouinscattering in a chalcogenide
photonic
crystal fiber.
We
measured an effective
cooling of 219 K fromroom temperature.

⋅ Friday 30 June 2023

Room 14c ICM

Room Osterseen ICM

Room 21 ICM

Room 22a ICM

CL-5.2 FRI

EJ-3.2 FRI

EC-1.2 FRI

8:45

Rotational FourierTransform Mid-IR
spectroscopy with a
Quantum Cascade
Laser frequency
comb
S. Markmann, M.
Franckié, M. Bertrand,
M. Shamohammadi,
A. Forrer, P. Jouy, M.
Beck, J. Faist, and ∙G.
Scalari; Institute forQuantum Electronics,
Department of Physics,
ETH Zürich, Zürich,
SwitzerlandWedemonstrate
fast, high-resolution
Mid-Ir spectroscopy
employing a quantum cascade laser
frequency comb anda fast rotational delay
line.
9:00

Mobile Raman
sensors for on-sitemeasurements toaddress agriphotonic and life
science applications∙K. Sowoidnich, M.
Maiwald, T. Filler, L.
Wittenbecher, and B.
Sumpf;
FerdinandBraun-Institut,
Leibniz-Institut
fürHöchstfrequenztechnik,
Berlin,Germany
Dual-wavelength
diode laser basedlightsourcesforshiftedexcitation
Raman
difference
spectroscopy
andtheir implementation
into portable Raman
sensor systems is presented. Application
examples on agricultural fields and in

9:00

Breath-Resolved
Monitoring of Metabolic Trace Gases
with Photothermal
Spectroscopy∙S. Wolf1 , C. Lindner1 ,T.
Trendle1 ,J.
Kießling1 ,J.
Wöllenstein1,2 ,1and F. Kühnemann ;1
Fraunhofer Institutefor Physical Measurement Techniques IPM,
Freiburg, Germany;
2
Laboratory for Gas
Sensors, Departmentof Microsystems Engineering, University
of Freiburg, Freiburg,
Germany
We present a photothermal
sensingsystem for metabolic
products in breathgas trace analysis.
The key features of
the used method
183

9:00

Nonlinear Propagation of Extreme
Pulsed Light: Ab
initio Computational
Study
A. Yamada1 ,∙S.
Yamada2 , and K.
Yabana3 ; 1 Research
Organization for Information Science andTechnology,
Tokyo,
Japan; 2 Kansai Photon
Science Institute, Kyoto, Japan; 3 Universityof Tsukuba, Tsukuba,Japan
Ab initio computational method for
propagation of highintensity
ultrashortpulsed light has beendeveloped.
Changefrom dielectric response to plasmareflection as wellas propagation ofhigh harmonics are

9:00

Edge state opticalfrequency combs inthe microresonatorbased Su-SchriefferHeeger model∙A. Tusnin1 , X. Ji1 , J.
Riemensberger1 ,A.
Stroganov2 , A. Tikan1 ,and T. Kippenberg1 ;1
Swiss Federal Institute of Technology
Lausanne(EPFL),
Lausanne,
Switzerland; 2 LIGENTEC SA,
Lausanne, Switzerland
We demonstrate thefirst observation of
opticalfrequency
combs in the edge
state of the SuSchrieffer-Heeger
model of coupled
opticalmicroresonators.
We show
soliton-induced edgebulk interaction andedge-state hopping

NOTES

CLEO

Room 1 ICM

CM-8.4 FRI

9:15

Laser-Induced Engineering of Nanomaterial Phase andShape for 3D Light
Control at the Nanoscale∙M. Elizarov, N. Li,
and A. Fratalocchi;
King Abdullah University of Science andTechnology, Thuwal,
Saudi Arabia
We present a threedimensional platformleveraging
lightinduced
control
over nanomaterials’
phase and geometry.
We
demonstrate
this technology inheterogeneous oxidepolymer rigid andflexiblenanostructures, reporting thehighest wide-gamut
structural color forlarge-scale laser color
printing.

Room 2 ICM

CJ-7.3 FRI

9:15

Tapered chalcogenide-glass rods for
multi-octave midinfrared supercontinuum generation∙E.
Serrano1 ,D.
Bailleul1 ,F.
Désévédavy1 ,A.
Nakatani2 , T. Cheng2 ,Y. Ohishi2 , B. Kibler1 ,and F. Smektala1 ;1
Laboratoire Interdisciplinaire Carnot deBourgogne, UMR 6303
CNRS-UBFC, Dijon,
2
France;ResearchCenter for Advanced
PhotonTechnology,
Toyota Technological
Institute,
Nagoya,Japan
We
demonstratethat tapered GeSe-Te
glass
rods
with
femtosecond
pumpingenables
efficient mid-infrared
supercontinuum
generationfrom
1.7 to 16 μm. This
alternative approach
opens up a new wayof stepping into the
15-20 μm waveband.

Room 3 ICM

EA-6.2 FRI

9:15

Quantum Holography with Heralded Single-photon
Source∙D.
Abramović1,2 ,N. Demoli1,2 ,M.
Stipčević2 ,andH.
Skenderović1,2 ;1Institute of Physics,
Zagreb,Croatia;2
RudjerBoskovic
Institute,
Zagreb,Croatia
We introduce holographic
quantum
imaging
schemebased on singlephoton states andbasicholographic
setup.
Our resultswith single photons
show enhancementof contrast in both
amplitude and phase
image compared toclassical light.

®

/Europe-EQEC 2023

Room 4a ICM
Institute for Materials
Research(WPI-AIMR), Tohoku
University,
Sendai
980-8577,
Japan,
Sendai, Japan
We study the edge toedge transfer of topological states in diamond photonic lattices via modifying the
wavelength of the input laser. In this way,
we observe the dynamical evolution of
the system.
CK-12.4 FRI

9:15

Mesoscopic SelfCollimation under
oblique incidence inhexagonal-latticemesoscopic photonic
crystal
S.I. Flores Esparza,∙O. Gauthier-Lafaye,
and A. Monmayrant;
LAAS-CNRS,
Toulouse, France
We demonstrate numerically mesoscopic
self-collimation
underarbitraryobliqueincidencein hexagonal-latticemesoscopic photonic
crystal and propose
a fast and simple
methodology
fordesign and parametric
exploration of suchgeometries.

⋅ Friday 30 June 2023

Room 4b ICM

EI-1.3 FRIRoom 11 ICM

Room 12a ICM

Room 12b ICM

CE-8.4 FRI

ED-5.3 FRI

rope Ltd, Cambridge,
United Kingdom
Practical applicationsofsatellite
QKD
require high encoding
rates in order to
distribute sufficient
key material in a shortperiod of time. We
show our efforts inbuilding
high-rate
QKD systems operating over free-spacelinks.

9:15

Nonlinear all-opticalcoherent manipulation and read-out ofvalleys in atomicallythin semiconductors∙P.
Herrmann1 ,S.
Klimmer1,2 ,T.
Lettau3 ,M.
Monfared3 ,U.
Peschel3,4 , and G.
1,4 1
Soavi ; Institute ofSolid State Physics,
Friedrich
Schiller
University Jena, Jena,
2
Germany;
ARC
Centre of ExcellenceforTransformative
Meta-Optical
Systems, Department ofElectronic Materials
Engineering, Research
School of Physics, The
Australian National
University, Canberra,
Australia; 3 Instituteof Condensed Matter
Theory and Optics,
Friedrich
Schiller
University Jena, Jena,
4
Germany;
Abbe
Center of Photonics,
Friedrich
Schiller
University Jena, Jena,
Germany
We report the coherent
ultrafast
generation and detection of valleys inatomically thin semiconductors,
based
on optical Stark shift
and second harmonic
generation.
Our
results are supported
by simulations basedon time-dependent
densityfunctional
theory.
184

Room 5 ICM

CC-4.4 FRI

9:15

Cryogen-free, QCLbased Free Space
THz Communication link∙A.
Sorgi1 ,M.
Meucci1 ,M.A.
Umair1 , F. Cappelli1 ,L. Viti2 , M. Vitiello2 ,J. Catani1 , and L.
Consolino1 ; 1 National
Institute of OpticsCNR(CNR-INO)
and LENS, Sesto
Fiorentino (Florence),
Italy; 2 NEST, CNR Istituto Nanoscienzeand Scuola Normale
Superiore, Pisa, Italy
Realizationofacryogen-free
FreeSpace Optical Communication (FSOC)
link between a 2.83
THz Quantum Cascade Laser (QCL)
as the source anda Graphene based
field-effecttransistor (GFET) as theroom-temperature
receiver.

9:15

Microscope Projection Photolithography-Enabled Structuring with Subwavelength Resolution∙L. Zheng1,2 ,C.
Reinhardt3 , and B.
1
Roth1,2 ;Leibniz
University Hannover,Hannover, Germany;2
Cluster of Excellence
PhoenixD(Photonics, Optics, andEngineering–Innovation
AcrossDisciplines),
Hannover, Germany;3
Bremen Universityof Applied Science,
Bremen, Germany
In this work, a lowcost UV-LED-based
projection lithography
technique is proposed
for rapid and efficient
high-resolution structuring. Gratings andcrossed waveguides
with subwavelengthfeaturesizes
aredemonstrated.

9:15

Nanometric Position
Metrology with
Topologically
Structured Light∙R.T. Sam1 , J.-Y. Ou1 ,K.F. MacDonald1 , andN.I. Zheludev1,2 ; 1 Optoelectronics ResearchCentre and Centre
for Photonic Metamaterials, UniversityofSouthampton,
Southampton, United
Kingdom; 2 Centre for
Disruptive Photonic
Technologies,
TPI,
SPMS, Nanyang Technological University,
Singapore, Singapore
We introduce an‘optical ruler’ forsingle-shot,
realtime detection of
nanometricdisplacements,
down
to λ/400, throughthe visualization of
singularities in thefield generated by aPancharatnam-Berryphase
metasurface,
using a polarizationsensitive camera.

CLEO

Room 13a ICM

Room 13b ICM

gies without a clear
winner.

hibiting asymmetricbound-state in thecontinuum
mode.
Over 25% amplitude
modulation
is observed with
25ps relaxation time,
driven by carrier
injection.

Room 14a ICM®

/Europe-EQEC 2023

Room 14b ICM⋅ Friday 30 June 2023

Room 14c ICM

clinical environments
will be discussed.

Room Osterseen ICM

Room 21 ICM

and the implicationsofbreath-resolved
measurementsarediscussedattheexample of breath
N2O.

described in a unified
way.

Room 22a ICM

EC-1.3 FRI

JSIII-3.3 FRI 9:15

CD-11.3 FRIArtificial Neural
Network Training on
an Optical Processor
via Direct Feedback
Alignment∙K.
Müller1 ,J.
1Launay , I. Poli1 ,M. Filipovich1 , A.
Capelli1 , D. Hesslow1 ,I. Carron1 , L. Daudet1 ,F. Krzakala1,2 , and S.
Gigan1,3 ; 1 LightOn,
Paris,
France;2
École PolytechniqueFédérale de Lausanne,
Lausanne,
Switzer3
land;
Laboratoire
Kastler Brossel, Paris,
FranceWe
trainneuralnetworks up to one
millionparameterswith
anopticalprocessor via Direct
Feedback
Alignment.
Simulations
show it can scale toover half a billion
parameters.
We
compare its performance to traditional
backpropagation.

Second harmonic
generation in periodical metal-insulator-metal nanoparticle arrays∙S. Beer1 , J. Gour1 , U.
Mir1 , A. Alberucci1 ,U.D. Zeitner1,2,3 , and
S. Nolte1,2 ; 1 Friedrich
Schiller
University
Jena,
Institute ofApplied Physics, Jena,
Germany; 2 Fraunhofer
Institute for Applied
Optics and Precision
Engineering IOF, Jena,
3
Germany;
MunichUniversity of Applied
Sciences, Department
of Applied SciencesandMechatronics,
Munich, GermanyWeexperimentallyinvestigate
secondharmonic generationfrom periodic arraysof nano-bars featuring
verticallystackedmetal-insulator-metal
nano-junctions. We
prove how the propagation of nonlocal
plasmonsstrongly
affects the emission
by determining thephase of the nonlinear
dipoles.

9:15

EF-7.4 FRI

9:15

Spatio-temporal
Mode Characterization of Disordered
Weakly Nonlinear
Graded-index
Multimode Fibers∙M.
Zitelli1 ,V.
Couderc2 ,M.
Ferraro1 , F. Mangini1 ,P. Parra-Rivas1 , Y.
Sun1 , and S. Wabnitz1 ;1
Department of Information Engineering,Electronics
andTelecommunications,
Universitàdegli Studi di Roma
Sapienza,
Rome,
Italy; 2 Université deLimoges, XLIM, UMR
CNRS 7252, Limoges,
FranceWe
experimentally
analyze the steadystate output modal
distribution producedby linear random
mode-coupling andweak nonlinearity inmultimode fibers. The
modal
distribution
is reconstructed by anovel 3D propagation
method, accounting
for dispersive effects
and loss of coherence.

CH-13.4 FRI

9:15

EE-2.2 FRI (Invited) 9:15

CL-5.3 FRI

Detecting the
hybridization of
circulating tumor
DNA by nitride
surface-enhanced
Raman spectroscopy∙T.A.N. Nguyen, C.L. Luo, F.-C. Chien,
and K.-Y. Lai; National Central University, Taoyuan , Taiwan
Surface-enhanced
Raman spectroscopy(SERS) is a promising tool for cancer
diagnosis. However,
SERS biosensors face
the challenges oftedious process andsignalfluctuation.
InGaN
quantum
wells can address theissues and achieve
the single-moleculesensitivity.

Ultrafast physics ofBessel beam interaction with solid
dielectrics: dense
plasma formation,
second harmonic
and THz radiation
K.
Ardaneh,M.
Hassan, B. Morel, L.
Furfaro, L. Froehly,
R. Giust, and ∙F.
Courvoisier; FEMTOST Institute, Univ.
Franche-Comte and
CNRS,
Besancon,FranceWhenpropagating
insidesapphire,
an ultrafast Bessel
beam creates a highaspect ratio cylinderof plasma with asubwavelength
diameter that extends
over several tensofmicrometers.
Particle-in-cell simulations reveal SHG
and THz radiation.

Rapid rasterscanning fieldresolved infrared
spectroscopy∙H.
Mirkes1 ,D.
Gerz1,2,3 ,F.
Lindinger1,2 ,M.
Huber2,3 ,and I.
Pupeza1,2,3 ; 1 Ludwig
Maximilians University Munich, Facultyof Physics, Garching,
2
Germany;Max
Planck Institute of
Quantum
Optics,Garching, Germany;
3
Leibniz Institute of
Photonic Technology,
Jena, Germany
By raster-scanning aprobe in a high-speed
electro-opticsampling spectrometer, we demonstratebroadband infrared
spectro-microscopy
with spatial resolutionof 18 μm and an
intensity
dynamic
range of 315000 for
45x5000-pixel images
acquiredin140
seconds.

185

9:15

EJ-3.3 FRI

9:15

Dissipative light bullets and 3D breathers
in a passive coherently driven multimode
Kerr cavity∙Y. Sun1 , P. ParraRivas1 , C. Milián2 ,Y.V.
Kartashov3 ,M.
Ferraro1 ,F.
Mangini1 , M. Zitelli1 ,R.
Jauberteau1 ,F.R. Talenti1 , andS.
Wabnitz1,4 ;1Sapienza Universityof Rome,Roma,
2
Italy;
Universitat
Politècnica de València, València, Spain;
3
RussianAcademyof Sciences, Moscow,
4
Russia;Istituto
Nazionale di Ottica,
Pozzuoli, Italy
We study the formation and bifurcation
structure of robust
lightbullets
and3D breathers in a
coherently
driven,passivemultimode
Kerr cavity with athree-dimensional
potential.

9:15

PT-Symmetric Topological Insulator in a
Photonic Waveguide
Array
∙A.
Fritzsche1,2 ,T.
Biesenthal1 ,L. Maczewsky1 , K.
Becker1 , M. Ehrhardt1 ,M.
Heinrich1 ,R.
Thomale2 ,Y.
Joglekar3 ,and A.
Szameit1 ; 1 Institute ofPhysics, University of
Rostock, Rostock, Germany; 2 DepartmentofPhysics
andAstronomy,
JuliusMaximiliansUniversität Würzburg,
Würzburg, Germany;
3
DepartmentofPhysics,
Indiana
University-Purdue
University
Indianapolis(IUPUI),
Indianapolis, USAWe
presenta
two-dimensional PTsymmetric topologicalinsulator experimentally realized in aphotonic waveguidearray. The discussed
model is based on aperiodicallydriventopological insulator
and relies on thespatiotemporal distribution of gain and
loss.

NOTES

CLEO

Room 1 ICM
CM-8.5 FRI

9:30

Room 2 ICM
CJ-7.4 FRI

9:30

Room 3 ICM
EA-6.3 FRI

9:30

®

/Europe-EQEC 2023

Room 4a ICM

Room 4b ICM

CK-12.5 FRI

EI-1.4 FRI

9:30

Laser-induced surface metallisation for
the fabrication of 3D
printed electronics∙E. Kabouraki1 , A.
Chrostek-Mroza2 ,T.L. See2 , C. Powley2 ,M. Farsari1 ,andR.N.
Esfahani2 ;1
IESL/FORTH,
Heraklion,
Greece;2
Manufacturing
Technology
Centre,Coventry,
UnitedKingdom
The manufacturing of
3D printed electronics is presented, involving laser patterning on i) a commercial polymer used in
3D printing and ii) a
synthesized resin thatcan be spray coated onany 3D printed part.

Towards Watt-level,
Spectrally Flat Supercontinuum frommid-IR Mode-locked
Fibre Laser∙B. Dutta Gupta1,2,3 ,I.
Hendry1,2,3 ,S.
Tang1,2,3 ,M.
Erkintalo1,2 ,andC.
Aguergaray1,2,3 ;1
DepartmentofPhysics, University of
Auckland, Auckland,
New Zealand; 2 The
Dodd-Walls
Centrefor Photonic andQuantum Technologies, Dunedin, New
Zealand; 3 The Photon
Factory, University of
Auckland, Auckland,
New ZealandWe
numericallydemonstrate supercontinuum generationinErbium-doped
ZBLAN fibres from a
2.8 μm seed source.
We achieve significantly
improved
spectral flatness withmore than 60% of output power converted
to 3-4.8 μm region.

Quantum Ghost
Imaging in reverse
START-STOP with a
2D SPAD array∙V.F.
Gili1 ,
D.
Dupish1 , A. Vega2 ,M. Gandola2 ,E.
Manuzzato2 ,M.
Perenzoni2 ,L.
Gasparini2 ,T.
1,3Pertsch ,andF.
Setzpfandt1,3 ;1Friedrich-SchillerUniversität
Jena,
Institute of Applied
Physics, Abbe Centerof
Photonics,
Jena,
Germany;2
Fondazione Bruno
Kessler, Trento, Italy;3
Fraunhofer Institutefor Applied Optics andPrecision Engineering,
Jena, Germany
We present a quantum ghost imaging
implementation basedon a 2D SPAD array,enabling to image an
object in 10 seconds,
without
frame-rateand delay line limitations, advancing thestate-of-the-art.

Watching Polaritonson the Fly: From
Enhanced Diffusion
to Ultrafast Ballistic
Motion∙M.
Balasubrahmaniyam,
A.
Simkhovich,A.
Golombek, G. Sandik,
and T. Schwartz;
PhysicalChemistry
Department, Facultyof Exact Sciences, Tel
Aviv University, TelAviv, Israel
Using ultrafast microscopy, we revealthat strong lightmatter coupling canenhance the diffusionof excitons by 106
and even boost theirtransport to ballistic at
2/3 the speed of lightover
macroscopic
distances, completely
overcoming different
scattering processes.

CM-8.6 FRI

CJ-7.5 FRI

EA-6.4 FRI

CK-12.6 FRI

9:45

Progress in Preforming Whispering Gallery Mode Resonant
Disks via Femtosecond Laser Machining∙P.-A.
Lacourt1 ,F. Courvoisier1 , J.
Safioui2 , L. Furfaro1 ,andL.
Larger1 ;1
Institut FEMTO-ST,
Université de FrancheComté,
Besançon,France; 2 Femto Engineering, Besançon,FranceA novel production
technique of Whis-

9:45

Mid-Infrared AllSpliced Cascaded
Supercontinuum
Generation∙C.R. Petersen1,2 andO. Bang1,2 ; 1 DTU
Electro, Kgs. Lyngby,
Denmark; 2 NORBLISApS, Virum, Denmark
We present an investigation into all-spliced
supercontinuum generation based on silica, germania, fluoride, and chalcogenide
fibers. We review theliterature and present

9:45

Rydberg Atomic
Microwave-to-Optical Converter in a
Free-Space Continuous-Wave Operation
Mode∙S. Borówka1,2,3 , U.
Pylypenko1,2 ,M.
Mazelanik1,2 , and M.
1
Parniak1,4 ;Centrefor Quantum Optical
Technologies, Centreof New Technologies, University of
Warsaw,
Warsaw,
Poland; 2 Faculty ofPhysics,
University⋅ Friday 30 June 2023

9:45

FRET-mediatedcollective blinking ofself-assembled stacks
of semiconducting
nanoplatelets
Z.
Ouzit1 ,∙G.
Baillard1 , J. Pintor1 ,L.
Guillemey2 ,B.
Wagnon2 ,B.
Abecassis2 , and L.
1 1
Coolen ; Institut desNanosciences de Paris,
Paris, France; 2 Ecolenormale supérieur ,Lyon, FranceWeuse
microphotoluminescence

9:30

Radiative suppression of exciton-exciton annihilation in a
two-dimensional
semiconductor∙L. Sortino1 ,M.
Gülmüş1 , B. Tilmann1 ,L. de Souza Menezes1 ,and S.A. Maier2,3,1 ;1Chair in Hybrid
Nanosystems,
FacultyofPhysics,
Ludwig-MaximiliansUniversität München,
Munich,Germany;2School of Physics
andAstronomy,
MonashUniversity,
Clayton,Australia;
3
The Blackett Laboratory, Department of
Physics, Imperial College London, London,
United Kingdom
Exciton-exciton
annihilation(EEA)
processes set a fundamental limit for
the applications of
2D semiconductors.
Here, we demonstratesuppression of EEA ina monolayer WS2 via
enhancement of lightmatter interaction in
hybrid 2D-dielectric
nanophotonic
platforms.
EI-1.5 FRI

9:45

High-speed acoustooptic modulation at
optical communication band by ultrafast-laser-induced
hypersonic vibrational coherence∙T.G. Park1 ,E.T.
Oh1 , H.R. Na2 , S.-H.
Chun2 ,
S.
Lee2 ,and F. Rotermund1 ;1
DepartmentofPhysics, Korea Advanced Institute of186

Room 5 ICM
CC-4.5 FRI

9:30

Room 11 ICM

Room 12a ICM

Room 12b ICM

CI-5.4 FRI

CE-8.5 FRI

ED-5.4 FRI

9:30

High-performanceFrequency Combs
with Planarized THz
Quantum Cascade
Lasers∙U.
Senica1 ,A.
Forrer1 , T. Olariu1 ,P. Micheletti1 ,S.
Gloor1 , S. Cibella2 , G.
Torrioli2 , M. Beck1 ,J. Faist1 , and G.
Scalari1 ; 1 Institute forQuantum Electronics,
Zurich, Switzerland;
2
Istituto di Fotonica e
Nanotecnologie, CNR,
Rome, Italy
We present several
newplanarizedwaveguidecomponents for highperformanceTHzquantum
cascadelaser
frequency
combs with improved
comb
bandwidths,
high-temperature
operationandhigh-power surface
emission
intoanarrow beam.

Cylindrical Vector
Vortex Beams
Generation with aSingle Phase
Encoded Spatial
Light Modulator∙A. Srinivasa Rao1,2,3 ,P. Kumar1,2 ,andT.
Omatsu1,2 ;1Graduate School ofEngineering,
Chiba
University,
Chiba,
2
Japan;
Molecular
Chirality
Research
Centre, Chiba University, Chiba, Japan;
3
Institute for Advanced
AcademicResearch,
Chiba
University,
Chiba,Japan
We demonstrate acompact, robust andlow-cost technique toconvert a Gaussianlaser beam into acylindrical
vectorvortexbeamof
all possible orders
through the modulation of a single-phasepattern with an SLM.

CC-4.6 FRI

CI-5.5 FRI

9:45

Improving the performance of terahertz quantum cascade laser sources
based on Cherenkov
difference-frequency
mixing throughphase matching∙W.
Oberhausen1 ,I.
Lubianskii1 ,G.
Boehm1 ,A.
Strömberg2 ,B.
Manavaimaran2 , D.
Burghart1 , Y.-T. Sun2 ,and M.A. Belkin1 ;1
WalterSchottkyInstitut and Depart-

9:45

Characterizing alloptical biasing andreadout of a superconducting optoelectronic circuit∙F. Thiele, T. Hummel,
J. Brockmeier, M.
Protte, S. Lengeling,
V. Quiring, C. Eigner,
C. Silberhorn, and T.
Bartley; Institute for
Photonic
Quantum
Systems, Paderborn,
GermanyWedemonstrate
all-optical operationof an SNSPD. Us-

9:30

Liquid Phase Epitaxy
growth and spectroscopy of Tb3+-doped
LiYF4 crystalline
layers for visible
waveguide lasers∙A. Baillard1 ,P.
Loiko1 , G. Brasse1 ,R.M.
Solé2 ,
M.
Aguiló2 , F. Díaz2 , X.
2
Mateos , A. Benayad1 ,A. Braud1 , and P.
Camy1 ; 1 Centre deRecherche sur les Ions,
les Matériaux et la
Photonique (CIMAP),
UMR 6252 CEACNRS-ENSICAEN,
Université de Caen
Normandie,
Caen,
France; 2 Universitat
Rovira i Virgili (URV),
Tarragona, Spain
Tb3+,Gd3+-codoped
LiYF4
singlecrystalline
layerswere grown on LiYF4
substrates by Liquid
Phase Epitaxy. The
polarized
spectroscopic
properties
of Tb3+ ions werestudied showing agreat potential for thedevelopment of green
and yellow waveguidelasers.
CE-8.6 FRI

9:45

Ductile dicing for
optical facets andwaveguides in silicon
nitride∙P.C. Gow,
G.M.
Churchill, V. Vitali,
T. Dominguez Bucio, P. Petropoulos,
F.Y. Gardes, C.B.E.
Gawith,and J.C.
Gates;
Optoelectronics
Research
Centre,UniversityofSouthampton,
Southampton, United

9:30

Dual-comb laserinterferometer for
temperature independent strain
sensing∙H.J. Kbashi1 ,B.
Sheil2 ,and A.M.
1
Perego1 ;Aston
University,
Aston
InstituteofPhotonics
Technologies,
Birmingham, United
Kingdom; 2 Universityof Cambridge, Laing
O’Rourke
CentreforConstruction
Engineering and Technology,
Cambridge,
United Kingdom
Weexperimentallydemonstrate a modelocked fiber laser
exhibiting dual-comb
interferencedue
to an intracavity
Mach-Zehnder interferometer.
Suitably
stretching the laser
cavity causes changes
in the optical andRF spectrum hence
enabling temperatureindependent
strainsensing.
ED-5.5 FRI

9:45

Single-Shot, Wavelength-Resolved Polarization Measurement of Ultrafast
Lasers based on
Dispersed Divisionof-Amplitude∙L. Gao1 , Q. Wu1 , Y.
Cao1 , S. Wabnitz2,3 ,Z.
Chang1 ,A.
Liu1 ,
J. Huang1 ,L. Huang1 , and T.
1
Zhu1 ;
Chongqing
University, Chongqing,
2
China;
Sapienza
Università di Roma,
Roma, Italy; 3 Istituto

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Room 13a ICM

Room 13b ICM

Room 14a ICM

Room 14b ICM

JSIII-3.4 FRI 9:30

CD-11.4 FRI

EF-7.5 FRI

CH-13.5 FRIPhotonic Neuromorphic Accelerator
Com- bined with an
Event-Based Neuromorphic Camera for
High-Speed Object
Classification∙A. Tsirigotis1 ,I.
Tsilikas2 , K. Sozos3 ,A.
Bogris3 ,andC.
Mesaritakis1 ;1
University of the
Aegean,Dept.
Information and Communication Systems
Engineering, Samos,
2
Greece;National
Technical Universityof Athens,
Dept.
Applied Physics andMathematics, Athens,
Greece; 3 3. Universityof West Attica, Dept.
Informatics and Computer
Engineering,
Egaleo, Greece
Here we provide experimental evidence
that an unconventional
photonic
convolutional accelerator based on optical
spectrumslicing,
when combined witha high-speed neuromorphic camera canoffer a classification
accuracy
increaseby 19% in object
classification.

Enhancing Nonlinear Effects throughLattice Plasmon
Excitation in Plasmonic Metasurfaces∙J. Gour1 , S. Beer1 , A.
Alberucci1 , C. David2 ,S. Nolte1,3 , and U.D.
Zeitner1,3,4 ; 1 Friedrich
Schiller
University
Jena,
Institute ofApplied Physics, Jena,
Germany; 2 Friedrich
Schiller
University
Jena, Institute of Condensed Matter Theory
and Optics, Jena, Ger3
many;
Fraunhofer
Institute for Applied
Optics and Precision
Engineering IOF, Jena,
4
Germany;
MunichUniversity of Applied
Sciences, Department
of Applied SciencesandMechatronics,
Munich, Germany
We conduct a parametric study andshow an enhancementof second and third
harmonic generationfromplasmonic
metasurfaces.
Themaximum enhancement occurs either
at the double resonance condition orwhen two counterpropagating
lattice
plasmons exist.

JSIII-3.5 FRI 9:45

Performance enhancement via synaptic plasticity in
an integrated photonic recurrent neuralnetwork with phasechange materials∙A.
Lugnan1 ,S.
Aggarwal2 ,F.
BrückerhoffPlückelmann3 ,W.H.P.
Pernice3 ,CD-11.5 FRI

9:30

9:45

Bandwidth-Engineered Ultra-Fast
Time-Variant Metasurfaces∙Z. Yang1 , M. Liu1 ,D.
Smirnova1 ,A.
Komar1 ,M.
Shcherbakov2 , and D.
Neshev1 ; 1 Australian
National University,
Canberra,
Aus-

9:30

Single-source FM
SRS with pixel-topixel contrast improvement∙K.
Wallmeier1 ,T.
Würthwein1 ,T.
Hellwig2 ,M.
Brinkmann2 ,N.
Lemberger1 , and C.
Fallnich1,3 ; 1 Instituteof Applied Physics,
University of Münster,
Münster,
Germany;2
Refined Laser Systems GmbH, Münster,Germany; 3 Cells in
Motion Interfaculty
Centre, University of
Münster,Münster,
GermanyFrequency
modulation
stimulated
Raman
scattering
is presented with asingle light source
onlyby
exploiting
pulse-to-pulse
wavelength-switchingwith the result of up
to 8.3-fold contrast
improvement and 50% lower pixel dwelltime.

EF-7.6 FRI

CH-13.6 FRI

9:45

Room 14c ICM

9:30

Light-by-lightcontrol enabled byincoherent beam
superpositions in
multimode fibres
T.
Mansuryan1 ,Y. Arosa Lobato2 ,∙A. Tonello1 ,M.
Ferraro3 , M. Zitelli3 ,F. Mangini3 , Y. Sun3 ,K. Krupa4 , B. Wetzel1 ,S. Wabnitz3 , and V.
Couderc1 ; 1 Universityof Limoges , Limoges,
2
France;Universityof Santiago de Compostela, Santiago deCompostela,
Spain;
3
DIET,
Sapienza,
University of Rome,
Rome, Italy; 4 Instituteof Physical Chemistry,
Polish Academy of
Sciences,
Warsaw,
PolandWe demonstrate lightby-light control of a
weak wave by a strong
pump at a different
wavelength in GRIN
multimode fibre. We
obtained an increasing or decreasing M2
as a function of thepump power.
Advanced spatiotemporal manipulation of nonlinear
waves and solitons
using a recirculatingfiber loop
∙F. Copie, P. Suret, and
S. Randoux; Laboratoire PhLAM, Université de Lille, Villeneuved’Ascq, France
We present experiments realized in arecirculating
fiber
loop
demonstrating
spatiotemporal
manipulationof⋅ Friday 30 June 2023

9:45

A highly sensitive
SERS substrate fordetection of nanoplastics in water∙A. Bibi1 , J. Tate2 , D.
Hill1 , and C. Cao2 ;1Aston Institute of
Photonic Technologies,
Aston
University,
Birmingham, United
Kingdom; 2 Institutefor
GlobalFood
Security, School of
Biological
Sciences,
Queen’s University ofBelfast, Belfast, United
Kingdom

EE-2.3 FRI

9:45

Retrieving Optical
Information
Through Propagation in Strongly
Nonlinear and Turbulent Systems Using
Neural Networks∙P.
Konstantakis1,2 ,M.
Manousidaki1 ,V.Y. Fedorov3 , andS.
Tzortzakis1,2,3 ;1Institute of Electronic
Structure and Laser,
Foundation for Research and Technology
Hellas(FORTH),
Heraklion,
Greece;187

Room Osterseen ICM

Room 21 ICM

Room 22a ICM

CL-5.4 FRI

EJ-3.4 FRI

EC-1.4 FRI

9:30

9:30

9:30

Dual-Color Confocal
Fluorescence Characterizations of Antibody Loading in Bioengineered Nanovesicles∙M.
Sanaee1 ,K.G.
Ronquist2 ,J.M.
Morrell2 ,E.
Sandberg1 ,J.
Widengren1 , and K.
Gallo1 ; 1 Department
of Applied Physics,
KTH Royal Institute of Technology,
Stockholm, Sweden;
2
DepartmentofClinical Sciences, SLU
Swedish University ofAgricultural Sciences,
Uppsala, Sweden
An ad-hoc experimental methodology
based on dual-color
confocal fluorescencemicroscopy
hasbeen developed forquantitative characterizations of bioengineered nanovesicles
loaded with Ab anddUTPmolecules,
demonstrating theirsuccessful loading at
single vesicle level.

Deep-Learningbased VCSEL transmitter emulator
S. Deligiannidis1 , N.
Argyris2 , S. Dris2 ,D.
Kalavrouziotis2 ,P.
Bakopoulos2 ,C.
Mesaritakis3 ,and∙A.
Bogris1 ;1
University of West
Attica,Department
of Informatics andComputer Engineering, Egaleo, Greece;
2
NVIDIA,
Athens,3
Greece;Universityof the Aegean, Dept.
Information and Communication Systems
Engineering, Samos,
GreeceWe train two recurrent neural networkmodels to mimic thenonlinear dynamics
of a directly PAM-4
modulated
VCSEL.
The prediction accuracy in different
operatingregimesachieves mean squareerror down to 2%.

Efficient and direct
design of edge andinterface states∙H.
Schomerus;
Lancaster University,
Lancaster,
UnitedKingdom
I describe an efficientapproach that allows
to design edge statesat arbitrary energies.
The approach canmake effective use of
topological symmetries, but also applies
tonon-Hermitianandnonreciprocalsystems.

CL-5.5 FRI

EJ-3.5 FRI

EC-1.5 FRI

9:45

Inclusive development of Ramanbased prostatecancer diagnostic
device: lessons froman ethnically-diverse
clinical trial∙S.J. van Breugel1,2,3 , I.
Low4 , M.L. Christie4 ,M.R. Pokorny4 , H.U.
Holtkamp1,3 ,M.K.
Nieuwoudt1,2,3 , M.C.
Simpson1,2,3,5 ,K.
ZargarShoshtari4,6 ,andC.
Aguergaray2,3,5 ;1School of Chemical

9:45

Long-range Prediction of Nonlinear
Dynamics in Fibre
Optics Using Transformer-based Neural
Network∙R.K.Y. Chan1 , Y.
Zhou1 , and K.K.-Y.
Wong1,2 ; 1 Department
of Electrical and Electronic
Engineering,
The University of Hong
Kong, Pokfulam Road,
Hong Kong, China;
2
Advanced Biomedical
Instrumentation
Centre, Hong Kong

9:45

Exploring the nonHermitian topology
of exceptional points
in lasers and fibreloops
A. Schumer1,2 , H.
Nasari2,3 , Y.G.N. Liu2 ,G. Lopez-Galmiche3 ,J.
Leshin3 ,H.E.
Lopez-Aviles3 ,L.
2Ding , Y. Alahmadi3,4 ,A.U. Hassan3 , Q.
Zhong3 , ∙S. Rotter1 ,P. Likam Wa3 , D.N.
Christodoulides3 , andM.
Khajavikhan2 ;1
TU Wien, Vienna,

NOTES

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⋅ Friday 30 June 2023

Room 1 ICM

Room 2 ICM

Room 3 ICM

Room 4a ICM

Room 4b ICM

Room 5 ICM

Room 11 ICM

Room 12a ICM

Room 12b ICM

pering Gallery Mode
Resonators from bulk
calcium fluoride is
proposed, based on
femtosecond
laser
processing. Processing times are halved
whilemaintaining
performanceandimproving reliability.

our own results withsplicing different combinations of fibers.

of Warsaw, Warsaw,
3
Poland;DoctoralSchool of Exact andNaturalSciences,
University of Warsaw,
Warsaw,
Poland;4
Niels Bohr Institute,
University of Copenhagen, Copenhagen,Denmark
We present an experimental realization of
free-space continuous
microwave-to-opticalphotonic conversion
in room-temperature
Rydberg rubidium-85
atomicvapours.
We
achieve
unprecedented
51dB
dynamic range and
16MHz bandwidth at
13.9GHz microwave
frequency.

todemonstratecollective
blinkingofself-assembled
stacks of around70
semiconducting
nanoplatelets.
Thiseffect is explained
and modelled as
Förster-resonant
energy tranfer (FRET)
funneling all the
excitons from a chain
portion to a single
blinking quencher.

Science and Technology, Daejeon, South
Korea; 2 Departmentof Physics and Astronomy,
SejongUniversity,
Seoul,South Korea
We present interlayervibration-assisted
acousto-optic modulation of Bi2Se3
at
opticalcommunication
band,
initiated by ultrashortpulses.
High-speed(~102 GHz) andstrongmodulationof optical properties
can be achieved bylight-driven nanomechanical interactionsat ultrafast timescale.

ment of Electricaland Computer Engineering,Technische
Universität München,
Garching, Germany;
2
DepartmentofApplied
Physics,
KTH-Royal
Institute of Technology,
Stockholm, SwedenWetheoreticallyand experimentallyinvestigate the effectof phase matching forterahertz generationin terahertz quantum
cascade laser sources
based on intra-cavity
Cherenkov differencefrequency generation.
The results indicate
significant
deviceperformance
improvement via phasematching.

ing only cryogenic
opto-electronic components and opticalinterconnects,
weoperate the SNSPD
electrically decoupledfrom room temperature electronics andwith a heatload of
75μW at 1K.

Kingdom
Ultra-precision dicing
was used to define
waveguides and perform optical quality
facet cuts in a silicon
nitrideplatform,without need forfurtherpolishing.
These methods canbe extended to otherplatforms such as
silicon-on-insulator.

Nazionale di Ottica,
Pozzuoli , Italy
We propose a new
method for singleshot,wavelengthresolved polarization
measurementby
exploiting divisionof-amplitude method
under the far-fieldtransformation.
Asaproof-of-concept
demonstration,
wereveal the complex
polarization dynamics
in the build-up of
dissipative solitons.

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

CM-9: Laser-induced periodic
surface structures

CJ-8: Pulsed fiber
sources

EA-7: Atomic
systems

CK-13: Advanced
photonic devices

Chair:
SebastianBlatt,LudwigMaximiliansUniversität, München,
Germany

Chair: Stéphane Clemmen, Ghent University,
Belgium

CC-5: THz spectroscopy andtechniques

CI-6: Modulationand demodulation

CE-9: Lithium
niobate platform

Chair:Jakub Boguslawski,Wrocław
University of ScienceandTechnology,
Poland

EI-2: Nonlinear
and quantum
optics with vander Waals layeredmaterials

Chair:
GiacomoScalari, ETH, Zurich,
Switzerland

Chair: Thomas Roger,
Toshiba
Research
Europe, Cambridge,
United Kingdom

ED-6: Frequency
combs: Sources
and characterization

CM-9.1 FRI 10:30

CJ-8.1 FRI (Invited) 10:30

EA-7.1 FRI

10:30

CK-13.1 FRI 10:30

EI-2.1 FRI

10:30

CC-5.1 FRI (Invited) 10:30

CI-6.1 FRI

Impact of plasmonicmodes and metal
thermophysical properties on the formation of self-organised
nano-patterns inthin films

Omitting conventional saturable
absorbers in modelocked fibre lasers∙M. Chernysheva andD.C. Kirsch; Leibniz
Institute of Photonic

Driving the Superfluid-supersolid
Phase-transition by
HeatingJ. Sánchez-Baena1,2 ,C.
Politi3,4 ,∙F.
Maucher5,1 ,F.

Observation of
Brillouin spin-orbit
interaction in a silica
optical nanofiber∙M. Zerbib1 ,M.
Romanet1 ,T.
Sylvestre1 ,C.

Towards compact
phase-matched andwaveguided nonlinear optics in atomically layered semiconductors
X.
Xu1 ,
∙C.

Miniaturised terahertz photonic chips
Y.
Lampert1 ,F.
Bertot1 , A. Herter2 ,A.
Shams-Ansari3 ,A.
Tomasino1 ,S. Rajabali1 ,M.

Kerr Nonlinearity
Tolerance with Reference Constellation
Adaptation
S.A.
Mir1 ,
L.N.
Venkatasubramani1,2 ,∙S. S J1 , L. Barry2 ,Chair: Jörn Bonse,
Bundesanstalt
fürMaterialforschungund -prüfung (BAM),
Berlin, Germany

Chair:
Fang Liu,
Stanford University,
San Francisco, USA

188

10:30

Chair: Katia Gallo,
KTH, Stockholm, Sweden

CE-9.1 FRI

10:30

A heterogeneously
integrated lithium
niobate-on-silicon
nitride photonic
platform∙M. Churaev1 , R.N.
Wang1 , V. Snigirev1 ,Chair: Oliver Heckl,
Vienna University, Vienna, Austria
ED-6.1 FRI

10:30

Microresonator
Soliton Frequency
Combs Enabled by
Quintic Dispersion∙T. Bi1,2 , S. Zhang1 ,L. Hill3 , and P.
1
Del’Haye1,2 ;
Max

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H.
Bhaskaran2 ,and P. Bienstman1 ;1
Photonics ResearchGroup, INTEC Department,
Ghent
University – imec,
Ghent 9052, Belgium;
2
University of Oxford,
Departmentof Materials, Parks
Road, Oxford OX1
3PH, United Kingdom; 3 University of
Münster, Departmentof Physics, CeNTech,
Heisenbergstraße
11, 48149 Münster,GermanyWeexperimentallydemonstrate synaptic plasticity in an
integrated photonic
recurrent neural network, employed forreservoir computing.
The
performanceon a time seriesclassification task isimproved by plastic
adaptation of thereservoir network.

tralia; 2 University ofCalifornia,
Irvine,USA
We present and numerically demonstrate
ultra-fast time-variant
metasurfaces
withtime-engineered
bandwidth. This engineering is achievedbytheinterplay
betweengeometric
and photo-carrier induced asymmetries tocontrol the radiationofbound-statein-the-continuum
modes.

thedynamics
ofnonlinear waves via
synchronous
phase
modulation. Amongother things, we showthat quadratic modulations can expulse or
trap solitons.

A simple and costeffective
methodfor forming a hydrophobic
SERS
substrate is presented.
The substrate wascharacterised using
R6G and used todetectultra-low
concentrations (0.001
mg/ml) of 50nm
and 100nm diameter
nanoplastics in water.

2

Department
ofMaterials Science andTechnology, Universityof Crete, Heraklion,
3
Greece;Arts &
Sciences, Texas A&M
University at Qatar,
Doha, Qatar
Neural networks areshown to successfully
retrieve optical information encoded in
the spatial intensity oflaser holograms that
propagate in strongly
nonlinear and turbulent media resulting
in the formation of
speckle patterns.

Sciences, University of
Auckland, Auckland,
New Zealand; 2 The
Dodd-Walls
Centrefor Photonic andQuantum Technologies, Dunedin, New
Zealand; 3 The Photon
Factory,
Universityof Auckland, Auckland, New Zealand;
4
Counties Manukau
District Health Board,
Auckland,New
Zealand; 5 Departmentof Physics, Universityof Auckland, Auckland, New Zealand;
6
Faculty of Medicaland Health Sciences,
University of Auckland, Auckland, New
Zealand
Raman spectroscopy
data of prostate cancer
tissue is assessed toensure ethnic bias
in the data set isminimized. Results
show differences inRaman spectra but
similar classification
performancefor
NZ-European, Māori,
and Pasifika men.

Science Park, Shatin,
New Territories, Hong
Kong, China
We demonstrate theuse of transformerbased deep learningmodel in predicting
nonlinear dynamics
in fibre optics overa long distance. It isalmost 4 times moreaccurate and 10 times
faster than recurrent
neural network.

Austria; 2 University ofSouthern California,
Los Angeles, USA;
3
The College of Optics and Photonics(CREOL),
Orlando,USA; 4 Cemter of Excellence for Telecomm
Applications, Riyadh,
Saudi Arabia
We investigate thetopologicalaspectsofencircling
anexceptional
point.
Specifically, we show
how to create topological lasing modes
in a waveguide-laserand how to observea chiral state transfer
without encircling the
singularity.

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

10:30 – 12:00

JSIII-4: Photonic
accelerators II

CD-12: Stimulated Brillouin scattering

EF-8: Symmetry
breaking in coupled resonators

CH-14: Photothermal and photoacoustic sensing

EE-3: Ultrafast
XUV and soft Xray spectroscopy

CL-6: Advanced
microscopy I

EJ-4: Tailored
light and opticaldesignEC-2: Photonic
band topology

Chair: Anderson S L
Gomes, Federal University of Pernambuco,
BrazilChair: Mathias Marconi, Université Côted’Azur, Nice, France

Chair:
Christoph
Haisch,Technical
University of Munich,Germany

Chair:ICFO,
Spain

Chair: Bert Offrein,
IBM
Research
Zürich,Rüschlikon,
Switzerland

Jens Biegert,
Barcelona,

Chair: Keisuke Goda,
University of Tokyo,
Japan
CL-6.1 FRIJSIII-4.1 FRI (Invited) 10:30

CD-12.1 FRI 10:30

EF-8.1 FRI (Invited) 10:30

CH-14.1 FRI (Invited) 10:30

EE-3.1 FRI (Invited) 10:30

Photonic tensor coreand convolution chipfor machine learning
acceleration∙V. Sorger; George
Washington
University, Washington,

Inter-vortex forward
Brillouin scatteringby chiral phonons∙X. Zeng1 , P. Russell1 ,andB.
Stiller1,2 ;1Max-Planck institutefor the science ofSymmetry breaking
and zero modes inphotonic crystal
cavity arrays∙A.M.
Yacomotti,
K. Ji, M. Hedir, B.
Garbin,and J.A.

Imaging Circular
Dichroism of Single
Nanoparticles Using
Photothermal
Microscopy∙S. Adhikari, P. Spaeth,
and M. Orrit; Lei-

Ultrafast Dynamics
in Donor-Acceptor
Prototype Molecules
by XUV-IR Attosecond Spectroscopy∙F. Vismarra1,2 , R.
Borrego-Varillas2 , Y.
189

Chair: Joerg Goette,
University of Glasgow,
United Kingdom

Chair:
Henning
Schomerus, Lancaster
University,
UnitedKingdom

EJ-4.1 FRI

10:30

EC-2.1 FRI (Invited) 10:30

Supertoroidal anapoles∙R. Ravi Kumar1 ,N.
Papasimakis1 ,and N.I. Zheludev1,2 ;1Optoelectronics Research Centre & Centre

Three-dimensional
topological lighttransport induced bylattice dislocations∙J. Beck1 , E. Lustig2 ,L.
Maczewsky1 ,T. Biesenthal1 , M.

10:30

Multimodal Coherent Raman andMultiphoton Nonlinear Optical Microscopy Reveals Early
Risk of Tumour
Recurrence after
Anticancer Therapy
in Human Cells

NOTES

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P.
Lingos1 ,G.
Perrakis1 ,O.
Tsilipakos2,1 ,∙G.
Tsibidis1,3 , and E.
Stratakis1,4 ; 1 Instituteof Electronic Structureand Laser (IESL),Foundation for Research and Technology(FORTH), Heraklion,
Greece; 2 Theoreticaland Physical Chemistry Institute National
Hellenic
Research
Foundation, Athens,
3
Greece; Departmentof Material Science,
University of Crete,
Heraklion,
Greece;4
DepartmentofPhysics,
Universityof Crete, Heraklion,
Greecewe demonstrate thatthe excitation of coupled SPPs in air/metal
and metal/substrateinterfaces , alongwith other parameters
dictate the spatial
modulation of theabsorbed energy that
account for LIPSS
formation in thinfilms.

Technology, Jena, Germany
Principle limitations
for achieving stableultrashortpulse
generation and broad
tuningwavelength
ranges are generally
defined by traditionalmode-locking. This
presentation discusses
pathways to highly integrated and effective
self-mode-locking
methodologies
foradvancedultrafast
fibre lasers.

Ferlaino3,4 , and T.
Pohl1 ; 1 Center for
Complex
Quantum
Systems,
Department of Physics andAstronomy,
Aarhus
University,
Den2mark; Departamentde Física, Universitat
Politècnica
deCatalunya,
CampusNord
B4-B5,
Barcelona,
Spain; 3 Institut für
Quantenoptik
undQuanteninformation, Österreichische
AkademiederWissenschaften,
Innsbruck,
Austria;
4
InstitutfürExperimentalphysik,
Universität
Innsbruck,
Austria;5
DepartamentdeFísica,Universitat
de les Illes Balears &IAC-3, Campus UIB,Palma de Mallorca,
Spain
We show that generalising the extended
Gross-Pitaevskii
equation for dipolar
Bose-Einsteincondensatestoinclude temperaturefluctuations employing Bogoliubov theory
with local density approximation permits
the description ofrecent experiments,
includingheatinga superfluid into asupersolid.

Wolff2 , B. Stiller3 ,J.-C.
Beugnot1 ,andK.P.
Huy1 ;
1
FEMTO-ST Institute,
CNRS-UniversitédeFranche-Comtéand
SupMicrotech
ENSMM, Besancon,
France; 2 Center for
Nano Optics, University of Southern
Denmark,
Odense,3Denmark;Max
PlanckInstitutefor the Science ofLight, University ofErlangen-Nuremberg,
Erlangen, Germany
We report the observation of a Brillouin
spin-orbit
interaction in an optical
nanofiber in whichthebackscatteredsignal by the acoustic
TR21 vortex mode
undergoes a circularpolarization handedness reversal due toangular momentum
conservation.

Trovatello1 ,F.
Mooshammer1 ,Y.
Shao1 , S. Zhang1 , K.
Yao1 , D.N. Basov1 ,G. Cerullo2 , and P.J.
Schuck1 ; 1 Columbia
University, New York,
USA; 2 Politecnico di
Milano, Milano, Italy
Here we achieve
recordnonlinear
optical enhancement
from
3R-MoS2,>10^4 stronger thana monolayer, andwe show broadly
tunable SHG in a
waveguide geometry,
highlighting the potential of 3R-MoS2 forintegrated nonlinear
optical devices.

Loncar3 , and ∙I.-C.
Benea-Chelmus1 ;1
HybridPhotonics
Laboratory,
EPFL,
Lausanne,
Switzer2
land;
Quantum
Optoelectronics
Group,
ETHZ,
Zurich, Switzerland;
3
Laboratoryfor
Nanoscale
Optics,Harvard University,
Cambridge, USA
This talk will highlight
opportunities
for terahertz scienceand technology from
nonlinear integrated
photonic circuits by
exploring
waveguides, resonators andterahertz
antennas.
Their present andfuture applications inmetrology, emission
and waveform control
are discussed.

R.D.
Koilpillai1 ,and D. Venkitesh1 ;1
Department
ofElectrical Engineering,
Indian Institute ofTechnology
Madras, Chennai, India;
2
Radio and OpticalCommunication Laboratory, Dublin City
University,
Dublin,IrelandWe
demonstrate
the use of a simple
learning
approachtothereference
constellations
totolerate the phase perturbation due to fiber
Kerr-nonlinearity,
while simultaneously
performing
carrierphase recovery.

A. Riedhauser2 , T.
Blésin1 , C. Möhl2 ,Y.
Popoff2 ,U.
Drechsler2 , D. Caimi2 ,J.
Riemensberger1 ,P.
Seidler2 ,andT.
Kippenberg1 ;1Institute of Physics,
Swiss Federal Institute of Technology
Lausanne(EPFL),
Lausanne,
Switzerland; 2 IBM Research- Europe,
Zurich,Switzerland
We present a LiNbO3
integrated photonic
platform with <0.1
dB/cm optical propagation loss and <2.5
dB/facetfiber-chipcoupling loss basedon a silicon nitride
PIC. We demonstrateelectro-optic modulators, frequency-agile
lasers, optical splitters, and other deviceson the platform.

Planck Institute for the
Science of Light, 91058
Erlangen, Germany;
2
DepartmentofPhysics,
FriedrichAlexander-Universität
Erlangen-Nürnberg,
91058
Erlangen,3
Germany;
SUPA
and Department of
Physics, University ofStrathclyde, Glasgow,
G4 0NG, Scotland,,
United Kingdom
Soliton combs atnear-zerogroup
velocity dispersion are
the key to broadband
frequency
combs.
Here, we present thefirst solitons mediated by fifth-orderdispersion and thefirst zero-dispersion
microcombs pumped
by a continuous-wave
laser.

CI-6.2 FRI

CE-9.2 FRI

ED-6.2 FRI

CM-9.2 FRI 10:45

Influence of Substrate and Film Thickness on Polymer
LIPSS Formation
J. Prada-Rodrigo1,2 ,R.I.
RodriguezBeltrán1,3 ,T.A.
Ezquerra4 ,P.
1Moreno , and ∙E.
1
Rebollar2 ;Grupo
de Aplicaciones delLáser
yFotónica(ALF-USAL), Universidad de Salamanca,
Salamanca,
Spain;
2
Instituto de Química
FísicaRocasolano,
IQFR-CSIC, Madrid,EA-7.2 FRI

10:45

Conversion of laser
light into (anti)bunched light in an
atom-based two-photon interferometer∙M. Cordier,M.
Schemmer,P.

CK-13.2 FRI 10:45

A nonlinear activation function for
optical neural networks using a MachZehnder interferometer with a III-Von-Si amplifier∙Y.
Zhang1,2 ,H.
Deng1,2 ,E.
Soltanian1,2 ,J.
Zhang1,2 ,G.
1,2Roelkens ,andW.
Bogaerts1,2 ;1Photonics ResearchGroup,INTECdepartment,
Ghent
University-IMEC,
Ghent,
Belgium;

EI-2.2 FRI

10:45

Four-Wave Mixing at
Excitonic Resonances in the Telecom
Spectral Range∙S.
Klimmer1,2 ,A.
Sinelnik1,3,4 ,T. Pertsch3,4,5 ,I.
Staude1,3,4 ,H.
Rostami6,7 , and G.
Soavi1,4 ; 1 Institute ofSolid State Physics,
Univ.
Jena, Jena,
2
Germany;
ARC
Centre of ExcellenceforTransformative
Meta-Optical
Systems, Department ofElectronic Materials
Engineering, Research
School of Physics, The
Australian National
Univ.,
Canberra,
Australia; 3 Instituteof Applied Physics,
Univ. Jena, Jena, Germany; 4 Abbe Centerof Photonics, Univ.
Jena, Jena, Germany;
5
Fraunhofer Institutefor Applied Optics and
190

10:45

Nonlinearity Free
Operation of SOA
for Co-Packaged
Optics Based on
Advanced Modulation Format∙T. Kurosu, S. Suda,
S. Namiki, and T.
Amano;
National
Institute of Advanced
Industrial Science andTechnology, Tsukuba,
Japan
Toward high-capacity
co-packaged
opticsbasedondigitalcoherent
transmission, we demonstrate

10:45

Developing ZincIndiffused Periodically Poled Lithium
Niobate Ridge Waveguides for Quantum
Applications at
Visible Wavelengths∙N.
PalomarDavidson1 , G. Tawy1 ,G.M. Churchill1 , P.L.
Mennea1 ,R.H.S.
Bannerman1 , P.G.R.
Smith1 , L.D. Wright2 ,G.
BlanchardEmmerson2 ,J.C. Gates1 ,and
C.B.E.
Gawith1,2 ;1Optoelectronics

10:45

Thermal-Controlled
Scanning of a Bright
Soliton in a Photonic
Molecule∙I.
RebolledoSalgado1,2 , V. Durán3 ,Ó. Bjarki Helgason1 ,M. Girardi1 ,M.
Zelan2 , and V. Torres1
Company1 ;Dept.
Microtechnology
andNanoscience,
Chalmers
University of Technology,
Gothenburg, Sweden;
2
Measurement Scienceand Technology, RISE
Research
Institutes

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USA; Optelligence ,Upper Marlboro, USA
Here we present ourarchitecture for Silicon Photonic Tensor
Core (PTC) capableof accelerating computational needs ofneural networks andaugmented/virtual
reality applications.
We present a novel
fully-integrated PTC
including chip-basedlasers,modulators,
and photodetectors.

light, Erlangen, Germany; 2 DepartmentofPhysics,
Friedrich-AlexanderUniversität, Erlangen,Germany
We report forward
Brillouin scattering
between orthogonal
first-ordervortexmodes
inchiralphotonic crystal fibre.
The interaction ismediated by chiral“screw”
flexuralphonons,which
induce linear birefringence and haveacoustic topologicalcharge of 2.

Levenson;Centrede Nanosciences etde Nanotechnologies,
CNRS,
Université
Paris-Saclay,
Palaiseau, France
Photonic
crystalnanolasers can beengineered to enhance nonlinear andnon-Hermitian phenomena in coupledcavity arrays. Here I
will discuss three examples: spontaneous
symmetry breaking,exceptional
pointsand zero-mode lasing,with applications in
optical computing.

den University, Leiden,
Netherlands
Photothermal circulardichroism microscopyof single nanoobjects presents two
majoradvantages:(i) a high degree ofpolarization control
by using low-NA
pump
illuminationand (ii) a high spatial
resolutionusinghigh-NA illuminationof the probe.

Wu1,2 , D. Mocci1,2 , F.
Fernández-Villoria3,7 ,L. Colaizzi1 ,M.
Reduzzi1 , F. Holzmeier4 , L. Carlini5 ,P. Bolognesi5 ,R.
Ritcher6 , L. Avaldi5 , J.
7
González-Vázquez ,A.
Palacios7 ,J.
Santos3,8 , M. Lucchini1,2 , L. Bañares3,9 ,N.
Martin3,8 ,F.
Martin3,7 , and M.
Nisoli1,2 ; 1 Dep.
ofPhysics,
Politecnicoof Milano,
Italy;
2
IFN-CNR, Milano,
Italy; 3 IMDEA-Nanoscience,
Madrid,Spain; 4 imec, Leuven,
5
Belgium;
ISMCNR, Roma, Italy;
6
Sincro- trone Trieste,
Basovizza,
Italy;
7
D. de Quimica, U.
Autonoma de Madrid,
Spain; 8 D. de Quimica
Organica I, U. Complutense de Madrid,
Spain; 9 D. de Quimica
Fisica, U. Complutensede Madrid, Spain
The dynamics triggered by photo-ionization in nitroanilines, the simplest
donor/acceptor systems, are investigatedby combining ultrafast spectroscopy withPEPICOmeasurements and theoreticalsimulations.
We
appoint the ultrafast
processes to wavepacket spreading in
the cation.

∙A.
Bresci1 ,F.
Manetti1 ,S.
Ghislanzoni2 ,F.
Vernuccio1 ,S.
Sorrentino1 ,C.
Ceconello1 , R. Vanna3 ,I. Bongarzone2 , G.
Cerullo1,3 , and D.
Polli1,3 ; 1 Politecnico di
Milano, Departmentof Physics, Milan,
Italy; 2 IRCCS Istituto
Nazionale dei Tumori,
Milan, Italy; 3 CNR
Institute for Photonics
and Nanotechnology(IFN), Milan, Italy
We
combinevibrationalandmultiphoton nonlinear optical techniques
to distinguish andnon-invasively monitor therapy-induced
senescent cells, recently discovered todrive cancer recurrence in humans, at an
unprecedentedly earlystage of phenotype
commitment.

for Photonic Metamaterials, UniversityofSouthampton,
Southampton, United
Kingdom; 2 Centre for
Disruptive Photonic
Technologies,
The
Photonics
Institute,
School of PhysicalandMathematical
Sciences,
Nanyang
Technological
University,
Singapore,
Singapore
We report on a new
type of non-radiating,anapole excitations indielectric particles under illumination withtoroidal light pulses.
We show that suchanapoles are linked tosupertoroidal currents
induced in the particle.

Heinrich1 , Z. Yang3 ,Y. Plotnik2 , M. Segev2 ,and A. Szameit1 ;1Institute for physics,
University
Rostock,
Rostock,
Germany;2
Physics Department
and
Solid
State
Institute,
Technion– Israel Institute ofTechnology,
Haifa,
Israel; 3 Departmentof Physics, Zhejiang
University, Hangzhou,
ChinaWeexperimentallydemonstrate the first
three-dimensional
photonic topologicalinsulator comprising
two spatial and one
synthetic dimensions.
The 3D dynamics ofedge states inducedby lattice dislocations are observedusing
laser-written
waveguides.

CL-6.2 FRI (Invited) 10:45

EJ-4.2 FRI

Thermal wavefront
shaping: Applicationin fluorescent microscopy∙H.M.L. Robert1 , C.
Liu1 , N. Rutz2 , G.
Faini1 , A. Aggoun1 ,F. Del Bene1 , G.
Tessier1 , R. Quidant2 ,andP.
Berto1,3 ;1Sorbonne
Université, Institut de la
Vision, Paris, France;
2
Nanophotonic Systems Laboratory, ETH, Zürich, Switzerland;
3
Université Paris-cité,Paris, France

Propagation ofshaped light carrying
orbital angularmomentum throughturbid tissue-likescattering medium∙I. Lopushenko1 , A.
Sdobnov1 , A. Bykov1 ,and I. Meglinski1,2 ;1Optoelectronics
andMeasurement
Techniques
Unit,
ITEE, University ofOulu, Oulu, Finland;
2
College of Engineering and PhysicalSciences, Aston University, Birmingham,

CD-12.2 FRI 10:45

Wide-range
stimulated Brillouinscattering in a z-cut
magnesium fluoride
whispering gallery
mode resonator∙G. Lin and J. Tian;
Harbin Institute ofTechnology, Shenzhen,
China
We report over 2.5
GHzwide-range
stimulated Brillouinscattering (SBS) ina z-cut magnesium
fluoride
resonator.
A broad Brillouingain is revealed due

191

10:45

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Schneeweiss, J. Volz,and A. Rauschenbeutel;
HumboldtUniversität zu Berlin,
Berlin, Germany
We present a novel
type of interferometer, which realizes
interference in the
two-photon component of an incoming
laser light. As a consequence, it converts
the laser light into
a antibunched orbunched light.

Spain; 3 CONACYTCentro de Investigación Científica y de
Educación Superior
de Ensenada, Unidad
Foránea Monterrey,
Apodaca,
Mexico;4Instituto de Estructura de la Materia,
IEM-CSIC, Madrid,
Spain
Femtosecond Laser
Induced
Periodic
Surface
Structures(LIPSS)
formationon the surface ofpolymer materials is
studied as a functionof the substrate at
which the polymer isdeposited and of thefilm thickness.

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Center for Nano- andBiophotonics(NBPhotonics),
Ghent
University, Ghent ,BelgiumWeexperimentallydemonstrate a reconfigurable all-opticalnonlinear activation
function for neuralnetworks based on asilicon Mach-Zehnderinterferometer withaheterogeneously
integrated
opticalamplifier. It shows
both low activation
input power andsignificant
opticalamplification.

Precision Engineering,
Jena,
Germany;
6
DepartmentofPhysics,
Universityof Bath, Claverton
Down, Bath, United
Kingdom; 7 Nordita,
KTH Royal Instituteof Technology andStockholm
Univ.,
Stockholm, Sweden
We theoretically andexperimentally investigate broadband andresonant four-wave
mixing in the telecom
O-band in monolayer
MoS2 ,
where we
exploitexcitonictransitions to enhance
the nonlinear emitted
signal while keeping
the linear absorption
negligible.

2

CM-9.3 FRI 11:00

CJ-8.2 FRI

11:00

EA-7.3 FRI (Invited) 11:00

CK-13.3 FRI 11:00

Fresnel reflection reduction of standard
single mode fiber
end surfaces via fs
laser induced surface
structuring∙R.G. Krämer1 , M.P.
Siems1 , D. Richter1 ,andS.
Nolte1,2 ;1Friedrich
Schiller
University Jena, Abbe
Center of Photonics,
Institute of Applied
Physics, Jena, Germany; 2 2Fraunhofer
Institute for Applied
optics and Precision
Engineering
IOF,
Center of Excellencein Photonics, Jena,
GermanyWepresent
theimplementationoffemtosecond
laser
inducedperiodicsurface structures on
standard fused silica
fiber end surfaces for
successful
Fresnelreflection reduction.

7x7 multicore fiber,
nanosecond laser
system delivering
60 mJ pulse energy∙M.
Bahri1 ,C.
1Aleshire , A. Steinkopff1 , A. Klenke1,2,3 ,C.
Jauregui1 ,S.
4Kuhn ,
J. Nold4 ,N.
Haarlammert4 ,T. Schreiber4 ,A.
Tünnermann1,2,3,4 ,and J. Limpert1,2,3,4 ;1Institute of Applied
Physics, Abbe Center of
Photonics, FriedrichSchiller-Universität,
Jena,
Germany;2Helmholtz-InstituteJena, Jena, Germany;
3
GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt,
Germany; 4 Fraunhofer
Institute for Applied
Optics and Precision
Engineering,
Jena,
Germany
This work presents a
49-coreYtterbium-

Graph States ofAtomic Ensembles
Entangled by Light
E. Cooper, P. Kunkel,
A. Periwal, and ∙M.
Schleier-Smith; Stanford University, Stanford, CA, USA
We engineer continuous-variable graphstates of atomic spin
ensembles.
Our
approach combines
global light-mediatedinteractions in an
optical cavity with
local
addressing
to generate a programmable networkof entanglement.

Near-infrared Lightsensing and Emitting
III-V Micro- andNanopillar Unipolar
LEDs without p-type
Doping∙B. Jacob1 , F. Camarneiro1 , J. Borme1 ,J. Figueiredo2 ,J.
Nieder1 ,
and
B.
1
1
Romeira ;INL International Iberian
Nanotechnlogy Laboratory, Braga, Portugal; 2 Universidade
de Lisboa, Lisboa,
PortugalWe
demonstrate
seamless integrationofelectroluminescence, light-sensing
and negative differential
conductance in unipolar
micro/nanopillarLEDs.
The lightsensing-emitting
static and dynamic
properties are studied
paving the way for

EI-2.3 FRI

11:00

Light topology interplay in high harmonic generation fromgraphene∙A. García-Cabrera,R.
Boyero-García,
Ó. Zurrón-Cifuentes,
J. Serrano, J. San
Román, L. Plaja, and
C. Hernández-García;
Grupo de Investigaciónen Aplicaciones delLáser y Fotónica, Departamento de Física
Aplicada,
Universidad de Salamanca,
Salamanca, Spain
We explore the topology of the high-orderharmonics
fromgraphene driven bylinearlypolarized
vector beams with awell-defined Poincaré
index.
Graphene’s
nonlinear anisotropy
leads to a harmonics’
complexspatial192

Room 5 ICM

CC-5.2 FRI

11:00

A wide-band photonic spectrum analyser
for terahertz frequencies∙B.L.
Krause,F.
Reschke,andS.
Preu; TU Darmstadt,
Darmstadt, Germany
We show a photonic
spectrum
analyser based on
opticalfrequency
down-conversion
for the terahertz
frequency range. It
achieves competitive
performance, close toestablished electronic
spectrum analysers,
yet with a larger
bandwidth in anaffordable module.

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amplificationof
non-phase-locked
multi-wavelength
light by SOA. 16QAM
signals could be generated without quality
degradation due tofour-wave mixing byusing uneven channel
spacing.

Research
Centre,Southampton, United
Kingdom; 2 Covesion
Ltd.,
Southampton,
United Kingdom
Zinc-indiffused
PPLN diced ridge
waveguides for 1storder 532nm and3rd-order 375-390nm
generation have beenmodelled and fabricated, yielding peak
crystalconversion
efficiencies of 40%
and 0.7% respectively,
with ongoing optimisation
throughcharacterisation andnumerical modelling.

of Sweden, Borås,Sweden; 3 GROC-UJI,
InstituteofNew
Imaging Technologies,
University Jaume I,
Castellón, Spain
We report the tuning of the modes of abright soliton comb by
thermally tuning theresonances of a photonic molecule. We
implement a thermalcontrol feedback system to maintain a soliton state over 60 GHz.

CI-6.3 FRI

11:00

Optical Eigenvalue
Demodulation Using
Neural Network andEstimation of the
Number of Eigenvalues in the Preset
Region∙K. Nishida, Y. Terashi,
D. Hisano, K. Mishina,
and A. Maruta; Osaka University, Suita,Japan
We propose a demodulation methodof a neural network
and an estimationof the number of
eigenvalues.
Theback-to-back experiments transmittingafour-eigenvalue
signal achieved theerror-free operation<
2-dB penalty
compared with theconventional method.

CE-9.3 FRI

11:00

Characterization ofring resonators inthin-film lithium
niobate photonic
integrated circuit
platform∙J. César Cuello1 ,A. Money2 , J. Leo2 ,H.
Zarebidaki2 ,G.
Choong2 ,Y.
Petremand2 ,I.
Prieto2 , O. Dubochet2 ,M.
Despont2 ,H.
Sattari2 ,G.
Carpintero1 , and A.
Ghadimi2 ; 1 University
Carlos III of Madrid,
Leganes, Spain; 2 Swiss
Center for Electronics
and Microtechnology(CSEM), Neuchatel,
Switzerland
Here we present
high-yield fabricationof lithium niobate
PICs based on 6-inch
lithium niobate on
insulator
wafersand the statisticalmeasurements of hun-

ED-6.3 FRI

11:00

Long-Term Frequency Stability ofLaser Cavity Solitons∙A.
Cutrona1,2 ,M.
Rowley2 ,A.
Bendahmane2 ,V.
Cecconi1,2 ,L.
Peters1,2 ,L.
Olivieri1,2 , B. Little3 ,S. Chu4 , S. Stivala5 ,R. Morandotti6 , D.
Moss7 , J.S. Totero
Gongora1,2 ,M.
Peccianti1,2 ,andA.
Pasquazi1,2 ;1Emergent Photonics
Research
Centre,Dept.
of Physics,
Loughborough University, UK; 2 Emergent
Photonics (Epic) Lab,
Dept.
of Physics
andAstronomy,
Brighton, UK; 3 QXP
Technologies,
Xi’an,
China; 4 Departmentof Physics, City University of Hong Kong,
China; 5 Dipartimento
diIngegneria,
Universita’degliStudi di Palermo,
6
Italy;
INRS-EMT,
Varennes,
Canada;7
OpticalSciences
Centre,SwinburneCLEO

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to the large variationof the acoustic phasevelocity.

JSIII-4.2 FRI 11:00

CD-12.3 FRI 11:00

EF-8.2 FRI

11:00

CH-14.2 FRI 11:00

EE-3.2 FRI

Rapidly convergent
fabrication-errortolerant unitary
processor using
few-layer-redundantmulti-plane light
conversion∙Y.
Taguchi1 ,Y.
Wang2 , R. Tanomura1 ,T. Tanemura1 , and1
Y. Ozeki1 ;The
University of Tokyo,
Bunkyo-ku,
Japan;
2
Preferred Networks
Inc.,
Chiyoda-ku,
Japan
We propose a newarchitecture for programmable unitarytransformation that isrobust to fabrication
errors on integrated
photonics platforms.
Compared to previous studies, ourarchitecture achieves
orders of magnitude
better accuracy and a
20-fold speed-up.

Switchable analogueof Electromagnetic
induced Absorption
and Transmissionlike filter responses
using Stimulated
Brillouin Scattering∙M. Jha, R. Dhawan,
R. Parihar, and A.
Choudhary;
IndianInstitute of Technology,
Delhi, India
We propose a novel
technique for generating an analogueofelectronicallyinducedtransmission/Absorption-like response using
stimulated Brillouinscattering in a phasemodulated link. EIT
depth of 35 dB andEIA depth of 30dB isachieved.

Tracking Exceptional
Point above Laser
Threshold∙K. Ji1 , Q. Zhang2 , L.
Ge3 , G. Beaudoin1 ,I.
Sagnes1 ,F.
Raineri1 ,R.
ElGanainy2,4 , and A.M.
Yacomotti1 ; 1 Centre
de Nanosciences etde Nanotechnologies,
CNRS,
Université
Paris-Saclay,
Palaiseau,
France;2
DepartmentofPhysics,
MichiganTechnological
University,
Houghton,
USA; 3 Department of
Physics and Astronomy, College of Staten
Island, CUNY, New
York, USA; 4 Henes
Center for Quantum
Phenomena, Michigan
Technological
University,
Houghton,USA
We
experimentallyobserve and track

Trace-molecule detection below the ppt
level with doubly-resonant cantilever-enhanced photoacoustic spectroscopy∙J.
Pelini1,2 ,M.
Siciliani de Cumis3 ,Z. Wang4 , I. Galli2 ,I. Lopez Garcia2 , M.
Concetta Canino5 , P.
Cancio Pastor3 , N.
Akikusa6 , W. Ren4 ,P. De Natale2 , and S.
1Borri2 ;Universityof Naples ”Federico
II”, Naples, Italy;
2
CNR-INO (National
Instirute of Optics)
and LENS (European
Laboratories for Non
Linear Spectroscopy),
Florence , Italy; 3 ASI(Italian Space Agency),
Matera, Italy; 4 The
ChineseUniversityof Hong Kong, Hong
Kong, China; 5 CNRIMM, Bologna, Italy;
6
Hamamatsu
Pho-

Ultrafast Photodissociation Dynamics of NO2 Probed at
the N K-Edge∙Z.-Y. Zhang1 , L.
Restaino2 , A. Sen1 ,M.-O.
Winghart1 ,M.J.J. Vrakking1 , M.R.
Coates2 , M. Odelius2 ,M. Kowalewski2 , E.T.J.
NIbbering1 , and A.
Rouzée1 ; 1 Max-BornInstitute for Nonlinear
Optics and Short
Pulse
spectroscopy,
Max-Born-Strasse 2A,
12489, Berlin, Germany; 2 Departmentof Physics, Stockholm
University, SE-106 91,
Stockholm, Sweden
Femtosecond
N
K-edge X-ray absorption
spectroscopyofphotoexcited
NO2 monitors theelectronic structuraldynamics of NO2
following the pathway
of a conical inter193

11:00

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I will describe a novel
wavefront
shaping
concept where thetransmitted
lightisshapedusing
thermo-optics effect.
I will present ourarrays of electricallytuneable lenses andillustrate the potentialof this technique formicroscopy.

United Kingdom
A Monte Carlo model
is developed andutilized to trace theevolution of lightwith orbital angularmomentum propagating within the turbid
medium in order tostudy its potential
for biomedical diagnostics and tissue
characterization.

EJ-4.3 FRI

11:00

Inverse design of integrated phase-tunable beam couplers∙A. Nanda1,2 , M.
Kues1,3 , and A.C.
Lesina1,2 ; 1 HannoverCentre for Optical
Technologies,
ClusterofExcellence
PhoenixD,
Leibniz
University Hannover,Welfengarten 1, 30167
Hannover, Germany;
2
Institute of TransportandAutomation
Technology, Leibniz
University Hannover,Welfengarten 1, 30167
Hannover, Germany;3
Institute of Photonics,
Leibniz
University
Hannover, Nienburger
Strasse 17, 30167
Hannover, Germany
Beam splitters arefundamental component for integrated
linear quantum optics. However, phase
control is not present

Room 22a ICM

EC-2.2 FRI

11:00

Anomalous topology
in strongly amorphous networks∙Z.
Zhang1 ,P.
Delplace2 , and R.
1
1
Fleury ; Laboratoryof Wave Engineering,
School of ElectricalEngineering,
EPFL,
Lausanne,
Switzerland; 2 Ens de Lyon,
CNRS, Laboratoire dephysique, Lyon, France
Topological insulators
are crystalline materials with exceptional
immunity to local
disorder and random
structural deformations but only in small
levels.
We predictand observe a novel
topological photonic
phase,
survivingarbitrarilystronglevels of amorphism.

NOTES

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doped multicore fiber(MCF) in a MOPA
system, achieving apulse energy of up to
60 mJ in ns-class at
a repetition rate of 5
kHz from 3 mJ seed.

a new-class of III-V
n-typeoptoelectronic emitters anddetectors.

structure
breaking
thetopologicalconservation.

CM-9.4 FRI 11:15

CJ-8.3 FRI

11:15

CK-13.4 FRI 11:15

EI-2.4 FRI

Robustness of antiadhesion between
nanofibers and surfaces covered withnanoripples of varying spatial periodG.
Buchberger1 ,M. Meyer2 , C. Plamadeala1 , M. Weissbach2 , G. Hesser1 ,W.
Baumgartner1 ,∙J. Heitz1 , and A.-C.
Joel2 ; 1 Johannes Kepler
University Linz, 4040
Linz, Austria; 2 RWTH
AachenUniversity,
Institute for Biology
II, 52074 Aachen,
Germany
PET
foils
with
biomimetic
ripples, derived fromanti-adhesive nanostructures on spider
legs,
shows
the
same
pronounced
anti-adhesive effectagainst threads fromthe spider webs. Thiseffect is robust againstchanges in spatial
period.

Generation of femtosecond 1.3 μm pulses
through chirped
pulse amplification
based on praseodymium-doped
fluoride fibers
K. Yamaizumi, F.
Hondo, and ∙T. Fuji;
Toyota Technological
Institute,
Nagoya,Japan
We have investigatedthe design of a chirped
pulse
amplification
system based onpraseodymiumdoped fluoride fibers.
We have successfullycompressedtheamplified 1.3 μm
pulse down to 220 fs
without serious phase
distortion.

Monolithically Integrated WaveguideCoupled Single-Photon Avalanche Photodetector in a Visible-Light Silicon
Photonics Platform∙A. Govdeli1,2 , J.N.
Straguzzi1 ,W.D.
Sacher1 , and J.K.S.
Poon1,2 ; 1 Max Planck
InstituteofMicrostructure Physics,
Halle (Saale), Germany; 2 Department ofElectrical and Computer
Engineering,
University of Toronto,
CanadaWe demonstrate awaveguide-coupled
single-photon
avalanche
detector
in a visible-light
photonics platform.
Dark count rates <19
kHz and a photon
detection probability
of 5% were measuredatλ=488nmforan average photon
number of <1

Many-Body driven
extreme nonlinear
interactions inquasi-2D materials∙J.V. Moloney1 , J.
Hader1 , J. Neuhaus2 ,and S.W. Koch1,2 ;1Wyant College of
OpticalSciences,
University of Arizona, Tucson, USA;2
DepartmentofPhysics and Material
Sciences
Center,Philipps
University
Marburg, Germany
Semiconductor DiracBlochsimulations
withmany-body
Coulomb
contributions
includedof
nonperturbative
higherharmonic
generation in quasi2D transition metal
dischalcogenides
promoteenhancedemission signals andspectral broadening
primarily at energies
between the firstexciton and bandgap.

194

11:15

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CC-5.3 FRI

11:15

Optical cavity-referenced ultra-stableterahertz frequency
generation∙G. Kang, D.-C. Shin,
S.-W. Kim, and Y.-J.
Kim; Korea Advanced
Institute of Science andTechnology (KAIST),
Department of Mechanical Engineering,
291
Daehak-ro,
Yuseong-gu, Daejeon
34141, South Korea
Opticalcavityreferenced terahertz
generation with anextended frequency
range of 0.1–1.1 THz
isdemonstrated,yielding a 15-digit
frequency instability
at 1-s.

Room 11 ICM

CI-6.4 FRI

11:15

Modulation and
Demodulation
Method Robust
against Laser Phase
Noise∙R. Higuchi, T. Kuno,
R. Shiraki, Y. Mori,and H. Hasegawa;
NagoyaUniversity,
Nagoya, Japan
We propose a joint
modulation and demodulation methodthat achieves highphase noise tolerance
and low modulation
loss simultaneously.
Simulations and experiments show that32 Gbaud 16QAM
signals can be transmitted using low-costlasers.

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dreds of resonators,
demonstrating
intrinsic quality factor>2.5 millions, corresponding to linear
propagation
losses<0.14dB/cm.

University of Technology,
Hawthorn,
AustraliaWe
characterise
the long-term frequency stability offree running laser
cavity-soliton states.
We demonstrate Allan
deviations at one second averaging time of
3.55 × 10−10 (carrier)and 4.95 × 10−9 (repetition rate), paving theway for metrologicalapplications.

CE-9.4 FRI

ED-6.4 FRI

11:15

Erbium implantationin thin film Lithium
NiobateM. Adshead1 , M.
Sanaee2 , D. Blight1 ,∙A. Prencipe2 , R.J.
Curry1 , and K. Gallo2 ;1
PhotonScience
Institute University ofManchester, Manchester, United Kingdom;
2
KTH Royal Institute of Technology,
Stockholm, Sweden
We demonstrate Erbium implantation inlithium niobate on insulator and measure
the brightest photoluminescence peak at
1530nm (at 4K) froma doped area showing comparable surface quality (verified
through AFM imaging) before and after
implantation.

11:15

Mid-Infrared Quantum Cascade Laser
Frequency Comb
Tightly Locked by
Near-Infrared Light
Modulation∙K.N.
Komagata1 ,A.
Parriaux1 ,M. Bertrand2 ,J.
Hillbrand2 ,V.J.
Wittwer1 , J. Faist2 ,and T. Südmeyer1 ;1Laboratoire TempsFréquence, Institut dePhysique, Universitéde Neuchâtel, 2000
Neuchâtel,Switzerland; 2 Institute forQuantum Electronics,
ETH Zurich, 8093
Zurich, Switzerland
We demonstrate anear-infrared actuatorfortight-locking
mid-infrared quantum cascade laser
frequency combs witha 1-MHz actuation
bandwidth,which
surpasses
conventional drive-current
modulation. We thusachieve high spectral
purity pertinent for
mid-infrared metrological applications.

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Optimised Microwave Phase Shifterusing Brillouin-Induced Low Biasing∙R.
Parihar,R.
Dhawan,and A.
Choudhary;
Ultrafast
OpticalCommunications andHigh-Performance
Integrated Photonics(UFO-CHIP) Group,
Department of ElectricalEngineering,
Indian Institute ofTechnology (IIT) ,Delhi, India
Optimisation of theperformance metrics
ofamicrowave
photonic phase shifterisdemonstrated
by low-biasing thecarrierthrough
Brillouin scatteringwith
improvement
in noise figure andcompression dynamic
range by >2dB.

⋅ Friday 30 June 2023

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theexceptional
point above the laser
threshold in coupled
photonic
crystalcavities.

tonics K.K, Shizuoka,JapanWepresenta
new approach tocantilever-enhanced
photo-acoustic spectroscopy based on adouble standing wave
e effect (acoustic andoptical).
Our task
is to push the in-air
trace-gasdetection
limit
below
the
part-per-trillion.

section towards thephotodissocation
channel.

EF-8.3 FRI

CD-12.4 FRI 11:15/Europe-EQEC 2023

Room 14a ICM

JSIII-4.3 FRI 11:15

Lithium Niobate on
Insulator Photonic
Networks as an
Integrated Multiple
Scattering Platform∙X.S. Wang1 ,R.
Savo2 , A. Maeder1 ,F.
Kaufmann1 ,J.
Kellner1 ,A.
Morandi1 , S. Rotter3 ,R.
Sapienza4 ,andR.
Grange1 ;1ETH,Departmentof Physics,
Institute for Quantum
Electronics,
OpticalNanomaterial Group,
Zurich, Switzerland;
2
CentroRicerche
Enrico Fermi, Rome,
Italy; 3 . Institute for
Theoretical
Physics,
Vienna University ofTechnology , Vienna,
Austria; 4 The Blackett
Laboratory, DepartmentofPhysics,
Imperial
CollegeLondon,London,United Kingdom
We develop a graphbased
numerical
model for lithium
niobate on insulator
waveguide networks,
whose validity is verified experimentallyon small devices;larger networks areinvestigated numerically as an on-chip
multiplescattering platform withdesigned randomness.

®

11:15

Frequency control
and nonlinearity in asmall array of electrooptomechanical resonators∙G.
Jara-Schulz1 ,S. Barbay1 ,M.G.
Clerc2 ,andR.
1Braive1,3,4 ;Centrede Nanosciences etde Nanotechnologies,
CNRS,
Université
Paris-Saclay,
C2N,
Palaiseau,
France;2
DepartamentodeFísica and Millennium
Institute for Researchin Optics, Facultadde Ciencias Físicas y
Matemáticas,
Universidad de Chile,
Santiago,
Chile;
3
Université
ParisCité, Paris, France;
4
Institut Universitairede France (IUF), Paris,
FranceThanks to optics, westudied the mechanical response of asmall array of electrooptomechanicalphotonic
crystalresonators.
The
impact of external andinternal parameterson the dynamics
and synchronization
regime are characterized numerically andexperimentally.

CH-14.3 FRI 11:15

Phase-controlled
Fourier-transform
infrared spectroscopy with cantileverenhanced photoacoustic detection∙S.
Larnimaa1 ,M.
Roiz1 ,andM.
Vainio1,2 ;1DepartmentofChemistry, University
of Helsinki, Helsinki,
Finland; 2 Photonics
Laboratory,
Physics
Unit, Tampere University,
Tampere,FinlandA
13-fold
speed
improvementinbroadband
cantilever-enhanced
photoacoustic spectroscopy (CEPAS) has
been obtained using
Phase-controlled
Fourier-transform
spectroscopy(PCFTS). The absorption
spectrum of methane
in the mid-infrared
regionhas
beenmeasured as proof ofconcept.

EE-3.3 FRIRoom 21 ICM

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in prevalent losslessbeam splitters. Thus,
we demonstrate symmetric beam splitter
designs with phase
control using adjointbased
topology
optimization.

11:15

Ultrafast Soft X-ray
Spectroscopy of
Water-Mediated
Photoacid-BaseProton Transfer
Reactions∙M.-O.
Winghart1 ,P.
Han1 ,Z.-Y.
Zhang1 , C. Kleine1 ,S. Das2 , D. Garratt3 ,A.A.
Cordones3 ,G.L.
Dakovski4 ,D. DePonte4 ,K.
Kunnus4 , E. Ryland3 ,M.
Fondell5 ,R.
Mitzner5 ,K.J.
Gaffney3 , M. Odelius2 ,E. Pines6 , P. Wernet7 ,and E.T.J. Nibbering1 ;1
Max Born Institute,
Berlin,Germany;2
Stockholm University,
3
Sweden;PULSE
Institute,
Menlo
Park, USA; 4 SLAC
National
Accelerator
Laboratory,
Menlo Park, USA;
5
Helmholtz-Zentrum
Berlin, Germany; 6 Ben
Gurion University of
the Negev, Beersheva,
7
Israel;Uppsala
Universiy, Sweden
Employing transient
soft
X-ray
spectroscopy, we explore
the role of electronicstructuralchangesin reactants during
elementary acid-baseproton transfer eventsin solution phase,providingnovel
insights to the underlying microscopic
mechanisms of protontransport.
195

Room Osterseen ICM

CL-6.3 FRI

11:15

Focus-ISM enhances
optical sectioning insuper-resolution
microscopy∙A. Zunino1 ,G.
Tortarolo1,2 ,F.
Fersini1,3 , G. Garrè1,3 ,and G. Vicidomini1 ;1Molecular
Microscopy and Spectroscopy,
Istituto
Italiano di Tecnologia, Genoa, Italy;
2
Laboratory of Experimental
Biophysics,
EPFL,
Lausanne,
Switzerland; 3 DIBRIS,
University of Genoa,
Genoa, Italy
We
increasetheopticalsectioning
capabilities of image
scanning microscopeswith a novel dataprocessing technique.
We study the light
distribution on thedetector array to classify and discard thebackground without
losing any signal.

EJ-4.4 FRI

11:15

Influence of surface
roughness on theresonance frequencies and quality factors of optical cavities and plasmonic
nanoparticles∙P.T. Kristensen1,2 , T.
Kiel3 , K. Busch3,4 , and
F. Intravaia3 ; 1 DTU
Electro, Technical University of Denmark,Kgs.
Lyngby, Denmark; 2 NanoPhoton Center for Nanophotonics, Kgs. Lyngby,
3
Denmark;
Institut
für Physik, HumboldtUniversität zu Berlin,
Berlin,Germany;
4
Max-Born-Institut,
Berlin, Germany
We present a semianalytical approach toassess the influenceof surface roughness
on the distribution ofresonance frequencies
and quality factors ofgeneral electromagnetic resonators suchas leaky optical cavities and plasmonic
nanoparticles.

EC-2.3 FRI

11:15

Observation of thebulk-edge correspondence in anomalous
Floquet-Chern insulators in a synthetic
photonic lattice∙R. El Sokhen1 , A.
Adiyatullin1 ,A.
Gómez de León2 ,S.
Randoux1 ,P.
Deplace3 ,and A.
Amo1 ; 1 Univ. Lille,
CNRS, UMR 8523 –PhLAM – Physiquedes Lasers Atomes
et Molécules, Lille,
France; 2 Institute ofFundamental Physics
IFF-CSIC,
Calle
Serrano 113b, Madrid,
Spain; 3 ENS de Lyon,
CNRS, Laboratoire dePhysique (UMR CNRS5672), Lyon, FranceWe
experimentallymeasure the topological invariants ofatwo-dimensional
synthetic
photonic
lattice by integrating
the Berry curvature
over the Brillouinzone. The invariants
match the observed
number of edge states.

NOTES

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CM-9.5 FRI 11:30

CJ-8.4 FRI

Tailoring surface topographies on solids
with Mid-IR femtosecond laser pulses
S. Maragkaki1 , ∙G.
Tsibidis1,2 , L. Heizer3 ,Z. Papa3 , R. Flender3 ,B. Kiss3 , Z. Papa3 ,and E. Stratakis1,4 ;1Institute of Electronic
Structure and Laser(IESL),
Foundation
for Research andTechnology (FORTH),
Heraklion,
Greece;2
Department of Material Science, Universityof Crete, Heraklion,
Greece; 3 ELI-ALPS,
Szeged,Hungary;4
DepartmentofPhysics,
Universityof Crete, Heraklion,
GreeceWe investigate bothexperimentally andtheoretically the impact of laser sourceson the generation of
surface modification
related effects andon the subsequentsurfacepatterningofmetallic
andsemiconducting
materials.

Towards high-power
ultrafast short-wavelength-band Tmdoped fiber laser∙X. Liu1 , J. Sahu2 ,and R. Gumenyuk1,3 ;1Laboratoryofphotonics,
TampereUniversity,
Tampere,Finland;2
Optoelectronics Research Centre, University of Southampton,
Southampton, United
Kingdom; 3 Tampere
Institute for Advanced
Study,
TampereUniversity, Tampere,
Finland
We report an ultrabroadband
tunabledissipative
solitonTm-doped fiber laser
operating from 1.7μm
to 1.9μm.
Powerscalability of the laser
is demonstrated by asingle-stage amplifierdelivering
480fs
pulses with 141mW
of output power.

11:30

CM-9.6 FRI 11:45

CJ-8.5 FRI

Coherence Effects in
LIPSS Formation on
Silicon upon Picosecond Laser Pulse
Irradiations∙I. Mirza1 , Y. Levy1 , J.
Sladek1 , H. Papadaki2 ,E. Kaselouris2 , V. Dimitriou2 ,and N.
Bulgakova2 ; 1 HiLASE

Sub-100 fs all-fiberpolarisation maintaining tunable laserfrom 1870 nm up to
2050 nm∙A. Grande1,2 , D. Darwich1 , V. Freysz2 ,J. Boullet2 , and E.
1
Cormier1 ;Laboratoire
Photonique

11:45

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11:30

CK-13.5 FRI 11:30

EI-2.5 FRI

A robust half-W1
photonic crystal
waveguide platform
for interfacing
trapped cold atoms
with slow light∙A. Bouscal1 , A. Chochon1 , M. Kemiche2,3 ,S. Mahapatra2 , N.
Fayard4 ,J.
Berroir1 , T. Ray1 , J.-J.
Greffet4 , F. Raineri2 ,A. Levenson2 ,K.
Bencheikh2 , A. Urvoy1 , and J. Laurat1 ;1
Laboratoire Kastler
Brossel,Sorbonne
Université,
CNRS,
ENS-PSL,
Collègede France,
Paris,
France; 2 Centre deNanosciences et deNanotechnologies,
CNRS,
Université
Paris-Saclay,
Palaiseau,
France;3
IMEP-LAHC, Univ.
Grenoble Alpes, Univ.
Savoie Mont Blanc,
CNRS, Grenoble INP,
Grenoble,
France;4
Laboratoire Charles
Fabry,
Université
Paris-Saclay, IOGS,CNRS,Palaiseau,
FranceWe present a proposal
for trapping cold
Rubidium atoms neara novel high-index
photonic
crystalwaveguide, with adesignoptimized
againstfabrication
imperfections.
The
predicted
Purcellfactor is 100 times
higher than for optical
nanofibers.

Infrared-to-THz sensors based on whispering gallery mode
microresonators
D.
D’Ambrosio1 ,M. Capezzuto1 , S.
Avino1 , A. Giorgini1 ,P. Malara1 , A. Sorgi2 ,L. Consolino2 , M.
Vitiello3 ,P.
DeNatale2 ,and ∙G.
Gagliardi1 ; 1 Consiglio
Nazionaledelle
Ricerche,
Istituto
Nazionale di Ottica(INO), Pozzuoli (NA),2
Italy;
Consiglio
Nazionaledelle
Ricerche,
Istituto
Nazionale di Ottica(INO), Firenze, Italy;
3Consiglio Nazionaledelle Ricerche, Istituto di Nanoscienze(NANO), Pisa, Italy
A room-temperature
photodetector
isdemonstrated frommid-infrared to terahertz window using
a silica microsphere.
Whispering-gallery
modes are excitedwith a free-spacevisible laser without
guided-optics devices.
The readout reliesonlaser-frequency
lockingtothemicrocavity

Coherent State Manipulation of Single
Hexagonal Boron
Nitride Quantum
Emitters
J.A. Preuß1 , D. Groll2 ,R. Schmidt2 , T. Hahn2 ,P.
Machnikowski3 ,T.
Kuhn2 ,
R.
Bratschitsch1 ,∙D.
3,4
Wigger ,andS.
MichaelisdeVasconcellos1,5 ;1University of Münster, Department of
Physics and Center
for Nanotechnology,
Münster,
Germany;
2
University of Münster,InstituteofSolid State Theory,
Münster,
Germany;
3
Wrocław Universityof Science and Technology, Departmentof Theoretical Physics,
Wrocław,
Poland;4
School of Physics,
Trinity College Dublin,
Dublin , Ireland; 5 TU
Dortmund University,
Dortmund, GermanyWedemonstratecoherent state manipulation of hBN color
centers and investigate
coherence dynamics
and coupling between electronic andphononic excitations.
Our study reveals
the effects of spectral
jitter on ultrafast
coherence dynamics
and internal phonon
quantum dynamics.

EA-7.4 FRI

EA-7.5 FRI

11:45

Two-photon opticalshielding of collisions between ultra-

CK-13.6 FRI 11:45

Active Exciton Resonance Tuning inHybrid-2D Photodetectors∙T. Hoekstra and J.
van de Groep; VanderWaals-Zeeman
Institute, University of
Amsterdam, Amsterdam, Netherlands

EI-2.6 FRI

11:30

11:45

Bright single photon
source based on a
WSe2 monolayer inan open cavity∙V.
Mitryakhin1 ,J.-C. Drawer1 , H.
196

Room 5 ICM
CC-5.4 FRI

11:30

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Room 12b ICM

CI-6.5 FRI

CE-9.5 FRI

ED-6.5 FRI

11:30

11:30

11:30

Time-domain detection of multi-terahertz field vector
with polarizationmodulated electrooptic sampling∙N.
Kanda,
M.
Nakagawa, and R.
Matsunaga;
The
Institute for Solid State
Physics, The Universityof Tokyo, Kashiwa,JapanWe
demonstrated
a method for timedomain measurementof
multi-terahertz
electric field as avectorvalue
bymodulatingthepolarization of gate
pulses for electroopticalsamplingwith a photoelastic
modulator.

Ring Modulator
Based High-Sampling Rate Integrated
Photonic Sampler∙M.I.
Hosni1 ,A.
Vilson2 ,K.
Singh1 , J. Meier1 ,Y.
Mandalawi1 ,and T. Schneider1 ;1Technische Universität
Braunschweig,
Braunschweig,
Ger2
many;
Leibniz
Universität
Welfengarten 1, Hannover,Germany
We demonstrate acompact, integrated
9-branchphotonic
sampler based on silicon ring modulators.
By the convolution of
the signal spectrumwith a 9-line, flat
frequency comb asampling rate of 18
GSa/s was achieved

Redeposition-freeInductively-Coupled
Plasma Etching of
Thin-Film Lithium
Niobate on Insulator∙F. Kaufmann, G.
Finco, A. Maeder, and
R. Grange; Optical
Nanomaterial Group,
Institute for Quantum
Electronics, DepartmentofPhysics,
ETH Zurich, Zurich,
Switzerland
We investigate the behaviour of redepositedmaterial left after argon etching of lithium
niobate with respect toetch parameters andshow how to reach aregime, where the redeposition is removed
already during etching.

Feed-Forward Integration of an Optical
Frequency Comb
and a Single-Frequency DPSS Laser
Operating at the 87Sr
Magic Wavelength∙Y.S. Cheng1 ,B.
Szutor2 , and D. Reid1 ;1
Scottish Universities
Physics Alliance, Institute of Photonics andQuantum
Sciences,
School of Engineeringand Physical Sciences,
Heriot-Watt
University,
Edinburgh,
UnitedKingdom;
2
Skylark Lasers Ltd,
Ratho Park Phase One,88 Glasgow Rd, Ratho
Station, Newbridge,
Edinburgh,
UnitedKingdom
A Pr:YLF-Cr:LiCAF
solid-state
laser
operating at 813.42
nm,
the Sr-clock“magic wavelength”,
is integrated with a
Ti:sapphire frequency
comb
throughafeed-forward / feedback
combination.
Beat-note measurements demonstrate alinewidth as low as 65
kHz.

CC-5.5 FRI

CI-6.6 FRI

CE-9.6 FRI

ED-6.6 FRI

11:45

Quantitative Measurement of the dispersion of third-order nonlinearity insilica in the 1-25 THz
range
B. Zhou, M. Rasmussen, S. Yan, N.K.
Noori, O. Nagy, Y.
Ding, S.J. Lange, and11:45

Coherent PolMux reception using a lowcost Heterodyne ReceiverM.
Barrio,∙D.
Izquierdo, P. Sevillano,
and I. Garcés; Universidad de Zaragoza,
Zaragoza, Spain
We present the digital

11:45

Statistical characterization of MMI beam
splitters on thin filmlithium niobate on
insulator (LNOI)
platform at telecom
wavelength∙A. Monney1 , J. Leo1 ,G. Li2 , H. Zarebidaki1 ,G.
Choong1 ,
Y.

11:45

Highly coherent
triple frequency
comb generation in a
tri-core fiber for
four-wave-mixing
experiments∙E.-L. Bancel1 , E.
Genier1 , R. Santagata2 , M. Conforti1 , A.
Kudlinski1 , G. Bouw-

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JSIII-4.4 FRI 11:30

CD-12.5 FRI 11:30

EF-8.4 FRI

11:30

CH-14.4 FRI 11:30

EE-3.4 FRI

CL-6.4 FRI

EJ-4.5 FRI

EC-2.4 FRIThe Demonstrationof Photorefractive
Synaptic Connections for an Integrated Photonic Crossbar Array∙E.A. Vlieg, F. Horst,
R. Dangel, and B.J.
Offrein; IBM Research- Zurich, Rüschlikon,
SwitzerlandWedemonstrateprogrammable opticalsynaptic connections
inanintegrated
photorefractive
interconnect circuit.
These provide thebasic elements for an
integrated photonic
crossbar array for fastand efficient signal
processing in artificial
neural networks.

Temporal Dynamics
of On-Chip QuasiLight Storage∙M.
Merklein1 ,L. Goulden1 ,M.
Kiewiet1 , Y. Liu1 , C.K.
Lai1 , D.-Y. Choi2 ,S.J. Madden2 , C.G.
Poulton3 , and B.J.
Eggleton1 ; 1 UniversityofSydneyNano
Institute(SydneyNano), The University
of Sydney, Sydney,
2
Australia;
Laser
Physics Centre, The
Australian National
University, Canberra,
Australia; 3 School ofMathematicalandPhysicalSciences,
University of Technology Sydney, Sydney,
Australia
We investigate thetemporal dynamics
of on-chip quasi-lightstorage based on
stimulated Brillouinscattering and show
signal delays of over
100ns,
exceedingthe chip transit timeand intrinsic phonon
lifetime by an order ofmagnitude.

Spectral Control of
Coupled InP Nanolasers around Exceptional Points
through Selective
Excitation∙A.
Fischer1,2 ,T.V. Raziman2 , J.
Dranczewski1,2 ,D.
Saxena2 , H. Schmid1 ,3,4
K.
Moselund ,and R. Sapienza2 ;1IBMResearch
EuropeZurich,Zurich, Switzerland;
2
DepartmentofPhysics,
Imperial
CollegeLondon,London, United Kingdom; 3 Paul Scherrer
Institut,
Villigen,
Switzerland; 4 EPFL
Lausanne, Lausanne,
SwitzerlandWeexperimentally
study coupled semiconductor nanolasers,
that are selectively
excited, and explore
their mode landscapewhich is described bycoupled mode theory.
Wedemonstratevirtualexceptional
points,reversedpumpdependence,
wavelength switchingandPT-symmetry
breaking.

Optical Fiber
Ferrule-Top
Spirally-Suspended
OptomechanicalMicroresonators for
Photoacoustic
Spectroscopic Gas
Sensing∙T. LI, K.V. Krishnaiah, P.C. Zhao, andA.P. Zhang; Photonics Research Institute,
Department of Electrical Engineering, The
Hong Kong Polytechnic
University, Hong Kong,
China
An
opticalfiber
ferrule-top spirallysuspended optomechanicalmicroresonator is presented forphotoacoustic spectroscopic gas sensing.
It is fabricated by an
in-house optical 3D
μ-printing technology
and its frequency
response is measured
and compared withnumerical simulation.

Control of ultrafast
XUV-induced
dynamics in aminoacids by halogen
functionalization∙D.
Mocci1 ,R.
BorregoVarillas2 ,F. Vismarra1,2 , Y.
Wu1,2 , L. Colaizzi1 ,M.
Reduzzi1,2 ,M. Lucchini1,2 ,J.
Segarra-Martì3 ,V.
Dichiarante4 ,P.
Metrangolo4 , and M.
Nisoli1,2 ; 1 Departmentof Physics, Politecnico
di Milano, Milano,
Italy; 2 IFN-CNR, Milano, Italy; 3 Institutode Ciencia Molecular, Universitat deValencia,
Paterna,
Spain; 4 Departmentof Chemistry, Materials and Chemical
Engineering ”Giulio
Natta”, Politecnico di
Milano, Milano, Italy
We investigate by
ultrafast pump-probe
spectroscopy
the
role
of
halogenfunctionalization
in a small aminoacid following XUVphoto-ionization.
We demonstrate thatthephoto-induced
dynamics are dictatedby the electron affinityof the substituting
halogen.

High-resolution
Multiscale Imagingof Unstained Histological Paraffin
Embedded Tissue
Blocks with Hyperspectral Stokes
Polarimetry∙A. Bykov1 , O. Sieryi1 ,V.
Dremin1,2 , M.
Borovkova1 ,andI.
Meglinski1,2 ;1University of Oulu,
Oulu,
Finland;2
Aston
University,
Birmingham, United
KingdomWedemonstrateadual-mode
hyperspectralpolarization-based
imaging approach forthe characterizationof paraffin-embedded
tissue blocks at different spatial scales withhigh accuracy. The
results are validated
via the comparison
to the gold standard
histopathologicalanalysis.

Designing SiliconGermanium Photodetectors with
Numerical Optimization: The Tradeoff
Between Quantum
Efficiency & Phase
Noise
R. Islam, I.M. Anjum,
C.R. Menyuk, and ∙E.
Simsek; University of
Maryland Baltimore
County,Baltimore,USA
The tradeoff between
quantum
efficiency
and phase noise of
Si-Ge
photodetectors is studied withmodernnumerical
optimization
methods.

Extracting the Berryphase of dimer
chains in a synthetic
dimensionP.
St-Jean1 ,∙F.
Pellerin1 ,J.
DeLeon Mayeu1 , M.
Boisvert2 , W. Coish2 ,and I. Carusotto3 ;1
Université de Montréal,
Montréal,2
Canada;
McGillUniversity, Montréal,
3
Canada;Universita
di Trento, Trento, Italy
We emulate topological dimer chains withnearest-neighbor andlong-range couplings
inthesynthetic
frequency dimensionof an optical fiber
loop, and present a
novel experimental
scheme for extracting
the Berry phase.

JSIII-4.5 FRI 11:45

CD-12.6 FRI 11:45

EF-8.5 FRI

11:45

CH-14.5 FRI 11:45

EE-3.5 FRI

CL-6.5 FRI

EJ-4.6 FRI

EC-2.5 FRI

Combining (3+1)D
printed photonic
circuits and CMOS
technology for futurehigh-performance
integration∙A. Grabulosa1 , J.
Moughames1 ,X.
Porte1,2 ,and D.
Brunner1 ; 1 Institute

Order of magnitude
increase in storage
time of Brillouinbased memory∙A. Geilen1,2 ,S.
Becker1,2 ,and B.
1
Stiller1,2 ;Max
Planck Institute for
the Science of Light,
Erlangen, Germany;

Mapping Chaotic
Switching in a ring
resonator∙R. Dikande Bitha1 ,A.
Giraldo2 ,B.
Krauskopf1 ,and
N.G.R.
Broderick1 ;1
Dodd-Walls Centre
for Photonic andQuantum Technolo-

Sensitive Detectionof Ultrafast Photoacoustics Using
Modulated Asynchronous Optical
Sampling∙M. Velsink, M. Illienko, P. Sudera, and
S. Witte; Advanced
ResearchCenterAttosecond Rabi
oscillations revealedin EUV-driven highharmonic spectroscopy∙A. de las Heras1 ,C.
HernándezGarcía1 , J. Serrano1 ,T.
Popmintchev2,3 ,andL.
Plaja1 ;
197

11:30

11:45

11:30

11:45

Plug-and-play stimulated Raman microscopy system forbroadband coherent
vibrational imaging
F. Crisafi1 , B. Talone1 ,A. Ragni1 , G. Di
Noia1 , M. Rahman2 ,J. He3 , J. Marcellino3 ,G. Kar3 , Y. Samad3 ,

11:30

11:45

Semi-analytical
Approach for Modeling Strong Couplingof Quantum Emittersin Electromagnetic
Resonators∙M.
Abutoama1,2 ,G. Kountouris1,2 , J.
Mørk1,2 , and P.T.
Kristensen1,2 ; 1 DTU

11:30

11:45

Backscattering in
slow-light valleyHall photonic topological waveguides∙G.
Arregui1 ,C.A. Rosiek1 ,A.
Vladimirova1,2 ,M.
Albrechtsen1 ,B.
Vosoughi
Lahijani1,2 , R. Ellebæk

NOTES

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Centre, Institute ofPhysics of the Czech
Academy of Sciences,
Za Radnicí 828, 25241,
Dolní Břežany, Czech
2
Republic;
Instituteof Plasma Physics& Lasers - IPPL,
Hellenic
Mediterranean
University
Research Center, Tria
Monastiria
74100,
Rethymno, GreeceWedemonstrate
suitableregimewhere SPP excitation
along with Fresnel
diffraction lead to
LIPSS formation andtheir replication on
Si by carefully tuning
distance
betweenadjacent laser irradiation spots and theirrelative laser fieldpolarization

Numérique et Nanosciences (LP2N), UMR
5298,
CNRS-IOGSUniversité Bordeaux,Talence,
France;2
ALPhANOV, Talence,FranceWe present an all-fiberpolarization
maintaining tunable laser
systemdelivering
sub-100 femtosecond
pulses from 1870 nm
up to 2050 nm soliton
pulses using commercially available opticalfiber.

cold polar molecules
C. Karam1 , M. Meyer
zum Alten Borgloh2 , R.
Vexiau1 , M. Lepers3 ,S. Ospelkaus2 , N.
Bouloufa-Maafa1 ,L. Karpa2 , and ∙O.
Dulieu1 ; 1 Laboratoire
Aimé Cotton, CNRS,
U. Paris-Saclay, Orsay,
2
France;3InstitutfürQuantenoptik,
Leibniz Universität,
Hannover, Germany;
3
Laboratoire
interdisciplinaire Carnot
de Bourgogne, Dijon,
FranceWe propose a method
to engineer longrange
interactions
betweenultracold
ground-state
molecules
using
optical fields,toprevent short-range
collisional
losses.
It maps the microwave
shieldingonto a two-photontransition.

By leveraging exciton resonances inatomically thin WS2 ,we realize actively
tunablehybrid-2D
photodetectors. The
tuning efficiency isgreatlyenhancedthrough integration
with a Van der
Waalsheterostructure cavity and anon-local dielectricmetasurface.

Shan1 , S. Stephan1,2 ,M. Gittinger1 ,L.
Lackner1 , B. Han1 ,F. Eilenberger3 , R.
Banerjee4 , S. Tongay4 ,K.
Watanabe5 ,T. Taniguchi5 ,C.
Lienau1 , M. Silies2 ,C.
Anton-Solanas6 ,M. Esmann1 , and C.
Schneider1 ; 1 Carl vonOssietzky University,
Oldenburg, Germany;2
Hochschule
Emden/Leer,
Emden,
3
Germany; Friedrich
Schiller
University
Jena,
Jena,
Ger4
many; Arizona State
University,
Temple,5
USA;
National
Institute for Materials
Science,
Tsukuba,
Japan; 6 Universidad
Autónoma de Madrid,
Madrid, Spain
We report and inspect
the properties ofa bright and highpurity single photon
sourcebased
on
an atomically thincrystal coupled to atunable asymmetricalcavity boosting the
spontaneous emissionof single photons.

∙P.U. Jepsen; DTU
Electro, Technical University of Denmark,Kongens
Lyngby,Denmark
Novel measurementsof the third-ordernonlinearityofsilicaresponsibleforTHz-driven
second-harmonic
generation are performed by comparing
theupconversion
signal in Air Biased
Coherent Detection
with the detection
signal in a silica-basedsolid-state detector.

demultiplexingof
PolMuxchannels
using a polarization
independent
coherent
heterodyne
receiver.
The data
is successfully demultiplexed with areduced penalty andsensitivities
betterthan -28 dBm for
32 Gbps multiCAP
signals.

Petremand1 ,I.
Prieto1 , O. Dubochet1 ,M. Despont1 ,R.
Grange2 , H. Sattari1 ,and A.H. Ghadimi1 ;1
Swiss Center forElectronics
andMicrotechnology(CSEM), Neuchâtel,2
Switzerland;
ETH
Zurich, Department of
Physics, Institute forQuantum Electronics,
OpticalNanomaterial Group,, Zurich,
Switzerland
Lithium niobate on
insulator (LNOI) is
among the promising
integrated photonics
platform that offers
uniqueimportant
opticalproperties.
In this work we
present the staticalcharacterizationofourmulti-mode
interferometer (MMI)
beam splitters at
C-band.

mans1 , O. Vanvincq1 ,A. Cassez1 , and A.
Mussot1 ; 1 Univ. Lille,
CNRS, UMR 8523 PhLAM - Physiquedes Lasers Atomes
et Molécules, Lille,
2
France;ONERA,
Palaiseau, France
We present a highly
coherent self-phaselocked
tri-comb
light source, basedonspatiallightmultiplexing in a
tri-core
non-linear
fiber.
We demonstrate the coherence
between the combs
with a Four Wave
Mixing spectroscopy
experiment.

Foyer, 1st oor ICM
12:00 – 13:00
CLS-2: Career and diversity lunch for PhD
candidates
Chair: Crina Cojocaru, Universitat Politecnica deCatalunya, Barcelona, SpainNOTES

PhD candidates looking for the next steps in their career
will have the opportunity to share the challenges they arefacing in their research with their peers and more advanced researchers. Pre-registration is mandatory.

198

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Femto-ST, UniversitédeFranche-Comté,
CNRS
UMR6174,
Besançon,France;2
Institue of Photonics, Department of
Physics, University ofStrathclyde, Glasgow
G1
1RD,
UnitedKingdom
Using additive andCMOS
compatible
one- and two-photon
polymerization, i.e.
flash-TPP printing,we create low-loss 3D
integrated photonic
waveguides
andsingle-mode splittersfor scalable, dense andparallel interconnects,
which is challenging
to realize in 2D.

DepartmentofPhysics,
FriedrichAlexander Universität
Erlangen-Nürnberg,
Erlangen, GermanyWeexperimentallydemonstrate a cryogenic
optoacoustic
memory with an
intrinsic
storagetime beyond 135 ns.
Our scheme exceeds
previous results by afactor of 13, paving
the way towards a 1 μs
coherent all-opticalstorage.

gies, University of
Auckland, Auckland,
New Zealand; 2 Schoolof Computational Sciences, Korea Institutefor Advanced Study,
Seoul, Korea
We investigate thechanging symmetry
properties of delocalized chaotic attractors
in a ring resonatoras the parameters arevaried. We find spontaneous
symmetrybreaking along withthe merging of chaotic
attractors and suggest
this is a universal
feature.

for
Nanolithography,
Amsterdam,
Netherlands
Asynchronous opticalsampling(ASOPS)is inefficient if thepump-probe
measurement range ofinterest is shorter thanthepulse-to-pulse
time. We demonstrate
a frequency modulated ASOPS scheme
for detecting ultrafast
photoacoustics, enabling 20 times fastermeasurements.

1

Universidad de Salamanca, Salamanca,
Spain; 2 University ofCalifornia, San Diego,
3
USA;
Photonics
Institute, TU Wien,
Vienna, Austria
We report
highharmonic generation
driven by extreme
ultraviolet
pulsesshowing a trace of
attosecond
Rabi
oscillations.
Thisdemonstrates,forthe first time, thatultrafast resonant dynamics are a relevant
feature in strong-fieldinteractions
using
short-wavelength
lasers.

B. Mao3 , R. Vanna4 ,F. Hoffmann5 , O.
Guntinas-Lichius5 ,S. Ghislanzoni6 , I.
Bongarzone6 ,S.Y.
Set3 , A.C. Ferrari3 ,G. Cerullo7 , and ∙M.
Negro1,2 ; 1 Cambridge
Raman
Imaging
S.r.l., Milano, Italy;
2
Cambridge
Raman Imaging Ltd.,
Cambridge,
UK;
3
Cambridge Graphene
Centre,Universityof Cambridge, UK;
4
CNR IFN, Milano,
Italy; 5 Jena University
Hospital, Jena, Germany; 6 Department ofAdvanced Diagnostics,
Fondazione
IRCCS
Istituto
Nazionaledei Tumori, Milano,
Italy; 7 Dipartimento
di Fisica, Politecnico
di Milano, Italy
We combine an allfiber dual wavelength,self-synchronizedlaser and a dedicated multi-channel
detection unit toperform
state-ofthe-art
broadband
SRS
microscopy.
Our
synergistic
design simplifies SRS
implementation enabling plug-and-playbroadband coherent
vibrational imaging.

Electro, Technical University of Denmark,Lyngby,Denmark;
2
NanoPhoton - Center
for Nanonphotonics,
Lyngby, Denmark
We present a semianalytical approach to
calculate the couplingstrength between aquantum emitter andanelectromagnetic
resonator without theneed for fitting parameters and find an
extraordinary quantitative
agreementwithindependent
reference calculations.

Christiansen2,3 , and
S. Stobbe1,2 ; 1 DTU
Electro, Department
ofElectricalandPhotonics Engineering,Technical Universityof Denmark, Kgs.
Lyngby,Denmark;
2
NanoPhoton – Centerfor
Nanophotonics,
Technical Universityof Denmark, Kgs.
Lyngby,Denmark;
3
DTU
Construct,
Department of Civil
andMechanicalEngineering, Technical
University of Denmark, Kgs. Lyngby,
DenmarkWe
measurethe
propagation
lossesand scattered fields
instate-of-the-art
slow-light valley-Hall
waveguides and findbackscatteringtodominate over otherlossmechanisms,
thereforeraisingquestions about thevalue of topological protection forreciprocal slow light.

2

NOTES

199

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14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

CM-10: Dynamics oflaser-induced processes

CJ-9: Novel fibers

EA-8: Nonclassicalstates of light

CK-14: Recent advances in laser
technology

EI-3: Novel lowdimensional andfunctional materials

CC-6: THz devices

CI-7: Satellite andradio

CE-10: Doped
optical materials

Chair: Mahmoud Gaafar, Deutsches ElektronSynchrotron, DESY, Hamburg, Germany

Chair: Nicolò Maccaferri,Umeå University, Umeå,SwedenChair:
Victor TorresCompany,
Departmentof Microtechnology andNanoscience, Chalmers
University of Technology,
Gothenburg, Sweden

Chair:
Nadia Boetti,
LINKS
Foundation,
Torino, Italy

CK-14.1 FRI

14:00

EI-3.1 FRI (Invited) 14:00

CC-6.1 FRI (Invited) 14:00

CI-7.1 FRI

14:00

CE-10.1 FRI (Invited) 14:00

A fully photonic integrated circuit based
Erbium laser∙Y. Liu1,2 , Z. Qiu1,2 ,X. Ji1,2 , A. Bancora1,2 ,G.
Lihachev1,2 ,J.
Riemensberger1,2 ,
R.N.
1,2
1,2
Wang , A. Voloshin ,and T.J. Kippenberg1,2 ;1Institute of Physics, Swiss
Federal Institute of Technology Lausanne (EPFL),
CH-1015 , Lausanne,
2
Switzerland;Centerfor Quantum ScienceandEngineering,Swiss
Federal Institute of Technology Lausanne (EPFL),
Lausanne, Switzerland
We present a fully
photonic
integrated
circuit-based
Erbiumdoped waveguide Vernierlaser that can achieve
50 Hz intrinsic linewidth,> 72 dB side mode
suppression ratio, output
power up to 17 mW, and40 nm wide wavelength
tunability.

Optomechanics of suspended magnetic vander Waals materials∙J. Wolff, L. Moczko, J.
Thoraval, M. Romeo, S.
Berciaud, and A. Gloppe;
Institut de Physique etChimie des Matériaux deStrasbourg, Université deStrasbourg, CNRS, UMR
7405, Strasbourg, France
We probe magnetic phasetransitions of drum-likesuspendedmagnetic
van der Waals heterostructures combining
nano-optomechanics andopticalspectroscopies
and investigate the tuningof their light emission
and magnetic properties
by strain.

Holographic THz Imaging by Fourier-Domain
Detection with FeldEffect Transistors, andthe Quest for Phase
Retrieval by Physics-Informed Deep Learning
H. Yuan1 , M. Xiang1,2,3,4 ,A. Lisauskas1,5,6 ,L.
Wang2,3 , M. Thomson1 ,2,3
K. Zhou , and ∙H.
Roskos1 ; 1 Physikalisches
Institut,
GoetheUniversität,
Frankfurt
am Main,Germany;2Frankfurt Institute ofAdvanced Studies (FIAS),
Frankfurt am Main,
Germany; 3 Xidian-FIAS
International Joint Research Center, Frankfurt
am Main,Germany;
4
Xidian University, Xi’an,
5
China;
Institute ofApplied Electrodynamics
and Telecommunications,
Vilnius University, Vilnius, Lithuania; 6 Center
for Terahertz Researchand Applications (CENTERA), Institute of High
Pressure Physics, Polish
Academy of Sciences,
Warsaw, Poland
This presentation describes THz holographic
imagingbasedon
Fourier-plane heterodyne
detection with CMOS
field-effecttransistors.
We then discuss thepotential for less complex
imaging systems with

An Efficient Multiband
Transponder for
Satellite Ground Station
based on Photonics∙M. Imran1 , F. Scotti2 , A.
Bogoni1 , M. Presi3 , and P.
Ghelfi2 ; 1 Scuola SuperioreSant’Anna, TeCIP Institute,via Moruzzi 1, 56124,
Pisa, Italy; 2 CNIT, PNTlab, via Moruzzi 1, 56124,
Pisa, Italy; 3 Aerospazio
Tecnologie Srl, via Provinciale Nord 42a, 53040,
Rapolano Terme , Siena,
Italy
An innovative Multiband
Transponder for satellite
Ground Stations is proposed, managing simultaneous bidirectional communications in X and Ka
band with a single reference oscillator. Experimental tests show relevant performance of conversion loss and SNR.

Glass-based materialsfor (bio)photonic
applications∙L. Petit; Tampere University, Tampere, Finland
In this presentation, we
will review our work on
the development of new
bioactive glasses suitable
for the fabrication of optically active fibers and 3D
printed scaffolds.

Chair: Jan Siegel, Instituto de Optica - Consejo Superior de Investigaciones Científicas (CSIC),
Madrid, Spain

Chair:
Laurent Bigot,
CNRS-University of Lille,
FranceChair: Valentina Parigi,
Sorbonne Université, Laboratoire Kastler Brossel,
Paris, France

CM-10.1 FRI (Invited) 14:00

CJ-9.1 FRI (Invited) 14:00

EA-8.1 FRIThe switching cycle ofPhase-Change Materials: Time-resolved
diffraction after laser
excitation∙P. Zalden; European
XFEL, Schenefeld, Germany
Phase-Change
Materials can be cycled bylaser-excitation
between an amorphousand a crystalline state.
Time-resolved
X-ray
diffraction reveals how
glass formation and fast
crystallization is possible
in these materials.

Development of active
fibres with nanostructured cores∙R.
Buczynski1,2 ,M.
Franczyk1 ,D.
Pysz1 ,
J. Aubrecht3 ,G. Stȩpniewski1,2 , A.
Filipkowski1,2 ,M.
Kamrádek3 , I. Kasik3 , and
P. Peterka3 ; 1 Lukasiewicz
Research Network - Institute of Microelectronics
and Photonics, Warsaw,
2
Poland;Universityof Warsaw,
Warsaw,
Poland; 3 . Institute of
Photonics and Electronics
of the Czech Academy of
Sciences, Prague, Czech
Republic
Nanostructured opticalfibres are a new classof fibres with a corecomposed of various
glass nanorods ordered inarbitrary structures. With
this approach refractive
index, gain and photosensitivity
distribution
can be independently
shaped.

Multiport Cyclic Interferometer For Genuine
n-photon Indistinguishability Assessment∙R.
Albiero1,2 ,M.
3Pont , S.E. Thomas3 ,N.
Spagnolo4 ,F.
Ceccarelli2 , G. Corrielli2 ,A.
Brieussel5 ,N.
Somaschi5 , H. Huet3 , A.
3
3
Harouri , A. Lemaître , I.
Sagnes3 , N. Belabas3 , F.
Sciarrino4 , R. Osellame2 ,P. Senellart3 , and A.
Crespi1,2 ; 1 Dipartimento
di Fisica - Politecnico di
Milano, Milano, Italy;2
Istituto di Fotonica e
Nanotecnologie - Consiglio Nazionale delle
Ricerche(IFN-CNR),
Milano, Italy; 3 Centre
for Nanosciences andNanotechnology, CNRS,
Université Paris-Saclay,
Palaiseau,
France;4
Dipartimento di Fisica,
Sapienza
Università
di Roma, Roma, Italy;
5
Quandela SAS, Massy,
FranceWe introduce a novel
method to measure thegenuine indistinguishability of n photons statesusing a low-depth, cyclic
multiport interferometerand demonstrate experimentally this technique
for the case n = 4.

14:00

200

Chair: Clara Saraceno,
University of Bochum,
Bochum, Germany

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/Europe-EQEC 2023

⋅ Friday 30 June 2023

Room 13a ICM

Room 13b ICM

Room 14a ICM

Room 14b ICM

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

14:00 – 15:30

JSIII-5: Brain-inspired
photonic dedvices
and computing I

CD-13: Nonlinear
imaging and microscopy

EF-9: Topologicaland nonlinear effects

CH-15: Bio-sensing

EE-4: Ultrafast nonlinear optics in gases

CL-7: Advanced
microscopy II

CF-11: Parametricultrafast sources

Chair: Antonio Hurtado,
University of Strathclyde,
Glasgow, United Kingdom

Chair: Anderson S L
Gomes, Federal Universityof Pernambuco, Brazil

Chair: Valentina Shumakova, Class 5 Photonics
GmbH, Hamburg, Germany

Chair: Giuseppe Vicidomini, Istituto Italiano diTecnologia, Molecular Microscopy and Spectroscopy,
Center for Human Technologies, Genova, Italy

Chair:
Yoann Pertot,
Fastlite, Antibes, France

EC-3: Emerging
trends and singular
photonic topology

JSIII-5.1 FRI (Invited) 14:00

CD-13.1 FRI

CL-7.1 FRI

CF-11.1 FRIPhotonic neuromorphic
computing∙W. Pernice; Heidelberg
University,
Heidelberg,
Germany
In reconfigurable photonicarchitecturesin-memory computing
allows for overcoming
separation
betweenmemory and central
processing unit as a routefor designing artificial
neural networks, which
operate entirely in the
optical domain.

Polarization-resolved
third harmonic
generation (P-THG)
imaging of myelin
inside optic nerves∙M.
Kefalogianni1,2 ,L. Mouchliadis1 ,N.
Ktena3,4 , S.-I. Kaplanis3,4 ,I.
Kalafatakis3,4 ,S.
Psilodimitrakopoulos1 ,3,4
D. Karagogeos , and E.
Stratakis1,2 ; 1 Institute ofElectronic Structure andLaser, Foundation for
Research and TechnologyHellas,
HERAKLION,
2
Greece;Departmentof Physics, Universityof Crete, HERAKLION,
Greece; 3 Department of
Basic Sciences, Facultyof Medicine, Universityof Crete, HERAKLION,
4
Greece;Institute of
Molecular Biology andBiotechnology,
FoundationforResearchand Technology-Hellas,
HERAKLION, Greece
Intrinsic optical thirdharmonic
generation(THG) signal and its polarization sensitivity are
exploited for extracting
quantitative informationon the content andorientation of myelin innormal and abnormal
nervous tissues.

14:00

Chair: Sylvain Barbay,
C2N, Université Paris
Saclay, France

EF-9.1 FRIRoom 14c ICM

Chair: Marco Grande, Politecnico di Bari, Italy

14:00

CH-15.1 FRI (Invited) 14:00

EE-4.1 FRINonlinear Photonic
Topological Pump
∙M.S.
Kirsch1 ,Y.V.
Kartashov2 , V. Konotop3 ,A. Szameit1 , and M.
Heinrich1 ; 1 Institut für
Physik, Universität Rostock, Rostock, Germany;
2
Institute of Spectroscopy,
Russian Academy of
Sciences, Moscow, Russia;
3
Universidade de Lisboa,
Lisbon, PortugalWeexperimentallyobserve light transport
dynamics in a nonlinear
photonic Thouless pump.
The Kerr effect enables
excitations
initially
placed in the topologically trivial band to entera regime of topologicaltransport for sufficient
excitation powers.

Optical sensing in thebrain with tapered
optical fibers: fromphotoelectric free
optrodes to implantableneuroplasmonics∙F. Pisano1 , A. Balena1 , B.
Spagnolo1 , S. Andriani1,2 ,M. Bianco1 , D. Zheng1 , L.
Collard1 , R. Peixoto3 , M.
Grande4 , M. Valiente5 ,L.M. De La Prida6 ,B.L. Sabatini3 , M. De
Vittorio1,2,7 ,and F.
1
Pisanello1,7 ;Istituto
Italiano di Tecnologia,
Center For BiomolecularNanotechnologies, Lecce,
Italy; 2 Dipartimento di Ingegneria dell’Innovazione,
Università del Salento,
Lecce, Italy; 3 Howard
Hughes Medical Institute,
Department of
Neurobiology,
Harvard
Medical School, Boston,
4
USA;
Dipartimento
di Ingegneria Elettricaedell’Informazione
Politecnico di Bari, Bari,
Italy; 5 Brain Metastasis
Group, Spanish National
Cancer Research Center(CNIO), Madrid, Spain;
6
Instituto Cajal, CSIC,
Madrid, Spain; 7 Equally
Contributing, Lecce, Italy
Here we present the tapered optical fibers (TFs)
technology, which combines the peculiar optical and photonic properties of narrowing waveg-

A single-stage dispersion-controlled multipass cell setup to efficiently drive resonant
dispersive wave emission∙L.
Silletti1 ,T.F.
Grigorova2 , C. Brahms2 ,1
A.b.
Wahid , E.
Escoto3 , P. Balla3,4,5 , S.
Rajhans3,6 , K. Horn7,8 , L.
Winkelmann3 , V. Wanie1 ,A. Trabattoni1,9 , C.M.
Heyl3,4,5 , J.C. Travers2 ,and F. Calegari1,10,11 ;1
CFEL, DESY, Hamburg,
2
Germany;
School ofEngineering and PhysicalSciences,
Heriot-Watt
University,
Edinburgh,
United Kingdom; 3 DESY,
Hamburg,
Germany;4Helmholtz-Institut
Jena, Germany; 5 GSI,
Darmstadt,
Germany;
6
Universität Jena, Germany; 7 Department ofChemistry and Applied
Biosciences, Laboratoryof Physical Chemistry,ETH Zürich, Switzerland;
8
CMWS, DESY, Hamburg, Germany; 9 Instituteof
Quantum
Optics,
University Hannover, Germany; 10 The Hamburg
Centre for Ultrafast Imaging, Universität Hamburg,
Germany; 11 Institut fürExperimentalphysik,
Universität
Hamburg,
Germany
We demonstrate postcompression
of
an

201

14:00

Room Osterseen ICM

14:00

Two- and three-photon
microscopy of genetically encoded fluorescentindicators of oxidative
stress in mouse brain
cells in vivo
∙A.S. Chebotarev1,2 , A.A.
Lanin1,2 , V.A. Katrukha3 ,G.N.
Martynov1,2 ,Y.V. Khramova3 , I.V.
Kelmanson3 ,M.S.
Pochechuev1,2 ,G.P.
Linovskiy1 , D.S. Bilan3 ,V.V. Belousov3,4 , andA.B. Fedotov3 ; 1 Physics
Department,
M.
V.
Lomonosov Moscow State
University, Vorob’evy gory,Moscow, Russia; 2 Russian
Quantum Center, 143025
Skolkovo, Moscow Region,
Russia; 3 M.M. Shemyakin
and Yu.A. Ovchinnikov
Institute of Bioorganic
Chemistry, RAS, Moscow,
Russia; 4 Federal Center ofBrain Research and Neurotechnologies, Moscow,
RussiaWe performed deep
two- and three-photon
microscopy studies ofmouse brain cells in
fixed-slice, ex-vivo, andin-vivo formats using
optogenetic fluorescentprotein pH and hydrogen peroxide sensors,
revealing the dynamics
of oxidative stress during
strokeRoom 21 ICM

14:00

Sub-8 fs Pulses in the
Visible to Near Infraredfrom a Single Stage
Degenerate OpticalParametric Amplifier
T. Deckert, ∙A. Vanderhaegen, and D. Brida;
University of Luxembourg,
Luxembourg,
Luxembourg
A single-stage degenerate optical parametricamplifier (DOPA) with
broad
amplification
bandwidth
produces
sub-10
femtosecond
pulses with excellent
shot-to-shotstability.
Itcomplements
theexisting array of OPAs
in the visible to nearinfrared for advanced
spectroscopy.

Room 22a ICM

Chair: Stefan Rotter, Technical University of Wien,
AustriaEC-3.1 FRI

14:00

Topological insulator
quantum cascade laser
in synthetic space:towards a realization∙A. Dikopoltsev, P. Michelletti, U. Senica, M. Beck, J.
Faist, and G. Scalari; ETH
Zurich, Zurich, Switzerland
Topologicalinsulators
in synthetic dimensions
present protection forthe dynamics of spectral
components.
When
employed to lasers, it
unlockssuper-stablelasing of mode-locked
laser arrays. We suggest afirst realization, using RF
modulated QCL rings

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Room 1 ICM

Room 2 ICM

Room 3 ICM®

/Europe-EQEC 2023

Room 4a ICM

CK-14.2 FRI

EA-8.2 FRI (Invited) 14:15

Quantum engineeringof light with an intracavity Rydberg superatom
V. Magro, J. Vaneecloo,
S. Garcia, and ∙A. Ourjoumtsev; JEIP, CNRSUAR 3573, College deFrance, PSL University,
Paris, France
We achieved the first fully
deterministic preparationofWigner-negative
free-propagating statesof light, by mapping
the internal state of an
intracavity Rydberg superatom onto a coherent
superposition of 0 and 1
photons.

⋅ Friday 30 June 2023
Room 4b ICM

14:15

Spectral Control ofRandom Network Lasers∙T.V. Raziman1,2 , D.
Saxena1 , A. Arnaudon1,3 ,O.
Cipolato1 ,M.
Gaio1 , N.V. Trivino4 ,J. Dranczewski1,4 , A.
Fischer1,4 , A. Quentel1 , S.
Yaliraki5 , D. Pisignano6,7 ,A.
Camposeo6 ,H.
Schmid4 , K. Moselund8,9 ,M. Barahona2 ,and1
R. Sapienza1 ;The
Blackett
Laboratory,
Department of Physics,
Imperial College London,
UK; 2 Department ofMathematics,
Imperial
College London, UK;
3Blue Brain Project, École
PolytechniqueFédéralede Lausanne (EPFL),
Campus Biotech, Geneva,
Switzerland; 4 IBM Research Europe - Zurich,Rüschlikon, Switzerland;
5
Department of Chemistry, Imperial College
London, UK; 6 NEST,
Istituto Nanoscienze-CNR
and Scuola Normale
Superiore, Pisa, Italy;
7
Dipartimento di Fisica,
Università di Pisa, Italy;
8
Paul Scherrer Institut,
Villigen,
Switzerland;9
École PolytechniqueFédérale de Lausanne(EPFL), Switzerland
We show both theoretically and experimentallythat networks made ofdye-based polymer andIndium Phosphide areversatile random lasing
sources with fine spectrathat can be controlled by
non-uniform pumping,and driven by machinelearning.
202

Room 5 ICM

Room 11 ICM

phase retrieval frompower-detection
datausing physics-informed
deep learning.

CI-7.2 FRI

14:15

Pulse sharpened On-Off
Keying Optical modulation for Power Efficient
Satellite OpticalCommunication∙Y.-J. Hyun and S.-K. Han;
Yonsei University, Seoul,
South Korea
Satellite optical communication
requireshigh power and spectral
efficiency. A new modulation method which
provides 3dB enhanced
optical power without additional bandwidth using
half-bit Mach-Zehnderdelay interferometer is
proposed. A proof-ofconcept experiment has
been conducted.

Room 12a ICM

CLEO

Room 13a ICM

Room 13b ICM

CD-13.2 FRI

14:15

Ultrabroadband
Coherent Anti-Stokes
Raman Scattering
Microscopy For
Biological Applications
Via Supercontinuum
Generation in Bulk
Crystals∙F.
Vernuccio1 ,C.
Ceconello1 ,A.
1
Bresci ,F. Manetti1 ,S. Sorrentino1 , R. Vanna2 ,G. Cerullo1,2 , and D.
Polli1,2 ; 1 Department of
Physics, Politecnico di Milano, P.zza Leonardo daVinci 32, 20133 , Milano,
Italy; 2 CNR-Institute for
Photonics and Nanotechnologies (IFN-CNR), P.zza
Leonardo da Vinci 32,
20133 , Milano, Italy
We demonstrate ultrabroadband(500–3100
cm−1 )
coherent-anti
Stokes Raman scattering
microscopy of cancer
cells and tissues using
a 2-MHz Ytterbium
fiber laser system toproduce sub-20-fs precompressed Stokes pulses
via
supercontinuum
generation in bulk media.

Room 14a ICM

EF-9.2 FRI

14:15

Nonlinear optical dynamics probed with freeelectrons∙J.-W.
Henke1,2 ,Y.
Yang3,4 , F.J. Kappert1,2 ,A.S. Raja3,4 , G. Arend1,2 ,G. Huang3,4 , A. Feist1,2 ,Z. Qiu3,4 , R.N. Wang3,4 ,A. Tusnin3,4 , A. Tikan3,4 ,T.J. Kippenberg3,4 , and1
C. Ropers1,2 ;Max
Planck Institute for Multidisciplinary
Sciences,
Göttingen,Germany;2
4th Physical Institute,
University of Göttingen,Göttingen,Germany;3
Institute of Physics, Swiss
Federal Institute of Technology Lausanne (EPFL),
Lausanne, Switzerland;
4
Center for Quantum
Science and Engineering,
Swiss Federal Instituteof Technology Lausanne(EPFL),
Lausanne,
Switzerland
We probe the formationof nonlinear opticalstates like solitons ina photonic chip-based
microresonator using freeelectrons. The nonlinear
dissipative
structures
imprint unique featureson the electron spectra
related to the timedependent
intracavity
field.

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/Europe-EQEC 2023

⋅ Friday 30 June 2023

Room 14b ICM

Room 14c ICM

uides to non-planar micro and nanofabrication
methods to explore unconventional approaches
to interface with brain tissue

Ytterbium fibre laser
to sub-20 fs based on
spectral broadening ina single-stage gas-filled
multi-pass cell.
Additionally, we generate
few-femtosecond
UV
pulses by directly drivinga resonant dispersive
wave setup.
EE-4.2 FRI

14:15

Multipass cell pulse
post-compression at
515nm wavelength as
HHG driver efficiently
targeting 92 eV photon
energy∙M.
Karst1,2,3 ,P.
Pfaller1 , R. Klas1,2,3,4 ,P.
Gierschke1,4 ,M.
Abdelaal1 , Z. Wang1 ,
1,2,3,4J.
Rothhardt,
and J. Limpert1,2,3,4 ;1Institute of Applied
Physics, Jena, Germany;2
Helmholtz-Institute Jena,
Jena, Germany; 3 GSI
Helmholtzzentrum
fürSchwerionenforschung,
Darmstadt,
Germany;4
Fraunhofer
Institutefor Applied Optics andPrecision
Engineering,
Jena, Germany
We present a multipass cell based postcompression delivering
15.7 fs pulses with 0.44
mJ of pulse energy at 22.4
W of average power anddemonstrate its capability
as a highly efficient HHG
driver around 92 eV.

203

Room Osterseen ICM

CL-7.2 FRIRoom 21 ICM

Room 22a ICM

14:15

Imaging Intracellular
Metabolic Activity of
Mammalian Oocytes by
Dynamic Full-field
Optical Coherence
Microscopy∙S.
Morawiec1 ,P.
Stremplewski1 , A. Ajduk2 ,3,4
B. Kennedy , and M.
Szkulmowski1 ; 1 Instituteof Physics, Faculty ofPhysics, Astronomy andInformatics,
Nicolaus
Copernicus University in
Torun, Torun, Poland;
2
Department of Embryology,
Faculty ofBiology, University of
Warsaw, Warsaw, Poland;
3
BRITElab, Harry Perkins
InstituteofMedicalResearch, QEII Medical
Centre, Perth, Australia;
4
Department of Electrical,
Electronic & Computer
Engineering, School ofEngineering, The University of Western Australia,
Perth, Australia
Dynamic full-field opticalcoherencemicroscopy(FF-OCM) of living
oocytes provides highquality images of theintracellular structures
based solely on theirscattering potential. The
spatiotemporal analysis
of OCM images reveals
intracellularmotiondynamics, hence theinformation on the cell’smetabolic activity.

CF-11.2 FRI

14:15

Ultrashort-pulse OPAs:
Bridging the gap in
UV–VIS
T.
Juodagalvis1 ,K.
Jurkus1 , ∙J. Berzinš1 ,V. Sinkus1 , and R.
1
Budriūnas1,2 ;LightConversion,
Vilnius,2
Lithuania;
Vilnius
University Laser ResearchCenter, Vilnius, Lithuania
We will present several
techniques (alternative to
3H-pumped NOPAs) toobtain gapless wavelength
tunability for ultrashortpulses in UV–VIS range
using Yb-based lasers.

EC-3.2 FRI

14:15

Experimental demonstration of gauge confinement in point-wise
shifted periodic potentials∙A. Alberucci1 ,C.P.
Jisha1 , M. Monika2 , U.
2
Peschel , and S. Nolte1,3 ;1Friedrich Schiller University Jena, Institute ofApplied Physics, Jena,
2
Germany;Friedrich
Schiller University Jena,
Institute of Solid State
Physics and Optics, Jena,
3
Germany;
Fraunhofer
Institute for Applied
Optics and Precision
IOF Engineering, Jena,
GermanyWe
investigate
experimentally
andtheoretically the opticalpropagation in a periodic
potential subject to apoint-dependent delay.
The action of the delay
is interpreted as a gauge
field.

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Room 1 ICM
CM-10.2 FRI

14:30

Room 2 ICM
CJ-9.2 FRI

14:30

Carrier transport after
ultrashort-pulse-laser
excitation of dielectricmaterials leads to theformation of 10 MV/melectric fields
S.H. Møller, P.S. Sneftrup,
B. Julsgaard, and ∙P.
Balling; Aarhus University, Aarhus, Denmark
Solving the transport
equations in a model dielectric (SiO2) shows thatultrashort-pulse-laser
excitation is associatedwith the formation ofa strong electric field,
manifesting itself bytransient birefringenceand emission of THz
radiation.

Yellow (575 nm) laser bysingle-mode doubleclad structured Dy3+doped waterproof
fluoro-aluminate glass
fiber
∙A.
Koganei1 ,H.
Katsuragawa1 ,K.
Takahashi1 , O. Ishii2 ,M. Yamazaki2 ,andY. Fujimoto1 ; 1 Chiba
Instituteoftechnology, Narashino, Japan;
2
Sumita Optical Glass,Inc., Saitama, JapanWe
demonstratedayellow laser using asingle-mode double-clad
structured Dy3+-doped
waterproof
fluoroaluminate glass fiber.
The maximum output
power of 169.2 mW
was achieved with slope
efficiency of 33.6% at 575
nm wavelength.

CM-10.3 FRI

CJ-9.3 FRI

14:45

Photomechanical Laser
Fragmentation of
Iridium Oxide Microparticles Revealed by
Pump-Probe
Microscopy∙M.
Spellauge1,2 ,A.R.
Ziefuss2 ,S.
Reichenberger2 ,S.
Barcikowski2 , and H.P.
1
Huber1 ;Lasercenter,
Department of Applied
Sciences and Mechatronics, Munich UniversityofAppliedSciences
HM, Munich, Germany;
2
Technical Chemistry I
and Center for Nanointegration Duisburg-Essen(CENIDE), University ofDuisburg-Essen,
Essen,

Room 3 ICM

14:45

Low-loss Fused Silica
Hollow-Core Fiber
Delivery of Mid-infrared Light at 6-μm
∙Q. Fu, I.A. Davidson,
G.T. Jasion, L. Xu, F. Poletti, N.V. Wheeler, and
D.J. Richardson; Optoelectronics Research Centre,
University of Southampton, Southampton, United
Kingdom
We report record lowloss, ~7-dB/m, delivery of
6.045μm light via fusedsilica, single claddingring hollow-core fiber.
Quasi-single-mode
beams (3.4mW) weredelivered through a ~1m
fiber from quantum cas-®

/Europe-EQEC 2023

Room 4a ICM
CK-14.3 FRIRoom 4b ICM

14:30

Dynamic Random
Lasers of Reconfigurable Active Colloidal
Assemblies∙W.K. Ng1 , M. Trivedi2 ,D. Saxena1 , R. Sapienza1 ,and G. Volpe2 ; 1 The
Blackett
Laboratory,
Department of Physics,
Imperial College London,
London, United Kingdom;2
Department of Chemistry, University College
London, London, United
Kingdom
Self-organizedlasersare achieved throughthe reversible out-ofequilibrium self-assemblyof reconfigurable colloidal systems.
These
lasers demonstrate activeandprogrammablebehaviours that canpotentially be developed
for sensing and display
purposes.

EA-8.3 FRI

14:45

Anyonic two-photon
coincidence statistics inbirefringent waveguidecircuits∙M. Ehrhardt, M. Heinrich, and A. Szameit; Institute for Physics, University of Rostock, Rostock,Germany
We synthesize fractional
coincidence
statistics
for photon pairs inlaser-written waveguide
networks. To this end,
we show that arbitraryexchange phases canbe created by tailoring
waveguides birefringence
and an appropriate choiceof input polarizations.

CK-14.4 FRI⋅ Friday 30 June 2023

14:45

Perovskite quantum dot
topological laser basedon a one-dimensional
cavity∙J. Tian1,2 , Q.Y. Tan1,3 ,Y. Wang1,3 , Y. Yang1,2 ,G. Yuan1,2 , G. Adamo1,2 ,and C. Soci1,2 ; 1 Centre
for Disruptive Photonic
Technologies School ofPhysical and Mathematical Sciences Nanyang
Technological University,
Singapore,
Singapore;
2
PAP, School of Physical and Mathematical
Sciences, Nanyang Technological
University,
Singapore,
Singapore;3
ERI@N,
Interdisciplinary Graduate School,

EI-3.2 FRI

14:30

Measuring the bolometric response of superconducting magic-angle
twisted bilayer graphene∙G. Di Battista1 , P.
Seifert2 , K. Watanabe3 ,T. Taniguchi4 ,K.-C.
Fong5 , A. Prinicpi6 , and
D. K. Efetov1 ; 1 Fakultät
für Physik,
LudwigMaximilians-Universität,
Munich,Germany;2
Institute of Physics,
Faculty of Electrical Engineering and Information
Technology, Universität
der Bundeswehr , Munich,
3Germany;
ResearchCenter for Functional
Materials,
National
Institute for Materials
Science, Tsukuba, Japan;
4International
Centerfor Materials Nanoarchitectonics,
National
Institute for Materials
Science, Tsukuba, Japan;
5
Quantum Engineeringand Computing Group,
Raytheon BBN Technologies, Cambridge, USA;
6
Department of Physics
and Astronomy,
The
University of Manchester,Manchester,
UnitedKingdom
We measure the bolometricresponseofmagic-angle
twistedbilayer graphene andextract the temperaturedependenceofthethermalconductancein the superconducting
state. Our work lays thefoundation for future
thermal transport studies
on this system.
EI-3.3 FRI

14:45

2D high-temperature
superconducting
nanodetectors

204

Room 5 ICM
CC-6.2 FRI

14:30

Room 11 ICM
CI-7.3 FRI

14:30

Ultrabroadband singleshot waveform detectionof air-plasma based THz
sources
A. Ohrt, S. Zhou, Y. Ding,
P.U. Jepsen, and ∙B. Zhou;
Department of Electricaland Photonics Engineering, Technical Universityof Denmark, Kgs. Lyngby,
Denmark
We demonstrate thefirst single-shot THz
waveform detection witha two-color air-plasma
based THz source via
a non-collinear opticalprobe-THz beam geometry.
Single-shot THz
detection up to 12 THz isrealized.

Performance Optimization of a Frequency
Quadrupler based
Analog Radio-overFiber Fronthaul for 5G
mmWave∙S. S J, L. B, R. Ganti,
D. Koilpillai, and D.
Venkitesh; Indian Institute of Technology
Madras, Chennai, India
An analog optical frequency
quadruplingsystem is realized fortransport of 5G mmWave(26.4 GHz) over 2 km
fiber.
Optimizationofoperatingconditions for 100 MHz, upto
256QAM is demonstrated
experimentally.

CC-6.3 FRI

CI-7.4 FRI

14:45

Achieving Large andBroadband THz Optical
Activity via 3D ChiralMetamaterials∙A.D.
Koulouklidis1,2 ,I. Katsantonis1,3 ,M.
Manousidaki1 ,A.C.
Tasolamprou1,4 ,C.
Daskalaki1 , C. Kerantzopoulos2 ,I. Spanos5 ,S. Tzortzakis1,3 ,M.
Farsari1 ,
and
M.
1,3 1
Kafesaki ; Institute ofElectronic Structure andLaser, Foundation for
Research and TechnologyHellas,
Heraklion,
Greece; 2 Department of
Physics, University ofCrete, Heraklion, Greece;
3
Department of Materials

14:45

Stabilization of fastlaser chirps with multistage correction control
for time-reversal ofbroadband radiofrequency signal∙T. Llauze and A.
Louchet-Chauvet; Institut
Langevin, ESPCI Paris,
Universit´e PSL, CNRS,Paris, France
A multi-stage correction
scheme allows for fast andprecise frequency chirps
with a DBR laser, thatwill be used for the future
demonstration of analog
time-reversal of broadband radiofrequency signals.

Room 12a ICM
CE-10.2 FRI

14:30

A pathway to Er sites in
Si with long spin andoptical coherence times∙A.
Lyasota1 ,I.R.
Berkman1 , G.G. de Boo1 ,J.G.
Bartholomew2,3 ,B.C. Johnson4,5 ,J.C.
McCallum4 , B.-B. Xu1 ,S. Xie1 , R.L. Ahlefeldt6 ,M.J. Sellars6 , C. Yin1,7 ,and S. Rogge1 ; 1 Centre of
Excellence for Quantum
Computation and Comm.
Tech., School of Physics,
Univ.
of New South
Wales, Sydney, Australia;
2
Centre for Engineered
Quantum Systems, Schoolof Physics, The Univ. of
Sydney, Australia; 3 Nano
Institute, The Univ. of
Sydney, Australia; 4 Centreof Excellence for Quantum
Computation and Comm.
Tech., School of Physics,
Univ. of Melbourne, Australia; 5 School of Science,
RMIT Univ., Melbourne,
6Australia;
Centre of
Excellence for Quantum
Computation and Comm.
Tech., Research Schoolof Physics, AustralianNat.
Univ., Canberra,
Australia; 7 Hefei Nat.
Lab. for Physical Sciencesat the Microscale, CAS
Key Lab. of Microscale
Magnetic
Resonance
and School of PhysicalSciences, Univ. of Scienceand Technology of China,
Hefei, China
We present key parameters affecting optical andspin properties of Er in Si.
By optimising co-dopant
types and Er concentrations, we achieved long Er
coherence times making
Er a promising candidate
for future quantum applications.

CLEO

Room 13a ICM
JSIII-5.2 FRI

14:30

Room 13b ICM
CD-13.3 FRI

14:30

Room 14a ICM
EF-9.3 FRI

14:30

®

/Europe-EQEC 2023

Room 14b ICM
CH-15.2 FRI⋅ Friday 30 June 2023

Room 14c ICM

14:30

EE-4.3 FRI

14:30

Room Osterseen ICM
CL-7.3 FRI

14:30

Room 21 ICM
CF-11.3 FRI

14:30

Room 22a ICM
EC-3.3 FRI

14:30

III-V nanowire basedneuromorphic nanophotonic circuits∙V. Flodgren, D. Winge,
D. Alcer, M. Borgstrom,and A. Mikkelsen; NanoLund and Department of
Physics, Lund University,
Lund, Sweden
We explore an artificial
nanophotonic neural network circuit derived fromthe insect brain as implemented using highly efficient III-V semiconductor nanowires broadcasting in a single quasi 2D
waveguide.

CARS imaging allowed
by Four-Wave-Mixing
widely tunable bychirped pulses
C. Corso Silva1 , T.
Mansuryan2 , A. Tonello2 ,Y. Arosa-Lobato2,3 , Y.
Stepanenko1 , V. Couderc2 ,and ∙K. Krupa1 ; 1 Instituteof Physical Chemistry
Polish Academy of Sciences, Warsaw, Poland;
2
XLIM UMR CNRS
7252 Université de Limoges, Limoges, France;
3
Departamento de Fisica
Aplicada, Universidade deSantiago de Compostela,
Santiago de Compostella,
Spain
We developed a new tunable light source using input stretched pulses witha linear chirp propagating in a concatenationof a standard and a microstructure fibers. We
apply this light source
for selective CARS microscopy.

Octave spanningsupercontinuum
generation in water atmulti-kilohertz
repetition rates∙K.R. Keller1 , R. RojasAedo1 , A. Vanderhaegen1 ,M. Ludwig2 , and D.
Brida1 ; 1 Université duLuxembourg,
Luxembourg,
Luxembourg;
2
Deutsches ElektronenSynchrotron
DESY,
Hamburg, Germany
Water can be harnessedas an effective medium
for octave spanningsupercontinuum(SC)
generation with highsignal stability and superior spectral broadening
compared to crystals in
multi-kHz platforms bymeans of controlled waterflow rate.

Non-Contact Photoacoustic Lipid Imaging
by Remote Sensing onFirst Overtone of C-H
Bond∙G. Hu1 , X. Dong1 , Y.
Zhou1 , J. Kang1,2 , andK.K.Y. Wong1,2 ; 1 The
University of Hong Kong,
Faculty of Engineering,
Department of Electricaland Electronic Engineering, Hong Kong, China;
2
Advanced
Biomedical
Instrumentation Centre,
Hong Kong Science Park,
Hong Kong, China
A label-free and bondselective photoacoustic
remotesensing
microscopy targeting at thefirst overtone of C-Hbond for lipid imaging is
proposed, which enables
high-performance tissue
scale lipid imaging inphantom samples andmodel organism.

Generation andCompression of HighEnergy Sub-10fs Pulses
at MHz Repetition Rates∙A. Alangattuthodi, M.
Emons, R. Fabbri, J.
Meier, J. Montano, R.-C.
Secareanu, S. Venkatesan,
U. Wegner, D. Rompotis,
M. Lederer, M. Meyer,
T. Mullins, and D.E.
Rivas; European XFEL,
Hamburg, Germany
We report on the development of high repetition rate ultrafast laser
to be used in synchronization with European
XFEL pulses for providing new experimental capabilities and hence having unprecedented accessto fundamental science.

Ultrasound-induced
light focusing inside
scattering media∙B. Mestre Torà and M.
Duocastella; Universitat
de Barcelona, Barcelona,
Spain
We present an extended
study of the capability
that shaped ultrasonicwaves offer to guide lightinside turbid media. Our
results
demonstratedanenhancementinlight-confinement of afactor of 7 compared toconventional methods.

Visible NOPO with
Broadband Intracavity
Sum-Frequency Mixing
for the Generation of
Rapidly Tunable Femtosecond Near-UV Pulses∙F.J. Geesmann1 ,R.
Mevert1,2 , D. Zuber1,2 ,and U. Morgner1,2,3 ;1Institute of Quantum
Optics, Leibniz Universität Hannover, Hannover,Germany; 2 Cluster of
Excellence
PhoenixD(Photonics, Optics, andEngineering-Innovation
Across Disciplines), Hannover, Germany; 3 Laser
Zentrum Hannover e.V.,
Hannover, Germany
Femtosecond
pulsesfrom 333-413 nm withaverage powers up to 90
mW were generated via
non-collinear SFG in a
NOPO producing visible
light. Rapid tuning overthe entire spectral range
was demonstrated with
43.9 Hz.

Dirac Points Embeddedin the Continuum ofhyperbolic waveguides∙P. Pujol-Closa1 ,L.
Torner1,2 ,andD.
1Artigas1,2 ;ICFO InstitutdeCiencies
Fotoniques, The Barcelona
Institute of Science andTechnology, Castelldefels,
Spain; 2 Department of
Signal Theory and Communications, Universitat
Politècnica de Catalunya,
Barcelona, Spain
Dirac Points embedded in
the continuum are a new
topological entity raisingfrom the interaction of
two bound states in thecontinuum. The result isa single Hermitian Diracpoint surrounded by
non-hermitian radiatingstates.

JSIII-5.3 FRI

CD-13.4 FRI

EF-9.4 FRI

CH-15.3 FRI

EE-4.4 FRI

CL-7.4 FRI

CF-11.4 FRI

EC-3.4 FRI

14:45

A Large Photonic Spiking Neural Network∙R. Talukder, A. Skalli,
and D. Brunner; FEMTOST Institute, Besancon,
FranceWe have experimentally
implemented a large scale
photonic neural network,
comprising of more than
30,000 neurons in it. This
proof-of-concept experiment serves as next generation bio-inspired learning test bed for photonic
neural networks.

14:45

Smart Control of Supercontinuum Generationby Machine Learning
Towards Multiphoton
Microscopy Applications
V.T. Hoang, Y. Boussafa,
L. Sader, S. Février, V.
Couderc, and ∙B. Wetzel;
XLIM Research Institute,
CNRS UMR 7252, University of Limoges, Limoges,
FranceWe numerically study
how the suitable adjustment of femtosecond
pulse patterns in combination with machinelearning can be leveraged
to maximize the output
spectral intensities and

14:45

Two-Photon Pumped
Exciton-Polariton Condensation∙N.
Landau1 ,D.
Panna1 , S. Brodbeck2 ,C.
Schneider3 ,S.
Höfling2 , and A. Hayat1 ;1
Department of Electricaland Computer Engineering, Technion – Israel
Institute of Technology,
Haifa, Israel; 2 Technische
Physik,Universität
Würzburg,Germany;3
Institute of Physics, Carlvon Ossietzky Universität
Oldenburg, Germany
We report the firstexperimental observationof two-photon pumped
polariton
condensa-

14:45

A Dual-Region FiberOptic SPR Biosensor
with Self-Referencing
Compensation of Bulk
Refractive Index andTemperature Effects∙V. Bello1,2 , W. Vandezande2,3 , D. Daems2 ,and J. Lammertyn2 ;1
Department of Electrical, Computer andBiomedical Engineering,
UniversityofPavia,
Italy; 2 MeBioS-Biosensor
Group, Department of
Biosystems, KU Leuven,
3
Belgium;
Centre for
Membrane Separations,
Adsorption,
Catalysisand Spectroscopy for
Sustainable
Solutions,

14:45

The Effect of Nitrogen
Rotational Response on
Ultra-Flat Supercontinuum Generation in GasFilled Hollow-Core
Photonic Crystal Fiber∙M. Sabbah, F. Belli, C.
Brahms, and J.C. Travers;
School of Engineeringand Physical Sciences,
Heriot-Watt University,
Edinburgh,
UnitedKingdom
We demonstrate flatsupercontinuum
generation in argon andnitrogen-filled
antiresonant
hollow-core
fibre. In nitrogen, we
observe reduced spectral
power density in the

205

14:45

Metabolic Imaging of
2D and 3D live cell
models using a beamscanning SyncRGBFLIM microscope∙M.L.
Ribeiro1 ,C.
Maibohm1 ,T.
Magalhães3 ,M.
Miranda2 , V. Amorim2 ,P.T.
Guerreiro2 ,R.
Romero2 , H. Crespo2,3 ,and J.B. Nieder1 ; 1 INL- International Iberian
Nanotechnology Laboratory, Ultrafast Bio- andNanophotonics
group,Braga, Portugal; 2 Sphere
Ultrafast Photonics, Porto,
3
Portugal;
IFIMUP-IN
and Dept.
of Physics
and Astronomy, Porto,

14:45

Compact Low Repetition Rate Optical Parametric Oscillators
Enabled By Herriott
Cells∙E. Allan1 , D. Bajek2 ,and R.A. McCracken1 ;1
Scottish
Universities
Physics Alliance (SUPA),
Institute of Photonics
and Quantum Sciences,
School of Engineeringand Physical Sciences,
Heriot-Watt University,
Edinburgh, United Kingdom; 2 Photodynamic
Therapy, Ninewells Hospital, Division of Molecular
and Clinical Medicine,
University of Dundee,
Dundee, United Kingdom

14:45

Measuring the topological aberration of
optical vortices∙R. Barros, S. Bej, R.
Fickler, and M. Ornigotti;
Tampere University, Tampere, Finland
We report the first experimental observation of the
topologicalaberrationof optical vortices uponreflection. We show that
topological aberrations
can be measured forimperfect vortices bycomputing their acquired orbital angularmomentum sidebands.

CLEO

Room 1 ICM

Room 2 ICM

Germany
The role of photomechanicalprocesses
during ultrashort laser
fragmentation of iridiumoxide
microparticles
wasinvestigatedbypump-probe microscopy.
The results aid in theunderstanding of microparticle fragmentation
dynamics on timescales
ranging from ps to μs.

cade laser at a coupling
efficiency of 85%.

CM-10.4 FRI

CJ-9.4 FRI

15:00

From femtosecond laserinduced plasma formation inside glass tostress wave generationand propagation:
Experiments andmodelling∙A.
Mouskeftaras1 ,O.
Koritsoglou1 ,G.
Duchateau2 ,and O.
1
Uteza1 ;Aix-Marseille
Université, CNRS, LP3,
UMR7341,
Marseille,
France; 2 CEA-CESTA, Le
Barp, France
In this work, we are
addressing the need forbetter understanding of
the mechanical effects
involved in the femtosecond laser processing oftransparent
materials
by combined experimental and theoreticalinvestigation.

15:00

Er-Ce Co-doped Aluminosilicate Fibres for C
and L-Band Amplifiers∙Z. Zhai, A. Halder, andJ.K. Sahu; Optoelectronics Research Centre, University of Southampton,
United Kingdom
We report the gain and
NF
of
Er/Ce-doped
aluminosilicate
fibre
amplifiers with different
Ceconcentrations,demonstrating a maximum 48dB gain andcorresponding 5.6dB NF
in the C-band and >20dB
gain across the L-band of
1565-1615nm.

Room 3 ICM

EA-8.4 FRI

15:00

Order-Invariant TwoPhoton Quantum Correlations in PT-Symmetric Interferometers∙T.A.W. Wolterink, M.
Heinrich, S. Scheel, andA. Szameit; Universityof Rostock,
Rostock,
Germany
We identify types of sequences of concatenatedtwo-mode linear opticaltransformations whose
two-photon behavior isinvariant under reversalof the order. We experimentally verify thissystematic behavior inparity-time-symmetriccomplex interferometerarrangements of varying
composition.

®

/Europe-EQEC 2023

⋅ Friday 30 June 2023

Room 4a ICM

Room 4b ICM

Room 5 ICM

Nanyang Technological
University,
Singapore,
Singapore
Current realizations of
topological lasers often
require complex design
and fabrication thathinder their operation
at small wavelengths.
Here we demonstratealithography-free,
one-dimensionalvertical-cavity perovskite
quantum dot topologicallaser emitting in thegreen.

∙R. Luque Merino1,2,3 ,P. Seifert1,4 , J. Durán
Retamal1,5 , R. Hadfield6 ,and D.K. Efetov2,3 ; 1 ICFO
- Institute of Photonic Sciences, Barcelona, Spain;
2
Fakultät für Physik
Ludwig-MaximiliansUniversität,
Munich,3Germany;
MunichCenter for Quantum
Science and Technology(MCQST), Munich, Germany; 4 Universität der
Bundeswehr
München,Munich,Germany;5
Catalan Institute of
Nanoscience and Nanotechnology(ICN2),
Barcelona,
Spain;
6
University of Glasgow,
Glasgow, Scotland
We combine van der
Waals
fabrication
techniques with novel
non-destructive nanopatterning to define 2D
cuprate nanostructuresthat enable ultrasensitive photodetection attelecomwavelengths
at moderate cryogenic
temperatures.

Science and Technology,
University of Crete, Heraklion, Greece; 4 Sectionof Electronic Physics andSystems, Department of
Physics, National andKapodistrian Universityof Athens, Athens, Greece;
5Department of Engineering Science, University of
Oxford, Oxford, United
Kingdom
We demonstrate a 3D
chiralmetamaterial
structure that presents
a large and ultrabroadband pure THz
optical activity up to 25
degreesaccompanied
by zero ellipticity for afrequency range over 1
THz.

CK-14.5 FRI

15:00

Narrow-linewidth frequency-agile integrated
laser sources using thinfilm lithium niobate∙V. Snigirev1 , A. Riedhauser2 , G. Likhachev1 , J.
Riemensberger1 , R. Ning
Wang1 , C. Moehl1 , M.
Churaev1 , A. Siddharth1 ,G. Huang1 , Y. Popoff2,3 ,U. Drechsler2 , D. Caimi2 ,S. Hoenl2 ,J. Liu2 ,P. Seidler2 , and T.J.
1
Kippenberg1 ;EPFL,
Lausanne, Switzerland;
2
IBM Research Europe,
Zurich,Switzerland;
3
ETH Zurich, Switzerland
We demonstrate thinfilm lithium niobatebasedfrequency-agile
integrated laser sourcewith lasing frequency
tuning rates up to 12
PHz/s
and
intrinsic
linewidth of 3 kHz. We
also make a system-level
demonstration of FMCW
LiDAR.

EI-3.4 FRI

15:00

Giant switchable broadband volatile thermooptic properties of phasechange semiconductors∙K. Kim and B. Gholipour;
University of Alberta, Edmonton, Canada
We show that common
chalcogenidephasechange semiconductors
currently being exploredwidely for inclusion asdata storage elements insilicon photonic circuits
possess giant switchable
broadband thermo-optic
coefficients across visible
to telecom frequencies.

206

CC-6.4 FRI

15:00

Fano to BIC Resonances
Transitions in 3D Printed Photonic Crystals
L.
Pilozzi1,2 ,∙M.
Missori1,3 ,
and
C.
1,2,3
1
Conti
; Institute forComplex Systems, National Research Council of
Italy (ISC-CNR) , Rome,
Italy; 2 Research Center
Enrico Fermi, Rome, Italy;
3
Department of Physics,
University
Sapienza,
Rome, Italy
We have designed andrealized,
by
means
of
three-dimensional
printing technology, ofTHz photonic crystal
slab exhibiting boundstates in the continuum(BIC) to be used as highly
sensitive and low-cost
THz sensors.

Room 11 ICM

Room 12a ICM
CE-10.3 FRI

CI-7.5 FRI

15:00

Coherent beam combining of very high power
optical amplifiers for
optical feeder links∙V. Billault1 , S. Leveque2 ,A. Maho2 , M. Welch3 ,J. Bourderionnet1 , E.
Lallier1 , M. Sotom2 , A. Le
Kernec2 , and A. Brignon1 ;1
Thales Research andTechnology,
Palaiseau,
France; 2 Thales Alenia
Space, Toulouse, France;
3
G&H, Torquay, United
Kingdom
We present the coherent
beam combination of
high
power
opticalamplifiers for opticalfeeder links. We obtained
90W output power, 98%
combining
efficiency,with 25Gb/s telecom
signals on the opticalcarrier with <1dB power
penalty.

14:45

Evidencing the resonant
and non-resonant
contributions to theindex of refraction of a
Nd:YAG rod amplifier∙M. Maillard1,2 ,G.
Amiard-Hudebine1 , M.
Tondusson1 , M. Orain2 ,and E. Freysz1 ; 1 Univ.
Bordeaux,CNRS, LOMA
UMR 5798,
Talence,
France; 2 ONERA/DMPE,
Université de Toulouse,
Toulouse, France
Measuring at both 532
nm and 1064.5 nm thetemporal evolution of thelens induced in a Nd:YAG
rod amplifier, we reveal
the resonant and nonresonant contribution of
the Nd3+ ions to the refractive index.
CE-10.4 FRI

15:00

Metal transition doped
Zn1.3Ga1.4Sn0.3O4
persistent phosphors foranti-counterfeiting
applications∙G. Cai1,2 , L. Giordano1 ,T. Delgado1 , C. Richard2 ,and B. Viana1 ; 1 PSL
University, Chimie ParisTech, IRCP-CNRS,, Paris,
France; 2 Université Paris
Cité, CNRS, INSERM,UTCBS,
FacultédePharmacie,, Paris, France
Persistentluminescence (PersL) property
offers great potentialforanti-counterfeiting
applications. We propose
Zn1.3Ga1.4Sn0.3O4
nanoparticles(NPs)with strong PersL at
700 nm (NIR-I) and at
1300 nm (NIR-II) andevaluate a multi-levelanti-counterfeiting technology in dual-windows.

CLEO

Room 13a ICM

JSIII-5.4 FRI®

/Europe-EQEC 2023

⋅ Friday 30 June 2023

Room 13b ICM

Room 14a ICM

Room 14b ICM

Room 14c ICM

Room Osterseen ICM

Room 21 ICM

temporal waveforms at
wavelengths relevant for
multi-photon imaging.

tion, demonstrated byangle-resolved
photoluminescence in a
GaAs-based microcavity.
Our results pave the way
towards polariton-based
THz lasing and coherent
control of collective
quantum states withindividual qubits.

Department of Microbial
and Molecular Systems,
KU Leuven, BelgiumWe
have
designedandinvestigatedaninnovative dual-region
self-referencing
fiberoptic surface plasmon
resonancebiosensor
withtwodifferent
configurations to study
binding reactions andcompensate for bulk refractive index changes ortemperature oscillation,
simultaneously.

visible region due togain suppression of therotational Raman Stokes
generation.

Portugal
The patented SyncRGBFLIM
microscopy
method, which deploys asub-10 fs ultrabroadband
laser for multi-color excitation, was used to trackthe efficiency of cancer
treatments
through
metabolic imaging of 2D
and 3D live cell cancer
models.

We propose an ultrafast optical parametricoscillator as a laser
source for three-photon
fluorescence microscopy.
Employing an intracavity
Herriott cell we can meetthe performance required
at a lower cost while
maintaining a compact
footprint.

CD-13.5 FRI

EF-9.5 FRI

CH-15.4 FRI

EE-4.5 FRI

CL-7.5 FRI

CF-11.5 FRIRoom 22a ICM

15:00

Synaptic weighting of
spiking VCSEL-neurons
using integrated photonic microring weight
banks
∙M.
Hejda1 ,E.A.
Doris2 , S. Bilodeau2 , J.
Robertson1 , L. Xu2 , B.
Shastri3 , P.R. Prucnal2 ,andA.
Hurtado1 ;1Institute of Photonics,
SUPA Department of
Physics,
Universityof Strathclyde,
Glasgow, United Kingdom;2
Department of ElectricalEngineering,
Princeton
University,
Princeton,
USA; 3 Department of
Physics,
Engineering
Physics and Astronomy,
Queen’s
University,
Kingston, Canada
We present an experimental
neuromorphic
system, combining together a spiking photonic
VCSEL-neuron and an
integrated, silicon photonics microring-based
weightbank.
Synaptic
weighting functionality ofthe sub-ns optical spikes
from VCSEL-neuron isdemonstrated.

15:00

Diminishing Speckle
Noise during Nonlinear
Phase-Only Beam
Shaping∙L. Ackermann1,2 , C.
Roider1 , K. Cvecek1,2 ,N. Barré1,2 , and M.
Schmidt1,2 ; 1 Institute of
Photonic
Technologies,
Friedrich-Alexander-Universität Erlangen-Nürnberg, Erlangen, Germany;2
School of Advanced
OpticalTechnologies(SAOT),FriedrichAlexander-Universität
Erlangen-Nürnberg,
Erlangen, Germany
The combination of
nonlinear beam shaping
andhighlyefficient
speckle averaging enables
tailoring beam profilesof high quality anduniformity beyond thespectral limits of theliquid crystal spatial light
modulator (LC-SLM).

15:00

Refraction of a soliton
by a soliton gas in arecirculating fiber loop
P. Suret 1 , M. Dufour1 ,G. Roberti2 , G. El2 , F.
Copie1 , and ∙S. Randoux1 ;1
Laboratoire
PhLAM,
Université de Lille, Villeneuve d’Ascq, France; 2
Northumbria University,
Newcastle upon Tyne,
United Kingdom
We report an optical fiber
experiment where we
investigate the interaction
between an individual(tracer) soliton and adense soliton gas. This
results in a refraction
phenomenon interpretedusing the kinetic theoryof soliton gases.

15:00

Voltage Driven Surface
Plasmon Resonance
Biosensors with integrated Nanoholes Array∙.
Rohit1 and J.-J.
1
Huang1,2 ;Graduate
Institute of Photonics
andOptoelectronics,
National Taiwan University, Taipei City, Taiwan;
2
Department of ElectricalEngineering,
National
Taiwan University, Taipei
City, Taiwan
A novel optical-biosensor
wasdesignedusingahybrid-plasmonic
andelectrochemical
phenomenon.
Goldnanohole-array on glasssubstrate was fabricatedand tested for CRPconcentrations ranging
from
1-1000μg/mL,with a concentrationdependent
response
modulated by varying
DC-voltages or AC-bias
frequencies.

15:00

Supercontinuum Generation in Methane-Filled
Hollow-Core Fibres
through a Combinationof Modulation Instability and Stimulated
Raman Scattering∙B. Plosz, A. Lekosiotis, M.
Sabbah, F. Belli, and J.C.
Travers; Heriot-Watt University, Edinburgh, United
Kingdom
We report the generationof exceptionally flat
Raman-enhanced
supercontinuum spanningfrom 300 nm to 1.7 μm
by pumping a methanefilled hollow-core fibre in
the anomalous dispersion
regime at 1030 nm with
220 fs 5μJ pulses.

207

15:00

Flexible and tunable
nonlinear microscopy
platform∙G. Hehl1 , A. Tripathi1 , S.
Goncharov1 , K. Fritsch1,2 ,and O. Pronin1 ; 1 Helmut
Schmidt
University,
Hamburg,
Germany;2n2-Photonics, Hamburg,
Germany
In this study,
weperformed two,andthree-photon
imagingwith varying pulse duration, repetition rate andaverage power and systematically investigated
the fluorescence signal
strength depending on
those parameters.

15:00

Ultrafast Optical Parametric Oscillator Employing High Refractive
Index Brewster Mirrors∙D.E. Hunter and R.A.
McCracken;
Scottish
Universities
Physics
Alliance (SUPA), Instituteof Photonics and Quantum Sciences, School ofEngineering and PhysicalSciences,
Heriot-Watt
University,
Edinburgh,
United Kingdom
We present a highlystable ultrafast opticalparametricoscillator
cavity employing a pairof high refractive index
inverted prisms acting as
Brewster mirrors. The
cavity is robust against
misalignment
withpromise for applicationsin harsh environments.

EC-3.5 FRI

15:00

Nano-optical Metrology
with Phase Singularities∙T. Grant1 , E. Plum1 ,K.F.
MacDonald1 ,and N.I. Zheludev1,2 ;1Optoelectronics ResearchCentre & Centre for
Photonic Metamaterials,
University of Southampton, Southampton, United
Kingdom; 2 Centre for
Disruptive
Photonic
Technologies,
Nanyang
Technological University,
Singapore, Singapore
We show how the
exploitation of phasesingularities in topologically structured lightfields can enable dramatic
sensitivity improvementsindiffraction-based
optical displacement anddimensional metrology.

CLEO

Room 1 ICM
CM-10.5 FRI

15:15

Room 2 ICM
CJ-9.5 FRI

15:15

Room 3 ICM
EA-8.5 FRI

15:15

®

/Europe-EQEC 2023

Room 4a ICM
CK-14.6 FRI⋅ Friday 30 June 2023
Room 4b ICM

15:15

EI-3.5 FRI

15:15

Room 5 ICM
CC-6.5 FRI

15:15

Room 11 ICM
CI-7.6 FRI

15:15

Room 12a ICM
CE-10.5 FRI

15:15

Towards an Experimentally Validated Model of
Ultrafast Laser Ablation
J. Winter, M. Spellauge,
D. Redka, G.E. Hallum,and ∙H.P. Huber; Lasercenter, Department of Applied Sciences and Mechatronics, Munich Universityof Applied Sciences HM,
Munich, Germany
We validate a new modelof aluminum laser ablation with predicted timeresolved and final-state
observables. In addition,
we emphasize the strong
photo-mechanical natureof laser fragmentation of
iridium oxide microparticles immersed in water.

Design and characterization of thulium-doped
fiber with depressed
cladding for amplifiers
operating in the region
from L-band to 1.8 um∙J.
Aubrecht1 ,J.
Pokorný1,2 ,M.
Kamrádek1 ,B.
Jiříčková1,2 ,
and
P.
1
1
Peterka ;Institute of
Photonics and Electronics
of the Czech Academyof Sciences,
Prague,Czech Republic; 2 Czech
Technical University in
Prague, Faculty of Nuclear
Sciences and PhysicalEngineering,
Prague,Czech Republic
A novel design of adepressed-cladding
thulium-doped
fiber
for tunable laser andamplifier applications isreported.
This design
results in blue-shifted
gain spectrum in the
sub-1.8-μm
regionand highly suppressed
amplifiedspontaneousemission.

Ultra-efficient resonant
generation of time-energy entangled photon
pairs in a InGaP Photonic Crystal Cavity∙A.
Chopin1,2 ,A.
Barone3 , I. Ghorbel1 , S.
Combrié1 , D. Bajoni4 ,F. Raineri2,5 , M. Galli3 ,and A. De Rossi3 ; 1 Thales
Research & Technology,
1 Avenue Augustin Fresnel, Palaiseau, France;
2
Centre de Nanosciences
et de Nanotechnologies,
CNRS, Palaiseau, France;
3
Dipartimento di Fisica,
Università degli Studi diPavia, Via Bassi 6, Pavia,
Italy; 4 Dipartimento diIngegneria
Industrialeedell’Informazione,
Università degli Studi
di Pavia, Via Adolfo
Ferrata 5, Pavia, Italy;
5
Université Côte d’Azur,
Institut de Physique deNice, CNRS UMR 7010,
Sophia Antipolis, France
Photonic crystal cavities
are introduced as a novel
platform for integrated
quantum photonics withthe demonstration ofultra-efficient generationof time-energy entangled photon pairs withvisibility of 97% due tovery small confinement
volume.

Hybrid III-V on Silicon-On-Insulator twodimensional photonic
crystal nanolaser
F.
Manegatti1 ,K.
Moratis1 , ∙B. Garbin1 ,A.
Demarchi1 ,G.
Beaudoin1 , K. Pantzas1 ,I. Sagnes1 ,and F.
1
Raineri1,2 ;Université
Paris-Saclay,
CNRS,
Centre de Nanosciences
et de Nanotechnologies,
91120 Palaiseau, France;
2
Université Côte d’Azur,
Institut de Physique deNice, CNRS–UMR 7010,
Sophia Antipolis, FranceWe
experimentallydemonstrate the firstelectrically-pumped
asymmetrictwodimensional
photonic
crystal nanolaser. Our
devices
open
great
prospects for on-chip
optical interconnections.

Polarization-driven
reversible deformation
in a light-responsive
amorphous polymer
blend∙D. Urban1 , D.R. Hjelme1 ,andE.
Descrovi2 ;1
Norwegian University of
Science and Technology,
Trondheim,
Norway;2
Polytechnic University ofTurin, Torino, Italy
Using
commerciallyavailable
constituents,
we show the fabricationof polymer materials
that can be locally andreversibly stretched bypolarized light along
arbitrary
directions.
Planar substrate stretches
and more complex 3D
actuator deformations arepresented.

Comb-Locked Terahertz
Spectroscopy of Critically Coupled Ultrahigh-Q WhisperingGallery Mode Resonators∙S. Müller1,2 , T. Puppe1 ,Y. Mayzlin1 , R. Wilk1 ,B. Schmauss2 , and D.
1
Vogt3,4 ;TOPTICA
Photonics AG, Graefelfing,
Germany; 2 Institute ofMicrowaves and Photonics, Friedrich-Alexander
University,
Erlangen,Germany; 3 Departmentof Physics, Universityof Auckland, Auckland,
4
New Zealand;
The
Dodd-Walls Centre for
Photonic and Quantum
Technologies, Dunedin,
New Zealand
A novel spectrometer isbased on tuneable diodelasers phase-locked toan externally shiftedfrequency comb.
We
demonstrateprecisionterahertz spectroscopyof critical coupling in
Ultra-high Q whisperinggallery silicon resonatormodes.

Dual-chirp Waveforms
with Optical Filter-less
Photonic Dechirping for
Distance and Velocity
Measurement in FMCW
RADARs
D. Parida, ∙R. Dhawan,
andA.
Choudhary;
Ultrafast Optical Communications and Highperformance Integrated
Photonics (UFO-CHIP)
group, Department ofElectricalEngineering,
Indian Institute of Technology (IIT), Delhi, New
Delhi, India
We propose an opticalfilterlessdechirping
RADAR receiver basedon a dual-drive MachZehnder-modulator for
distance and velocity
estimation. The systemis tested for different
velocities showing amaximum error of 7.4%
for velocity estimation

Erbium doped nanocrystalline and PMMAbased composite materials∙K. Anders1,2 , A. Jusza1,2 ,A. Bieniek1 , P. Mergo3 ,R.
Łyszczek3 ,andR.
Piramidowicz1,2 ;1Warsaw University ofTechnology, Institute ofMicroelectronics
andOptoelectronics, Warsaw,
Poland; 2 LightHouse sp.
z o.o., Lublin, Poland;
3
Maria Curie-Sklodowska
University, Faculty ofChemistry, Lublin, Poland
We present the research results on shortwavelength
emission
properties of the PMMAbased
nanocomposites
doped with oxide andfluoride nanocrystals activated with erbium ionsdedicated to applicationin polymer fiber lasers
and incoherent lightsources.

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Room 5 ICM

Room 11 ICM

Room 12a ICM

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

CM-11: Laser additive
manufacturing II

CJ-10: 2-micron
fiber sources

EA-9: Optomechanical systems

CK-15: Micro- andnano-optical cavities

CC-7: THz applications

Chair: Pavel Peterka, Inst.
of Photonics and Electronics, Czech Academy of Sciences, Prague, Czech Republic

Chair: Olivier Dulieu,
Université Paris-Saclay,
FranceChair:
StefanoPelli,CNR-IFAC,Sesto
Fiorentino,Italy

CI-8: Frequency
combs and microwave photonics

CE-11: Fabrication
methods

Chair: Johannes Heitz, Johannes Kepler University,
Linz, Austria

EI-4: Ultrafast dynamics in layeredmaterials
Chair: Chiara Trovatello,
Columbia University, New
York, USA

208

Chair: Jeremy Johnson,
Brigham Young University, Provo, UT, USA

Chair: Juerg Leuthold,
ETH Zurich, Zürich,
Switzerland

Chair: George Tsibidis,
FORTH,
Heraklion,
GreeceCLEO

Room 13a ICM
JSIII-5.5 FRI

15:15

Room 13b ICM
CD-13.6 FRI

15:15

Room 14a ICM
EF-9.6 FRI

15:15

®

/Europe-EQEC 2023

Room 14b ICM
CH-15.5 FRI⋅ Friday 30 June 2023

Room 14c ICM

15:15

EE-4.6 FRI

15:15

Room Osterseen ICM
CL-7.6 FRI

15:15

Room 21 ICM
CF-11.6 FRI

15:15

Room 22a ICM
EC-3.6 FRI

15:15

Tunable Optoelectronic
Neuromorphic Synaptic
Link based on Nanoscale Resonant Tunnelling Diode-Photodetector Spiking Neurons∙W. Zhang1 , M. Hejda
1, Q.R.A. Al-Taai 2 , B.
Romeira 3 , J. Figueiredo
4, E. Wasige 2 , and A.
Hurtado 1 ; 1 Universityof Strathclyde,
Glasgow, United Kingdom;
2
University of Glasgow,
Glasgow, United King3
dom;
International
Iberian Nanotechnology
Laboratory, Braga, Portugal; 4 Universidade deLisboa, Lisboa, Portugal
We report an optoelectronic
neuromorphic
synaptic link built withhigh-speed
nanoscaleresonant
tunnelling
diode-photodetectors(RTD-PDs),
which
reproduces
temporalcoded spike generationand transmissions inbiological neurons andsynapses.

Enhancing Nonlinear
Interferometers for
Imaging with Undetected Photons: Seeding andHigh-Gain∙E. Pearce1 , J. Flórez1 ,N.R. Gemmell1 , M. Abire
Karzazi1 , Y. Ma1 , G.
Bressanini1 , R.A. Battle1 ,R.T. Murray1 ,M.S.
Kim1 , C.C. Phillips1 ,R.F. Oulton1 , and A.S.
Clark1,2 ; 1 Department of
Physics, Blackett Laboratory, Imperial College
London, London, United2
Kingdom;
QuantumEngineering Technology
Labs, University of Bristol,
Bristol, United Kingdom
We present a comprehensive model of an SU(1,1)
interferometer for imaging with undetected photons. We confirm experimentally that interference visibility and contrast are enhanced for coherent state seeding andin the high gain regime.

Distorsion of the nonlinear spectrum ofsolitonic pulses induced
by stimulated Raman
scattering∙M. Dufour, S. Randoux,
F. Copie, and P. Suret;Laboratoire PhLAM, Université de Lille, Villeneuved’Ascq, France
We look at how the
well-known stimulated
Raman scattering andsoliton fission manifest
in the Inverse Scattering
Transform
spectrum(nonlinear
spectrum)using a single shotmeasurement of both
amplitude and phase of
the optical signal.

UV-Photodeactivationof Proteins for Inscription of BIO-Gratings
A. Juste-Dolz1 ,∙M.
Delgado-Pinar2 ,M.
Avellà-Oliver1,3 ,E.
Fernández1 , J.L. Cruz2 ,M.V. Andrés2 , and Á.
1
Maquieira1,3 ;IDM,
Universitat
Politècnicade València, Universitat
de València, Valencia,
Spain; 2 LFO-UV, ICMUV, Universitat deValència, Valencia, Spain;3
Chemistry Department,
Universitat Politècnica deValència, Valencia, Spain
We present the UVphotoinscriptionofmolecular BIO-gratings
by deactivating the BSA
molecules of a uniform
biolayer in a patternedmanner. The fabrication
is optimized to enhancethe diffractive efficiency
andtopology
after
incubation of aBSA.

Ultrafast, all-optical,
and highly efficient
imaging of molecularchirality∙R.
Picciuto1 ,J.
Broughton1 ,K.
Kowalczyk1 ,H.
Allegre1 , J.W.G. Tisch1 ,J.P.
Marangos1 ,O.
Smirnova2,3 , D. Ayuso1,2 ,andM.
Matthews1 ;1Imperial College London, London, United2
Kingdom;
Max-BornInstitut, Berlin, Germany;
3
Technische Universität
Berlin, Berlin, Germany
Towards
all-opticalmethod, that relies onpurelyelectric-dipole
interactions, to probechirality on ultrafast
timescales. We aim tomeasure the chiral dipole
response, of a liquid
microjet, into the far-fieldusing a non-collinear
setup.

Non-destructive Direct
Pericarp Thickness
Measurement of Sorghum Kernels with Fiberbased Extended Focus
Optical Coherence
Microscopy∙A. Fernandez, D. Sen,
D. Crozier, B. Henrich,
A. Sokolov, M. Scully, W.
Rooney, and A. Verhoef;
Texas A&M University,
College Station, USA
We apply high-resolution
Bessel-beam
extendedfocus optical coherence microscopy for
non-destructive
morphological phenotypingof sorghum seeds. We
obtain accurate thickness
measurements with areduced tendency tooverestimate the thickness of thin phenotypes.

Hybrid-Amplified THzRepetition-Frequency
Bursts∙V.
Stummer1 ,M.
Schneller1 , T. Flöry1 ,E. Kaksis1 , M. KitzlerZeiler1 , A. Pugzlys1,2 , and
A. Baltuska1,2 ; 1 Photonics
Institute,
TU Wien,Vienna, Austria; 2 Center
for Physical Sciences& Technology, Vilnius,
Lithuania
We demonstrate hybrid amplification of
femtosecond
pulse
bursts, in which spectral
modulations are deliberately suppressed in a
chirped-pulse amplifier
and then recovered in
an optical parametricamplifier,anticipating
several exciting resonant
multiphoton applications.

Accelerating Poincaré
vortices∙A.
Brimis1,3 ,K.G.
1,3Makris ,and D.G.
Papazoglou1,2 ; 1 Instituteof Electronic Structureand Laser,
Foundation for Research andTechnology-Hellas(FORTH),
Heraklion,
2
Greece;Departmentof Material Science andTechnology, University ofCrete, Heraklion, Greece;
3
ITCP, Department of
Physics, University ofCrete, Heraklion, Greece
We theoretically investigate
polarization
singularities that exhibit
radialandangularacceleration upon propagation. By combining two
orthogonally polarizedstates, consisting of apure and a vortex phasemodulated
ring-Airybeam,
weproduceaccelerating polarization
singularities.

Room 13a ICM

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Room 14c ICM

Room Osterseen ICM

Room 21 ICM

NOTES

16:00 – 17:30

16:00 – 17:30

16:00 – 17:15

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

16:00 – 17:30

JSIII-6: Brain-inspired
photonic dedvices
and computing II

CD-14: Quantum
applications

EF-10: Extreme
events and forecasting techniques

CH-16: Environmental optical sensing

EE-5: Ultrafast manipulation and control

CL-8: Novel laser
sources

CF-12: Mid-IR
sources

Chair:
Cristian
Focsa,UniversityofLille,France

Chair:John
Travers,Heriot-Watt
University, UK

Chair: Kenneth Kin-Yip
Wong, The University ofHong Kong, Hong Kong

Chair:
Eric Cormier,
University of Bordeaux,FranceChair: Bruno Romeira,
INL, Braga, Portugal

Chair:
Robert Fickler,
TampereUniversity,
FinlandChair: Alejandro Giacomotti, C2N, Université
Paris Saclay, France

209

CLEO

Room 1 ICM

Room 2 ICM

CM-11.1 FRI (Invited) 16:00

CJ-10.1 FRI

Laser Induced Forward
transfer: Digital Additive Manufacturing solution for electronics∙I. Zergioti;
National
Technical University ofAthens, Greece
We demonstrate the potential of LIFT as a digital
and additive micromanufacturing
tools
delivering structures andpatterns consisting ofadvanced nanostructured
materials and 2D layeredmaterials. The prospectsof this technology within
the concept of industrial
applicability
willbe
discussed.

Tm:fiber CPA driven,
nonlinear pulse compression delivering
mJ-level, sub-two cycle
pulses at 2 μm with>100 W average power∙Z. Wang1 , T. Heuermann1,2,3 ,M. Gebhardt1,2,3,4 , M. Lenski1 ,P.
Gierschke1,5 ,R.
Klas1,2,3,5 ,J.
Rothhardt1,2,3,5 , C. Jauregui1 ,and J. Limpert1,2,3,5 ;1Institute of Applied
Physics, Abbe Centerof Photonics, University Jena,
Germany;2Helmholtz-InstituteJena, Germany; 3 GSI,
Darmstadt,
Germany;
4
Current address: Schoolof Engineering and Physical Sciences, Heriot-Watt
University,
Edinburgh,
UnitedKingdom;
5
Fraunhofer
Institutefor Applied Optics andPrecision
Engineering,
Jena, Germany
We report on the nonlinear pulse compression of ahigh-power thulium-fiber
laser, delivering mJ-level,
sub-two cycle pulses with
about 80 GW peak powerand 132 W average power
at 101 kHz repetition rate.
CJ-10.2 FRI

16:00

16:15

Ultrabroadband, highly
efficient mid infrared
generation driven by a
Tm-doped fiber laser
system∙T.
Heuermann1,2,3 ,Z. Wang1 , M. Lenski1 ,and J. Limpert1,2,3,4 ;1
University, Jena, Germany; 2 Helmholtz Institute Jena, Germany; 3 GSI,
Darmstadt,
Germany;4
Fraunhofer
Institutefor Applied Optics andRoom 3 ICM
EA-9.1 FRI

16:00

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/Europe-EQEC 2023

Room 4a ICM

Room 4b ICM

Room 5 ICM

16:00

EI-4.1 FRI (Invited) 16:00

CC-7.1 FRI

16:00

CE-11.1 FRI (Invited) 16:00

Lightshift of exciton andexciton-polarons in a 2D
semiconductor.
∙B. Evrard, T. Uto, M.
Kroner, and A. Imamoglu;
Institute of Quantum
Electronics, ETH Zurich,
Zürich, Switzerland
The lightshift of an exciton can be dominantly
driven by interactions
with virtual excitations.
Interestingly, this effectis dramatically enhanced
by polaron dressing of
the exciton with free
carriers in a doped 2d
semiconductor.

In-vivo skin hydration
monitoring using a robust Terahertz handheld laser; clinicalopportunities
A. Hernandez-Serrano,∙X. Ding, and E. PickwellMacPherson; Universityof Warwick, Coventry ,United Kingdom
A non-invasive THz
portable laser scanner isutilised to evaluate thehydration dynamics ofthe dorsal aspect of theforearm of 95 healthy
volunteers. Increments inhydration are observed
during one minute of test

Tuneable laser locking
to Optical Frequency
Comb∙W. Indra1 , Z. Feng1 , J.
Vojtěch2 , B. Shi1 , and R.
Slavík1 ; 1 Optoelectronics
Research Centre, University of Southampton,
SOUTHAMPTON,
UnitedKingdom;
2
CESNET a.l.e, Praha,
Czech Republic
Tuneable laser is phaselocked to optical frequency
comb
with
per-tone power as low
as 1nW (entire comb
power of 40μW). The
system will allow for
up to 25 lasers locked
simultaneously to 1mW
comb.

Laser based 3D printingof fused silica glass∙M.
Fokine1,2 ,T.
Oriekhov2 ,andC.
Liu2 ; 1 Royal Institute ofTechnology, Stockholm,
Sweden; 2 Nobula3D AB,
Stockholm, Sweden
A bench-top glass 3D
printer using non-contact
CO2-laser heating offilaments is presented.
Printing at temperaturesof ~2000 C with a small
hot-zone enables true 3D
printing of transparent
glass without need ofsupport structures.

EA-9.2 FRICK-15.2 FRI

CC-7.2 FRI

CI-8.2 FRI

16:15

Twenty Million Q-Factor for Suspended Triangular Nanobeam
Cavities∙C. Maynard1 , D. Beggs1 ,M. Wale2 , A. Bennett3 ,and J. Hadden3 ; 1 Schoolof Physics and Astronomy, Cardiff University,
Cardiff, United Kingdom; 2 Department ofElectronic and ElectricalEngineering, University
College London, London,
United Kingdom; 3 Schoolof Engineering, Cardiff
University, Cardiff, United
Kingdom
Photonic
crystal210

16:15

Substrate-integrated
hollow waveguides forterahertz gas sensing∙D.
Theiner1,2 ,B.
Limbacher1,2 , M. Jaidl1,2 ,M. Ertl1,2 , M. Hlavatsch3 ,K. Unterrainer1,2 ,B.
Mizaikoff3,4 ,and J.
1
Darmo1 ;TU Wien,Institut für Photonik, Vienna, Austria; 2 TU Wien,
Zentrum für Mikro- und
Nano-Strukturen, Vienna,
Austria; 3 University ofUlm, Institute of Analytical and Bioanalytical
Chemistry, Ulm, Germany; 4 Hahn-Schickard,
Ulm, GermanyCI-8.1 FRIRoom 12a ICM

Bloch Surface Waves ina photo-tunable, anisotropic microcavity
N. Marcucci1 ,M.C.
Giordano2 , G. Zambito2 ,F. Buatier de Mongeot2 ,and∙E.
Descrovi1 ;1
Politecnico di Torino,
Torino, Italy; 2 Università
di Genova, Genova, Italy
An anisotropic resonant
structure is presented,
anisotropy being due
toboth
topography
and a light-controlled
molecular orientation in
the constitutive materials.
Two orthogonal surface
modes are spectrally detuned by operating on the
induced birefringence.

16:15

16:00

Room 11 ICM

Ultralow Dissipation
Mechanical Resonators
for Cavity-Free Quantum Control∙N.J. Engelsen1,2 ,A.
Arabmoheghi1,2 ,M.J.
Bereyhi1,2 , A. Beccari1,2 ,S.A.
Fedorov1,2 ,
Y.
1,2
Xia ,
G. Huang1,2 ,A. Zicoschi1,2 , and T.J.
1
Kippenberg1,2 ;SwissFederal Institute of Technology Lausanne (EPFL),
Lausanne, Switzerland;
2
Center for Quantum
Science and Engineering, EPFL, Lausanne,
Switzerland
We fabricate mechanical resonators withrecord quality factors(Q > 3 × 109 at room
temperature) and show
efficient interferometricmeasurement of theirmotion.
Technical
improvementsmayallow cavity-free coolingclose to the ground state
without a cavity.

Demonstration ofpiezo-orbital backaction
force in a bulk rareearth ion-doped crystal∙A.
Louchet-Chauvet1 ,P. Verlot2 , J.-P. Poizat3 ,andT.
Chanelière3 ;1
Institut Langevin, CNRS,ESPCI, Université PSL,
Paris, France; 2 Lumin,
CNRS, Université ParisSaclay, ENS Paris-Saclay,
CentraleSupelec, Orsay,
France; 3 Institut Néel,
CNRS, Grenoble INP,
Univ.
Grenoble Alpes,
Grenoble, France
We demonstrate a conservative, optomechanical

CK-15.1 FRI⋅ Friday 30 June 2023

16:15

80-Gb/s fiber–terahertz
system in 300-GHz bandusing stable optical frequency comb generation∙P. Tien Dat1 , M. Isao 1 , S.
Norihiko 1 , I. Keizo 1 , K.
Atsuhi 1,2 , Y. Naoktatsu
1, and A. Kouichi 1 ;1National Institute ofInformation and Communications Technology(NICT), Tokyo, Japan;
2
Nagoya Institute ofTechnology, Aichi, JapanWe
demonstrateasimple yet high-speed
fiber–terahertz
systemin 300-GHz band using
a single Mach-ZehnderCLEO

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/Europe-EQEC 2023

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JSIII-6.1 FRI (Invited) 16:00

CD-14.1 FRI (Invited) 16:00

EF-10.1 FRI

16:00

CH-16.1 FRI (Invited) 16:00

EE-5.1 FRIScalable and autonomous
photonic neural networks
A.
Grabulosa1 ,A.
Skalli1 , J. Moughames1 ,X. Porte2 , J. Lott3 , S.
Reitzenstein3 , and ∙D.
Brunner1 ; 1 FEMTO-ST,
UniversitéFrancheComté
CNRS
UMR
6174, Besancon, France;
2
SUPA Department of
Physics, University ofStrathclyde,
Glasgow,
United Kingdom; 3 Institut
fürFestkörperphysik,Technische
Universität
Berlin, Germany
Using CMOS compatible
3D photonic integration
we implement dense
and complex networks
which pose a challenge
toconventional
2D
integration, and basedon multimode semiconductor lasers we realizeafully
autonomous
photonic neural network.

Fully On-chip Laserintegrated Quantum
Source of Entangled
Photon States∙H.
Mahmudlu1,2,3 ,R.
Haldar1,2,3 ,R.
Johanning1,2,3 , A. Kho1,2,3
dadad Kashi, A.v.
Rees4 , J. P. Epping5 ,K.-J. Boller4 , and M.
1
Kues1,2,3 ;
Instituteof Photonics, Leibniz
University
Hannover,Hannover,
Germany;
2
Hannover Centre for
OpticalTechnologies,
Leibniz
University
Hannover,Hannover,3
Germany;
Cluster of
Excellence
PhoenixD,
Leibniz
University
Hannover,Hannover,4
Germany;
Universityof Twente, Enschede,5
Netherlands;
QuiX,
Enschede, Netherlands
We demonstrate thefirst fully on-chip laserintegrated
quantum
light source of entangled
photonstates.
The hybrid InP-Si3N4
sourcecreates
twoandhigh-dimensionalfrequency-bin entangledstatesattelecomwavelength and brings
the required scalability
to photonic quantum
processing.

Forecasting extreme
events from nonlocal
partial information in a
spatially extended
microcavity laser
V.A. Pammi1 ,M.G.
Clerc2 , S. Coulibaly3 , and
1 1∙S. Barbay ; Université
Paris-Saclay,
CNRS,
Centre de Nanosciences
et de Nanotechnologies, Palaiseau, France;2
Departamento de Física
and Millennium Institutefor Research in Optics,
FCFM, Universidad deChile, Santiago, Chile;
3
UniversitédeLille,
PhLAM
Physiquedes Lasers, Atomes etMolécules, Lille, France
We address the modelfree
forecastingof
extreme events from experimental data acquired
in a spatiotemporally
chaotic microcavity laser.
We use transfer entropy
to identify precursors
enabling useful nonlocal
prediction exceeding 7.5
times the Lyapunov time.

Chemical sensing oftrace gases and particulate matter with opticalcavities∙W. CHEN; Universitédu Littoral Côte d’Opale,
Dunkerque, France
Cavity-enhanced
optical sensing of key
atmosphericspecies(tracegases/particles)
willbeoverviewed.
Development of novel
optical cavity based onprisms as cavity reflectors
operating in a broadbandof 400-1600 nm will bepresented as well.

Coherent Generation
and Field-Resolved Detection of Nonlinear χ (3)Spectral Broadening in
the Multi-THz Regime∙C. Schönfeld,
A.-C.
Heinrich, L. Feuerer,
A. Baserga, D. Bossini,and A. Leitenstorfer;
Department of Physics
and Center for Applied
Photonics,
Konstanz,
Germany
Nonlinear spectral broadening of mid-infraredtransients with peak electric fields exceeding 100
MV/cm is demonstrated.
Field-resolved analysis
by electro-optic sampling
directly reveals solitonic self-compression
and self-steepening on
femtosecond timescales.

EF-10.2 FRI

16:15

Machine Learning analysis of temporal instability peaks under Continuous Wave excitationin optical fiber Modulation Instability∙M. Mabed1 , L. Salmela2 ,A.V.
Ermoleav1 , C.
3
Finot , G. Genty2 , andJ.M. Dudley1 ; 1 Universitéde Franche-Comté, Institut Femto-ST, Besançon,
2
France;Photonics
Laboratory,
TampereUniversity,
Tampere,Finland; 3 Université deBourgogne, Laboratoire
Interdisciplinaire Carnot
de Bourgogne, Dijon,

Room 14b ICM⋅ Friday 30 June 2023

Room 14c ICM

EE-5.2 FRI

16:00

16:15

Manipulation of singlephoton wave packets via
Kerr-nonlinear refractive index fronts∙S. Bose1,2 , A.M. Angulo M.1,2 , S. Wijaya1 ,O.
Melchert2,3 ,P.
Rübeling1 , R. Halder1,2 ,D. Ghosh4 , U. Morgner2,3 ,A.
Demircan2,3 ,I.
Babushkin2,3 , and M.
1
Kues1,2 ;Institute of
Photonics,
University
Hannover,
Germany;
2
Cluster of Excellence
PhoenixD,
University
Hannover,
Germany;3
Institute of Quantum
Optics, University Han211

Room Osterseen ICM
CL-8.1 FRI

16:00

Room 21 ICM
CF-12.1 FRI

16:00

Dual Amplification
850 nm FDML Laser∙M. Klufts1 , S. Lotz1 ,M.A. Bashir1 , T. Pfeiffer2 ,A. Mlynek2 , W. Wieser2 ,A.
Chamorovskiy3 ,V.
Shidlovski3 ,A.
Podoleanu4 ,and R.
1
Huber1 ;Institute of
Biomedical
Optics,
University of Lübeck,Lübeck,Germany;
2
Optores GmbH, Munich,
3Germany;
Superlum
Diodes Ltd., Cork, Ireland; 4 School of Physicalsciences, university ofKent, Canterbury, United
Kingdom
We demonstrate a newcavity design for FDML
laser providing dual amplification in one roundtrip. The laser is sweeping
over 20 nm around 850
nm with a repetition rateof 409 kHz.

Hyper spectral imaging
using sub-half-cycle
mid-infrared pulses
Y. Zhao1 , S. Kusama1 ,Y. Furutani2 ,W.-H.
Huang3 , C.-W. Luo3 ,and ∙T. Fuji1 ; 1 Toyota
Technological Institute,
Nagoya, Japan; 2 Nagoya
Institute of Technology,
Nagoya, Japan; 3 National
Yang Ming Chiao Tung
University,
Hsinchu,
TaiwanWe have demonstrated
hyper spectral imaging
using
sub-half-cycle
mid-infrared
pulsesgeneratedthrough
two-color filamentation.
Up-conversion of the
MIR pulse transmitted
through the sample at theimage plane significantly
improve the performanceof the spectral imaging.

CL-8.2 FRI

CF-12.2 FRI

16:15

Ultra-short pulse modulation with electro-optic
modulators∙S. Meyer1 , T.F. Kutscher1 ,P.
Lamminger1 ,F.
Sommer1,2 , and S. Karpf1 ;1
Institute of Biomedical
Optics, Lübeck, Germany;
2
Leibniz
InstituteofVirology,
Hamburg,
Germany
To overcome the limitations of expensive
electrical pulse generators,
electro-opticalmodulators (EOM) wereoperated with a fast edge
with an amplitude of twotimes Vpi, allowing the

16:15

Low-noise 2-W Average
Power, 112-fs Kerr-lensMode-locked Ho:CALGO
Laser at 2.1 μm∙W. Yao1 , Y. Wang1 , S.
Ahmed1 , S. Tomilov1 ,M. Hoffmann1 ,M.v.
Delden2 , T. Musch2 , andC.J. Saraceno2 ; 1 Photonics
andUltrafast
Laser
Science, Ruhr-Universität
Bochum,Bochum,Germany; 2 Institute ofElectronic Circuits, RuhrUniversität
Bochum,Bochum, Germany
We report a low-noise,
2-W, 112-fs, Kerr-lensmode-locked Ho:CALGO

NOTES

CLEO

Room 1 ICM

CM-11.2 FRI

16:30

Multi-Photon Polymerization with Upconversion Nanoparticles for
Adaptive Feature-Size
3D Printing∙Q. Zhang1 , A. Boniface1 ,V.K. Parashar2 , and C.
1
Moser1 ;Laboratoryof Applied Photonics
Devices,
SchoolofEngineering, Ecole Polytechnique Fédérale deLausanne, Switzerland;
2
Laboratory of Microsystems LMIS2,
Schoolof Engineering, Ecole
Polytechnique Fédérale deLausanne, Switzerland
We investigate the polymerization
dynamicsof the multi-photon
polymerization based on
UCNPs and shows how it
can be used for adaptive
feature-size
printing,
which is promising forfasthigh-resolution
additive manufacturing.

®

/Europe-EQEC 2023

Room 2 ICM

Room 3 ICM

Room 4a ICM

Precision
Engineering,
Jena, Germany
We report on the efficient generation of midinfrared radiation driven
by a Tm-doped fiber laser
system, reaching 3.6% ofconversion efficiency withan output spectrum spanning more than one octave.

backaction force in an
ensemble of rare-earth
ions embedded in a crystal. This ”piezo-orbital
backaction” induces anovel kind of ion-ion
interaction mediated bystrain.

nanobeam
cavities(PCNCs) provide convenient and monolithic
integration of highQuality-factor (Q) opticalcavities on photonic
integrated circuits (PICs).
We show how to achievea nanobeam cavity with
Q ~ 20,000,000 throughapodization.

CJ-10.3 FRI

16:30

Highly efficient, in-band
pumped, thuliumdoped fibers in highpower amplifier and mJ
Q-switched regime∙M. Lenski1 , T. Heuermann1,2,3 ,M. Gebhardt1,2,3,4 , Z. Wang1 ,C. Aleshire1 , C. Gaida5 ,C. Jáuregui1 , and J.
1
Limpert1,2,3,6 ;Institutof Applied Physics, Abbe
Center of Photonics,
Schiller-Universität, Jena,
2
Germany;
HelmholtzInstitute Jena, Germany;
3
GSI,
Darmstadt,
4
Germany;
School ofEngineering and PhysicalSciences,
Heriot-Watt
University,
Edinburgh,
UnitedKingdom;
5
Active Fiber Systems
GmbH, Jena, Germany;
6
Fraunhofer
Institutefor Applied Optics andPrecision
Engineering,
Jena, Germany
We report on a thuliumdoped fiber amplifier andQ-switched laser pumped
at 1692 nm. Comparedwiththetraditional
793 nm pumping, thein-band pumping allows
for significantly higher
efficiency in combination
with excellent pulse
energy capability.

EA-9.3 FRI

16:30

Mechanical squeezing ofa nanoparticle levitatedin a hybrid RF-opticaltrap
E. Bonvin, L. Devaud, L.
Novotny, and ∙M. Frimmer; Photonics Laboratory, ETH Zurich, Zurich,
Switzerland
We introduce a hybrid
RF-optical trap. We show
thermal squeezing of themechanical state of a silica nanoparticle by dropping it from the stiff optical to the less-stiff RF trap
in vacuum.

CK-15.3 FRI⋅ Friday 30 June 2023
Room 4b ICM

16:30

Monolithic cavity for
optomechanics featuring a bound state in thecontinuum∙C. Péralle1 , S. Kini
Manjeshwar2 , A. Ciers2 ,W. Wieczorek2 , and P.
1
Tassin1 ;Departmentof Physics,
Chalmers
University of Technology,
Gothenburg,
Sweden;2
Department of Microtechnologies
andNanoscience, Chalmers
University of Technology,
Gothenburg, Sweden
We design and study amonolithic
photoniccrystal-based microcavity
foroptomechanics.
Our new design exhibits a bound state in
the continuum with adissipative-loss-limited
quality factor of over
105 and is amenabletofabricationwithnanolithography.

EI-4.2 FRI

16:30

Ultrafast optical nonlinearities of excitonpolaritons in atomicallythin MoS2 embedded inplanar microcavities∙A. Genco1 , C. Louca2 ,C.
Trovatello3 ,C.
Cruciano1 , S. Randerson2 ,P.
Claronino2 ,R.
Jayaprakash2 ,K.
Watanabe4 ,T.
Taniguchi4 , D.G. Lidzey2 ,A.I. Tartakovskii2 , G.
Cerullo1,5 , and S. Dal
1
Conte1 ;Dipartimento
di Fisica,
Politecnico
diMilano,Milano,2
Italy;
Department of
Physics and Astronomy,
University of Sheffield,
Sheffield, United Kingdom; 3 Department of
Mechanical Engineering,
Columbia University, New
York, USA; 4 Advanced
Materials
Laboratory,
National Institute for Materials Science, Tsukuba,
Japan; 5 IFN CNR, Milano,
Italy
Pump-probe microscopy
experiments
providedemonstration of giant
nonlinear responses of
exciton-polaritonsinatomically thin MoS2 microcavities, on ultrashorttimes and at low excitation powers, unveilingthe great potential of such
systems for nonlinear
optical applications.

212

Room 5 ICM

Room 11 ICM

Substrate-integrated
hollow waveguides andan opto-electronic THz
source enable a highly
flexible THz sensing
platform,that offers
real-time control of the
probing THz frequencies,
state-of-the-art volumeto-optical path ratios andrequire small sample gas
volumes <2mL.

modulator-based opticalfrequency comb generation. An OFDM signal
with a line rate of over
80 Gb/s was successfullytransmitted.

CC-7.3 FRI

CI-8.3 FRI

16:30

Terahertz assisted Atom
Probe Tomography:
Effect of THz properties
on ion’s behavior∙M. Karam, L. Rousseau,
G. Damarla, J. Houard,
and A. Vella; Université deRouen, Rouen, France
Terahertz
monocycle
pulses are amplified bytheir interaction withneedled-shaped sample
in order to generate an
intense field allowing
the emission of surface
atoms. We demonstrate
the effect of the monocycle shape on theirtrajectories.

16:30

Field demonstration ofmulti-wavelength
optical transmission
with microresonatorfrequency combs∙K.
tanikawa1 ,S.
fujii2 , S. kogure1 , S.
tanaka1 , S. tasaka1 , K.
wada1 , H. kumazaki1 ,S. kawanishi1 , and T.
tanabe1 ; 1 department ofelectronics and electricalengineering, faculty of science and technology, Keio
university,
yokohama,
Japan; 2 department ofphysics, faculty of scienceand technology, Keio
university,
yokohama,Japan
weperformed
fielddemonstrationofmulti-wavelength
optical transmission withmicroresonator-based
opticalfrequency
combs. We used a 9-km
round-trip single-mode
optical fiber installed
in a metropolitan area
and realized low-latency
andhigh-capacitytransmission.

Room 12a ICM

CE-11.2 FRI

16:30

High-transparency andheavy-durability 3D
micro-optics made via
ultrafast laser lithography combined withatomic layer depositionand calcination
K. Galvanauskas1 , R.
Žvirblis1 , G. Balčas1 ,D.
Gailevičius1 ,D.
Astrauskytė2 ,L.
Grinevičiūtė2 ,and
1 1∙M. Malinauskas ; VU
LRC, Vilnius, Lithuania;
2
CPST, Vilnius, Lithuania
We report on hightransparency
andheavy-durability glassceramic
free-frommicro-optics
madeemploying ultrafast laser
3D
nano-lithographyofhybridorganicinorganic
SZ2080T M
combined with atomic
layer deposition andhigh-temperature
calcination.

CLEO

Room 13a ICM

Room 13b ICM

Room 14a ICM®

/Europe-EQEC 2023

Room 14b ICM

FranceWe show that a neuralnetwork can predict
temporal instability peaks
from spectral data inideal CW modulation instability, and we establish
limits on the predictive
power of the networkwith distance.

JSIII-6.2 FRI

16:30

Excitability in a PhC
nanolaser with an
integrated saturable
absorberM. Delmulle1,2 ,∙B.
Garbin1 , L.M. Massaro1 ,A. Bazin1 , I. Sagnes1 , K.
Pantzas1 , S. Combrié2 ,A. De Rossi2 , and F.
1
Raineri1,3 ;Université
Paris-Saclay, CNRS, Centre de Nanosciences et deNanotechnologies, 91120
Palaiseau, France; 2 Thales
Research and Technology,
Campus Polytechnique, 1
avenue Augustin Fresnel,
91767 Palaiseau, France;
3
Université Côte d’Azur,
Institut de Physique deNice, CNRS–UMR 7010,
Sophia Antipolis, FranceWe
experimentallydemonstrate the first
all-integrated excitable
nanolaser. We achieve
on-demand generationof optical pulses in a
waveguide with a few
femtojoule perturbationlevels.

CD-14.2 FRI

16:30

Increasing photon-pairs
source brightness basedon inhibited-coupling
hollow-core fiber∙Y. Asselah1 , A. Reigue1 ,A. Chambinaud1 , M.
Cordier3 , F. Amrani1,2 , B.
Debord1,2 , F. Gérôme1,2 ,andF.
Benabid1,2 ;
1GPPMM group, Xlim
Research Institute, CNRSUMR 7252, Université deLimoges, Limoges, France;
2
GLOphotonics, Limoges,
3
France;Departmentof Physics, HumboldtUniversität zu Berlin,
Berlin, Germany
We report on the feasibility of Raman-freeand GHz-level brightness single photon andphoton-pair source basedon Xenon-filled hollowcore
photonic-crystal
fiber with manufacturable
fiber parameters.

EF-10.3 FRI

16:30

Identifying extreme
localization and rogue
waves in fibre optics
using data-driven
dominant balance∙A.V. Ermolaev1 , M.
Mabed1 ,C.
Finot2 ,G. Genty3 , and J.M.
Dudley1 ; 1 Université deFranche-Comté, Institut
FEMTO-ST,
Besançon,France; 2 Université deBourgogne, Laboratoire
Interdisciplinaire Carnot
de Bourgogne, Dijon,
3
France;Photonics
Laboratory,
TampereUniversity,
Tampere,Finland
We use data-driven dominant balance to identify
different regions of dispersive and nonlinear interactions in a nonlinear
Schrödinger equation fibre system. We particularly apply the method togain new insights into fibre modulation instability
dynamics.

CH-16.2 FRI

16:30

Mid-infrared Supercontinuum-based Spectroscopy for Open-path
Measurements∙R. Krebbers, K. van
Kempen, F.J.M. Harren,
A. Khodabakhsh, and
S.M. Cristescu;
Life
Science Trace Detection
Laboratory, Institute for
Molecules and Materials,
Radboud
University,
Nijmegen, Netherlands
The broadband, spatiallycoherent beam of supercontinuum
sources
was used for monitoring
greenhouse gases andpollutants over open
paths.
The detectionof emissions in an outdoor environment wasachieved, including theeffects of air turbulences.

⋅ Friday 30 June 2023

Room 14c ICM

Room Osterseen ICM

Room 21 ICM

nover, Germany; 4 Fiber
Optics and Photonics
Division, CSIR-Central
Glass and Ceramic Research Institute, Kolkata,India
We demonstrate, experimentally, that Kerr
nonlinearity-induced refractive index fronts canbe employed efficiently
to control the opticalmanipulation of single
broadband photons ina nonlinear photonic
crystal fiber

generation of on-demand
optical pulses of 10 ps.

laser, representing thehighest average poweramongmode-locked
Tm/Ho solid-state lasersin 100-fs scale.

CL-8.3 FRI

CF-12.3 FRI

EE-5.3 FRI

16:30

Spectro-temporal Characterization of Tunable
Supercontinuum using
X-FROG Measurements∙B. Chaves1 , V.T. Hoang1 ,V. Couderc1 , B. Little2 ,S. Chu3 , D. Moss4 , R.
Morandotti5 ,and B.
Wetzel 1 ; 1 XLIM ResearchInstitute, CNRS UMR
7252,
UniversityofLimoges, France; 2 QXP
Technologies ,Xi’an,
China; 3 City Universityof Hong Kong, China;
4
Swinburne University ofTechnology, Hawthorn,
5
Australia;
Institut
National de la Recherche
Scientifique - Centre
ÉnergieMatériaux
Télécommunications,
Varennes, CanadaWeexperimentallydemonstrate the spectrotemporal characterization and optimization ofbroadband signals via
asynchronous X-FROG
measurements. We showthat wave-packets with
tailored properties canbe obtained by suitableon-chip pulse preparationand controlled nonlinear
fiber propagation.

213

16:30

1190 nm FDML laser:
Challenges and Strategies∙M.A. Bashir1 , S. Lotz1 ,M. Klufts1 , C. Jirauschek3 ,and R. Huber1,2 ; 1 Institut
Für
Biomedizinische
Optik,
Lübeck,Ger2
many;
Medizinisches
Laserzentrum
LübeckGmbH, Lübeck, Germany;
3
Technische Universität
München,München,Germany
We demonstrate challenges and strategies for
Fourier domain mode
locked laser (FDML)
centered at 1190 nm with
2x410 kHz sweep repetition rate, a sweeping
range of 100 nm and 2.5
mW output power.

16:30

Dual-crystal high power
MIR OPCPA source
tunable from 2.5 μm to
8 μm
N.
Thiré1 ,R.
Maksimenka1 ,A.M.
Stingel2 ,P.
BeringPetersen2 , N. Forget1 , and∙Y. Pertot1 ; 1 Fastlite, 165
rue des Cistes, 06600,
Antibes, France; 2 RuhrUniversität
Bochum,Physikalische Chemie II,
Universitätsstr. 150 -NC
7/72, 44801 Bochum,
Germany
We present a dual-crystal
MIR OPCPA tunablesource at 100 kHz repetition rate. The dual-crystal
scheme allows for ~50fs
pulses in the 2.5-3.7
μm range, while ~100fs
pulses are obtained from
3.5-8 μm.

NOTES

CLEO

Room 1 ICM
CM-11.3 FRI

16:45

Two-Photon Polymerization of an In-Vivo
Multiphoton Imaging
Window∙R. Martínez Vázquez1 ,A. Nardini2 , M. Marini3 ,C. Conci2 , B.S. Kariman4 ,M. Bouzin3 , M. Collini3 ,G.
Chirico3 ,M.T.
Raimondi2 , R. Osellame1 ,andG.
Cerullo4 ;1National Research Council (CNR), Institute for
Photonics and Nanotechnologies, Milan, Italy;
2
Chemistry Department,
Materials and Chemical
Engineering“Giulio
Natta”, Politecnico di
Milano, Milan, Italy;
3Physics
Departament,
Università degli StudidiMilano-Bicocca,
Milan, Italy; 4 Physics
Department, Politecnico
di Milano, Milan, Italy
We present an innovative
intravital imaging window, fabricated by 2PP,
composed of microlenses
andmicroscaffolds.
The fabrication process
is optimized and theopticalfluorescenceimaging properties of the
microlenses have beenvalidated in stained cells.
CM-11.4 FRI

17:00

Fabrication and analysis
of 3D asymmetric pillarshaped metamaterial for
low terahertz (THz)application∙S.
Papamakarios1,2 ,O. Tsilipakos4 , A. Koulouklidis1 , S.T. Tzortzakis1,3 , M. Kafesaki1,3 ,andM.
Farsari1 ;1
IESL/FORTH,
Heraklion, Greece; 2 Departmentof Physics, University ofCrete, Heraklion, Greece;
3
Department of Materials

Room 2 ICM
CJ-10.4 FRI

16:45

Nanosecond-pulsed
hybrid thulium-Raman
fiber amplifier at 2.1 μm∙A.W.
Edvardsen1,2
andL.G.
Holmen1 ;1Norwegian
DefenceResearch Establishment(FFI), Kjeller, Norway;
2
Department of Technology Systems, University ofOslo, Kjeller, Norway
We present a hybrid
thulium-Raman
fiber
amplifier at 2.1 μm thatdelivers 20 ns pulses at
100 kHz with 8.42 W
average power, achieving
a conversion efficiency of
85% w.r.t. 1.95 μm pumplight.

CJ-10.5 FRI

17:00

Single-end-pumped
Tm3+ :Ho3+ -codoped
all-fiber laser at 2120 nm∙P. Forster1,2 , D. Panitzek1 , C. Romano1 , D.
Lorenz1,2 , J. Schneider1,2 ,M. Eichhorn1,2 , and C.
1
Kieleck1 ;Fraunhofer
IOSB (Institute of Optronics, System Technologies
and Image Exploitation),
Ettlingen,Germany;2
Institute of Control
Systems (IRS), Karlsruhe,
Germany
We present a Tm3+ :Ho3+ codoped all-fiber laser
emitting at 2120 nm
relying on an FBG-based
single oscillator cavity.
The fiber laser delivers

Room 3 ICM
EA-9.4 FRI

16:45

Tabletop squeezed light
optomechanics with SiN
patterned membranes∙P.-E. Jacquet1 , M. Croquette 1 , G. Dangoisse
1, S. Chua 2 , and P.-F.
Cohadon 1 ; 1 Laboratoire
Kastler Brossel (ENS, Sorbonne Université, CNRS,
Collège de France), Paris,
France; 2 Centre for Gravitational Physics, The Australian National University, Canberra , Australia
Our project aims at beating the Standard Quantum Limit on a wide frequency range by measuring the mechanical displacement of an ultrahigh Q silicon nitride mechanical resonator using a
NIR frequency dependent
squeezed light source.

EA-9.5 FRI

17:00

Strong Optomechanical
Coupling with Bulk
Acoustic Waves at Room
Temperature∙S. Tarrago Velez, S.
Nielsen, U. Hoff, and
U. Andersen; Center for
Macroscopic
Quantum
States, Department of
Physics, Technical University of Denmark, Kgs.
Lyngby, Denmark
We use an optomechanical system consisting ofa bulk crystal in a FabryPerot optical cavity. We
show how to drive the system in a doubly-resonantway, and use it to demonstrate lasing and strong
coupling.

®

/Europe-EQEC 2023

Room 4a ICM
CK-15.4 FRI

Room 4b ICM

16:45

Localization of light andquasi-bound-state in thecontinuum in photonic
moiré microcavities atmagic configurations∙C. Saadi1 , H.S. Nguyen1 ,S. Cueff1 , L. Ferrier2 , S.
Mazauric3 , S. Callard1 ,and X. Letartre1 ; 1 Univ
Lyon, Ecole Centrale deLyon, CNRS, INSA Lyon,
Univ Claude Bernard
Lyon 1, CPE Lyon, CNRS,
INL, UMR5270, 69130
Ecully, France; 2 Univ
Lyon, INSA Lyon, CNRS,
Ecole Centrale de Lyon,
Univ Claude Bernard
Lyon 1, CPE Lyon,
INL, UMR5270, 69621
Villeurbanne,
France;3
Univ Lyon, CPE Lyon,
CNRS, INSA Lyon, Ecole
Centrale de Lyon, Univ
Claude Bernard Lyon 1,
INL, UMR5270, 69616
Villeurbanne, France
Our study investigates
how light confinementin periodic moiré patterns is preserved in
finite-size
structureswith few supercells.
Tight-bindingmodel
was used to study moiré
microcavities. Potential
fabrication methods ofthese structures are also
discussed.
CK-15.5 FRI⋅ Friday 30 June 2023

17:00

Direct Laser-Written
Optomechanical
Membranes in Fiber
Fabry-Perot Cavities∙L. Tenbrake1 , A. Faßbender2 , S. Hofferberth1 ,S. Linden2 , and H.
1
Pfeifer1 ;Institute ofApplied Physics, Bonn,
2
Germany;
Institute ofPhysics, Bonn, Germany
We present a novel
platformforcavityEI-4.3 FRI

16:45

Free Charge Carrier andExciton Contributions
to Ultrafast Bandgap
Renormalization in
Layered Semiconductors∙T. Deckert and D. Brida;
University of Luxembourg,
Luxembourg,
Luxembourg
We observe the ultrafast
bandgap renormalization
dynamics in layered semiconductors caused by thedistinct effect induced either by excitons or free
carriers.

EI-4.4 FRI

CC-7.4 FRI

16:45

Room 11 ICM
CI-8.4 FRI

16:45

Room 12a ICM
CE-11.3 FRI

16:45

Lithium Niobate BasedSingle-Cycle THz
Source with 643 mW of
Average Power∙T. Vogel and C.J. Saraceno;
Ruhr-University
Bochum,Bochum,Germany
We demonstrate power
scaling of a THz source
based on the tilted-pulse
front method in lithium
niobate to a record-highaverage power of 643 mW,
obtained at 40 kHz repetition rate.

High-Gain, NarrowBand Optical Amplification for Photonic Microwave Applications Using
Stably Injection-Locked
Semiconductor Lasers∙G.-T. Lu1 , C.-H. Tseng1 ,and S.-K. Hwang1,2 ;1Department of Photonics, National Cheng
Kung University, Tainan,
2
Taiwan;Advanced
Optoelectronic Technology
Center, National Cheng
Kung University, Tainan,
TaiwanA narrow-band high-gain
opticalamplification
schemebasedonsemiconductor
lasersoperatingatstablelocking dynamics is
proposed and experimentally demonstrated.
Optical signals can begreatly amplified without
deterioration with theproposed scheme.

Shape Correction of
Glass Using Femtosecond Lasers
G. Chen and ∙J. Qiao;
Rochester Institute ofTechnology,
Rochester,USA
We demonstrate shapecorrectionusingafemtosecond laser.
Asinusoidal 5-cycle/mm
pattern on a glass substrate was successfully
reduced to the subnanometer level.
Thisresult opens a path for the
reduction of detrimental
mid-spatial-frequency
errors.

CC-7.5 FRI

CI-8.5 FRI

CE-11.4 FRI

17:00

Tracking the interlayer
formation dynamics in a
2D heterostructure
V.
Policht1 ,H.
Mittenzwey2 ,O.
Dogadov1 , M. Katzer2 , A.
Villa1 , Q. Li3 , B. Kaiser4 ,A. Ross1 , F. Scotognella1 ,X. Zhu3 , A. Knorr2 , M.
Selig2 , G. Cerullo1 , and ∙S.
Dal Conte1 ; 1 Departmentof Physics, Politecnico
di Milano, Milan, Italy;
2
Institut fur Theoretische
Physik, Nichtlineare Optik
und Quantenelektronik,
Technische
Universitat
Berlin,Berlin,Ger3
many;
Department ofChemistry,
Columbia
University, New York,
4
USA;
Zuse-Institut,
Berlin, Germany
We use optical pumpprobe spectroscopy tomeasure directly thetransient optical responseof interlayer excitons in a
2D heterostructure. We
attribute the ps build-up
time to hot interlayer
exciton thermalization
process.

214

Room 5 ICM

17:00

Improving Terahertz
Output with Layered
Organic Crystal
Structures∙D.J.H.
Ludlow,A.
Alejandro, P.K. Petersen,
K.M. Holland, F. N’diaye,T.
Manwaring,
D.J.
Michaelis,
andJ.A.
Johnson; Brigham Young
University, PROVO, USA
We have improved theterahertz (THz) output
and damage thresholdof yellow organic THz
generation crystals byfusing them to sapphireand using liquid crystal
as index matching fluid
to reduce reflective losses.

17:00

Luminescent Concentrators For Next Generation Microwave Photonics∙J. Sathian1 , L. Lopez2 ,S. Long1 , B. Ford1 , H.
Torun1 , and F. Balembois2 ; 1 Northumbria University, Newcastle upon
Tyne, United Kingdom;
2
Université Paris-Saclay,
Institut d’Optique Graduate School, CNRS, Laboratoire Charles Fabry,
Palaiseau, France
Luminescent concentrators attained increased
attention in recent years
due to their applications
insolid-state
laser

17:00

High-yield mass
produced meta-optics
for consumer electronics∙E.G. Carnemolla1 , M.
Fissore1 , H. Mohamad2 ,L. Dilhan2 , J.E. Callaghan1,3 ,E.
Cox1 ,
B. Johnson1 , and J.
1
Downing1 ;STMicroelectronics (R&D) Ltd,
Edinburgh,
United2
Kingdom;
STMicroelectronics,
Grenoble,
3
France;Institute of
Photonics and Quantum
Sciences,
Heriot-Watt
University,
Edinburgh,
United Kingdom
We demonstrate the capability to mass-produceCLEO

Room 13a ICM
JSIII-6.3 FRI

16:45

Room 13b ICM
CD-14.3 FRI

16:45

Room 14a ICM
EF-10.4 FRI

16:45

®

/Europe-EQEC 2023

Room 14b ICM
CH-16.3 FRI⋅ Friday 30 June 2023

Room 14c ICM

16:45

EE-5.4 FRI

16:45

Room Osterseen ICM
CL-8.4 FRI

16:45

Room 21 ICM
CF-12.4 FRI

16:45

GHz-Rate Photonic
Spiking Neural Networkwith a Single VCSEL∙D. Owen-Newns,
J.
Robertson, M. Hejda,
and A. Hurtado; Instituteof Photonics, Universityof Strathclyde, Glasgow,
United Kingdom
Aphotonic
spikingneural network is constructed using a single
VCSEL, running at GHz
rates (250ps per spikingnode).
The network
is shown to be able toaccurately classify ahighly complex dataset.

experimental demonstration of hyper-entangled pulse modes
and frequency bins
∙F. Chiriano, J. Ho, C.
Morrison, F. Graffitti, and
A. Fedrizzi; Heriot-Watt
University , Edinburgh,
United Kingdom
We demonstrate photonic
hyper-entanglement of
frequency
bins
and
pulse
modes
via
downconversion in adomain-engineered
PPKTP crystal.
The
state is characterised
via time-of-flight spectroscopy and two-photon
interference.

Modulation Instability
Control via Optical
Seeding and Machine
Learning Optimization∙L. Sader1 , V.T. Hoang1 , Y.
Boussafa1 , R. Haldar2,3 ,V. Kermene1 , M. Kues2,3 ,and B. Wetzel1 ; 1 XLIM
Research Institute, CNRSUMR 7252, Universityof Limoges, Limoges,
France; 2 Institute of Photonics, Leibniz University
Hannover,Hannover,
Germany; 3 Cluster of
Excellence
PhoenixD,
Leibniz
University
Hannover,Hannover,
GermanyWeexperimentally
study the control ofnoise-driven modulation
instability during nonlinear fiber propagation.
Using weak and coherent
optical seeding, we showtheoptimizationofincoherent
nonlinear
dynamics and spectral
correlations
throughmachinelearning
strategies.

Fluorinated Graphene
Flakes as Overlayer on a
Tilted Optical Fiber
Bragg Grating for Ammonia Vapor Detection
E.
Grantzioti1,2 ,K.
Bhorkar3 , N. Samartzis3 ,S. Pissadakis 1 ,S.
Yannopoulos3 , and ∙M.
Konstantaki1 ; 1 Institute ofElectronic Structure andLaser (IESL), Foundation
for Research and Technology – Hellas (FORTH),, Heraklion , Greece;2
Physics
Department,
University of Crete, Heraklion, Greece; 3 Instituteof Chemical Engineering
Sciences(ICE-HT),Foundation for ResearchandTechnology-Hellas(FORTH),, Patras , Greece
We report on thecladding and Bragg mode
wavelength shift responseof an optical fibre tilted
Bragg grating with afluorinatedGraphene
Flakes overlayer in thepresence of Ammonia
vapours.

Spatio-Spectral Vector
Fields∙L. Kopf, R. Barros, and
R. Fickler; Tampere University, Photonics Laboratory, Physics Unit, Tampere, FinlandWe
present
spatiospectral vector fields,
which are light fields witha varying polarization
structure in space as well
as frequency. The beam
only exhibits its vectorial
nature when all relevant
degrees of freedom areresolved.

13.4 MHz FDML Laser
for Intra-Surgical Optical Coherence Tomography∙S. Lotz1 , M. Göb1 , W.
Draxinger1 , A. Dick1 ,and R. Huber1,2 ; 1 Institut
fürBiomedizinische
Optik, Universität zu
Lübeck, Lübeck, Ger2
many;
Medizinisches
Laserzentrum
LübeckGmbH, Lübeck, Germany
We present a 13.4 MHz
Fourier domain locked
laser (FDML) sweeping
over 113 nm centeredat 1300 nm to enablehigh-resolution
video
rate intra-surgical opticalcoherence tomography(OCT).

Generation of Tunable
MIR/LWIR Femtosecond Pulses by Combination of SRS and DFG∙J. Roman1 , R. Jutas1 , I.
Astrauskas1 , A. Imani1 ,P.
Carpeggiani1 ,P.
Polynkin2 , E. Kaksis1 , T.
Floery1 , A. Baltuška1,3 ,andA.
Pugžlys1,3 ;1Photonics Institute, TU
Wien, Vienna, Austria;
2
Collegeof
OpticalSciences, The Universityof Arizona, Tucson, USA;
3
Center for PhysicalSciences & Technology,
Vilnius, Lithuania
Microjoule-energy femtosecond pulses tunable
between 6 and 10 μm are
generated as a CEP-stable
seed for a high-energy
mid-IR OPCPA. We apply
difference-frequencymixing in LGS crystal
between 200-fs 1030-nm
laser pulses and their
Raman-shifted replicas.

JSIII-6.4 FRI

CD-14.4 FRI

EF-10.5 FRI

CH-16.4 FRI

EE-5.5 FRI

CL-8.5 FRI

CF-12.5 FRI

17:00

Online image recognition with ultrafast
spiking microlaser
neurons∙A.H. Masominia, L. Calvet, and S. Barbay; Centre de Nanosciences et deNanotechnologies, Université Paris-Saclay, CNRS,
Palaiseau, France
We present a novel approach for image recognition using ultrafast photonic spiking neurons, inspired by receptive fields
and rank coding classification, eliminating the offline computing step. We
illustrate it numericallyon a simple task.

17:00

Tailoring photon pairemission characteristics
via bi-chromatic excitation of an integrated
nonlinear cavity∙A.M. Angulo M.1,2 ,J. Heine1 , J.S.S. Durán
Gómez1 , H. Mahmudlu1 ,R. Haldar1,2 , C. Klitis3 ,M. Sorel3,4 , and M.
Kues1,2 ; 1 Institute of Photonics, Leibniz University
Hannover,Hannover,
Germany; 2 Cluster of
Excellence
PhoenixD,
Leibniz
University
Hannover,Hannover,3
Germany;
School ofEngineering, University ofGlasgow, Glasgow, United

17:00

Chaotic dynamics andintense wave formationfrom multiple soliton
collisions and the role ofextra dimensions
F. Xin1,2 , ∙L. Falsi1 ,D.
Pierangeli1,3 ,C.
Conti1,3 , F. Fusella1 , G.
Perepelitsa4 , Y. Garcia4 ,A.J. Agranat4 , and E.
DelRe1,3 ; 1 Dipartimento
di Fisica, Universita diRoma “La Sapienza”,
Rome, Italy; 2 College ofPhysics and Materials
Science, Tianjin Normal
University,
Tianjin,3
China;ISC-CNR,
Universita di Roma “La
Sapienza”, Rome, Italy;

17:00

A Hot Extractive Differential Optical Absorption Spectroscopy
System for SO2 andNOx Monitoring inIndustrial Plants∙A. Roy, P. Pingale, R. Fernandes, Y. Rajeshirke, andC. Mitra; Forbes MarshallPvt. Ltd., Pune, India
We report the design,development and validation of a highly sensitive
UV differential opticalabsorption spectroscopy
system for hot extractive
measurement of sulphur
dioxide (SO2) and oxides
of nitrogen (NOx) at
industrial stacks.

17:00

Shaping resonant
dynamics in condensed
matter systems bytailored ultrafast pulses∙O.
Meron1,2 ,S.
Nehemya1,2 , U. Arieli1,2 ,E. Bahar1,2 , M. BenShalom1 ,andH.
Suchowski1,2 ; 1 Condensed
Matter Physics Department, School of Physics
and Astronomy, Facultyof Exact Sciences, Tel Aviv
University, Tel Aviv, Israel;
2
Center for Light–Matter
Interaction,
Tel–Aviv
University, Tel Aviv, IsraelWeexperimentallydemonstrate a novel
controlmethod
for

215

17:00

Ultra-compact widely
tunable dual-wavelength
fiber-based sources for
CARS and SRS imaging
E. Shestaev1 , F. Just1 , O.
Herrfurth1 , C. Gaida1 ,S. Breitkopf1 , T. MeyerZedler2 , J. Popp2 , ∙T.
Eidam1 , and J. Limpert1 ;1
Active Fiber Systems
GmbH, Jena, Germany;
2
Leibniz-Institut
fürPhotonische Technologien
Jena e.V, Jena, Germany
We present a compact
dual-wavelength source
for CARS/SRS covering <630cm^-1 up to2250cm^-1 with a tuning
time of a few seconds

17:00

Resolving the modelocking riddle inquantum cascade lasers∙G. Steinmeyer and W.
Chen; Max-Born-Institut,
Berlin, Germany
Solving the Haus masterequation, we deliver a
simple explanation for
the alleged mode-locking,soliton formation, andfrequency comb formation of quantum cascadelasers.

NOTES

CLEO

Room 1 ICM

Room 2 ICM

Science and Technology,
University of Crete, Heraklion, Greece; 4 National
Hellenic Research Foundation (N.H.R.F.), Athens,
GreeceA state of the art electromagnetic metamaterial
design for low THz
applications is reported.
The metallic fabricatedstructure was measured
and exhibited promising
results for transmission
filter in specific operating
wavelengths.

160 W of output with aslope efficiency of 46.6 %.

CM-11.5 FRI

CJ-10.6 FRI

17:15

Efficient Implementation of Spatial Light
Modulator (SLM) for
Ultra-High Throughput
2-Photon Lithography∙L.
Jonušauskas1,2 ,D. Andrijec1 , and K.
1
Stonkus1 ;Vital3D
Technologies,
Vilnius,2
Lithuania;
Vilnius
University,
Vilnius,
Lithuania
We present a methodology that allows us totune 2-Photon Lithography resolution during
printing using a spatial light modulator.
This allows increasing
printing
throughput
more than 100 times
in comparison to thecurrent state-of-the-art
systems.

17:15

Temperature-dependent
emission cross-section
spectra at 1.8 um of thethulium-doped fibers
cooled down to cryogenic temperatures∙B.
Jiříčková1,2 ,R.
Švejkar2 , M. Grábner1 , C.
Jauregui3 , J. Aubrecht1 ,O. Schreiber1,2 , and P.
Peterka1 ; 1 Institute of
Photonics and Electronics,
Prague, Czech Republic;2
Czech Technical University in Prague, Facultyof Nuclear Sciences andPhysicalEngineering,
Prague, Czech Republic;3
Institute of Applied
Physics, Abbe Center of
Photonics, Jena, Germany
Thermal management of
thulium-doped fibers is
crucial for high-power
laser systems as temperature affects spectroscopic
properties. We present
results of temperaturedependent
emissioncross-section
spectraof thulium-doped silica
fibers in the temperature
range 77-475 K.

Room 3 ICM®

/Europe-EQEC 2023

Room 4a ICM

Room 4b ICM

optomechanicalexperiments
featuring
3D-direct-laser-written
mechanical membranes
directly
integrated
into fiber Fabry-Perotcavities.
The flexible
fabrication
enablesvariousapplications
like fiber-tip-integrated
sensing, and multimodemechanicalresonator
systems.

EA-9.6 FRI

17:15

Anharmonic mechanical oscillator implemented with a single
trapped ion∙B. Deng, M. Göb, D.
Wang, and K. Singer; Institute of Physics, University of Kassel, Kassel, Germany
Here, we implement ananharmonic
oscillator
with a single ion trappedinafunnel-shaped
potential, quantitatively
characterize its nonlinearity, and discuss its
potential application inforce sensing.

CK-15.6 FRI⋅ Friday 30 June 2023

17:15

Experimental realization of extreme light
confinement in an InP
nanocavity∙M. Xiong, R. E. Christiansen, F. Schroeder,
Y. Yu, L. N. Casses, E.
Semenova, K. Yvind, N.
Stenger, O. Sigmund, and
J. Moerk; NanoPhoton Center for Nanophotonics,
Technical University ofDenmark, Kgs. Lyngby,
DenmarkWe
experimentallydemonstrate that light
can be concentrated
far below the so-called
diffraction limit in a
III-V
semiconductor
nanocavity designed by
topology optimization.
The results open a path
towards nanoscale active
devices and nonlinear
elements.

EI-4.5 FRI

17:15

Ultrafast cooling of hot
carriers in magic angle
twisted bilayer graphene∙J.D.
Mehew1 ,R.
Luque Merino2,3,4 , H.
Ishizuka5 , A. Block1 ,J. Diez Merida2,3,4 , A.
Diez Carlon2,3,4 ,K.
Watanabe6 ,T. Taniguchi7 , L.S. Levitov8 ,D.K. Efetov3,4 , and K.-J.
Tielrooij1,9 ; 1 Catalan Institute of Nanoscience andNanotechnology (ICN2),
Barcelona, Spain; 2 ICFO
- Institut de Ciencies
Fotoniques,
Barcelona,3
Spain;
Fakultat fur
Physik, LMU, Munchen,4
Germany;
MunichCenter for Quantum
Science and Technology(MCQST),
Munchen,Germany; 5 Departmentof Physics, Tokyo Instituteof Technology, Japan;
6
Research Center for
Functional
Materials,
National Institute for Material Sciences, Tsukuba,
7
Japan;
International
Center for Materials
Nanoarchitectonics,
National Institute for Material Sciences, Tsukuba,
Japan; 8 Department of
Physics,
Massachusetts
Institute of Technology, Cambridge, USA;
9
Department of Applied
Physics, TU Eindhoven,
Netherlands
We reveal a novel
Umklapp
scattering
mechanism
betweenelectrons and phonons
in magic angle twisted
bilayer graphene thatenables ultrafast hot
carrier cooling fromroom temperature down
to 5K.

216

Room 5 ICM

CC-7.6 FRI

17:15

Emission dynamic ofions by monocycle THz
pulse∙J. Houard, G. Darmala,M. Karam, O. Bhorade,and A. Vella; CNRS,
Univ Rouen Normandie,
INSA Rouen Normandie,
Groupe de Physique desMatériaux UMR 6634
F-76000, Rouen, France
Light ions emission
dynamic by TeraHertz
monocycle from nanometric needle apex isstudied measuring timeof flight at sub-ns resolution and pump probe
experiments.
Multipletimescale effects will be
shown

Room 11 ICM

Room 12a ICM

pumping.
Here wereport the results of aroom-temperature microwave MASER pumped
by a high-brightness
LED-luminescentconcentrator.

opticalmetasurfaces
on a standard 300mm
semiconductor
process typically used for
consumerelectronics.
Products show highopticalperformance:transmitted zeroth order
lower than 0.2% andfabrication yields of 99%.

CI-8.6 FRI

CE-11.5 FRI

17:15

Highly Reconfigurable
Microwave Photonic
Bandstop Filters using
Ultra-Low Brillouin
Gain
K. Girish1 , R. Parihar2 ,P.
Raj2 ,
and∙A.
Choudhary2 ; 1 National
Institute of Technology,
Tiruchirapalli,
India;
2
IndianInstituteofTechnology Delhi, New
Delhi, India
We demonstrate a lowpower wideband bandstop microwave photonic
filter with bandwidth up
to 1 GHz achieved byadvanced phase engineering of an analog photonic
link and harnessing thephase response of stimulated Brillouin scattering.

17:15

Holographically fabricated 2D grating
coupler for integrated
large beam delivery∙Q.S. Ahmed, J.W. Field,
D.-W. Ko, P. Horak, C.
Holmes, C.B.E. Gawith,
P.G.R. Smith, P.C. Gow,
and J.C. Gates; Optoelectronics Research Centre,
University of Southampton, Southampton, SO17
1BJ, UK, Southampton,
United Kingdom
We demonstrate a 2D
grating coupler (4.4 mm
× 3.9 mm) in doped
planar silica using aholographic UV laser
inscription technique forout-of-plane free-spacecoupling of beams.

CLEO

Room 13a ICM

JSIII-6.5 FRI

17:15

Pulse collision computing with spiking micropillar lattices
L. Soun1 , K. AlfaroBittner2 , A. Masominia1 ,R. Braive1,3 , K. Pantzas1 ,G. Beaudoin1 , I. Sagnes1 ,J.-R. Coudevylle1 , M.G.
Clerc4 , and ∙S. Barbay1 ;1Centre de Nanosciences
et de Nanotechnologies, Palaiseau, France;
2
Université Paris-Cité &Institut Universitaire deFrance, Paris, France;
3
Universidad Rey Juan
Carlos, Madrid, Spain;
4
Departamento de Fśica
and Millennium Institutefor Research in Optics,
FCFM, Universidad deChile, Santiago, Chile
We investigate numerically a lattice of coupled
ultrafast photonic microlaser neurons anddemonstrate how pulse
collisions enable therealization of temporal
logical gates, including
the non linearly separable
XOR gate. Preliminary
experimental results are
discussed.

Room 13b ICM
Kingdom; 4 Institute ofTechnologies for Communication,Information
andPerception(TeCIP),Sant’Anna
SchoolofAdvanced
Studies, Pisa, Italy
Enabling
degenerately
and non-degenerately excited SFWM processes by
bi-chromatic excitation
in a nonlinear cavity, wedemonstrate enhanced
photon pair generationand control of theirspectral structure. This
allowstime-frequency
states manipulation for
quantum
processing
applications.
CD-14.5 FRI

17:15

Squeezed vacuum froma photonic crystal fibre
parametric oscillator∙A.O.C. Davis1 ,A.I.
Flint2 , W.A.M. Smith1 ,P.J. Mosley1 ,R.H.S.
Bannerman2 ,K.
Harrington1 , C. Parry1 ,and
P.G.R.
Smith2 ;1
Centre for Photonics andPhotonic Materials, University of Bath, Claverton
Down,
United King2
dom;
Optoelectronics
Research Centre, University of Southampton,
Southampton,
UnitedKingdom
We introduce a novel
squeezed light source
design, comprising a
Bragg-reflector
FabryPerot
resonatorinmonolithic
photonic
crystal fibre supportingdual-pumpdegenerate
four-wave mixing. Our
work promises all-fibresqueezing for quantum
communication
andinformation applications.

Room 14a ICM®

/Europe-EQEC 2023

Room 14b ICM

The Brojde Center for
Innovative Engineeringand Computer Science,
The Hebrew University,
Jerusalem, Israel
Our study of multiple
soliton collisions showsthat if the dimensionality
hosting the collision islarger than that of thenonreciprocalinteraction, conditions can befound in which multiple
solitons fuse without
chaotic behavior.
4

CH-16.5 FRI

17:15

Development of a
Breathalyzer for Ethanol
Detection using a Quantum Cascade Laser
Array and a Dense
Pattern Multipass Cell
∙C. Jacquemin1,2 ,R.
Vallon1 , B. Parvitte1 , G.
Maisons2 , M. Carras2 ,and V. Zeninari1 ; 1 Groupede Spectrométrie Moléculaire et Atmosphérique,Reims, France; 2 mirSense,
Palaiseau, France
A QCL DFB laser arrayemitting around 10 μm,
driven by dedicated electronics, is coupled to an
innovative dense pattern
multipass cell to detect
gas-phase ethanol.

⋅ Friday 30 June 2023

Room 14c ICM

Room Osterseen ICM

ultrafast coherent quasiparticle dynamics in
2D semiconductors andplasmonic nanoparticles.
We
selectively
steer
resonant
nonlineargeneration, rearranging
the interfering quantum
pathways from destructive
toconstructive
interferences.

over the full range,
repetition-rates up to
10MHz and <13cm^-1
bandwidth.

EE-5.6 FRI

CL-8.6 FRI

17:15

Mid-Infrared Excitationof Rotational Wave
Packets at High-Lying
Vibrational States∙H. Tsusaka, I. Morichika,
and S. Ashihara; Institute of Industrial Science,
The University of Tokyo,
Tokyo, Japan
we report on successful
demonstration of multiquantum
vibrational
excitation in the antisymmetric stretch (󰜈3 ) of
gas-phase CO2 molecules
up to the 󰜈3 = 8 stateand observation of therotational wave packet inthe 󰜈3 = 0 to 8 states.

217

17:15

Advanced light source
for speckle-free multiexposure imaging at
multi-MHz frame rates∙J. Mur, Ž. Lokar, V.
Agrež, J. Petelin, J.J.
Kočica, and R. Petkovšek;
University of Ljubljana,
Faculty of MechanicalEngineering, Ljubljana,
Slovenia
Shock wave evolution inwater, travelling above
the speed of sound(1500 m/s), was imaged
using a multi-exposuretechnique. The advanced
light source enables
speckle-freecamerasynchronizedimaging
at up to 10 MHz frame
rates.

Room 21 ICM

CF-12.6 FRI

17:15

Few-cycle 50 μJ Pulses at
11.2 μm from a Singlestage OPCPA at 1 kHz
M. Bock, P. Fuertjes, and∙U. Griebner; Max Born
Institute, Berlin, Germany
A single-stage opticalparametric chirped pulse
amplifier based on GaSe
generating idler pulses
around 11 μm with 180 fs
duration and 50 μJ energy
at a 1-kHz repetition rate
is presented.

NOTES

CLEO

®

/Europe-EQEC 2023

⋅ Friday 30 June 2023

Hall B0
13:00 – 14:00

CC-P.5 FRI

CC-P.9 FRI

CC-P.13 FRI

CC-P: CC Poster session

Demonstration of The Imaging-Free Wedged
Nonlinear Echelon Slab Terahertz Pulse Source∙G. Krizsán1,2,3 , G. Polónyi2,3 , T. Kroh4,5 , G. Tóth1,2 , Z.
Tibai1 , N.H. Matlis4 , G. Almási1,2 , F.X. Kärtner4,5 , and
J. Hebling1,2,3 ; 1 Institute of Physics, University of Pécs,
Pécs, Hungary; 2 Szentágothai Research Centre, Universityof Pécs, Pécs, Hungary; 3 ELKH-PTE High-Field Terahertz
Research Group, Pécs, Hungary; 4 Center for Free-Electron
Laser Science, DESY, Hamburg, Germany; 5 The Hamburg Centre for Ultrafast Imaging, University of Hamburg,
Hamburg, Germany
A novel compact, imaging-free, tilted-pulse-front
pumped terahertz (THz) source based on a LiNbO3
slab with a small wedge angle (<8∘ ) and with an echelon
microstructure on its input surface has been demonstrated.

Possibility of CO2 Laser Pumped Terahertz Sources∙G. Illés1 , G. Nazymbekov1 , G. Almási1,2 , G. Tóth1,2 , and
J. Hebling1,2,3 ; 1 Institute of Physics, University of Pécs,
Pécs, Hungary; 2 Szentágothai Research Center, Universityof Pécs, Pécs, Hungary; 3 ELKH-PTE High-Field THz Research Group, Pécs, Hungary
The possibility of CO2 laser pumped semiconductorbased THz-source was widely investigated numerically.
Due to the long wavelength, high pump intensity canbe used while avoiding multiphoton absorption and 1%
THz conversion efficiency can be reached.

Investigation of Terahertz Pulse Generation in
Semiconductors Pumped at Long Infrared
Wavelengths∙G. Polónyi1,2 , G. Tóth1,2,3 , N. Mbithi2,3,4 , Z. Tibai1,3 ,I. Benabdelghani2,3 , L. Nasi2,3 , G. Krizsán1,2,3 , G. Illés3 ,and J. Hebling1,2,3 ; 1 ELKH-PTE High Intensity Terahertz
Research Group, Pécs, Hungary; 2 Szentágothai ResearchCentre, Pécs, Hungary; 3 University of Pécs, Pécs, Hungary; 4 Garissa University, Garissa, Kenya
Numerical simulations performed to determine thepractical limit on pumping wavelength that is not prosperous to exceed when GaP and GaAs semiconductors
are pumped to generate THz pulses without the presenceof strong multi-photon absorption.

CC-P.1 FRI

400 kHz repetition rate THz-TDS with 24 mW of
average power driven by a compact industrial
Yb-laser∙C. Millon1 , S. Houver2 , and C.J. Saraceno2 ; 1 Ruhr University Bochum, Bochum, Germany; 2 Paris Cite University, Paris, France
We demonstrate a 24 mW average power THz-TDS at
400 kHz repetition rate, driven directly by a commercial
fs-laser. We show no thermal effects on the generated
THz while varying the repetition rate.
CC-P.2 FRIUltrafast carrier dynamics in n-doped Ge driven bystrong-field THz pulses∙A. Gupta1,2 , K. Chordiya1,2 , V. Gupta1 , J. Bohus1 , M.
Kahaly1 , A. Sharma1 , and J. Fulop1 ; 1 ELI-ALPS, Szeged,
Hungary; 2 Institute of Physics, University of Szeged,
Szeged, Hungary
A detailed experimental study is presented on strongfield THz driven ultrafast carrier dynamics in ndoped Ge at two different temperatures, by using THz
pump—THz probe spectroscopy up to near 0.5 MV/cm
field strength.
CC-P.3 FRI

THz Characterization and Generation of
Temperature-Controlled Organic Crystal BNA∙S. Mansourzadeh1 , T. Vogel1 , M. Shalaby2 , and C.J.
Saraceno1 ; 1 Ruhr-University Bochum, Bochum, Germany; 2 Swiss Terahertz Research-Zurich, Zurich, Switzerland
We present THz generation experiments andtemperature-dependent (80K – 300K) refractive index and absorption for BNA for the first time. We show
increased THz field strength corresponding to a reduced
THz absorption at low temperatures.
CC-P.4 FRI

THz Spectroscopy of Graphene Layers using
Guided-Mode Resonance Notch Filter
H.S. Bark1 , M.-W. Park2 , and ∙T.-I. Jeon2 ; 1 Gwangju Institute of Science and Technology, Gwangju, South Korea;
2
Korea Maritime and Ocean University, Busan, South Korea
We measured sheet conductivity of mono-, bi, andtriple-layer graphene using an all-dielectric single-layer
guided-mode resonance filter (GMRF) operating in thehigh-frequency terahertz (THz) region.

CC-P.6 FRIJitter Correction for Asynchronous Optical Sampling
Terahertz Time-Domain Spectroscopy based on
Free-Running Pulsed Lasers∙M. Nakagawa, N. Kanda, T. Otsu, I. Ito, Y. Kobayashi,
and R. Matsunaga; The Institute for Solid State Physics,
The University of Tokyo, Kashiwa, JapanWe developed a new method of asynchronous opticalsampling terahertz time-domain spectroscopy based ona pair of free-running laser oscillators without any feedback control, which is realized by recording and processing jitter information.
CC-P.7 FRITerahertz radiation from a large-area
photoconductive emitter via high average powerYb-oscillator∙M. Khalili1 , T. Vogel1 , S. Mansourzadeh1 , S. Winnerl2 ,and C.J. Saraceno1 ; 1 Photonics and Ultrafast Laser Science, Ruhr Universität Bochum,, Bochum, Germany;2
Helmholtz-Zentrum Dresden-Rossendorf, Institute ofIon Beam Physics and Materials Research, Dresden, Germany
We present first steps of power scaling large area photoconductive emitter for THz generation, excited with 1 W
of average optical power by a frequency-doubled, homebuilt, ultrafast oscillator with 90 MHz repetition rate.
CC-P.8 FRIHigh-Power Narrowband THz Generation∙N.K. Green, C. Rader, M.F. Nielson, and J.A. Johnson;
Brigham Young University, Provo, USA
Using a Ti:Sapphire laser and BNA bonded to sapphirein tandem with a chirp-and-delay technique, we test thelimits of intense narrowband THz generation (0.1 to 5
THz).

CC-P.10 FRIBroadband characterization of 6G microelectronics
packaging materials: EN-A1 alkali-freeboroaluminasilicate glass substrates
M. Zhai1,2 , ∙H. Shi1,2 , M. Swaminathan1 , A. Locquet1,2 ,and D.S. Citrin1,2 ; 1 Georgia Institute of Technology, Atlanta, USA; 2 Georgia Tech Lorraine, Metz, France
EN-A1 alkali-free boroaluminasilicate glass was characterized by terahertz time-domain spectroscopy. Moderately high dielectric constant, low loss tangent, and excellent CTE indicate that EN-A1 glass is an attractive alternative for 6G heterogeneous microelectronics packaging applications.
CC-P.11 FRITerahertz-to-Optical Carrier Conversion Using
Optical-Comb-Injection-Locked Dual-Wavelength
Laser Light and Electro-Optic Polymer Modulator
Y. Matsumura1 , E. Hase1 , Y. Tokizane1 , N. Kuse1 , J.-i.
Fujikata1 , H. Kishikawa1 , M. Haraguchi1 , Y. Okamura1 ,T. Kaji2 , A. Otomo2 , A. Kanno2,3 , S. Hisatake4 , and∙T. Yasui1 ; 1 Tokushima University, Tokushima, Japan;
2
National Institute of Information and Communications
Technology, Koganei, Japan; 3 Nagoya Institute of Technology, Nagoya, Japan; 4 Gifu University, Gifu, Japan
THz-to-optical carrier conversion was demonstrated by
a combination of optical-comb-injection-locked dualwavelength laser light and electro-optic polymer modulator, enabling all-photonic detection of THz wave.
CC-P.12 FRIRaman-supressed 200-300 kW Multicycle Parametric
Source at 5.7 THz∙M.-H. Wu, C.-H. Kuo, Y.-J. Lin, and Y.-C. Huang; Institute of Photonics Technologies/National Tsing Hua University, Hsinchu, Taiwan
We report the generation of 200-kW peak power coherent radiation at 5.7 THz from a KTP differencefrequency generator. The THz radiation consists of ~500
cycles in 83-ps pulse width.

218

CC-P.14 FRI

Photo-Carrier Dynamics of MAPbI3 Perovskite
Depending on Grain Size Through Time-Resolved
Terahertz Spectroscopy∙B. Son1 , D. Kim4 , S.H. Park4 , N.-E. Yu2,3 , and D.-K.
Ko1,3 ; 1 Department of Physics and Photon Science, GIST,
Gwangju, South Korea; 2 Advanced Photonics ResearchInstitute, GIST, Gwangju, South Korea; 3 Research Center for Photon Science Technology, GIST, Gwangju, South
Korea; 4 Department of Physics, Pukyong National University, Busan, South Korea
Carrier Density and optical conductivity of differentsized MAPbI3 perovskites are observed by time-resolved
terahertz spectroscopy utilizing 400nm optical pump.
The carrier density has 0.3~3x10^18cm-3, which is related to grain size.
CC-P.15 FRI

Acceleration of Electrons from Krypton Gas Plasma
Using THz Pulses∙S. Turnár1,2 , B.R. Sarkadi1 , S.W. Jolly4 , J. Hebling1,2,3 ,and Z. Tibai1 ; 1 Institute of Physics, University of Pécs,
Pécs, Hungary; 2 ELKH-PTE High Field Terahertz Research Group, Pécs, Hungary; 3 Szentágothai ResearchCentre, University of Pécs, Pécs, Hungary; 4 Service
OPERA-Photonique, Université Libre de Bruxelles (ULB),Brussels, Belgium
We have numerically investigated the effect of the ionization on the acceleration results and thereby we could
optimize our newly presented table top electron accelerator model using General Particle Tracer and EPOCH(particle-in-cell) code.
CC-P.16 FRI

Nonlinear Transmission of FUS Protein Solution andWater at 0.5 THz∙Q.M. Thai1 , I. Ilyakov2 , M. Raj1 , D. Dornbusch2 , A.
Arshad2 , T. de Oliveira2 , M. Jahnel1,3 , J.-C. Deinert2 , A.

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Ponomaryov , S. Kovalev , and E.M. Adams ; Clusterof Excellence Physics of Life (PoL), TU Dresden, Dresden, Germany; 2 Helmholtz-Zentrum Dresden-Rossendorf(HZDR), Dresden, Germany; Center for Molecular andCellular Bioengineering, Biotechnology Center, TU Dresden, Dresden, Germany

Here, the nonlinear transmission of a FUS protein solution and water at 0.5 THz - indicating a perturbed hydrogen bonding network are investigated, along with theTHz laser induced heat effect on the experimental results.

13:00 – 14:00

lence advanced Manufacturing Engineering (GSaME),
University of Stuttgart, Nobelstraße 12, 70569 Stuttgart,
Germany
A large-core tubular inhibited-coupling-guiding hollowcore photonic-crystal fiber with low dispersion was designed, produced, and characterized. The produced fiber
shows losses below 30 dB/km and a dispersion below 1.5
ps/(nm⋅km) between 900 nm and 1150 nm.

CI-P.8 FRI

versity, Shanghai, China; 3 Shanghai Huawei Technologies
Company, Ltd., Shanghai, China
Precisely processing broadband signals are demanding
in the tunable photonic aperiodic filtering and digitizing
system. The rules to achieve hundreds of MHz filteringin the system design are presented and verified.

2

2

1,2 1

CI-P: CI Poster session
CI-P.1 FRIInput Ordinal Invariant Neural Network based
Eigenvalue Demodulator for On-Off Encoded4096-ary Multi-Eigenvalue Signal∙D. Hisano, T. Kozuno, K. Mishina, and A. Maruta; Osaka University, Suita, Japan
This paper experimentally demonstrates employing input ordinal invariant neural network on eigenvalue demodulation with 4096-ary (=12 bit/symbol) eigenvalues.
We obtained the error-free operation at BER = 3.8 × 10−3
in 50-km fiber transmission.
CI-P.2 FRIResonator Design For High-Brightness LuminescentConcentrator Pumped MASERs∙S. long, B. Ford, M. Elsdon, H. Torun, and J. Sathian;Northumbria University, Newcastle, United Kingdom
Designing efficient resonator cavities is crucial for advanced microwave photonics applications. Here we report improved microwave resonator design for a miniaturised and efficient room-temperature MASER pumped
by a luminescent concentrator at record luminance andpower.
CI-P.3 FRIExperimental Investigations of Orientation-based
Solar Noise in Underwater Optical WirelessCommunication System
S.K. Mahapatra, M. Howlader, S.K. Roy, ∙M. Pradhan, and S.K. Varshney; Indian Institute of Technology,
Kharagpur, India
The impact of orientation-based solar noise on the
UOWC system has been investigated experimentally.
The experimental results show a good agreement withthe theoretical predictions.
CI-P.4 FRI

Design, production, and characterization of a
Large-Mode Area tubular Inhibited-Coupling
Guiding Hollow-Core Fiber with low dispersion∙T. Kühlthau1 , B. Chen1,2 , G. Kleem1 , T. Graf1 ,and M. Abdou Ahmed1 ; 1 Institut für Strahlwerkzeuge(IFSW), University of Stuttgart, Pfaffenwaldring 43,70569 Stuttgart, Germany; 2 Graduate School of Excel-

3

CI-P.5 FRIDesign and Fabrication tolerances Analysis of the
Polarization-Maintaining Inhibited-Coupling
Guiding Hollow-Core Fibers∙B. Chen1,2 , T. Kühlthau1 , C. Röhrer1 , T. Graf1 ,and M. Abdou Ahmed1 ; 1 Institut für Strahlwerkzeuge(IFSW), University of Stuttgart, Pfaffenwaldring 43,70569 Stuttgart, Germany; 2 Graduate School of Excellence advanced Manufacturing Engineering (GSaME),
University of Stuttgart, Nobelstraße 12, 70569 Stuttgart,
Germany
Numerical simulations were conducted to analyze theinfluence of design parameters of tubular inhibitedcoupling guiding hollow-core photonic crystal fibers on
the bending-induced phase shift. After proposing two
polarization-maintaining fiber designs, the fabrication
tolerances were investigated.
CI-P.6 FRI

Non-line-of-sight optical communication using 1DSpeckle Information
P.S. Badavath, V. Raskatla, ∙H.J. Pandit, and V. Kumar; National Institute of Technology Warangal, Warangal,
India
One-to-three non-line-of-sight optical communication
channels employing Orbital angular momentum-Shift
keying (OAM-SK) based on 1D speckle information are
established with an average classification accuracy of
79% among all three channels.
CI-P.7 FRI

Gradient Boosting for Nonlinear Equalization in
Optical Transmission Systems∙E. Sedov; Aston Institute of Photonic Technologies, Birmingham, United Kingdom
This study demonstrates the use of Gradient Boosting asa tool for nonlinear equalization in optical transmission
systems. We show an improvement in Q-factor by 0.65
dB and decrease in BER from 0.051 to 0.039.

Restricted Boltzmann Machine Classifier for
Nonlinear Compensation in DP-16QAM Single and
WDM Coherent Optical Communication Systems
A. Singh, ∙N. Gautam, B. Lall, and A. Choudhary; Indian
Institute of Technology Delhi, Delhi, India
A semi-supervised Restricted Boltzmann Machine andlogistic regressor learning technique is proposed for
nonlinearity compensation in coherent-optical communication systems. Results show Q-factor improvement of
up-to 1dB over linear equalization in single channel and
WDM systems.
CI-P.9 FRIOptimization of Bending Loss for Higher Order
Modes of Anti-Resonant Hollow Core Fibers∙. Suchita, A. Kaushalram, and A. Bhardwaj; Department
of Instrumentation and Applied Physics, Indian Instituteof Science Bangalore, Bengaluru, India
Bending loss is optimized by tuning the design parameter of anti-resonant hollow-core fiber. The optimized
loss is < 10-1 dB/turn for fundamental mode and larger
for higher order mode at bending radius ≥ 40 cm.
CI-P.10 FRIAn Arbitrary Biased EOM-based Pulse-Picker with
Programmable Repetition Rate using FPGA
∙J. Dutta1 , K. Singh2 , S. S J1 , and D. Venkitesh1 ;1
Indian Institute of Technology Madras, Chennai, India;
2
National Institute of Technology Kurukshetra, Kurukshetra, India
We experimentally demonstrate an arbitrarily biased
electro-optic Mach-Zehnder modulator-based pulse
picker with variable repetition rate (from 50 MHz to
500kHz) by using a fast synchronized FPGA. We reporta maximum pulse extinction ratio of 34 dB.
CI-P.11 FRI

Tunable High Precision Signal Processing Based on
the Simultaneous Photonic Filtering and Digitizing
System∙Y. Sun1,2 , Q. Tan1 , D. Wang1 , D. Liang1 , S. Wang2,3 , J.
Gong1 , and G. Wu2 ; 1 China Academy of Space Technology, Xi’an, China; 2 The state Key Laboratory of Advanced
Optical Communication Systems and Networks, Shanghai
Institute for Advanced Communication and Data Science,
Dept of Electronic Engineering, Shanghai Jiao Tong Uni-

219

CI-P.12 FRIRadio-frequency Multiplication without Phase Noise
Degradation in an Electro-optic Frequency-shifting
Loop∙L. Alliot de Borggraef, V. Carlet, M. Brunel, and H. Guillet de Chatellus; Univ Rennes, CNRS, Institut FOTON UMR 6082, 35000 Rennes, France
We report a photonic architecture enabling the multiplication of input radio frequencies in the GHz range.
In contrast to conventional analog frequency multipliers, the system does not degrade the phase noise of thesignal.
CI-P.13 FRIMultiple Scattering Layers As Physical Unclonable
Functions For Optical Wireless Communication∙A. Rates1 , J. Vrehen2 , B.L. Mulder1 , W.L. IJzerman2,3 ,and W.L. Vos1 ; 1 Complex Photonic Systems (COPS),MESA+ Institute for Nanotechnology, University ofTwente, Enschede, Netherlands; 2 Signify, Eindhoven,
Netherlands; 3 Department of Mathematics and Computer
Science, Eindhoven University of Technology, Eindhoven,
Netherlands
We study the correlation of light speckle between multiple scattering layers. Based on this, we propose an opticalwireless communication scheme using scattering media
as physical unclonable functions.
CI-P.14 FRI

Coherent combination of low-power optical signals:
A case study
J. Paczos1 , ∙K. Banaszek1,2 , and M. Jarzyna2 ; 1 Faculty ofPhysics, University of Warsaw, Warsaw, Poland; 2 Centre
for Quantum Optical Technologies, CeNT, University of
Warsaw, Warsaw, Poland
We analyze theoretically the quantum limit on combining coherently two light beams whose relative phase undergoes Gaussian diffusion. A threshold for the light intensity below which beam combination no longer operates efficiently is given.

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Hall B0
13:00 – 14:00

CJ-P.5 FRI

CJ-P.9 FRICJ-P: CJ Poster session
Compressive strain gradient for Stimulated Brillouinscattering mitigation in optical fibers∙A. Liméry, F. Gustave, L. Lombard, A. Durécu, and J. LeGouët; ONERA, Palaiseau, France
We report on our understanding of the compressive
strain gradient effect on the SBS Stokes spectrum, the
SBS threshold power and PER modification for single
mode Er:Yb doped fiber and PMF passive fiber.

Influence of Quantum Efficiency and Core
Propagation Loss on the Performance ofCladding-pumped Thulium-doped Fibre Lasers∙M. Buckthorpe and W. Clarkson; Optoelectronics Research Centre, University of Southampton, Southampton,
United Kingdom
A method for determining quantum efficiency and propagation loss in Thulium-doped fibres is presented. Results obtained using different doping profiles indicatethat propagation loss presents a major issue for power
scaling to the kilowatt regime.

Spectral broadening of low repetition rate pulses in afibre gain-managed nonlinear amplifier.
∙D. Stoliarov, E. Manuylovich, A. Koviarov, D. Galiakhmetova, and E. Rafailov; Aston Institute of Photonic
Technologies, College of Engineering and Physical Sciences, Aston University, Birmingham, United Kingdom
The impact of the modelocked low (1MHz) pulse repetition rate on spectral evolution in gain-managed nonlinear amplifiers based on a large mode area fibre wasnumerically and experimentally studied.

CJ-P.2 FRI

CJ-P.6 FRI

CJ-P.1 FRI

CJ-P.10 FRI

All-solid VLMA Yb-Doped Single-Mode PM Fiberwith 10dB/m Absorption for High Power Compact
Laser Applications∙A. Haboucha, L. Provino, T. Guezennec, A. Monteville,
D. Landais, and O. Legoffic; PHOTONICS BRETAGNE,LANNION, France
We report the design and manufacturing of a truly
single-mode VLMA fiber basis on a simple bend oriented all-solid step index principle, presenting an absorption about 10 dB/m and an optical efficiency up to70%.

Frequency Comb-based Seed Source for Spectral
Beam Combining with Enhanced Brillouin
Suppressing Properties∙S. Arora, S. Pal, L. C.G., and V.R. Supradeepa; Indian
Institute of Science, Bangalore, India
We demonstrate frequency comb-based seed source forspectral beam combining with enhanced Brillouin suppressing properties. We experimentally demonstrate
58% Brillouin threshold enhancement by line-shaping
the spectrum. We achieve 200GHz apart carriers required for beam combining.

Robust and low-phase noise all-PM figure-8
mode-locked fiber laser for spaceborne opticalfrequency comb
∙Y. Takeuchi1 , T. Kurihara1 , T. Yamada1 , S. Endo1 , S.
Matsushita2 , A. Suemasa2 , T. Sasaki2 , H. Takiguchi2 ,I. Kawano2 , S. Kogure2 , and M. Musha1 ; 1 The University of Electro-Communications, Chofu-shi, Japan; 2 Japan
Aerospace Exploration Agency, Tsukuba, Japan
We have developed a figure-8 mode-locked laser for aspaceborne photonic microwave generator, and its fceo
linewidth is less than 100kHz. The self-starting successrate of our laser is over 90% in space environment tests.

CJ-P.3 FRI

CJ-P.7 FRI

CJ-P.11 FRIInfluence of XPM in All-PM Fiber Oscillators
mode-locked using NPE in Linear Self-stabilized
Fiber Interferometers∙Y. Hua1 , M. Edelmann1,2 , F.X. Kärtner 1,2 , and I.
Hartl1 ; 1 Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany; 2 Department of Physics, Universität
Hamburg, Hamburg, Germany
In this work, we numerically demonstrate that asymmetric phase accumulation via XPM can distort modelocked steady-states in all-PM fiber laser mode-locked
by NPE in linear self-stabilized fiber interferometers.

Erbium-doped Lithium Niobate Waveguide
Amplifier∙M. Cai1 , K. Wu1 , D. Zhu2 , J. Long1 , and J. Chen1 ;1
State Key Laboratory of Advanced Optical Communication Systems and Networks, Department of Electronic
Engineering, Shanghai Jiao Tong University, Shanghai,
China; 2 Institute of Materials Research and Engineering,
Agency for Science, Technology and Research (A*STAR),
Singapore, Singapore
We demonstrate the Er-doped LNOI waveguide amplifier with 28.73 dB signal enhancement and 19.41 dB net
gain at 1531.5 nm, and the signal amplification at thewhole C band has been achieved.

3+

Investigation of wavelength tuning in Er : ZBLAN
fibre amplifier at 2.79 μm with nanosecond pulses∙P. Ray1 , A. Yadav1 , S. Cozic2 , F. Joulain2 , U. Hinze3,4 ,S. Poulain2 , E. Rafailov1 , and N. Chichkov1,3,4 ; 1 Aston
Institute of Photonic Technologies, Aston University,
Birmingam, United Kingdom; 2 Le Verre Fluor’e, Campus KerLann, Bruz, France; 3 Institute of Quantum Optics, Leibniz Universit¨at Hannover, Hannover, Germany;4
Laser nanoFab GmbH, Hannover, Germany
We investigate wavelength tunability in Er3+ : ZBLAN fibre amplifier operating in the mid-IR wavelengths centred at 2.79 μm, using nanosecond seed pulses generated
from a PPLN-OPO, demonstrating 26 dB gain and over
100 nm tunability.
CJ-P.4 FRICharacterization of power characteristics of 4-mm
ultra-short length laser cavity with a highly doped
Yb-Mg co-doped silica fiber∙Y. Matsui, Y. Koyama, and Y. Fujimoto; Chiba Instituteof Technology, Narashino, JapanThe 4-mm ultra-short length laser is fabricated using ahigh-concentration Yb-Mg co-doped fiber that can suppress the photodarkening effect. The output power of
145 μW is expected at pumping input of about 5 mW.

CJ-P.8 FRIExperimental Noise Characterization of a
Mid-infrared Mode-locked Er:ZBLAN Fiber Laser∙Y. Shi1 , C.R. Smith1 , C.R. Petersen1,2 , and O. Bang1,2 ;1DTU Electro, Technical University of Denmark, DK-2800
Kgs. Lyngby, Denmark; 2 NORBLIS ApS, Virumgade 35 D,
DK-2830 Virum, Denmark
We present for the first time characterization of therelative intensity noise in a mid-infrared mode-locked
Er:ZBLAN fiber laser. The results provide significant
value for noise-sensitive applications, such as supercontinuum generation.

CJ-P.12 FRI

Toward Super-continuum Generation in
Erbium-doped ZBLAN Fiber with Etched Fiber
Bragg Grating in the Mid-Infrared
I. Hendry1,2,3 , B. Dutta Gupta1,2,3 , S. Tang1,2,3 , M.
Erkintalo1,3 , and ∙C. Aguergaray1,2,3 ; 1 The University of
Auckland, Auckland, New Zealand; 2 The Photon Factory, Auckland, New Zealand; 3 The Dodd-Walls Centre
for Photonic and Quantum Technologies, Dunedin, New
Zealand
We report on our work attempting to generate supercontinua in the mid-infrared. We start by detailing
our mode-locked source laser constructions and perfor-

220

mance. We then state the performance of our amplification and nonlinear amplification steps, used to generate
supercontinua.
CJ-P.13 FRIFiber laser source for picosecond pulse generation
based on Mamyshev filtering∙V. Agrež, M. Marš, J. Petelin, and R. Petkovšek; University of Ljubljana, Faculty of Mechanical Engineering,
Ljubljana, Slovenia
A Laser diode, two-stage Mamyshev filtering, doublepass amplification in first stage and a tunable filter areused to achieve pulses with less than 4 ps duration withno addition pulse compression at the output.
CJ-P.14 FRI

Cascade lasing optimization in Dy-doped ZBLAN
fiber lasers for efficient yellow emission∙M. Federico and F. Poli; Department of Engineering andArchitecture, University of Parma., Parma, Italy
A self-developed, matrix-based simulation model using rate equations was applied to examine the influenceof mid-infrared cascade lasing around 3 μm on yellow
emission of ZBLAN Dy-doped fiber lasers, providing
useful guidelines for performance improvement.
CJ-P.15 FRIFiber optical parametric oscillator delivering signal
pulse tunable in wavelength and pulse duration∙M. Ghawas1 , O. Zurita-Miranda1 , V. Freysz2 , and E.
Freysz1 ; 1 Univ. Bordeaux,CNRS, LOMA UMR 5798,
Talence 33400, France; 2 Alphanov, Institut d’Optiqued’Aquitaine, Talence 33400, France
We designed and built an optical parametric oscillator
based on PCF fiber. Pumped by an ytterbium picosecond fiber oscillator, it delivers signal pulses tunable inwavelength and pulse duration. Its performances and capabilities are analyzed.
CJ-P.16 FRI

Replica Symmetry Breaking enabled by Rayleighscattering in a Random Fiber Laser∙B. Costa Lima1 , P. Tovar2 , A. Lima Moura3 , and J.P.
von der Weid1 ; 1 Center for Telecommunications Studies,
Pontifical Catholic University of Rio de Janeiro, Rio deJaneiro-RJ, Brasil; 2 Department of Physics, University ofOttawa, Ottawa, Canada; 3 Programa de Pós-graduação
em Física, Instituto de Física, Universidade Federal de
Alagoas, Maceió-AL, Brasil
We report the observation of Replica Symmetry Breaking in a Random Fiber Laser with oscillation sustainedby the weak backscattering of light. The conditions wereobtained by reducing environmental perturbation on the
scattering medium.

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Hall B0
CJ-P.17 FRI

CJ-P.19 FRI

CJ-P.21 FRIAsymmetric gain-guided pulses
S. Turitsyn1 , ∙A. Bednyakova2 , and E. Podivilov3 ;1Aston Institute of Photonic Technologies, Birmingham,
United Kingdom; 2 Novosibirsk State University, Novosibirsk, Russia; 3 Institute of Automation and Electrometry,
Novosibirsk, Russia
A generic model governing optical pulse propagation ina nonlinear dispersive medium with asymmetric gain is
introduced. Our results provide insight into the natureof asymmetric pulses capable to accumulate large nonlinear phase without wave-breaking.

70W, 1MHz, sub-50fs Yb-doped fiber laser system forhigh harmonic generation∙S. Malekmohamadi1,2 , M. Pergament1 , Y. Liu1,2 , M.
Seidel3 , M. Edelmann1,2 , M. Kellert1 , C.M. Heyl3,4 ,and F.X. Kaertner1,2 ; 1 Center for Free-Electron Laser
Science CFEL, Deutsches Elektronen-Synchrotron DESY,
Notkestr. 85, 22607 , Hamburg, Germany; 2 Departmentof Physics, Universität Hamburg, Jungiusstr. 9, 20355 ,Hamburg, Germany; 3 Deutsches Elektronen-Synchrotron
DESY, Notkestr. 85, 22607 , Hamburg, Germany;
4
Helmholtz Institute Jena, Fröbelstieg 3, 07743 , Jena, Germany
We present the development of a Yb-doped fiber laser
system that generates 44 fs laser pulses with a pulse energy of up to 70 μJ at a repetition rate of 1 MHz for highharmonic generation.

Spectrally and repetition rate tunable femtosecond
fiber laser for two-photon biomedical imaging
applications∙D. Stachowiak, J. Bogusławski, and G. Soboń; Laser &Fiber Electronics Group, Wrocław University of Scienceand Technology, Wrocław, Poland
We present a femtosecond frequency-doubled erbiumdoped fiber laser which is spectrally and repetition rate
tunable. These features, as well as its compactness, makeour source an attractive alternative to commercial andcommonly used titanium-sapphire lasers.

CJ-P.18 FRI

1.2 W average power deep-UV light at 229 nm
generated by a frequency-quadrupled Nd-doped fiber
laser
K. Le Corre1,2 , R. Florentin1 , A. Barnini2 , T. Robin2 ,B. Cadier2 , H. Gilles1 , S. Girard1 , and ∙M. Laroche1 ;1
CIMAP, Caen, France; 2 Exail, Lannion, France
We present a frequency quadrupled Nd-doped fiber laser
system generating >1W at 229nm. The laser configuration is based on a gain-switched laser diode and Nddoped PM fiber amplifiers optimized for the laser transition at 900nm.

13:00 – 14:00
CL-P: CL Poster session
CL-P.1 FRI

Towards the development of a SWIR-LEDs based
optoelectronic system for urea monitoring duringhaemodialytic therapy∙E. Bodo, V. Bello, and S. Merlo; Department of Electrical, Computer and Biomedical Engineering, University ofPavia, Pavia, Italy
We provide the proof of concept of urea concentration
detection by means of amplitude measurement, specifically exploiting the urea absorption band around λ =2.15 μm, that can provide valuable information about
dialysis efficiency.
CL-P.2 FRIClassification of clinically significant prostate cancer
using Raman spectroscopy and Support Vector
Machine classification∙S.J. van Breugel1,2,3 , I. Low4 , M.L. Christie4 , M.R.
Pokorny4 , H.U. Holtkamp1,3 , M.K. Nieuwoudt1,2,3 ,CJ-P.20 FRIRaman lasing in multimode diode-pumped
graded-index fiber with fs-inscribed random
structures
A.G. Kuznetsov, A.A. Wolf, ∙Z. Munkueva, A.V. Dostovalov, and S.A. Babin; Institute of Automation and Electrometry SB RAS, Novosibirsk, Russia
We obtain Raman lasing in multimode diode-pumped
GRIN fiber with artificial random structures of Rayleightype or random array of short FBGs, for which 976-nm
Stokes power reaches 28W, beam quality M2~2.1, spectrum is stable.
M.C. Simpson1,2,3,5 , K. Zargar-Shoshtari4,6 , and C.
Aguergaray2,3,5 ; 1 School of Chemical Sciences, University of Auckland, Auckland, New Zealand; 2 The
Dodd-Walls Centre for Photonic and Quantum Technologies, Dunedin, New Zealand; 3 The Photon Factory, University of Auckland, Auckland, New Zealand;
4
Counties Manukau District Health Board, Auckland,
New Zealand; 5 Department of Physics, University of
Auckland, Auckland, New Zealand; 6 Faculty of Medicaland Health Sciences, University of Auckland, Auckland,
New Zealand
Raman spectroscopy and support vector machine classification are combined to detect clinically significant
prostate cancer on a data set of 152 patients. The reported cohort and classification performance are thehighest reported to date.
CL-P.3 FRIEx Vivo Breast Cancer Tissue Classification Using
Hyperspectral Endoscopy Imaging with Deep
Learning
S. Zhang1 , ∙S. Zeng2 , R.R.Z. Tan1 , W. Liao1 , and M.

CJ-P.22 FRIThulium Fibre Lasers for Quantum Applications∙A. Pertoldi1,2 , P. Varming2 , and P. Bowen Montague2 ;Niels Bohr Institute, University of Copenhagen, Blegdamsvej 17, 2100 Copenhagen, Denmark, Copenhagen,Denmark; 2 NKT Photonics, Birkeroed, Denmark
Thulium is a gateway element for fiber lasers to deliver
new wavelengths in atomic cooling experiments. Lownoise modular lasers and frequency conversion systems
will allow the development of a new generation of compact atomic clocks.
1

CJ-P.23 FRIHighly efficient frequency doubling of
ultrashort-pulse fiber laser at 1700 nm in PPLN bulk
and waveguide crystals∙A. Koviarov, D. Stoliarov, D. Galiakhmetova, and E.
Olivo1 ; 1 Institute of Materials Research and Engineering(IMRE), Singapore, Singapore; 2 Université de Technologie, Troyes , France
We present a hyperspectral imaging endoscope with anultrathin imaging fiber for the classification of ductal
carcinoma, non-ductal carcinoma, and healthy breast
tissues. Deep learning was applied, and an accuracy of
97.89% was achieved.
CL-P.4 FRILabel-Free Cancer Classification Using Hyperspectral
Imaging Microscopy and Machine Learning
S. Zhang1 , ∙S. Zeng2 , W. Liao1 , R.R.Z. Tan1 , and M.
Olivo1 ; 1 Institute of Materials Research and Engineering(IMRE), Singapore, Singapore; 2 Université de Technologie, Troyes , France
Hyperspectral imaging combined with darkfield andphase contrast microscopy was used to image label-freeunstained breast tissue slides. Machine learning was applied for cancer classification and an accuracy above 96%
was achieved.

221

Rafailov; Aston Institute of Photonic Technologies, Aston
University , Birmingham, United Kingdom
The laser system based on frequency-doubling of 16251700 nm radiation was demonstrated. Both waveguideand bulk PPLN crystals were used for SHG. Up to 54
mW/10 MHz was obtained with pulse duration of ~100fs.
CJ-P.24 FRI

All-Fiber Bandpass Spectral Filter Based on Negative
Curvature Hollow-Core Optical Fiber (NC-HCF)∙A. Borodkin, A. Jasim, O. Podrazký, and P. Honzátko; Institute of Photonics and Electronics, The Czech Academyof Sciences, Prague, Czech Republic
Bandpass spectral filter based on a hollow-core fiber
compatible with standard single-mode fibers is presented. Insertion loss less than 1 dB and the minimumtransmission band of 33 nm at 1 μm are achieved.
CJ-P.25 FRIAdvances in YAG derived optical fibre∙C.M. Harvey and M. Fokine; KTH Royal Institute ofTechnology, Stockholm, Sweden
We explore the performance of a CO laser-based draw
tower for YAG-core silica-clad optical fibre. The minimal
hot zone demonstrated a significant reduction in silicondiffusion into the YAG core during fabrication.

CL-P.5 FRIHolography of biomimetic structures based on
butterfly wings for image sensing∙H. Skenderovic, N. Demoli, A. Mardan Dezfouli, D.
Abramovic, and M. Rakic; Institute of Physics, ZAGREB,
Croatia
An outlook for a compact imaging device withbiomimetic focal plane array based on holographic
reading and fast numeric reconstruction, operating in a
broad spectral range is described.
CL-P.6 FRI

Tissue Structure Information Retrieval from
Backscattering Polarization Sensitive Measurements
L. Roth, ∙A. Stefanov, and M. Frenz; Institute of Applied
Physics, University of Bern, Bern, Switzerland
We present a method based on Cloude decomposition toquantify the degree of anisotropy of brain tissue and theorientation of the nerve fibers by polarimetric measurement of the backscattered light.

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Hall B0
Short Time HRV Assessment Based on a Fiber Optic
Sensor∙W. Lyu, Y. Li, S. Chen, Q. Wang, and C. Yu; Photonics Research Institute, Department of Electronic and Information Engineering, The Hong Kong Polytechnic University,
Hong Kong, China
A fiber optic sensor-based vital signs mornitoring system can assess short time heart rate variability (HRV).
The HRV of subject with cardiovascular disease is significantly different from that of healthy people.

Física de Materiales, Facultad de Ciencias, Universidad
Autónoma de Madrid, Madrid 28049, Spain; Nanomaterials for Bioimaging Group (nanoBIG), Instituto Ramón yCajal de Investigación Sanitaria, Hospital Ramón y Cajal,
Madrid, Spain
It was demonstrated how shifting the operation rangeof luminescent nanothermometers to the third biological window opens the venue to reliable thermal sensing within tissues. This possibility has been experimentally demonstrated by using Yb3+/Er3+/Tm3+:CaF2
nanoparticles.

CL-P.8 FRI

CL-P.11 FRI

CL-P.7 FRI

A realistic determination of the thermal effects
generated in human skin during laser-skin thermal
treatment∙J. Toumi; Higher Institute of Laser Research and Applications, Damascus University, Damascus, Syria
We take in-vivo measurements of optical parameters ofhuman skin and couple them to simulation to predictheat distribution in skin during laser-skin treatment.
The results are verified with thermal measurements tooptimize the treatment.
CL-P.9 FRI

GaSe-based fiber optic sensor for human healthmonitoring∙C. Odaci1,2 , M.S. Khan2 , M. Grüneberg2 , T. Beduk2 , M.
Montagnese2 , A. Roshanghias2 , and U. Aydemir1 ; 1 Bursa
Uludag University, Bursa, Turkey; 2 Silicon Austria Labs
GmbH, Villach, Austria
We report on a SPR-based fiber optic sensor coated with
GaSe material for lactate detection for human healthmonitoring. The sensor is characterized for change in therefractive index with respect to lactate concentration.
CL-P.10 FRI

Lanthanide Doped Nanoparticles for Reliable andPrecise Luminescent Nanothermometry in the Third
Biological Window
A.C.C. Soares1 , T.O. Sales1 , E.C. Ximendes2 , D. Jaque2 ,and ∙C. Jacinto1 ; 1 Group of Nano-Photonics andImaging, Instituto de Física, Universidade Federal de
Alagoas, 57072-900, Maceió-AL, Brazil; 2 Nanomaterials
for Bioimaging Group (nanoBIG), Departamento de

Optical trapping of micro-particles and bacterial
cells in a flow-focusing microfluidic device∙A. Esan1,2 , C. Steed1,2 , C. McGoverin1,2 , S. Swift3 ,and F. Vanholsbeeck1,2 ; 1 Department of Physics, University of Auckland, Auckland, New Zealand; 2 The
Dodd-Walls Centre for Photonic and Quantum Technologies, Dunedin, New Zealand; 3 Department of Molecular
Medicine and Pathology, University of Auckland, Auckland, New Zealand
We present the optimal trapping power and hydrodynamic flow conditions for achieving single-cell opticaltrapping of bacterial cells in a microfluidic device that
integrates optical tweezers and incorporates both vertical and horizontal flow-focusing.
CL-P.12 FRIBrightness-enhanced Light Sources for Medical
Imaging∙B. Ford, S. Long, and J. Sathian; Northumbria University,
Newcastle, United Kingdom
Luminescent concentrators generate intense light, suitable for medical illumination applications. However, extraction of this light is challenging. We report a simple fibre coupling system allowing significant light extraction
alongside long lifetime for ageing technology replacement.

Design structural patterns, replace metal and dielectricmaterials with graphene to generate surface plasmons,and achieve modulation effects. A molecular fingerprintof mock analyte immunoglobulin G.

short-wave infrared (SWIR) light to image biomedical
samples in 3D is reported. Contrast for sample structures is provided by specific absorption or fluorescencein the SWIR spectral range.

CL-P.14 FRI

CL-P.17 FRIImage Reconstruction Improvement of Variable
Coded Aperture using Deep Learning Method for
Gamma and Lensless Imaging Applications∙A. Schwarz1 , A. Shemer1 , E. Danan2 , N.E. Cohen3 , and
Y. Danan1 ; 1 Department of Electrical and Electronics Engineering, Azrieli College of Engineering, Jerusalem, Israel; 2 Faculty of Engineering, Bar-Ilan University, Ramat
Gan, Israel; 3 School of Software Engineering and Computer Science, Azrieli College of Engineering, Jerusalem,
Israel
A combination of deep convolutional encoder-decoder
neural network with time multiplexed coded aperture isused for gamma imaging in nuclear medicine and lensless imaging. The method improves sensitivity and SNR
while challenging inverse filter limitations.

Impact of pulse modulation for Moses Ho: YAG laser
lithotripsy in urinary tract model∙K. Kim1 , Y.-S. Seo2 , and J.B. Eom1 ; 1 Departmentof Biomedical Science, Dankook University School of
Medicine, Cheonan , South Korea; 2 R&D center, Wontech
Co. Ltd., Daejeon, South Korea
We compared the efficiency of lithotripsy and bubble
characteristics according to pulse modulation for Moses
Ho: YAG laser lithotripsy using a high-speed camera in
the urinary tract model.

CL-P.15 FRI

Eight-wavelength Digital Inline Holography andBrightfield Imaging in a single microscope∙S. Dixneuf1 , T. Olivier2 , Z. Sedaghat1 , L. Thibon1 ,R. Montvernay3 , E. Degout-Charmette3 , N. Faure3 , C.
Kolytcheff3 , C. Fournier2 , C. Védrine1 , Q. Josso3 , and F.
Mallard3 ; 1 BIOASTER, Bioassays, Microsystems and Optical Engineering Unit, Lyon, France; 2 Laboratoire Hubert Curien UMR 5516, F-42023, Saint-Etienne, France;
3
bioMérieux SA, Clinical Unit, Marcy l’Etoile, France
We propose a double modality microscope based on (incoherent) Brightfield imaging and 8-wavelength Digital Inline Holographic Microscopy (DIHM) to compare
standardization and informativeness in the context of thediscrimination of stained microbiological objects.
CL-P.16 FRIMeasurement of Immunoglobulin G Based on
Infrared-Enhanced Absorption Spectroscopic
Biosensing with Graphene
Y.-H. Chen, ∙Y.-A. Wei, and C.-S. Yang; National Taiwan
Normal University, Taipei , Taiwan.

Development of an Optical Projection Tomography(OPT) Setup Operating in the Short-Wave Infrared(SWIR) Region∙S.M. Steinecker, C. Pilger, M. Müller, J.C. Schürstedt,
G. Wiebusch, M. Schüttpelz, and T. Huser; Biomolecular
Photonics, Bielefeld University, Bielefeld, Germany
An optical projection tomography system that uses

13:00 – 14:00

EC-P.1 FRI

1

EC-P: EC Poster session

Observation of interaction-induced topological
doublon states∙J. Beck1 , H. Drüeke1 , M.J. Meschede1 , M. Heinrich1 , F.S.
Piccioli1,2 , S. Weidemann1 , D. Bauer1 , and A. Szameit1 ;CL-P.13 FRIInstitute for physics, University Rostock, Rostock, Germany; 2 INO-CNR BEC Center and Dipartimento di
Fisica, Universita‘ di Trento, Trento, Italy
We present the first observation of propagating topologically protected doublon states in an anomalous Floquet

222

CL-P.18 FRICompact Multichannel Imaging System with Wide
FOV and 4x Optical Magnification∙C. Katopodis1 , I. Zergioti1 , and D. Papazoglou2,3 ;1
Department of Physics, National Technical Universityof Athens, Athens, Greece; 2 Institute of Electronic Structure and Laser, Foundation for Research and TechnologyHellas, Heraklion, Greece; 3 Department of Material Science and Technology, University of Crete, Heraklion,
GreeceA novel multichannel imaging system based on commercially available micro-lens arrays and a micro-scanningtechnique to achieve high resolution and wide field ofview (7 x 7mm2) at 4x optical magnification.
CL-P.19 FRIExploring Spinal Cord Regeneration in Zebrafish by
Using the Plasmid-Carried Fluorescent Carbon
Nanodots∙F.-C. Chien, Y.-C. Huang, C.-C. Cheng, Y.-W. Li, W.
Chung, and C.-L. Luo; Department of Optics and Photonics, National Central University, Taoyuan 32001, Taiwan
Small-sized plasmid-carried fluorescent carbon nanodot, manifesting low toxicity, good biocompatibility,
superior photoluminescence signal, and high efficiency
of cell uptake was fabricated to improve the neuron differentiation and spinal cord repair in zebrafish.

driven 1D array. Using dimensional mapping, the two
repulsive interacting particles in 1D were observed in 2D
laser-written waveguide lattices.

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Hall B0
EC-P.2 FRI

Bimorphic Floquet Topological Insulators for Light∙J. Beck1 , G.G. Pyrialakos2,3 , M. Heinrich1 , L.J.
Maczewsky1 , M. Khajavikhan4 , N.V. Kantartzis3 , A.
Szameit1 , and D.N. Christodoulides2 ; 1 Institute forphysics, Univ. Rostock, Germany; 2 College of Optics &Photonics-CREOL, Univ. of Central Florida, Orlando,
USA; 3 Department of Electrical and Computer Engineering, Aristotle Univ. of Thessaloniki, Greece; 4 Ming Hsieh
Department of Electrical and Computer Engineering,
Univ. of Southern California, Los Angeles, USA
We introduce a novel class of Floquet topological insulators simultaneously hosting Chern-type and anomalousedge states. The driving mechanism is implemented ina chained honeycomb lattice, allowing us to observe its
different chiral edge states.
EC-P.3 FRIFractal photonic topological insulators for light∙M. Heinrich1 , T. Biesenthal1 , L. Maczewsky1 , Z. Yang2 ,M. Kremer1 , M. Segev3 , and A. Szameit1 ; 1 Institut
für Physik, Universität Rostock, Rostock, Germany;
2
Department of Physics, Zhejiang University, Zhejiang,
China; 3 Physics Department and Solid State Institute,
Technion, Haifa, Israel
We present the first experimental observation of a fractal
topological insulator for light and demonstrate how the
self-similar properties of the Sierpinski gasket systematically enhance wave transport its topologically protectededge states.
EC-P.4 FRI

Physical limits on non-Hermitian topology in passive
systems∙H. Schomerus; Lancaster University, Lancaster, United
Kingdom
I contrast fundamental limits on physical properties inpassive and active non-Hermitian systems. While active
systems suffer from noise, passive systems are limited bycausality - making many desirable effects difficult to observe.

laterra, Spain; University of Aveiro, Aveiro, Portugal
We propose a method to implement any n-root of the
Su-Schrieffer-Heeger model in a lattice of optical ring
resonators, which displays an asymmetric coupling distribution that allows to build non-Hermitian systems.
2

EC-P.6 FRIStrong-field valley polarization in inversion
symmetric bulk 2H-MoS2∙I. Tyulnev1 , Á. Jiménez-Galán2 , J. Poborska1 , L. Vamos1 ,O. Smirnova2,3 , M. Ivanov2,4,5 , and J. Biegert1,6 ; 1 ICFO
- Institut de Ciencies Fotoniques, The Barcelona Institute of Science and Technology, Barcelona, Spain; 2 MaxBorn-Institut, Berlin, Germany; 3 Technische Universität
Berlin, Berlin, Germany; 4 Institut für Physik, HumboldtUniversität zu Berlin, Berlin, Germany; 5 Department of
Physics, Imperial College London, London, United Kingdom; 6 ICREA - Institución Catalana de Investigación yEstudios Avanzados, Barcelona, Spain
We demonstrate a novel mechanism of strong-field induced valley control in inversion symmetric MoS2, independent of limitations imposed by resonant valley selection rules.
EC-P.7 FRIOptical dispersion in waveguides based upon the
Pancharatnam-Berry phase∙S.V. Arumugam1 , C.P. Jisha1 , A. Alberucci1 , and S.
Nolte1,2 ; 1 Friedrich Schiller University, Institute of Applied Physics, Albert-Einstein-Str. 15, 07745,, Jena, Germany; 2 Fraunhofer Institute for Applied Optics and Precision Engineering IOF, Albert-Einstein-Str. 7, 07745, Jena,
Germany
A Pancharatnam-Berry phase (PBP) based waveguideconfines light in the absence of a refractive index gradient. We theoretically investigate the dispersion properties and the robustness of the PBP waveguide.
EC-P.8 FRI

n-Root of the Su-Schrieffer-Heeger Model on a
Photonic Ring Resonator Lattice∙D. Viedma1 , A.M. Marques2 , R.G. Dias2 , and V.
Ahufinger1 ; 1 Universitat Autònoma de Barcelona, Bel-Power Eigenchannels of non-Hermitian media∙K. Makris1,2 and D. Psaltis3 ; 1 ITCP-Physics Department, University of Crete, Heraklion, Greece; 2 Instituteof Electronic Structure and Laser (IESL)-FORTH, Heraklion, Greece; 3 Optics Laboratory, Ecole Polytechnique Federale de Lausanne (EPFL), Lausanne, Switzerland
We introduce the concept of non-Hermitian eigenchannels based on the singular value decomposition of the

13:00 – 14:00

EI-P.1 FRI

EI-P: EI poster session

Miniaturized Spectrometer with Bias-Configurable
Two-Dimensional Semiconductor/Metal Schottky
Junction

EC-P.5 FRI

associated propagator. Thus we determine the optimal
wavefronts that lead to maximal/minimal amplificationin any non-Hermitian guided structure.
EC-P.9 FRIState Tomography of Complex Electromagnetic
Pulses∙L. Vignjevic1 , Y. Shen1 , S. Pidishety1 , N. Papasimakis1 ,and N. Zheludev1,2 ; 1 Optoelectronics Research Centre& Centre for Photonic Metamaterials, University ofSouthampton, Southampton, United Kingdom; 2 Centre
for Disruptive Photonic Technologies, Nanyang Technological University, Singapore, Singapore
We present a new approach to characterising complex transient electromagnetic excitations and experimentally demonstrate it on light pulses of toroidal
topology quantifying their space-polarization and spacefrequency nonseparability and fidelity with respect totheoretical expectations.
EC-P.10 FRI

Tailoring Intensity Statistics of 3D Speckles∙S. Han1 , N. Bender2 , and H. Cao1 ; 1 Yale University, New
Haven, USA; 2 Cornell University, Ithaca, USA
We develop a method for tailoring optical speckle intensity statistics in three dimensions. By wavefront shaping of a laser beam, we generate volumetric speckle fields
with target intensity statistics and distinct topologies atmultiple planes.
EC-P.11 FRIFabrication of symmetric SOI photonic crystal slabs
and their topological bandgaps and edge modes
A. Begum1,2 , Y. Yao1,2 , T. Kuroda1 , Y. Takeda1,2 , N.
Ikeda1 , Y. Sugimoto1 , T. Mano1 , H. Koyama1 , and∙K. Sakoda1 ; 1 National Institute for Materials Science,
Tsukuba, Japan; 2 University of Tsukuba, Tsukuba, Japan
We fabricated symmetric SOI photonic crystals with
topological bandgaps and edge modes for the lowestorder symmetric TE-like modes by EB lithography and
PECVD of a SiO2 capping layer, which we confirmed byangle-resolved reflection spectroscopy.
EC-P.12 FRIExperimental observation of optical Hilbert’s Hotelin vector beam
∙A. Ghosh1 , S. Kumar1,2 , C. Kaushik1,2 , A. Shiri3 , G.

∙X. Cui, F. Nigmatulin, M. Du, A.C. Liapis, H.H. Yoon,
and Z. Sun; QTF Centre of Excellence, Department ofElectronics and Nanoengineering, Aalto University, Espoo, Finland
223

Gbur3 , S. Sharma4 , and G.K. Samanta1 ; 1 Physical Research Laboratory, Ahmedabad, India; 2 Indian Institute of Technology Gandhinagar, Ahmedabad, India;
3
Department of Physics and Optical Science, Universityof North Carolina Charlotte, Charlotte, USA; 4 Dynotech
Instruments Pvt Ltd, New Delhi, India
We report on the simple experimental implementationof Hilbert’s hotel using a fractional vector beam generated by illuminating the spiral phase-plate of integer
topological charge for a designed wavelength by supercontinuum laser of tunable wavelength.
EC-P.13 FRIAiry – like beam with nonhomogeneous polarization
structure and bimeronic lattice∙J. Berškys and S. Orlov; State research institute Center for
Physical Sciences and Technology, Vilnius, Lithuania
Airy beam with a nonhomogeneous polarization structure is introduced and properties, including its Fourier
spectrum and possible ways of generation, are examined.
Also, the bimeronic lattice in the domain of the normal
to the polarization ellipse is observed.
EC-P.14 FRI

Identifying Topology of Photonic Lattices with
Machine and Deep Learning∙L. Smirnov1 , E. Smolina1 , D. Leykam2 , and D.
Smirnova3,4 ; 1 Nizhny Novgorod State University, Nizhny
Novgorod, Russia; 2 National University of Singapore, Singapore, Singapore; 3 Australian National University, Canberra, Australia; 4 RIKEN, Wako-shi, Japan
We show how the machine learning can be applied toclassify topological phases in photonic lattices. We design a neural network determining topology from theoutput intensity distribution in dimerized waveguide arrays with leaky channels.
EC-P.15 FRI

Near-normal incidence photonic spin Hall effect formaterial characterization∙J.J. Panda, G. Rajalakshmi, and T.N. Narayanan; Tata
Institute of Fundamental Research, Hyderabad, India
We demonstrate the ability to characterize optical properties of dielectric materials using the photonic spin Hall
effect (PHE) in near-normal incidence configuration.
This approach provides significant advantages over theconventional PHE measurement technique.

The computational reconstruction algorithm has openeda new pathway for spectrometer miniaturization via optoelectronics. Based on this algorithm, we demonstrate
a miniaturized spectrometer with a bias-configurable
Schottky junction.

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Hall B0
EI-P.2 FRI

The initial time-delay response of reflectivity changes
in photoexcited two-dimensional layered
semiconductor 2H − MoTe2∙T. Fukuda1 , P. Fons2 , K. Makino3 , Y. Saito3 , K. Ueno4 , J.
Afalla1 , and M. Hase1 ; 1 University of Tsukuba, Tsukuba,
Japan; 2 Keio University, Yokohama, Japan; 3 National Institute of Advanced Industrial Science and Technology,
Tsukuba, Japan; 4 Saitama University, Saitama, Japan
Ultrafast reflectivity changes ΔR/R of two-dimensional
layered semiconductor 2H − MoTe2 have been investigated by pump-probe spectroscopy.
Fluencewavelength-dependence measurements revealed that thephotoexcited electron-hole plasma dramatically modified the ΔR/R spectra in early time delay within 1 ps.
EI-P.3 FRIMicroscopic Z-Scan for Measuring Nonlinear
Absorption of Mechanically Exfoliated Transition
Metal Dichalcogenide Monolayers∙T. Possmayer1 , L. Sortino1 , S.A. Maier2,3,1 , and
L.d.S. Menezes1,4 ; 1 Nano-Institut München, Fakultät für
Physik, Ludwig-Maximilans-Universität München, 80539

13:00 – 14:00

München, Germany; School of Physics and Astronomy, Monash University, Clayton, Victoria 3800, Australia; 3 Department of Physics, Imperial College London,
London SW7 2AZ, United Kingdom; 4 Departamento deFísica, Universidade Federal de Pernambuco, 50670-901
Recife-PE, Brazil
We demonstrate a microscopic Z-scan setup capable ofcharacterizing mechanically exfoliated monolayers withsizes below 10 μm. This is used to measure the nonlinear
absorption of common transition metal dichalcogenides
around the exciton resonances.

FORTH/ICE-HT, Patra, Greece; 6 Naval Research Laboratory, Washington, USA; 7 Dept. of Physics and Astronomy, Univ. of Sussex, Brighton, United Kingdom; 8 Schoolof Physics, Dept. of Solid-State Physics, Aristotle Univ. ofThessaloniki, Greece
The locally deformed armchair orientation of a strainedmonolayer WS2 is imaged with optical means using Polarization Resolved Second Harmonic Generation. A
characteristic cross-shaped pattern is proven to be thefingerprint of strain.

EI-P.4 FRIS-SNOM Imaging of Stacking Order in Few-Layer
Graphene∙D. Beitner1,2,3 , S. Amitay3 , S. Sallah Atri3 , S. Richter 1,2 ,H. Suchowski 2,3 , and M. Ben Shalom2,3 ; 1 Department ofMaterials Science and Engineering Faculty of Engineering
Tel Aviv University, Tel Aviv, Israel; 2 University Centre for
Nanoscience and Nanotechnology Tel Aviv University, TelAviv, Israel; 3 School of Physics and Astronomy, Faculty of
Exact Sciences, Tel Aviv University,, Tel Aviv, Israel
Tetralayer graphene has three unique stacking configurations. Using single wavelength Near Field Scanning

2

Identification of non-uniform strain in WS2
monolayers using P-SHG∙G. Kourmoulakis1,2 , S. Psilodimitrakopoulos1 , G.
Maragkakis1,3 , L. Mouchliadis1 , A. Michail4,5 , J.
Christodoulides6 , M. Tripathy7 , J. Parthenios5 , K.
Papagelis5,8 , E. Stratakis1,3 , and G. Kioseoglou1,2 ;1FORTH/IESL, Heraklion, Greece; 2 Dept. of Materials Science and Technology, Univ. of Crete , Heraklion,
Greece; 3 Dept. of Physics, Univ. of Crete , Heraklion,
Greece; 4 Dept. of Physics, Univ. of Patra, Patra, Greece;

JSIII-P: JSIII Poster session- based laser direct writing in polymer on glass and onchip for neuromorphic computational networks.

JSIII-P.1 FRIJSIII-P.3 FRI

A 3-layer injection-locked multimode semiconductor
laser neural network∙E. Robertson1,3 , A. Skalli2 , R. Lance2 , X. Porte2 , J.
Wolters1,3 , and D. Brunner2 ; 1 Institut für Optische Sensorsysteme, Deutsches Zentrum für Luft und Raumfahrt, Berlin, Germany; 2 Institut FEMTO-ST, UniversitéFranche-Comté, Besancon, France; 3 Institut für Optik
und Atomare Phyik, Technische Universität Berlin, Berlin,
Germany
We present a deep photonic network created by cascading three mutually coupled large vertical cavity surface
emitting lasers, demonstrate their locking to an external
injection laser, and investigate their spectral and spatial
response.

Study of the C-band dynamical response of an
injection locked LA-EEL for fully integrated
telecommunication data processing∙R. Lance1 , A. Skalli1 , X. Porte2 , and D. Brunner1 ;1Université Bourgogne Franche-Comté, FEMTO-ST, Optics Department, Besançon, France; 2 Institute of Photonics, Department of Physics, University of Strathclyde,
Glasgow, United Kingdom
Fully parallel high bandwidth photonic reservoir implemented using injection locking effect in highly multimodal semiconductor laser. Spatial projection and imaging on a digital micromirror device provides reading
and allow hardware integration of programmable output
weights.

JSIII-P.2 FRI

JSIII-P.4 FRI

3D Polymer Interconnects for Neuromorphic
Photonics Technologies
A. Andrishak, T.L. Alves, R.M.R. Adão, C. Maibohm,
B. Romeira, and ∙J.B. Nieder; INL-International Iberian
Nanotechnology Laboratory, Ultrafast Bio- and Nanophotonics Group, Braga, Portugal
Free standing and crossing 3D optical interconnects
spanning several hundreds of micrometers were successfully fabricated using two photon polymerisation (TPP)

Visualizing and Understanding Optoelectronic
Neural Networks via the Orbital Angular Momentumof Light∙H. Wang1 , J. Hu2 , Z. Zhan1 , X. Fu1 , and Q. Liu1 ;1Tsinghua University, Department of Precision Instrument, Beijing, China; 2 Laboratoire Kastler Brossel, Collège de France, Paris, France
We propose a hardware-algorithm-united model interpretation method for optoelectronic neural networks

5

EI-P.5 FRIMicroscopy, we demonstrate the ability to detect all threepossible stacking configurations. By an analytical model,
we can quantitively extract dielectric parameters.
EI-P.6 FRISecond-order nonlinearity of excitons in
hBN-encapsulated monolayer transition metal
dichalcogenides∙S. Takahashi1 , S. Kusaba1 , K. Watanabe2 , T. Taniguchi3 ,K. Yanagi4 , and K. Tanaka1,5 ; 1 Department of Physics,
Kyoto University, Kyoto, Japan; 2 Research Center for
Functional Materials, National Institute for Materials Science, Tsukuba, Japan; 3 International Center for Materials Nanoarchitectonics, National Institute for Materials
Science, Tsukuba, Japan; 4 Department of Physics, Tokyo
Metropolitan University, Tokyo, Japan; 5 Institute for Integrated Cell-Material Sciences, Kyoto, Japan
P-series excitons besides s-series were observed by sum
frequency generation spectroscopy in monolayer transition metal dichalcogenides. New insights into nonlinear
optical responses were obtained from energy level structures and polarization dependences.

when measuring orbital angular momentum of light tounderstand the feature-extraction mechanisms of optical layers and to improve the detection efficiency up to
25-fold.

plex™ platform, a hyperspectral imaging concept that
addresses the high cost and slow acquisition of current
state-of-the-art hyperspectral imaging systems by using
universal metasurface hardware encoders.

JSIII-P.5 FRIJSIII-P.7 FRI

Improving the performance of photonic delay-based
reservoir computing by phase modulating the input
signal∙I. Bauwens1 , K. Harkhoe1 , P. Bienstman2 , G.
Verschaffelt1 , and G. Van der Sande1 ; 1 Applied Physics
Research Group, Vrije Universiteit Brussel, Brussels,
Belgium; 2 Photonics Research Group, Department ofInformation Technology, Ghent University-IMEC, Ghent,
Belgium
Based on numerical studies of a delay-based reservoir
computing system with semiconductor lasers, we areable to improve the performance of such systems bymodulating the phase, rather than the amplitude of theinjected signal.

Influence of absorber carrier lifetimes on the
excitability regime of an integrated two-section InP
laser neuron∙L. Puts, D. Lenstra, K. Williams, and W. Yao; Eindhoven
University of Technology, Eindhoven, Netherlands
The Yamada model is used to investigate the effects ofsaturable absorber carrier lifetimes on the excitability
operation regime of an integrated InP laser neuron. A
short lifetime results in a large excitability window.

JSIII-P.6 FRIMetasurface Light Encoders Enable Real-Time
Hyperspectral Imaging and Video Understanding∙M. Makarenko, A. Burguete-Lopez, Q. Wang, F. Getman,
S. Giancola, B. Ghanem, and A. Fratalocchi; King Abdullah University of Science and Technology, Thuwal, Saudi
ArabiaIn this work, we present a recently developed Hy-

224

JSIII-P.8 FRIPhotonic delay-based reservoir computers as deepneural network preprocessors∙I. Bauwens1 , G. Van der Sande1 , P. Bienstman2 , and G.
Verschaffelt1 ; 1 Applied Physics Research Group, Vrije Universiteit Brussel, Brussels, Belgium; 2 Photonics ResearchGroup, Department of Information Technology, Ghent
University-IMEC, Ghent, Belgium
Based on numerical studies we show that the reservoir
from a photonic reservoir computing system can be efficiently used to preprocess data that is inputted to a deepneural network, leading to improved computational performance.

CLEO

®

/Europe-EQEC 2023

⋅ Friday 30 June 2023

Hall B0
JSIII-P.9 FRIStability analysis of photonic Ising machines∙J. Lamers, G. Verschaffelt, and G. Van der Sande; Applied
Physics Research Group, Vrije Universiteit Brussel, Brussels, Belgium
Photonic Ising machines are promising candidates to efficiently solve NP-hard optimization problems. However, they don’t always find the optimal solution. We perform a stability analysis to predict regions in parameter
space with higher success rate.
JSIII-P.10 FRI

High-resolution consistency analysis for performance
evaluation of photonic time-delay reservoir
computers∙l. oliverio1,2 , d. rontani1,2 , and m. sciamanna1,2 ;
1Chaire Photonique,
LMOPS, Metz,
France;2CentraleSupélec, Université de Lorraine, Metz, France
We theoretically analyze the dynamical consistency of atime-delayed laser-based reservoir computer. Our highresolution mapping unveils unexplored parameter regions with high consistency and good computing performances, hence revisiting earlier claims.
JSIII-P.11 FRI

Implementation of an optoacoustic activation
function based on stimulated Brillouin scattering∙S. Becker1,2 , J. Storp1 , and B. Stiller1,2 ; 1 Max Planck
Institute for the Science of Light, Erlangen, Germany;

Department of Physics, Friedrich-Alexander-Universität
Erlangen-Nürnberg, Erlangen, Germany
We present an in-fiber optoacoustic activation function
based on stimulated Brillouin scattering. We demonstrate its optically controllable input-output behavior
and frequency selectiveness, filling a gap in the landscapeof optical activation functions.
2

JSIII-P.12 FRI

Machine learning empowers large-scale opticalsensors for ultrasensitive detection∙N. Li, Q. Wang, Z. He, A. Burguete-Lopez, F. Xiang, and
A. Fratalocchi; King Abdullah University of Science andTechnology (KAUST), Thuwal, Saudi Arabia
We report a platform technology for sensing based onsuitable engineered artificial intelligence nanophotonics
hardware that can measure glucose concentration in realtime as low as 10−20 mol/L.
JSIII-P.13 FRIIntegrated photonic modulators using dispersion
engineered phase change metasurfaces∙Y. Cui, J. Davis, and B. Gholipour; University of Alberta, Electrical and Computer Engineering, Edmonton,
CanadaWe show that dispersion engineered subwavelength nanostructured phase-change/oxide composite
waveguide-integrated metasurfaces enable engineered
insertion losses and modulation contrasts without al-tering circuit architecture or phase-change material
composition with active region footprints as small as
14.2um.

pled through time-delayed feedback, solitons serving as
memory emerge from sustained periodic pulses.

JSIII-P.14 FRIExperimental investigation of refractory time of
optically induced spiking in resonant tunnelling
diode photodiodes
J. Lourenço1 , Q. Al-Taai2 , E. Wasige2 , and ∙J. Figueiredo1 ;1
Centra-Ciências and Departamento de Física, Faculdadede Ciências da Universidade de Lisboa, Lisboa, Portugal;
2High Frequency Electronics Group, University of Glasgow, Glasgow, United Kingdom
Due to their nonlinearity and excitability, receiver circuits based on resonant tunneling diode photodetectors (RTD-PDs) show promise as neuron like opticallytriggered spike firing elements to process information
through the timing of the spikes.

Taming Optical Computing Architectures: fromextreme learning machines to diffractive neuralnetworks∙N. Silva, D. Silva, F. Moreira, and T. Ferreira; INESC
TEC, Centre for Applied Photonics, Porto, Portugal
In this communication, by deploying experimental setups and associated digital twins, we extensively explore
the capabilities of distinct optical computing architectures, aiming at understanding their specific capabilities
and better mapping their potential toward real-world applications.
JSIII-P.15 FRI

Pulse Generation and Memory in Opto-Electronic
Neurons with Time-Delayed Feedback∙J. Mayer Martins1 , S.V. Gurevich1 , and J. Javaloyes2 ;1Institute for Theoretical Physics, University of Münster,Wilhelm-Klemm-Str. 9 and Center for Nonlinear Science(CeNoS), University of Münster, Corrensstrasse 2, 48149
Münster, Germany; 2 Departament de Física and IAC-3,
Universitat de les Illes Balears, C/ Valldemossa km 7.5,
07122 Mallorca, Spain
In a neuromorphic circuit composed of a nano resonant tunneling diode and a nano laser diode cou-

NOTES

225

JSIII-P.16 FRIJSIII-P.17 FRIDeep Reservoir Computing Based on Frequency
Multiplexing∙A. Lupo, M. Zajnulina, and S. Massar; Laboratoired’Information Quantique, Université libre de Bruxelles,
Bruxelles, Belgium
Deep Reservoir Computing outperforms traditional RC.
We experimentally test a deep-RC that concatenates two
photonic reservoirs. It exploits frequency-domain interference to process information encoded in frequency
combs. It achieves a two-orders-of-magnitude improvement on channel-equalization task.

Authors' Index

The index entries consist of the following data: <session key>.<paper in the session> <day> (p<page>). Presenting authors are marked by ∙.

A
A. Madigawa, Abdulmalik∙EB-P.33 THU (p178)
A.S., Lal Krishna . . . . . . . . ∙EJ-P.10 MON (p80)
A. Sukhorukov, Andrey . . CD-3.4 MON (p70)
Aalto, Timo . . . . . . . . . . . . . . . CB-5.5 TUE (p96)
Abad, Begoña . . . . . . . . . . . JSVI-1.2 TUE (p85)
Abazi, Adrian . . . . . . . . . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118)
Abbas, Omar A . . . . . . . . . CM-P.20 MON (p78)
Abdelaal, Mahmoud . . . . . . EE-4.2 FRI (p203)
Abdelaziz, Moheb . . . . . . . CK-P.19 TUE (p105)
Abdollahi, Shahab . . . . . . ∙PP-1.10 MON (p64),
CB-P.22 MON (p76), ∙CB-6.3 WED (p126),
CI-4.5 WED (p133), ∙EF-P.4 WED (p139)
Abdolvand, Amin . . . . . CM-P.30 MON (p78),
CK-P.13 TUE (p104)
Abdou Ahmed, Marwan CB-P.10 MON (p76),
CA-4.1 TUE (p82), CA-9.2 WED (p130),
CA-10.4 THU (p144), CI-P.4 FRI (p219),
CI-P.5 FRI (p219)
Abdou Ahmed, Mawan . CE-P.19 THU (p172)
Abdurakhimov, Nursulton∙CH-9.5 THU (p149)
Abe, Hiroshi . . . . . . . . . . . . EB-11.1 THU (p149)
Abecassis, Benjamin . . . . . CK-12.6 FRI (p186)
Abedin, Kamal A.A.M. . . . CM-6.3 TUE (p94)
Abire Karzazi, Mariame . . CD-13.6 FRI (p209)
Abou Khalil, Alain . . . . . ∙CM-P.25 MON (p78)
Abouraddy, Ayman . . . . . . . . CF-4.2 TUE (p83),
CF-P.5 TUE (p102), CH-7.6 WED (p127)
Abramović, Denis . . . . . . . . ∙EA-6.2 FRI (p184),
CL-P.5 FRI (p221)
Abrashitova, Ksenia . . . . . CH-2.3 MON (p60),∙CH-P.9 WED (p136),
CH-12.2 THU (p165)
Absil, Olivier . . . . . . . . . . . . JSII-3.5 MON (p73)
Abtahi, Fatemeh . . . . . . . . . . EG-5.3 TUE (p94),∙CK-P.24 TUE (p105)
Abutoama, Mohammad . . . ∙EJ-4.6 FRI (p197)
Acconcia, Giulia . . . . . . . . . CH-9.3 THU (p145)
Aceves, Alejandro . . . . . . . . EF-P.5 WED (p139)
Achour, Kailene . . . . . . . . CH-P.11 WED (p136)
Ackermann, Lisa . . . . . . . . ∙CD-13.5 FRI (p207)
Ackermann, Roland . . . . . . CL-3.6 THU (p163)
Adamo, Giorgio . . . . . . . . . . PP-1.6 MON (p64),
PP-1.7 MON (p64), EG-3.2 MON (p66),
CH-P.4 WED (p136), CH-P.8 WED (p136),
CK-10.4 THU (p160),
CH-12.6 THU (p169), CK-14.4 FRI (p204)
Adams, Ellen M. . . . . . . . . . CC-P.16 FRI (p218)
Adamska, Lyudmyla . . . . . . . CG-2.2 TUE (p97)
Adão, Ricardo M. R. . . . . . JSIII-P.2 FRI (p224)
Adappattu Ramachandran, Anjali∙CE-P.11 THU (p172)
Adcock, Jeremy C . . . . . . . . . EJ-2.4 MON (p62),∙EA-3.5 THU (p152)
Adhikari, Subhasis . . . . . . ∙CH-14.1 FRI (p189)
Adiyatullin, Albert . . . . . . . . EC-2.3 FRI (p195)
Adler, Steffen . . . . . . . . . . . . ∙CB-2.5 MON (p72)
Adnan, Sakib . . . . . . . . . . . . CF-8.3 WED (p125)
Adshead, Mason . . . . . . . . . . . CE-9.4 FRI (p194)
Afalla, Jessica . . . . . . . . . . . . . . EI-P.2 FRI (p224)

Afanasiev, Dmytro . . . . . . . CG-5.1 THU (p157)
Agarwal, Manoram . . . . ∙CG-P.11 THU (p174)
Aggarwal, Keshav . . . . . . CD-P.32 TUE (p102)
Aggarwal, Samarth . . . . . . JSIII-3.5 FRI (p187)
Aggoun, Anis . . . . . . . . . . . . . . CL-6.2 FRI (p191)
Agio, Mario . . . . . . . . . . . . . EB-7.5 WED (p119)
Agnesi, Antonio . . . . . . . . . . CD-6.1 TUE (p92),
CA-10.2 THU (p142)
Agranat, Aharon J. . . . . . . . EF-10.5 FRI (p215)
Agresti, Iris . . . . . . . . . . . . . . EB-6.1 WED (p109)
Agrež, Vid . . . . . . . . . . . . . . . . CL-8.6 FRI (p217),∙CJ-P.13 FRI (p220)
Aguergaray, Claude . . . . . PP-2.8 WED (p121),
CJ-7.4 FRI (p186), CL-5.5 FRI (p187),∙CJ-P.12 FRI (p220), CL-P.2 FRI (p221)
Aguiló, Magdalena . . . . . CA-P.19 MON (p75),
CA-P.20 MON (p75), CA-9.1 WED (p128),
CJ-6.2 THU (p143), CE-8.5 FRI (p186)
Aguiló-Aguayo, Noemí
CM-LIM.5 WED (p119)
Ahlefeldt, Rose L. . . . . . . . . CE-10.2 FRI (p204)
Ahmad, Belal . . . . . . . . . . . . CH-2.4 MON (p60)
Ahmadi, Mustafa . . . . . . CH-P.15 WED (p137)
Ahmadi, Peyman . . . . . . . . . CJ-6.6 THU (p149)
Ahmed, Areeb . . . . . . . . . . . JSI-P.4 WED (p141)
Ahmed, Mohammad . . . . . JSI-P.6 WED (p141)
Ahmed, Q. Salman . . . . . CK-P.12 TUE (p104),
CM-7.4 WED (p112),∙CE-P.17 THU (p172), ∙CE-11.5 FRI (p216)
Ahmed, Sanny . . . . . . . . . . ∙JSII-3.2 MON (p69)
Ahmed, Shahwar . . . . . . . . . CF-12.2 FRI (p211)
Ahsan, Md S. . . . . . . . . . . . . CG-3.2 THU (p143)
Ahufinger, Verònica . . . . . . . EC-P.5 FRI (p223)
Aivalioti, Chrysa . . . . . . . CM-P.12 MON (p77)
Ajduk, Anna . . . . . . . . . . . . . . CL-7.2 FRI (p203)
Ajia, Idris . . . . . . . . . . . . . . . ∙EH-5.4 THU (p166)
Akagla, Herman . . . . . . . . . ∙CA-4.2 TUE (p82),∙CA-4.5 TUE (p86)
Akahane, Kouichi . . . . . . CH-7.1 WED (p123),
CI-3.2 WED (p125), EE-P.11 WED (p139),
CB-10.5 THU (p160)
Akakpo, Edem Kossi . . . . . ∙EJ-P.5 MON (p80),∙EF-5.6 THU (p162)
Akcaalan, Onder . . . . . . . . . JSI-P.4 WED (p141)
Akdemir, Ozan . . . . . . . . . CK-P.37 TUE (p106),∙EG-P.7 TUE (p107)
Akerboom, Evelijn . . . . . . ∙EH-2.3 THU (p144)
Akers, Aiden . . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Akikusa, Naota . . . . . . . . . CH-14.2 FRI (p193)
Akozbek, Neset . . . . . . . . . CD-7.5 WED (p112),
EH-P.19 THU (p179)
Aksakal, Ozan . . . . . . . . . . . . EG-P.4 TUE (p107)
Aksnes, Astrid . . . . . . . . . . . . CH-3.1 TUE (p82)
Aksu, Serap . . . . . . . . . . . . ∙EH-P.11 THU (p179)
Al-Haddad, Andre . . . . . . JSI-1.2 WED (p110),
JSI-1.4 WED (p112), JSI-3.2 WED (p124),
JSI-4.1 WED (p128)
Al-Nuwaider, Jassim . . . . . . PP-1.5 MON (p64),
CD-P.2 TUE (p100)
Al-Taai, Qusay . . . . . . . . . JSIII-P.16 FRI (p225)
Al-Taai , Qusay R A . . . . . . JSIII-5.5 FRI (p209)
Alabastri, Alessandro . ∙JSIV-1.5 WED (p120)
Alahmadi, Yousef . . . . . . . . . EC-1.5 FRI (p187)

Alangattuthodi, Aswan . . JSI-P.2 WED (p141),∙EE-4.3 FRI (p205)
Alasgarzade, Namig . . . . . CM-2.6 MON (p62)
Albar, Esra Ilke . . . . . . . . ∙EH-P.10 THU (p179)
Albarrán-Diego, Cesar . . . CL-4.5 THU (p169)
Albeladi, Fwoziah T. . . . . . . ∙CB-4.5 TUE (p91)
Albeladi, Tahani R. . . . . . . . . CB-4.5 TUE (p91)
Alberti, Sebastian . . . . . . . . . CH-3.1 TUE (p82)
Alberucci, Alessandro . . . CM-2.6 MON (p62),
EH-2.5 THU (p148), CE-6.3 THU (p159),
CD-11.3 FRI (p185), CD-11.4 FRI (p187),∙EC-3.2 FRI (p203), EC-P.7 FRI (p223)
Albiero, Ricardo . . . . . . . . . EB-6.1 WED (p109)
Albiero, Riccardo . . . . . . . . . ∙EA-8.1 FRI (p200)
Albrechtsen, Marcus . . . . . . EC-2.5 FRI (p197)
Alcalà, Jordi . . . . . . . . . . . . . CD-7.1 WED (p108)
Alcer, David . . . . . . . . . . . . . JSIII-5.2 FRI (p205)
Aldia, P. E. Collin . . . . . . . CF-8.3 WED (p125)
Alejandro, Aldair . . . . . . . CC-1.1 THU (p149),
CC-3.2 THU (p165), CC-7.5 FRI (p214)
Aleksandrov, Veselin . . . ∙CF-P.23 TUE (p103)
Aleshire, Christopher . . . . CJ-2.4 WED (p113),
CJ-8.2 FRI (p192), CJ-10.3 FRI (p212)
Aleshkina, Svetlana . . . . . . CJ-5.3 WED (p131)
Aleshkina, Svetlana S. . . . CJ-3.1 WED (p115)
Alexander, Oliver . . . . . . . ∙JSI-4.6 WED (p134)
Alexander, Tristram J. . . . . EF-P.9 WED (p139)
Alfaro-Bittner, Karin . . . . JSIII-6.5 FRI (p217)
Alibart, Olivier . . . . . . . . . . . EB-P.2 THU (p176)
Alisauskas, Adam . . . . . . . . . CD-4.2 TUE (p82)
Alisauskas, Skirmantas . . JSI-P.4 WED (p141),
JSI-5.3 THU (p145), JSI-5.4 THU (p147)
Alkhazraji, Emad . . . . . . . . . ∙CB-5.6 TUE (p98)
ALLAIN, Tituan . . . . . . . . ∙JSII-1.5 MON (p57)
Allam, Srinivasa Rao . . . . . . CA-4.4 TUE (p86)
Allan, Ewan . . . . . . . . . . . . . ∙CF-11.4 FRI (p205)
Allaria, E. . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Allayarov, Izzatjon . . . . . . . ∙EG-2.5 MON (p62)
Allegre, Hortense . . . . . . . . ∙CG-1.4 TUE (p87),
CG-3.1 THU (p143), EE-4.6 FRI (p209)
Allen, Euan . . . . . . . . . . . . . EB-P.16 THU (p177)
Allerbeck, Jonas . . . . . . . . ∙EG-3.5 MON (p70),
EG-4.2 TUE (p84), EH-2.4 THU (p146)
Allevi, Alessia . . . . . . . . . . . EB-P.28 THU (p178)
Allford, Craig . . . . . . . . . . . . . CB-4.5 TUE (p91)
Alliot de Borggraef, Louis∙CH-11.1 THU (p157), ∙CI-P.12 FRI (p219)
Allisy, Baptiste . . . . . . . . . . . CL-2.4 THU (p153)
Allix, Mathieu . . . . . . . . . . . . . CE-4.5 TUE (p99)
Almási, Gábor . . . . . . . . . . . . CC-P.5 FRI (p218),
CC-P.9 FRI (p218)
Almuneau, Guilhem . . . CH-P.16 WED (p137)
Alonso, Benjamín . . . . . . . . CF-3.5 MON (p73),
CF-4.4 TUE (p87)
Alonso-Ramos, Carlos . . . . CD-5.5 TUE (p91)
Alonso-Urquijo, Diego . JSIII-1.2 THU (p158)
Alouini, Mehdi . . . . . . . . . . . CI-2.3 WED (p121)
Alsaif, Naseem . . . . . . . . . . . CE-1.1 MON (p53)
Altmann, Yoann . . . . . . . . . . CH-4.5 TUE (p98)
Altwaijry, Najd . . . . . . . . . ∙CF-P.16 TUE (p103)
Alu, Andrea . . . . . . . . . . . . EH-1.3 WED (p132),
EH-3.1 THU (p148), EH-5.1 THU (p162)
Alvarez-Alegria, Miguel . CM-P.1 MON (p77)
Alves, Tiago L. . . . . . . . . . . . JSIII-P.2 FRI (p224)

226

Amano, Takeru . . . . . . . . . . . . CI-6.2 FRI (p190)
Amanti, Maria . . . . . . . . . . . EB-6.6 WED (p115)
Amaral, Anderson M. . . . CH-P.7 WED (p136),
CE-P.28 THU (p173)
Amezcua-Correa, Rodrigo
JSII-1.2 MON (p55), PP-1.12 MON (p65),
JSII-P.2 MON (p80)
Amiard-Hudebine, Gabriel
CE-10.3 FRI (p206)
Amidullah, Meharunissa . CE-5.2 THU (p151)
Amirabadi, Mohammad Ali
CI-4.2 WED (p131)
Amirtharaj, Sakthi Priya . ∙EG-3.4 MON (p68)Amit, Omer . . . . . . . . . . . . . . ED-1.3 MON (p55)
Amitay, Shaked . . . . . . . . . . . . EI-P.5 FRI (p224)
Amitonova, Lyubov V. . . . CH-2.3 MON (p60),
CH-P.3 WED (p136), CH-P.9 WED (p136),
CH-12.2 THU (p165)
Amiune, Nicolas . . . . . . . . . . CD-6.3 TUE (p94)
Ammouri, Nor . . . . . . . . . . CB-11.2 THU (p164)
Amo, Alberto . . . . . . . . . . . CK-12.3 FRI (p182),
EC-2.3 FRI (p195)
Amorim, Vitor . . . . . . . . . . . . CL-7.4 FRI (p205)
Amotchkina, Tatiana . . . . CD-7.2 WED (p108)
Amrani, Foued . . . . . . . . CM-P.25 MON (p78),
CD-8.3 WED (p118), CJ-4.2 WED (p123),
CD-14.2 FRI (p213)
An, Bo . . . . . . . . . . . . . . . . . . . PP-1.7 MON (p64),
CH-P.8 WED (p136)
Anantharaman, Surendra B.
CA-9.3 WED (p130)
Anantharaman, Surendra Babu
CE-3.6 MON (p73)
Anashkina, Elena A. . . . . . EB-2.1 MON (p59)
Anastasios D. Koulouklidis, Anastasios D.
∙CC-6.3 FRI (p204)
Anastasiou, Antonios D . . CL-3.5 THU (p161)
Anastasoaie, Veronica . . . . CK-2.2 TUE (p86)Ancsin, Philippe . . . . . . . ∙EB-P.31 THU (p178)
Anders, Krzysztof . . . . . . . CK-P.9 TUE (p104),
CK-P.23 TUE (p105),
CH-11.6 THU (p163), ∙CE-10.5 FRI (p208)
Anders, Lasse . . . . . . . . . . . . ED-P.3 MON (p79)
Andersen, Ulrik . . . . . . . . EB-P.30 THU (p178),
EA-9.5 FRI (p214)
Andersen, Ulrik L. . . . . . . EB-P.23 THU (p177)
Andersen, Ulrik Lund . . PP-1.11 MON (p64),
EJ-P.1 MON (p79)
Anderson, Miles . . . . . . . . . ∙EF-3.2 THU (p142)
Anderson, Miles H. . . . . . . EF-2.3 WED (p133)
Andrade, Jose. R. C. . . . . . CF-P.19 TUE (p103)
Andral, Ugo . . . . . . . . . . . . . CD-8.1 WED (p114)
André, Yves-Bernard . . . . CD-P.7 TUE (p100),
CD-8.1 WED (p114)
Andreasson, Joakim . . . . . . . EG-4.2 TUE (p84)
Andreev, Andrey . . . . . . . . . CB-9.5 THU (p152)
Andrekson, Peter A. . . . . . . CD-2.6 MON (p62)
Andrés, Miguel V. . . . . . . CD-P.22 TUE (p101),
CH-15.5 FRI (p209)
Andrés, Miguel Vicente CH-11.3 THU (p159)
Andresen, Esben . . . . . . . . CH-P.1 WED (p136),
CH-10.1 THU (p149)
Andresen, Esben R. . . . . CH-12.2 THU (p165)
Andrews, Aaron M. . . . . . . . CC-4.2 FRI (p180)

Andriani, Samuela . . . . . . . CH-15.1 FRI (p201)
Andrianov, Alexey V. . . . . . EB-2.1 MON (p59)
Andrieux, Aurore . . . . . . . CE-7.5 THU (p169)
Andrijec, Dovilė . . . . . . . . CM-11.5 FRI (p216)
Andriolli, Nicola . . . . . . . . JSIII-3.2 FRI (p183)
Andrishak, Artur . . . . . . . . JSIII-P.2 FRI (p224)
Androvitsaneas, Petros . EA-P.20 THU (p175)
Andrushchak, Anatolii . CM-P.28 MON (p78)
Anelli, Francesco . . . . . . . ∙CE-1.5 MON (p57),
CE-5.3 THU (p151)
Anghel, Iulia . . . . . . . . . . . . . CA-P.4 MON (p74)
Angulo M., Alí M. . . . . . . ∙CD-14.4 FRI (p215),
EE-5.2 FRI (p211)
Anjum, Ishraq Md . . . . . . . . . EJ-4.5 FRI (p197)
Annunziata, Andrea . . . . . CF-2.5 MON (p63)
Annunziato, Andrea . . . . . CE-1.5 MON (p57),
CE-5.3 THU (p151)
Annurakshita, Shambhavee∙EG-4.4 TUE (p86)Anquetin, Yann . . . . . . . . . CM-P.32 MON (p79)
Ansquer, Mathieu . . . . . . . EB-13.6 THU (p169)
Ansquer, Matthieu . . . . . . EA-3.2 THU (p150)
Antipenkov, Roman . . . . . CA-8.3 WED (p118)
Anton, Oliver . . . . . . . . . . . . . EB-1.4 MON (p57)
Anton-Solanas, Carlos . . . . . EI-2.6 FRI (p196)
Antonelli, Cristian . . . . . . . CI-4.2 WED (p131)
Antonik, Piotr . . . . . . . . . . JSIII-2.6 THU (p168)
Antonio, Guillermo Nava . . CA-5.3 TUE (p96)
Antony, Cleitus . . . . . . . . . . CI-3.3 WED (p125)
Anttu, Nicklas . . . . . . . . . . . . . EG-4.4 TUE (p86)Anus, Muhammad . . . . . . . CG-4.5 THU (p153)
Aoki, Takao . . . . . . . . . . . . . CK-6.4 WED (p126)
Aouji, Samar . . . . . . . . . . . . . CE-1.2 MON (p53)
Aperathitis, Elias . . . . . . . CM-P.12 MON (p77)
Appas, Felicien . . . . . . . . . . EB-9.4 WED (p133)
Appel, Heiko . . . . . . . . . . . EH-P.10 THU (p179)
Apra, Pietro . . . . . . . . . . . . . . CM-4.2 TUE (p82)
Arabmoheghi, Amirali . . . . EA-9.1 FRI (p210)
Aragón, Jose L. . . . . . . . . . . CH-8.6 WED (p135)
Araneda, G. . . . . . . . . . . . . . . . ED-5.1 FRI (p180)
Arantchouk, Leonid . . . . . . CD-P.7 TUE (p100)
Arar, Bassem . . . . . . . . . . . CB-10.4 THU (p160)
Arcadi, Elizabeth . . . . . . . . JSII-3.3 MON (p69)
Arciniegas, Milena . . . . . . . . CE-4.3 TUE (p95)
Ardaneh, Kazem . . . . . . . . . . . EE-2.2 FRI (p185)
Ardini, Benedetto . . . . . . . CH-8.4 WED (p133)
Arend, Germaine . . . . . . . EG-6.2 WED (p108),EF-9.2 FRI (p203)
Arge, Tummas Napoleon∙PP-1.11 MON (p64), ∙EJ-P.1 MON (p79)
Argüello Ron, Diego . . . . ∙CI-4.4 WED (p133)
Argyris, Apostolos . . . . . JSIII-1.4 THU (p160),
JSIII-2.2 THU (p164)
Argyris, Nikos . . . . . . . . . . . . . EJ-3.4 FRI (p187)
Arias , Loïc . . . . . . . . . . . . . . . CD-4.5 TUE (p86)
Arie, Ady . . . . . . . . . . . . . . . CD-9.5 WED (p126)
Arieli, Uri . . . . . . . . . . . . . . . . . EE-5.5 FRI (p215)
Arkhipov, Mikhail . . . . . . . EE-P.4 WED (p138)
Arkhipov, Rostislav . . . . . ∙EE-P.4 WED (p138)
Armalytė, Simona . . . . . . . . CD-P.8 TUE (p100)
Armand, Rémi . . . . . . . . . ∙CK-4.3 WED (p112)
Arnaudon, Alexis . . . . . . . . CK-14.2 FRI (p202)
Arnold, Cord . . . . . . . . . . . CF-P.18 TUE (p103),
CG-4.6 THU (p155)

Authors' Index

Arnold, Cord L . . . . . . . . . . CF-1.3 MON (p57),
CF-5.2 TUE (p95), CG-5.2 THU (p159),
PD-1.3 THU (p170)
Arora, Shilpi . . . . . . . . . . . . . . ∙CJ-P.6 FRI (p220)
Arosa Lobato, Yago . . . . . . . EF-7.5 FRI (p187),
CD-13.3 FRI (p205)
Arpe, Riccardo . . . . . . . . . . CK-7.1 WED (p128)
Arregui, Francisco J. . . . . CE-5.6 THU (p155)
Arregui, Guillermo . . . . . . . ∙EC-2.5 FRI (p197)
Arregui Leon, Unai . . . . . . CD-11.2 FRI (p183)
Arshad, Atiqa . . . . . . . . . . . . CC-P.16 FRI (p218)
Arslan, Dennis . . . . . . . . . CK-10.6 THU (p162)
Arslan, Seval . . . . . . . . . . . CB-11.1 THU (p162),∙CB-11.3 THU (p166)
Artigas, David . . . . . . . . . . . . . EC-3.3 FRI (p205)
Artyukhin, Sergey . . . . . . . . CE-4.3 TUE (p95)
Arumugam, Stree Vithya . ∙EC-P.7 FRI (p223)
Arya, Chaitanya . . . . . . . . . JSVI-1.2 TUE (p85)
Asavanant, Warit . . . . . . . . . EA-2.2 THU (p142)
Asenbeck, Beate Elisabeth ∙EB-4.3 TUE (p87)
Asenjo-Garcia, Ana . . . . . . . ∙EG-4.1 TUE (p82)
Ashihara, Satoshi . . . . . . . CF-7.5 WED (p119),
EE-P.2 WED (p138), EE-5.6 FRI (p217)
Asif, Hira . . . . . . . . . . . . . . . ∙EH-P.9 THU (p179)
Aşırım, Özüm Emre . . . . . ∙CJ-3.3 WED (p117)
Askari, Meisam . . . . . . . . . . EH-4.6 THU (p162)
Asselah, Yasmine . . . . . . . ∙CD-14.2 FRI (p213)
Astrauskas, Ignas . . . . . . . . CA-1.5 MON (p56),
EF-P.19 WED (p140), CF-12.4 FRI (p215)
Astrauskytė, Darija . . . . . . . CE-11.2 FRI (p212)
Atsuhi , Kanno . . . . . . . . . . . . . CI-8.2 FRI (p210)
Attanasio, Alaina . . . . . . . . . . CB-5.4 TUE (p96)
Aubrecht, Jan . . . . . . . . . . . . . CJ-9.1 FRI (p200),∙CJ-9.5 FRI (p208), CJ-10.6 FRI (p216)
AUDO, Frédéric . . . . . . . . . CA-7.3 WED (p126)
Auer, Michael . . . . . . . . . . . PP-2.9 WED (p121),
EB-P.1 THU (p176)
Augsburger, Matthias . . . . CA-P.12 MON (p74)
Auguste, Thierry . . . . . . . . . CF-1.4 MON (p57)
Augustin, Sven . . . . . . . . . . JSI-1.2 WED (p110),
JSI-1.4 WED (p112), JSI-3.2 WED (p124),
JSI-4.1 WED (p128)
Aull, Stefan . . . . . . . . . . . . ∙EA-P.18 THU (p175)
Avaldi, Lorenzo . . . . . . . . . . . EE-3.1 FRI (p189)
Avella, Adolfo . . . . . . . . . . . . . CG-2.2 TUE (p97)
Avellà-Oliver, Miquel . . . . CH-15.5 FRI (p209)
Averchenko, Alexander . CM-P.20 MON (p78)
Averkiev, N. S. . . . . . . . . . . . . . EA-1.4 TUE (p87)
Avino, Saverio . . . . . . . . . . . CH-2.5 MON (p62),
CK-13.5 FRI (p196)
Awachi, Habib . . . . . . . . . . CE-P.15 THU (p172)
Awasthi, Saurabh . . . . . . . CM-P.10 MON (p77)
Awwad, Elie . . . . . . . . . . . . . CB-9.4 THU (p152)
Axner, Ove . . . . . . . . . . . . . . . . ED-4.1 TUE (p83)
Ayan, Arman . . . . . . . . . . . . . . CD-6.4 TUE (p96)
Aydemir, Umut . . . . . . . . . . CE-5.5 THU (p153),
CL-P.9 FRI (p222)
Aydin, Koray . . . . . . . . . . . . . JSVI-2.5 TUE (p99)
Aydin, Yavuz . . . . . . . . . . . . . CM-2.5 MON (p62)
Ayhan, Furkan . . . . . . . . . . JSII-2.4 MON (p63),∙CD-5.2 TUE (p90)
Ayuso, David . . . . . . . . . . . . . CG-1.5 TUE (p89),∙EE-P.1 WED (p138), EE-4.6 FRI (p209)
Azeem, Farhan . . . . . . . . CD-10.3 WED (p130),
CD-10.4 WED (p132)
Azoury, Doron . . . . . . . . . EE-P.14 WED (p139),

CG-5.4 THU (p161)
Azzolin, Agata . . . . . . . . . . . JSI-5.3 THU (p145),∙CG-3.2 THU (p143)

B
B, Lakshman . . . . . . . . . . . . . . . CI-7.3 FRI (p204)
Baalkhuyur, Fadiyah . . . CH-P.20 WED (p137)
Babar, Ali N. . . . . . . . . . . . . . EG-P.9 TUE (p107)
Babayigit, Ceren . . . . . . . . . CE-3.3 MON (p69)
Babichev, Andrey . . . . . . . . CB-9.5 THU (p152)
Babin, Sergey A. . . . . . . . . . . CJ-P.20 FRI (p221)
Baboux, Florent . . . . . . . . . ∙EB-6.6 WED (p115)
Babushkin, Ihar . . . . . . . . . . ∙EJ-2.3 MON (p60),
CF-P.19 TUE (p103), CF-6.2 WED (p109),
CD-9.4 WED (p124), EE-P.4 WED (p138),
EF-P.1 WED (p139), EF-5.3 THU (p158),
EE-5.2 FRI (p211)
Bacco, Davide . . . . . . . . . . . EB-P.22 THU (p177)
Bacellar, Camila . . . . . . . . . JSI-1.4 WED (p112)
Bachelard, Romain . . . . . . EB-11.5 THU (p153)
Bächle, Andreas . . . . . . . . . . CB-2.5 MON (p72)
Badano, Laura . . . . . . . . . . JSI-4.3 WED (p130)
Badavath, Purnesh Singh . . CI-P.6 FRI (p219)
Badtke, Moritz . . . . . . . . . ∙CA-6.1 WED (p108)
Bae, Ji Eun . . . . . . . . . . . . . ∙CA-9.1 WED (p128)Bækkegaard, Thomas . . . . . EB-P.5 THU (p176)
Baghban, Mohammad A. . CK-1.2 MON (p66)
Bagiante, Salvatore . . . . . . CC-1.2 THU (p151)
Bahar, Eyal . . . . . . . . . . . . . . . . EE-5.5 FRI (p215)
Bahr, Niklas . . . . . . . . . . . . . ∙EF-P.1 WED (p139)
Bahri, Mehran . . . . . . . . . . . CJ-2.4 WED (p113),∙CJ-8.2 FRI (p192)
Bai, Chuan . . . . . . . . . . . . . . ∙PP-1.2 MON (p64),
CA-P.13 MON (p74), ∙CA-P.21 MON (p75),
CA-10.1 THU (p142)
Bai, Zhenxu . . . . . . . . . . . . . . CA-5.2 TUE (p94),
CA-5.5 TUE (p98)
Baida, Fadi . . . . . . . . . . . . . . . CE-5.2 THU (p151)
Baillard, Amandine . . . . ∙CA-6.4 WED (p112),∙CE-8.5 FRI (p186)
Baillard, Guillaume . . . . . ∙CK-12.6 FRI (p186)
Bailleul, Damien . . . . . . . . . . . CJ-7.3 FRI (p184)
Bajek, David . . . . . . . . . . . . . CF-11.4 FRI (p205)
Bajoni, Daniele . . . . . . . . . . . . EA-8.5 FRI (p208)
Baklan, Denys . . . . . . . . . . CM-P.33 MON (p79)
Bakopoulos, Paraskevas . . . . EJ-3.4 FRI (p187)
Bakovic, Mark . . . . . . . . . . CM-7.1 WED (p108)
Bakule, Pavel . . . . . . . . . . . . CA-8.3 WED (p118)
Balabanov, Stanislav . . . . CA-11.2 THU (p150)
Balage, Pierre . . . . . . . . . . . CM-2.4 MON (p60),∙CM-3.6 MON (p72)
Balasubrahmaniyam, Mukundakumar∙CK-12.5 FRI (p186)
Balasubramanian, Krishna
EA-5.3 THU (p166)
Balčas, Giedrius . . . . . . . . . . CE-11.2 FRI (p212)
Baldini, Francesco . . . . . . . . CL-1.4 MON (p71)
Balembois, François . . . . . . ∙CE-4.1 TUE (p93),
CA-11.3 THU (p150),∙CE-P.29 THU (p173),∙CG-P.14 THU (p174), CI-8.5 FRI (p214)
Balena, Antonio . . . . . . . . . CH-15.1 FRI (p201)
Baliuka, Adomas . . . . . . . ∙PP-2.9 WED (p121),∙EB-P.1 THU (p176)
Ball, Adam . . . . . . . . . . . . . . . CE-7.1 THU (p163)

Balla, Prannay . . . . . . . . . . . . . EE-4.1 FRI (p201)
Ballance, C. J. . . . . . . . . . . . . . ED-5.1 FRI (p180)
Ballance, Chris . . . . . . . . . CM-7.5 WED (p112)
Ballato, John . . . . . . . . . . . . . . CD-6.2 TUE (p92),
CJ-1.2 TUE (p95), CD-7.6 WED (p114),
CE-7.1 THU (p163)
Ballester, Miguel Montesinos
JSII-2.2 MON (p61)
Balling, Peter . . . . . . . . . . CM-P.19 MON (p78),∙CM-10.2 FRI (p204)
Balram, Krishna C. . . . . . . . EB-1.5 MON (p57),
EB-6.5 WED (p113)
Baltuska, Andrius . . . . . . . . CA-1.5 MON (p56),
CD-2.2 MON (p58), CG-1.3 TUE (p87),
CF-9.2 WED (p131), EF-P.19 WED (p140),
CF-11.6 FRI (p209), CF-12.4 FRI (p215)
Bañares, Luis . . . . . . . . . . . . . . EE-3.1 FRI (p189)
Banaszek, Konrad . . . . . . . . ∙CI-P.14 FRI (p219)
Bancel, Eve-Line . . . . . . . . . ∙ED-6.6 FRI (p196)
Bancora, Andrea . . . . . . . . . . CB-5.4 TUE (p96),
CK-14.1 FRI (p200)
Bandhoe, Akje . . . . . . . . . . CH-P.3 WED (p136)
Banerjee, Rounak . . . . . . . . . . EI-2.6 FRI (p196)
Banfi, Francesco . . . . . . . . ∙JSVI-1.4 TUE (p89)Bang, Ole . . . . . . . . . . . . . . . . CH-1.4 MON (p55),
CD-P.23 TUE (p101), CJ-7.5 FRI (p186),
CJ-P.8 FRI (p220)
Bánhegyi, Balázs . . . . . . . . ∙EE-P.7 WED (p138)
Bannerman, Rex . . . . . . . . EF-P.11 WED (p140)
Bannerman, Rex H. S. . ∙CM-7.4 WED (p112),
CM-7.6 WED (p114), CA-6.3 WED (p110),∙CJ-5.5 WED (p133), CE-P.17 THU (p172),
CE-P.30 THU (p173), CE-9.2 FRI (p190),
CD-14.5 FRI (p217)
Bansal, Lalitkumar . . . . . . . . . CJ-1.1 TUE (p93)
Bányász, István . . . . . . . . . . . CK-P.3 TUE (p104)
Banys, Jonas . . . . . . . . . . . . . ∙CD-P.8 TUE (p100)
Banzer, Peter . . . . . . . . . . . . . . CH-3.2 TUE (p84)
Barahona, Mauricio . . . . . . CK-14.2 FRI (p202)
Barbato, Pasquale . . . . . . . . . CM-6.3 TUE (p94)
Barbay, Sylvain . . . . . . . . . . . EF-8.3 FRI (p195),
JSIII-6.4 FRI (p215), ∙JSIII-6.5 FRI (p217),∙EF-10.1 FRI (p211)
Barbé, Vincent . . . . . . . . . . ∙ED-1.1 MON (p53)
Barber, Matthew J. . . . . . . . CA-7.2 WED (p126)
Barbero, Cristian . . . . . . . . ∙CF-3.5 MON (p73)
Barbier, Margaux . . . . . . . . . . CD-4.1 TUE (p82)
Barbiero, Gaia . . . . . . . . . . CF-10.6 THU (p149)
Barcikowski, Stephan∙CM-LIM.1 WED (p115),
CM-10.3 FRI (p204)
Barh, Ajanta . . . . . . . . . . . . ∙CA-2.5 MON (p62),
CB-2.1 MON (p66)
Barimah, Eric K . . . . . . . . . . CL-3.5 THU (p161)
Barjot, Kevin . . . . . . . . . . . . JSII-1.3 MON (p55)
Bark, Hyeon Sang . . . . . . . . . CC-P.4 FRI (p218)
Barland, Stéphane . . . . . . CH-P.26 WED (p137)
Barmparis, Georgios D. . CM-P.31 MON (p78)
Barnini, Alexandre . . . . . . CJ-5.6 WED (p135),
CJ-P.18 FRI (p221)
Barone, Andrea . . . . . . . . . . . EA-8.5 FRI (p208)
Barra Burrillo, María . . . . . EG-3.1 MON (p66)
Barral, David . . . . . . . . . . . EB-8.3 WED (p125),
EB-12.2 THU (p159)
Barré, Nicolas . . . . . . . . . . . CD-13.5 FRI (p207)
Barreda, Angela . . . . . . . . . . . CE-4.2 TUE (p93),

227

CK-11.4 THU (p166)
Barrett, Laura . . . . . . . . . . . CM-1.6 MON (p56),∙CD-2.4 MON (p60)
Barrio, Miguel . . . . . . . . . . . . . CI-6.6 FRI (p196)
Barros, Rafael . . . . . . . . . . . . ∙EC-3.4 FRI (p205),
EE-5.4 FRI (p215)
Barros, Rafael F. . . . . . . . . EB-12.1 THU (p157)
Barrow, Peter . . . . . . . . . . . . . . EB-5.5 TUE (p97)
Barry, Liam . . . . . . . . . . . . . . . . CI-6.1 FRI (p188)
Bartholomew, John G. . . . . CE-10.2 FRI (p204)
Bartley, Tim . . . . . . . . . . . . . . . CI-5.5 FRI (p186)
Bartolo, Adrian . . . . . . . . . CD-8.4 WED (p118),
EF-4.2 THU (p152), EF-4.3 THU (p152),
CB-10.6 THU (p162), EF-5.2 THU (p158)
Barton, Janice . . . . . . . . . . . . CE-5.3 THU (p151)
Bartoníček, Jan . . . . . . . . . . CA-8.4 WED (p118)
Bartulevicius, Tadas . . . . . CA-1.5 MON (p56),∙CA-P.14 MON (p74)
Barvinska, Vanessa . . . . . CM-P.28 MON (p78)
Baserga, Alessandro . . . . . . . EE-5.1 FRI (p211)
Bashir, Danish . . . . . . . . . . CA-9.2 WED (p130)
Bashir, Muhammad Asim . CL-8.1 FRI (p211),∙CL-8.3 FRI (p213)
Bashiri, Ayesheh . . . . . . . . . . . CE-4.2 TUE (p93)
Basler, Paul Simon . . . . . CB-11.1 THU (p162),
CB-11.3 THU (p166)
Basov, D. N. . . . . . . . . . . . . . . . . EI-2.1 FRI (p188)
Basset, Francesco Basso . . EA-4.4 THU (p160)
Bassi, Andrea . . . . . . . . . . . CH-8.4 WED (p133)
Bassi, Angelo . . . . . . . . . . . . . . EB-5.4 TUE (p97)
Basso Basset, Francesco . . . . EB-5.3 TUE (p95)
Battle, Ronan . . . . . . . . . . . . . CD-4.3 TUE (p84)
Battle, Ronan A . . . . . . . . . ∙CL-3.2 THU (p159),
CD-13.6 FRI (p209)
Bauer, Carolin . . . . . . . . . . CF-7.1 WED (p115),
CF-9.1 WED (p129)
Bauer, Dieter . . . . . . . . . . . PP-2.10 WED (p121),
EC-P.1 FRI (p222)
Bauer, Stephanie . . . . . . ∙CK-11.5 THU (p168),
EA-P.12 THU (p175)
Bauerhenne, Bernd . . . . . . CG-3.5 THU (p147)
Baumann, Jan . . . . . . . . . . . . CB-P.5 MON (p75)
Baumann, Michael . . . . . . . CI-3.1 WED (p123)
Baumann, Thomas . . . . . . . JSI-P.2 WED (p141)
Baumberg, Jeremy . . . . . . . EG-6.4 WED (p112)
Baumgärtner, Kiana . . . . . JSI-3.4 WED (p126)
Baumgartner, Werner . . . . . CM-9.4 FRI (p194)
Bautista, Godofredo . . . . . . . EG-4.4 TUE (p86)
Bautista, Jessica E. Q. . . . CD-P.16 TUE (p100)
Bauwens, Ian . . . . . . . . . . . ∙JSIII-P.5 FRI (p224),∙JSIII-P.8 FRI (p224)
Bawamia, Ahmad . . . . . . . . CB-P.5 MON (p75),
CB-10.4 THU (p160)
Bayer, Eva Marie . . . . . . ∙CH-P.35 WED (p138)
Baylon, Antonio . . . . . . . . . CJ-3.6 WED (p121)
Bayraktar, Ömer . . . . . . . . . EB-6.4 WED (p113)
Bazin, Alexandre . . . . . . . . JSIII-6.2 FRI (p213)
Bazsó, Gábor . . . . . . . . . . . . . CE-P.6 THU (p171)
Beainy, Georges . . . . . . . . . . EG-P.5 TUE (p107)
Bearne, Kaden . . . . . . . . . CH-12.3 THU (p167)
Beattie, Eduardo . . . . . . . . . . EG-5.1 TUE (p92)
Beaudoin, Gregoire . . . . . CD-8.4 WED (p118),
EF-4.3 THU (p152), CB-10.6 THU (p162),
EF-5.2 THU (p158), EF-8.2 FRI (p193),
CK-14.6 FRI (p208), JSIII-6.5 FRI (p217)
Beausoleil, Ray . . . . . . . . . . CK-P.11 TUE (p104)

Beauvarlet, Sandra . . . . . . . JSI-4.6 WED (p134)
Bebeti, Engjell . . . . . . . . . . . . CF-5.1 TUE (p93)
Beccari, Alberto . . . . . . . . . . . EA-9.1 FRI (p210)
Becheker, Rezki . . . . . . . . . . CC-2.4 THU (p163)
Beck, Julius . . . . . . . . . . . ∙PP-2.10 WED (p121),∙EC-2.1 FRI (p189), ∙EC-P.1 FRI (p222),∙EC-P.2 FRI (p223)
Beck, Mattias . . . . . . . . . . . . EG-3.1 MON (p66),
CK-6.2 WED (p124), CB-8.3 THU (p144),
CB-8.5 THU (p146), CB-8.6 THU (p148),
CB-9.1 THU (p148), CB-9.3 THU (p150),
CC-4.1 FRI (p180), CC-4.3 FRI (p182),
CC-4.5 FRI (p186), CH-13.2 FRI (p183),
EC-3.1 FRI (p201)
Beck, Paul . . . . . . . . . . . . . . . . ∙CH-3.2 TUE (p84)
Beck, Uwe . . . . . . . . . . . . . . . CM-2.1 MON (p58)
Becker, Karo . . . . . . . . . . . . . . EC-1.3 FRI (p185)
Becker, Luise . . . . . . . . . . . . . CF-2.5 MON (p63)
Becker, Steven . . . . . . . . . . . CD-12.6 FRI (p197),∙JSIII-P.11 FRI (p225)
Beckert, Erik . . . . . . . . . . . . EB-P.10 THU (p176)
Bednyakova, Anastasia . . . ∙CJ-P.17 FRI (p221)
Beduk, Tutku . . . . . . . . . . . . . . CL-P.9 FRI (p222)
Beer, Sebastian . . . . . . . . . . EH-2.5 THU (p148),∙CD-11.3 FRI (p185), CD-11.4 FRI (p187)
Bega, Luca . . . . . . . . . . . . . . CH-6.4 WED (p118)
Beggs, Daryl . . . . . . . . . . . . . CK-15.2 FRI (p210)
Begum, Afshan . . . . . . . . . CK-P.17 TUE (p105),
EC-P.11 FRI (p223)
Beier, Maximilian . . . . . . . CB-11.2 THU (p164)
Beirow, Frieder . . . . . . . . . . . . CA-4.1 TUE (p82)
Beiser, Maximilian . . . . . . . CD-6.5 TUE (p96),
EF-2.4 WED (p133), CB-8.1 THU (p142),
CC-4.2 FRI (p180)
Beitner, Daniel . . . . . . . . . . . . ∙EI-P.5 FRI (p224)
Bej, Subhajit . . . . . . . . . . . . . EG-1.4 MON (p56),
CD-10.2 WED (p130), EC-3.4 FRI (p205)
Bek, Alpan . . . . . . . . . . . . . . . CM-2.5 MON (p62)
Belabas, Nadia . . . . . . . . . . . EB-3.1 MON (p67),
EB-6.1 WED (p109), EA-8.1 FRI (p200)
Belardini, Alessandro . . . . CE-3.5 MON (p71),
JSVI-2.4 TUE (p97)
Belchovski, Metodi . . . . . CD-P.31 TUE (p102),
EH-3.5 THU (p152)
Beléndez, Augusto . . . . . . CM-P.29 MON (p78)
Belkin, Mikhail A. . . . . . . . . CB-4.3 TUE (p91),
EH-3.1 THU (p148), CC-4.6 FRI (p186)
Belli, Federico . . . . . . . . . . . . PP-1.5 MON (p64),
CD-5.4 TUE (p91), CD-P.2 TUE (p100),
EE-4.4 FRI (p205), EE-4.5 FRI (p207)
Bellissimo, Alessandra . . . CF-9.2 WED (p131)
Bello, Valentina . . . . . . . . . PP-2.7 WED (p121),∙CL-2.6 THU (p155), ∙CH-15.3 FRI (p205),
CL-P.1 FRI (p221)
Bellone, Aurora . . . . . . . . CH-11.5 THU (p161)
Belloni, Valeria Viviana . . ∙CM-4.1 TUE (p82)
Bellouard, Yves . . . . . . . . . . . CM-8.1 FRI (p180)
Bellucci, Stefano . . . . . . . CM-P.18 MON (p78)
Belousov, V. V. . . . . . . . . . . . . CL-7.1 FRI (p201)
Belussi, Francesco Maria . JSVI-1.4 TUE (p89)
Ben Bakir, Badhise . . . . . CH-P.22 WED (p137)
Ben-Shalom, Moshe . . . . . . . EE-5.5 FRI (p215),
EI-P.5 FRI (p224)
Benabdelghani, Imene . . ∙CE-P.6 THU (p171),
CC-P.13 FRI (p218)
Benabdesselam, MouradCH-11.5 THU (p161)

Authors' Index

Benabid, Fetah . . . . . . . . . . . CE-2.3 MON (p61),
CM-P.25 MON (p78), CD-8.3 WED (p118),
CJ-4.2 WED (p123), CD-14.2 FRI (p213)
Benadouda Ivars, Salim . . EF-6.6 THU (p168)
Benayad, Abdelmjid . . . . . . CA-4.5 TUE (p86),
CA-9.4 WED (p132), CE-8.5 FRI (p186)
Bencheikh, Kamel . . . . . . . . EB-3.1 MON (p67),
EA-7.4 FRI (p196)
Bencivenga, Filippo . . . . JSI-1.5 WED (p114),∙JSI-P.1 WED (p141)
Bendahmane, Abdelkrim . . ED-6.3 FRI (p192)
Bender, Nicholas . . . . . . . . CH-1.2 MON (p53),
EC-P.10 FRI (p223)
Benea-Chelmus, Ileana-Cristina
CD-3.3 MON (p68), EH-5.2 THU (p164),
CC-3.4 THU (p167), ∙CC-5.1 FRI (p188)
Benedek, Peter . . . . . . . . . . CD-1.2 MON (p54),
EH-4.1 THU (p156)
Bengery, Zsolt . . . . . . . . . . . CF-P.21 TUE (p103)
Bengtsson, Samuel . . . . . . . JSI-2.5 WED (p118)
Benkelfat, Badr-eddine . . . CB-5.3 TUE (p94)
Benner, Maximilian . . . . . . CJ-2.2 WED (p111)
Bennett, Anthony . . . . . . . . CK-15.2 FRI (p210)
Bennett, Robert . . . . . . . . . . . EJ-2.5 MON (p62)
Bennetts , Shayne . . . . . . . EA-P.2 THU (p174)
Benoit, Aurélien . . . . . . . . ∙JSII-3.4 MON (p71),
CH-10.2 THU (p151)
Bentz, Misty . . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Berakdar, Jamal . . . . . . . . . ∙JSI-3.5 WED (p126)
Berciaud, Stéphane . . . . . . . . . EI-3.1 FRI (p200)
Beresna, Martynas . . . . . CH-P.13 WED (p136),
CH-P.32 WED (p138),
CH-10.6 THU (p155), CE-5.3 THU (p151)
Bereyhi, Mohammad J. . . . . EA-9.1 FRI (p210)
Berg, Andrej . . . . . . . . . . . . . CK-P.8 TUE (p104)
BERGER, Jean-Philippe . . JSII-1.5 MON (p57)
Berger, Robert . . . . . . . . . . EA-P.18 THU (p175)
Bergeron, Hugo . . . . . . . . . . ED-3.1 MON (p67)
Bergmann, Michael . . . . . . . CB-2.3 MON (p68)
Bering Petersen, Poul . . . . CF-12.3 FRI (p213)
Berisset, Michaël . . . . . . . CM-P.25 MON (p78)
Berkman, Ian R. . . . . . . . . . . CE-10.2 FRI (p204)
Bernal, Maria-Pilar . . . . . . CE-5.2 THU (p151)
Bernasconi, Alexandra . EB-13.2 THU (p165)
Bernhardt, Birgitta . . . . . CD-7.3 WED (p110),
CH-P.19 WED (p137)
Bernier, Martin . . . . . . . . . . CE-1.2 MON (p53),
CE-3.4 MON (p69), CM-P.14 MON (p77),
CJ-6.5 THU (p147)
Berrah, Nora . . . . . . . . . . . . JSI-4.6 WED (p134)
Berroir, Jérémy . . . . . . . . . . EA-2.3 THU (p144),
EA-7.4 FRI (p196)
Berroth, Manfred . . . . . . . CK-11.5 THU (p168)
Berškys, Justas . . . . . . . . . . ∙EC-P.13 FRI (p223)
Berthold, Lutz . . . . . . . . . . CH-6.2 WED (p116)
Berthou, Nicolas . . . . . . . . . . CH-4.4 TUE (p96)
Berti Ligabo, Joao Pedro
CK-P.36 TUE (p106), ∙EB-P.32 THU (p178)
Berto, Pascal . . . . . . . . . . . . . . CL-6.2 FRI (p191)
Bertolino, Mattias . . . . . . . JSI-4.3 WED (p130)
Bertoncini, Andrea . . . . . . CM-1.5 MON (p56),
CH-P.1 WED (p136)
Bertot, Francesco . . . . . . . . . CC-5.1 FRI (p188)
Bertrand, Mathieu . . . . . . ∙CB-8.4 THU (p144),
CB-8.5 THU (p146), CB-9.2 THU (p150),

CB-9.3 THU (p150), CH-13.2 FRI (p183),
ED-6.4 FRI (p194)
Berwian, Patrick . . . . . . . . EB-10.5 THU (p147)
Berz-Vöge, Dieter . . . . . . . EA-P.4 THU (p174)
Berzinš, Jonas . . . . . . . . . . . ∙CF-11.2 FRI (p203)
Besaga, Vira R. . . . . . . . . . ∙EB-P.34 THU (p178)
Besancon, Claire . . . . . . . . . . CB-5.3 TUE (p94)
Beugnot, J. C. . . . . . . . . . . . EF-P.15 WED (p140)
Beugnot, Jean-Charles . . CH-9.4 THU (p147),
CK-13.1 FRI (p188)
Beye, Martin . . . . . . . . . . . . JSI-2.6 WED (p120),
JSI-3.4 WED (p126)
Bezold, Vincent . . . . . . . . . . . EG-5.4 TUE (p96)
Bhadoria, Shikha . . . . . . . . CG-3.6 THU (p149)
Bhaktha, Shivakiran B N
EH-P.15 THU (p179)
Bhardwaj, Asha . . . . . . . . . . . . CI-P.9 FRI (p219)
Bhaskaran, Harish . . . . . . . JSIII-3.5 FRI (p187)
Bhattacharya, Utso . . . . . . CD-7.1 WED (p108)
Bhave, Sunil . . . . . . . . . . . . . . . CB-5.4 TUE (p96)
Bhorade, Onkar . . . . . . . . . EE-P.5 WED (p138),
CC-7.6 FRI (p216)
Bhorkar, Kapil . . . . . . . . . . . CH-16.3 FRI (p215)
Bi, Toby . . . . . . . . . . . . . . . . CK-5.1 WED (p114),
CD-10.5 WED (p132), CK-8.1 THU (p142),∙CK-8.6 THU (p148), EF-6.3 THU (p166),∙ED-6.1 FRI (p188)
Bi, Wei . . . . . . . . . . . . . . . . . . . CL-1.4 MON (p71)
Biabanifard, Mohammad
PP-2.11 WED (p121), EH-4.6 THU (p162),∙CL-4.6 THU (p169), EH-P.1 THU (p178)
Biagi, Gabriele . . . . . . . . . . . CK-P.6 TUE (p104)
Biagi, Nicola . . . . . . . . . . . . EB-P.22 THU (p177)
Biagioni, Paolo . . . . . . . . . . . EG-2.1 MON (p58)
Bianco, Giuseppe Valerio
EH-P.18 THU (p179), EH-P.19 THU (p179)
Bianco, Marco . . . . . . . . . . . CH-15.1 FRI (p201)
Bibi, Aisha . . . . . . . . . . . . . . ∙CH-13.6 FRI (p187)
Biegert, Jens . . . . . . . . . . . . . CD-P.5 TUE (p100),
CD-7.1 WED (p108), CG-3.5 THU (p147),
EC-P.6 FRI (p223)
Bieler, Mark . . . . . . . . . . . . . EE-1.4 WED (p113)
Bienert, Florian . . . . . . . . ∙CE-P.19 THU (p172)
Bieniek, Aleksandra . . . . . . . CB-5.2 TUE (p92),
CH-11.6 THU (p163), CE-10.5 FRI (p208)
Bienstman, Peter . . . . . . . . JSIII-3.5 FRI (p187),
JSIII-P.5 FRI (p224), JSIII-P.8 FRI (p224)
Biesenthal, Tobias . . . . . . . . EC-1.3 FRI (p185),
EC-2.1 FRI (p189), EC-P.3 FRI (p223)
Bigot-Astruc, Marianne . . . CD-4.1 TUE (p82)
Bilan, D. S. . . . . . . . . . . . . . . . . CL-7.1 FRI (p201)
Billard, Marie . . . . . . . . . . . EB-11.4 THU (p153)
BIllat, Adrien . . . . . . . . . . . . JSII-1.3 MON (p55)
Billault, Vincent . . . . . . . . . . ∙CI-7.5 FRI (p206)
Billet, Cyril . . . . . . . . . . . . . . . CM-4.1 TUE (p82)
Billotte, Thomas . . . . . . . CM-P.25 MON (p78)
Bilodeau, Simon . . . . . . . . . JSIII-5.4 FRI (p207)
Binnie, Iona . . . . . . . . . . . . . . CF-2.1 MON (p59)
Bird, David . . . . . . . . . . . . . . . CE-2.2 MON (p59)
Birks, Tim . . . . . . . . . . . . . . . JSII-2.1 MON (p59)
Birks, Tim A. . . . . . . . . . . . . CE-2.2 MON (p59),
CD-4.2 TUE (p82), CH-10.2 THU (p151)
Biswas, Rabindra . . . . . . . . . EJ-P.10 MON (p80)
Bitauld, David . . . . . . . . . . . . CB-5.3 TUE (p94)
Bitenc, Linda . . . . . . . . . . . CK-P.37 TUE (p106),
EG-P.7 TUE (p107)

Bizet, Laurent . . . . . . . . . . . CD-8.1 WED (p114)
Bjarki Helgason, Oskar . . CI-2.2 WED (p119),
ED-6.2 FRI (p190)
Blake, Alan . . . . . . . . . . . . . . . . CB-4.1 TUE (p90)
Blanc, Wilfried . . . . . . . . . CH-11.5 THU (p161)
Blanchard, François . . . . . CC-2.4 THU (p163)
Blanchard-Emmerson, Greg
CE-9.2 FRI (p190)
Blanchet, Valérie . . . . . . . . . JSI-5.5 THU (p149)
Blaser, Stéphane . . . . . . . . . CB-9.2 THU (p150)
Blatt, Rainer . . . . . . . . . . . . . . ∙EB-4.1 TUE (p83)
Blavette, Didier . . . . . . . . . CH-6.6 WED (p120)
Blázquez Martínez, Laura . ∙EF-7.3 FRI (p183)
Blésin, Terence . . . . . . . . . . . . CE-9.1 FRI (p188)
Blight, Daniel . . . . . . . . . . . . . CE-9.4 FRI (p194)
Blin, Stéphane . . . . . . . . . . CB-10.6 THU (p162)
Bloch, Daniel . . . . . . . . . . . . . ED-3.5 MON (p73)
Bloch, Jacqueline . . . . . . . . . ∙EC-1.1 FRI (p181)
Blöchl, Johannes . . . . . . . . . CK-1.6 MON (p72)
Block, Alexander . . . . . . . . . . . EI-4.5 FRI (p216)
Blondel, Christophe . . . . . CD-P.26 TUE (p101)
Blonskyi, Ivan . . . . . . . . . . . CM-2.5 MON (p62)
Blothe, Markus . . . . . . . . . . CM-2.3 MON (p60),∙CM-2.6 MON (p62), ∙CM-P.9 MON (p77)
Blum, Ivan . . . . . . . . . . . . . CH-6.6 WED (p120),
EE-P.5 WED (p138)
Blume, Gunnar . . . . . . . . ∙CB-11.5 THU (p168)
Bober, Marcin . . . . . . . . . . . . CE-3.2 MON (p67)
Bobkov, Konstantin . . . . . . CJ-5.3 WED (p131)
Bobzien, Laric . . . . . . . . . . . . EG-3.5 MON (p70)
Bock, Martin . . . . . . . . . . . CF-10.3 THU (p145),
CF-12.6 FRI (p217)
Bocoum, Maïmouna . . . . . CL-2.3 THU (p151)
Bodiou, Loïc . . . . . . . . . . . . CB-10.3 THU (p158)
Bodo, Elisabetta . . . . . . . . ∙PP-2.7 WED (p121),
CL-2.6 THU (p155), ∙CL-P.1 FRI (p221)
Boehm, Gerhard . . . . . . . . . . CC-4.6 FRI (p186)
Boemh, Gerhard . . . . . . . . . . . CB-4.3 TUE (p91)
Boes, Andreas . . . . . . . . . . . CK-4.3 WED (p112)
Boetti, Nadia . . . . . . . . . . . . CA-P.20 MON (p75)
Boetti, Nadia G. . . . . . . . . . ∙CJ-6.2 THU (p143)
Boeuf, Frédéric . . . . . . . . . . EB-3.1 MON (p67)
Bogaerts, Wim . . . . . . . . . . . CK-13.2 FRI (p190)
Bogdanowicz, Robert . . . . CE-7.4 THU (p169)
Bøggild, Peter . . . . . . . . . . . CC-1.3 THU (p153)
Bogoni, Antonella . . . . . . . . . CI-7.1 FRI (p200)
Bogris, Adonis . . . . . . . . CH-P.17 WED (p137),
CL-2.2 THU (p151), JSIII-1.1 THU (p156),
JSIII-3.4 FRI (p187), ∙EJ-3.4 FRI (p187)
Bogusławski, Jakub . . . . . ∙CD-P.3 TUE (p100),
CJ-P.21 FRI (p221)
Böhm, Fabian . . . . . . . . . . JSIII-1.2 THU (p158)
Böhm, Gerhard . . . . . . . . . . EH-3.1 THU (p148)
Bohus, János . . . . . . . . . . . . CG-P.3 THU (p173),
CC-P.2 FRI (p218)
Boikov, Ivan . . . . . . . . . . . ∙JSIII-2.1 THU (p162)
Boissier, Guilhem . . . . . . . . . CB-4.1 TUE (p90)
Boisvert, Mathieu . . . . . . . . . EC-2.4 FRI (p197)
Boivinet, Simon . . . . . . . . . . CJ-3.6 WED (p121)
Boll, Rebecca . . . . . . . . . . . . JSI-P.2 WED (p141),∙JSI-5.1 THU (p143)
Boller, Klaus-J . . . . . . . . . CD-10.1 WED (p128),
CD-14.1 FRI (p211)
Boller, Klaus-Jochen . . . . . . . CB-5.1 TUE (p92)
Bolognesi, Paola . . . . . . . . . . . EE-3.1 FRI (p189)
Boltersdorf, Eric . . . . . . . ∙CD-7.4 WED (p112)

228

Bonafe, Franco . . . . . . . . . EH-P.10 THU (p179)
Bonamis, Guillaume . . . . . CM-2.4 MON (p60),
CM-3.6 MON (p72)
Bonanomi, Matteo . . . . . . JSI-2.5 WED (p118),∙JSI-5.5 THU (p149)
Bonazzi, Thomas . . . . . . . . . . CH-4.4 TUE (p96)Bondani, Maria . . . . . . . . . EB-P.28 THU (p178)
Bonduelle, Myriam . . . . . ∙JSII-2.5 MON (p63),
JSII-P.3 MON (p80)
Bongarzone, Italia . . . . . . . CH-2.1 MON (p58),
CL-6.1 FRI (p189), CL-6.5 FRI (p197)
Bongs, Kai . . . . . . . . . . . . . EA-P.10 THU (p175),
EA-P.14 THU (p175)
Boni, Anisuzzaman . . . . . CB-11.1 THU (p162)
Boniface, Antoine . . . . . . . CM-1.3 MON (p54),
CM-11.2 FRI (p212)
BONNEAU, Marie . . . . . . CG-P.14 THU (p174)
Bonse, Jörn . . . . . . . . . . . . . ∙CM-2.1 MON (p58)
Bonvalet , Adeline . . . . . . . . CF-P.3 TUE (p102)
Bonvin, Eric . . . . . . . . . . . . . . . EA-9.3 FRI (p212)
Booker, Phillip . . . . . . . . . . CA-P.15 MON (p74)
Booth, Martin . . . . . . . . . . . CM-2.2 MON (p58)
Booth, Martin J. . . . . . . . . CM-7.5 WED (p112)
Bopp, Julian M. . . . . . . . . . CK-P.21 TUE (p105)
Borgstrom, Magnus . . . . . JSIII-5.2 FRI (p205)
Borisova, Gergana D. . . . . JSI-5.2 THU (p145)
Borme, Jerome . . . . . . . . . . . CK-13.3 FRI (p192)
Borne, Adrien . . . . . . . . . . . . EG-2.1 MON (p58)
Borodkin, Aleksei . . . . . . ∙CB-7.3 WED (p130)
Borodkin, Andrei . . . . . . . . ∙CJ-P.24 FRI (p221)
Boroviks, Sergejs . . . . . . . . . . EG-4.5 TUE (p88)
Borovkova, Mariia . . . . . . . . CL-6.4 FRI (p197)
Borówka, Sebastian . . . . . . . ∙EA-6.4 FRI (p186)
Borrego-Varillas, Rocio . . CF-1.3 MON (p57),
CF-2.4 MON (p61), CF-3.3 MON (p69),
CG-2.2 TUE (p97), PP-2.4 WED (p120),
CF-9.4 WED (p133), CG-5.3 THU (p159),
CG-P.1 THU (p173), EE-3.1 FRI (p189),
EE-3.4 FRI (p197)
Borri, Paola . . . . . . . . . . . . . . EG-P.4 TUE (p107),
CL-4.1 THU (p163)
Borri, Simone . . . . . . . . . . EF-P.16 WED (p140),
CH-14.2 FRI (p193)
Borsch, Markus . . . . . . . . . . CG-5.1 THU (p157)
Börzsönyi, Ádám . . . . . . . . . CF-P.6 TUE (p102),
CF-P.21 TUE (p103), CG-4.1 THU (p149),
CG-P.3 THU (p173)
Boschini, Fabio . . . . . . . . . . . CD-4.5 TUE (p86)
Boschker, Jos E. . . . . . . . . . . CB-P.5 MON (p75)
Bose, Surajit . . . . . . . . . . . . . . EJ-2.3 MON (p60),
CD-9.1 WED (p122), CD-9.4 WED (p124),∙EF-5.3 THU (p158), ∙EE-5.2 FRI (p211)
Bossini, Davide . . . . . . . . . . . . EE-5.1 FRI (p211)
Bostedt, Christoph . . . . . . JSI-1.2 WED (p110),
JSI-1.4 WED (p112), ∙JSI-4.1 WED (p128)
Bostedt, Chsirtoph . . . . . . JSI-3.2 WED (p124)
Botti, Silvana . . . . . . . . . . . . CG-3.3 THU (p145)
Botticelli, Michela . . . . . . . . CH-4.5 TUE (p98)
Bottrill, Kyle . . . . . . . . . . . . CK-6.3 WED (p124)
Boubekraoui, Ayoub . . . ∙CA-9.2 WED (p130)
Boubriak, Andriy . . . . . . ∙EB-P.16 THU (p177)
Boucaud, Philippe . . . . . . . CE-7.1 THU (p163)
Bouchard, Frédéric . . . . . . EB-7.3 WED (p117)
Boucher, Pauline . . . . . . . . . EA-3.3 THU (p150)
Bouchy, François . . . . . . . . JSII-2.4 MON (p63)
Boudebs, Georges . . . . . . . . CE-7.1 THU (p163)

Boudon, Vincent . . . . . . . . . ED-2.4 MON (p61)
Bougeard, Dominique . . . . . EG-4.3 TUE (p86)
Boullet, Johan . . . . . . . . . . . . . CJ-8.5 FRI (p196)
Bouloufa-Maafa, Nadia . . . . EA-7.5 FRI (p196)
BOURDAROT, Guillaume
JSII-1.5 MON (p57)
Bourderionnet, Jerome . . CJ-2.5 WED (p115),
CI-7.5 FRI (p206)
Bournet, Quentin . . . . . . . . CF-P.3 TUE (p102)
Bouscal, Adrien . . . . . . . . . . ∙EA-7.4 FRI (p196)
Bouscher, Shlomi . . . . . . . ∙EA-5.3 THU (p166),∙EB-13.5 THU (p169)
Boussafa, Yassin . . . . . . . CD-9.1 WED (p122),∙EF-P.10 WED (p140), EF-10.4 FRI (p215)
Boussafa, Yasssin . . . . . . . . CD-13.4 FRI (p205)
Boutin, Aurélien . . . . . . . . . CE-5.2 THU (p151)
Bouvier, Alexandre . . . . . . CE-5.2 THU (p151)
Bouville, David . . . . . . . . . . . CD-5.5 TUE (p91)
Bouwmans, Géraud . . . . CM-P.32 MON (p79),
CA-7.3 WED (p126), CH-P.1 WED (p136),
CH-10.1 THU (p149), ED-6.6 FRI (p196)
Bouwmeester, Dirk . . . . . . . . EB-5.5 TUE (p97),
EB-P.25 THU (p177)
Bouzin, Margaux . . . . . . . . CM-11.3 FRI (p214)
Bovolenta, Angela . . . . . . ∙CH-9.3 THU (p145)
Bowen Montague, Patrick CJ-P.22 FRI (p221)
Bowers, John . . . . . . . . . . . . EB-P.25 THU (p177)
Bowers, John E. . . . . . . . . . . . CB-5.6 TUE (p98)
Boxleitner, Winfried . . . . . EB-6.4 WED (p113)
Boyd, Keiron . . . . . . . . . . . . CA-8.1 WED (p114)
Boyer, Ambroise . . . . . . . . . . . EB-4.3 TUE (p87)
Boyero-García, R. . . . . . . . . CF-1.3 MON (p57)
Boyero-García, Roberto . . . . EI-2.3 FRI (p192)
Bozhevolnyi, Sergey . . . . . . CL-4.4 THU (p167)
Bozzio, Mathieu . . . . . . . . . . . EB-5.2 TUE (p93)
Bracker, Allan S. . . . . . . . . CE-P.21 THU (p172)
Bradley, Jonathan . . . . . . . CA-9.6 WED (p134)
Bradley, Thomas D. . . . . . . . CE-2.4 MON (p61)
Bragas, Andrea V. . . . . . . . . EH-3.2 THU (p150)
Brahms, Christian . . . . . . . . CF-3.3 MON (p69),
CD-4.2 TUE (p82), ∙CF-6.3 WED (p111),
EE-4.1 FRI (p201), EE-4.4 FRI (p205)
Braive, Rémy . . . . . . . . . . . . CK-12.1 FRI (p180),
EF-8.3 FRI (p195), JSIII-6.5 FRI (p217)
Brambilla, Gilberto . . . . CH-P.13 WED (p136),
CH-P.32 WED (p138),
CH-10.6 THU (p155)
Brambilla, Massimo . . . . . . CD-6.5 TUE (p96),
EF-2.4 WED (p133)
Bramerie, Laurent . . . . . . . . CD-4.1 TUE (p82),
CJ-2.3 WED (p113)
Brandenburg, Wolfgang . CA-6.6 WED (p114)
Brasch, Victor . . . . . . . . . . . JSII-2.4 MON (p63),
CD-5.2 TUE (p90)
Brask, Jonatan . . . . . . . . . . EB-P.30 THU (p178)
Brasse, Gurvan . . . . . . . . . . . . CE-8.5 FRI (p186)
Bratschitsch, Rudolf . . . . . . . . EI-2.5 FRI (p196)
Brauch, Uwe . . . . . . . . . . . . . CB-P.10 MON (p76)
Brauckmann, Michael . . CK-P.39 TUE (p106)
Braud, Alain . . . . . . . . . . . . . CA-3.2 MON (p68),
CA-3.3 MON (p68), CA-P.18 MON (p75),
CA-6.4 WED (p112), CA-9.4 WED (p132),
CA-11.2 THU (p150), CE-8.5 FRI (p186)
Brauda, Daniel . . . . . . . . . . CB-P.11 MON (p76)
Brecht, Benjamin . . . . . . CK-P.39 TUE (p106),
EA-4.5 THU (p160)

Authors' Index

Brecht, Olga . . . . . . . . . . . . . EA-4.5 THU (p160)
Bregolin, Filippo . . . . . . . CH-P.35 WED (p138)
Breitkopf, Sven . . . . . . . . . CF-P.21 TUE (p103),
CL-8.5 FRI (p215)
Brès, Camille-Sophie . . . . . . CD-6.4 TUE (p96)
Bresci, Arianna . . . . . . . . . . CH-2.1 MON (p58),∙CL-6.1 FRI (p189), CD-13.2 FRI (p203)
Bressanini, Gabriele . . . . . CD-13.6 FRI (p209)
Bretenaker, Fabien . . . . . . EF-P.12 WED (p140)
Breunig, Ingo . . . . . . . . . . . . ∙CD-6.3 TUE (p94),
CE-P.13 THU (p172)
Breuning, Felix . . . . . . . . . . . CF-3.1 MON (p67)
Brevet, Pierre-Francois . EG-6.1 WED (p108),
EH-P.6 THU (p178)
Brida, Daniele . . . . . . . . . . . EG-3.6 MON (p72),
EG-4.2 TUE (p84), EH-2.4 THU (p146),
EF-9.3 FRI (p205), CF-11.1 FRI (p201),
EI-4.3 FRI (p214)
Brieussel, Alexandre . . . . . . . EA-8.1 FRI (p200)
Brignon, Arnaud . . . . . . . . . . . CI-7.5 FRI (p206)
Brimis, Apostolos . . . . . ∙CM-P.11 MON (p77),∙CM-P.23 MON (p78), ∙EC-3.6 FRI (p209)
Brinkmann, Maximilian . EA-4.3 THU (p158),
CH-13.5 FRI (p187)
Britel, Adam . . . . . . . . . . . . . CM-4.2 TUE (p82)
Brito Carcaño, Jesus Eduardo∙CH-2.4 MON (p60)
Broasca, Alin . . . . . . . . . . . . CA-P.4 MON (p74)
Brockmeier, Julian . . . . . . . . . CI-5.5 FRI (p186)
Broda, Artur . . . . . . . . . . . . CB-P.12 MON (p76)
Brodbeck, Sebastian . . . . . . . EF-9.4 FRI (p205)
Broderick, Neil G. R. . . . . CJ-5.5 WED (p133),∙EF-P.11 WED (p140), EF-8.5 FRI (p197)
Brodzki, Jacek . . . . . . . . . . . EH-P.7 THU (p178)
Broeke, Ronald . . . . . . . . . CK-P.34 TUE (p106)
Brons, Jonathan . . . . . . . . . CF-10.6 THU (p149)
Brooks, Nathan J. . . . . . . . . . CF-2.1 MON (p59)
Brooks, William . . . . . . . . CH-10.3 THU (p151)
Broughton, Joseph . . . . . . . . EE-4.6 FRI (p209)
Brown, Ei Ei . . . . . . . . . . . . . ∙CA-3.1 MON (p66)
Brown, Tom . . . . . . . . . . . . . CL-3.5 THU (p161)
Brox, Olaf . . . . . . . . . . . . . . . . . CB-4.4 TUE (p91)
Bruce, Sandra . . . . . . . . . . CG-P.13 THU (p174)
Brückerhoff-Plückelmann, FrankJSIII-3.5 FRI (p187)
Brückner, Leon . . . . . . . . . . PD-1.7 THU (p170)
Brugnoni, Alessandro . . . CK-5.2 WED (p116)
Brune, Michel . . . . . . . . . . . . . EB-4.5 TUE (p89)
Brunel, Marc . . . . . . . . . . . . . CA-4.2 TUE (p82),
CA-4.5 TUE (p86), CI-P.12 FRI (p219)
Bruner, Barry D. . . . . . . . . . CG-5.4 THU (p161)
Brunk, Michael G. K. . . . . . CL-1.2 MON (p69)
Brunner, Daniel . . . . . . . JSIII-2.1 THU (p162),
JSIII-2.4 THU (p166), JSIII-4.5 FRI (p197),
JSIII-5.3 FRI (p205), ∙JSIII-6.1 FRI (p211),
JSIII-P.1 FRI (p224), JSIII-P.3 FRI (p224)
Brunner, Fabian . . . . . . . . CC-1.2 THU (p151),
CG-6.1 THU (p163)
Bruno, Giovanni . . . . . . . EH-P.18 THU (p179),
EH-P.19 THU (p179)
Bruno, Natalia . . . . . . . . . . EF-P.16 WED (p140)
Brunzell, Martin . . . . . . . . ∙CM-1.6 MON (p56)
BRYGOO, Stéphanie . . . . CG-P.14 THU (p174)
Buatier de Mongeot, Francesco
CK-15.1 FRI (p210)
Bubnov, Mikhail . . . . . . . . . CJ-5.3 WED (p131)

Bučar, K. . . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Bucci, Andrea . . . . . . . . . . . CH-6.4 WED (p118)
Buchberger, Gerda . . . . . . . . CM-9.4 FRI (p194)
Bucher, Tobias . . . . . . . . . CK-11.4 THU (p166)
Buchmann, Tobias O. . . . ∙CC-1.3 THU (p153)
Buchnev, Oleksandr . . . . . EH-P.7 THU (p178)
Buchvarov, Ivan . . . . . . . . CA-10.5 THU (p146),∙CD-11.2 FRI (p183)
Buck, Samuel . . . . . . . . . . . . CA-8.2 WED (p116)
Bucksbaum, Philip . . . . . . . JSI-4.6 WED (p134)
Buckthorpe, Martin . . . . . . . ∙CJ-P.5 FRI (p220)
Buckup, Tiago . . . . . . . . . . EH-P.14 THU (p179)
Buczynski, Ryszard . . . . EF-P.19 WED (p140),
CE-5.1 THU (p149), CE-7.4 THU (p169),∙CJ-9.1 FRI (p200)
Budai, Judit . . . . . . . . . . . . . EE-1.6 WED (p115),
EE-P.12 WED (p139), EH-2.2 THU (p144),
PD-1.2 THU (p170)
Budri ūnas, Rimantas . . CD-10.6 WED (p134),
CF-11.2 FRI (p203)
Bugar, Ignac . . . . . . . . . . . ∙EF-P.19 WED (p140)
Buldt, Joachim . . . . . . . . . . . CJ-2.2 WED (p111)
Bulgakov, Alexander . . . . CM-P.26 MON (p78)
Bulgakova, Nadezhda . . . CM-3.3 MON (p68),∙CM-P.7 MON (p77), CM-9.6 FRI (p196)
Bulygin, Andrey . . . . . . . . . . . EJ-P.4 MON (p80)Bundgaard-Nielsen, Matias
EG-1.1 MON (p52)
Bunel, Thomas . . . . . . . . . . ∙EF-3.3 THU (p144),∙PD-2.2 THU (p170)
Bürger, Andreas . . . . . CM-LIM.4 WED (p119)
Burghart, Dominik . . . . . . . ∙CB-4.3 TUE (p91),
CC-4.6 FRI (p186)
Burguete-Lopez, Arturo ∙CH-2.2 MON (p58),
JSIV-1.4 WED (p118), JSIII-P.6 FRI (p224),
JSIII-P.12 FRI (p225)
Burgy, Frédéric . . . . . . . . . . CG-P.4 THU (p173)
Burokas, Raimundas . . . . CA-P.14 MON (p74)
Burri, Florence . . . . . . . . . . . . CG-2.3 TUE (p99)
Busch, Kurt . . . . . . . . . . . . EA-P.16 THU (p175),
EJ-4.4 FRI (p195)
Busch, Robert . . . . . . . . . . CD-P.11 TUE (p100),
CD-P.16 TUE (p100)
Buse, Karsten . . . . . . . . . . . . . CD-6.3 TUE (p94),
CE-P.13 THU (p172)
Bussiere, Benoit . . . . . . . . . CG-P.3 THU (p173)
Busto, David . . . . . . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130)
Butaite, Une G. . . . . . . . . . . EG-6.6 WED (p114)
Butcher, Thomas . . . . . . . . CA-8.2 WED (p116)
Butkus, Antanas . . . . . . . . . CM-1.1 MON (p52)
Butkus, Arminas . . . . . . . . . CE-P.5 THU (p171)
Butkus, Simas . . . . . . . . . . . . CM-8.3 FRI (p182)
Butkutė, Agnė . . . . . . . . . . CM-P.27 MON (p78),∙CM-6.2 TUE (p92)
Butté, Raphaël . . . . . . . . . . CB-10.3 THU (p158)
Bux, Simone . . . . . . . . . . . . . CF-6.1 WED (p109)
Bykov, Alexander . . . . . . . . CL-1.5 MON (p73),∙EJ-P.6 MON (p80), CL-4.3 THU (p167),
CL-4.4 THU (p167), ∙CL-6.4 FRI (p197),
EJ-4.2 FRI (p191)
Bykov, Dmitry S. . . . . . . . . ∙PD-2.6 THU (p171)

C
C. Andrade, José R. . . . . . . ∙CM-6.4 TUE (p96)

C.G., Lakshmi . . . . . . . . . . . . . CJ-P.6 FRI (p220)
Cabrejo Ponce, Meritxell EB-P.3 THU (p176),
EB-P.20 THU (p177), EB-P.31 THU (p178)
Cáceres-Aravena, Gabriel CK-12.3 FRI (p182)
Cadier, Benoit . . . . . . . . . . . CJ-5.6 WED (p135),
CJ-P.18 FRI (p221)
Caffey, David . . . . . . . . . . . . . CD-6.5 TUE (p96)
Caglayan, Humeyra . . . . . . ∙EG-2.3 MON (p60)
Cai, Guanyu . . . . . . . . . . . . . . CE-4.5 TUE (p99),∙CE-10.4 FRI (p206)
Cai, Minglu . . . . . . . . . . . . . . ∙CJ-P.11 FRI (p220)
Caimi, Daniele . . . . . . . . . . . . CE-9.1 FRI (p188),
CK-14.5 FRI (p206)
Cajiao Vèlez, Felipe . . . . . . CG-P.8 THU (p174)
Cala Lesina, Antonio . . . . . EG-2.5 MON (p62)
Caldwell, Emily D. . . . . . . . ED-3.1 MON (p67)
Calegari, Francesca . . . . . ∙CF-1.1 MON (p53),
PP-1.5 MON (p64), CK-1.6 MON (p72),
CD-P.2 TUE (p100), JSI-5.3 THU (p145),
JSI-5.4 THU (p147), CG-3.2 THU (p143),
EE-4.1 FRI (p201)
Calero, Venancio . . . . . . . . . CE-5.2 THU (p151)
Callaghan, Jemma Elizabeth
CE-11.4 FRI (p214)
Callard, Ségolène . . . . . . . . CK-15.4 FRI (p214)
Callegari, C. . . . . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Callegari, Carlo . . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130), JSI-5.5 THU (p149)
Calvet, Laurie . . . . . . . . . . . JSIII-6.4 FRI (p215)
Calvez, Stéphane . . . . . . ∙CD-P.10 TUE (p100),
CH-P.16 WED (p137)
Calzavara, Florian . . . . . . . . CE-1.2 MON (p53)
Camacho, Joaquin J. . . . . CD-P.21 TUE (p101)
Camacho-Morales, Rocio CD-1.5 MON (p56),
PD-2.9 THU (p171)
Camarena, María . . . . . . . EG-6.4 WED (p112)
Camarneiro, Filipe . . . . . . . CK-13.3 FRI (p192)
Camenzind, Sandro . . . . . . CF-7.1 WED (p115)
Camenzind, Sandro L. . . . CC-2.2 THU (p161)
Campbell, Graeme . . . . . . . EF-6.3 THU (p166)
Campbell, Graeme N. . . . ∙CD-P.9 TUE (p100),∙EF-P.3 WED (p139)
Campos, Cecilia . . . . . . . . . CE-7.1 THU (p163)
Campos, Cecília L. A. V.CD-P.11 TUE (p100),∙CD-P.16 TUE (p100)
Camposeo, Andrea . . . . . . . CK-14.2 FRI (p202)
Camy, Patrice . . . . . . . . . . . . CA-2.4 MON (p62),
CA-3.2 MON (p68), CA-3.3 MON (p68),
CA-P.18 MON (p75), CA-4.5 TUE (p86),
CA-6.4 WED (p112), CA-9.4 WED (p132),
CA-11.2 THU (p150), CE-8.5 FRI (p186)
Canalias, Carlota . . . . . . . . . CD-2.4 MON (p60)
Canbaz, Ferda . . . . . . . . . . . ∙CE-P.5 THU (p171)
Cancio Pastor, Pablo . . . . CH-14.2 FRI (p193)
Canella, Francesco . . . . . . . PD-2.1 THU (p170)
Canioni, Lionel . . . . . . . . . . CE-3.4 MON (p69),∙CM-P.14 MON (p77)
Cankaya, Huseyin . . . . . . . . . CF-5.1 TUE (p93),
JSI-P.4 WED (p141)
Cannizzo, Andrea . . . . . . . JSI-1.2 WED (p110),
JSI-1.4 WED (p112)
Cao, Cuong . . . . . . . . . . . . . . CH-13.6 FRI (p187)
Cao, Huabao . . . . . . . . . . . ∙CF-P.11 TUE (p103)
Cao, Hui . . . . . . . . . . . . . . . . CH-1.2 MON (p53),∙CJ-1.5 TUE (p99), ∙CJ-6.6 THU (p149),

229∙EF-4.1 THU (p148), EC-P.10 FRI (p223)
Cao, Kaixiang . . . . . . . . . . . CK-5.3 WED (p116)
Cao, Yulong . . . . . . . . . . . . . . . ED-5.5 FRI (p186)
Capasso, Federico . . . . . . . . CD-6.5 TUE (p96),
EF-2.4 WED (p133), CB-8.1 THU (p142),
CB-8.2 THU (p142), CK-11.6 THU (p168),
EH-5.2 THU (p164)
Capelli, Alessandro . . . . . . JSIII-3.3 FRI (p185)
Capelli, Marco . . . . . . . . . . . . CA-5.3 TUE (p96)
Capezzuto, Marialuisa . . . CH-2.5 MON (p62),
CK-13.5 FRI (p196)
Capmany, Juan . . . . . . . . . . CD-P.33 TUE (p102)
Cappelli, Chiara . . . . . . . . . EJ-2.2 MON (p60),
EH-P.20 THU (p179)
Cappelli, Francesco . . . . EF-P.16 WED (p140),
CC-4.4 FRI (p184)
Cappenberg, Federico . . . . CF-3.3 MON (p69)
Caramia, Lorenzo . . . . . . EH-P.18 THU (p179)
Carbone, Fabrizio . . . . . . . . . CK-3.4 TUE (p96)
Cardinal, Thierry . . . . . . . . . CE-1.2 MON (p53)
Cardinali, Giulia . . . . . . . . . CB-2.3 MON (p68)
Cardoso, Gil . . . . . . . . . . . . CK-10.3 THU (p158)
Cardozo de Oliveira, Edson R.
JSVI-1.1 TUE (p83)
Carena, Andrea . . . . . . . . . ∙CI-4.2 WED (p131)
Cargioli, Alessio . . . . . . . . ∙CB-9.2 THU (p150)
Carlet, Vincent . . . . . . . . . . . CI-P.12 FRI (p219)
Carletti, Luca . . . . . . . . . . . . PD-2.8 THU (p171)
Carlini, Laura . . . . . . . . . . . . . EE-3.1 FRI (p189)
Carlström, Stefanos . . . . JSI-4.3 WED (p130),
CG-5.2 THU (p159)
Carmichael, Howard . . . . . . EA-1.3 TUE (p85),
EA-1.5 TUE (p87)
Carnemolla, Enrico Giuseppe∙CE-11.4 FRI (p214)
Carpeggiani, Paolo . . . . . . . CF-12.4 FRI (p215)
Carpeggiani, Paolo A. . . . . CD-2.2 MON (p58)
Carpintero, Guillermo . . . . . CE-9.3 FRI (p192)
Carrà, Luca . . . . . . . . . . . . . . . CD-6.1 TUE (p92)
Carraria Martinotti, Ludovico
JSIII-3.1 FRI (p181)
Carras, Mathieu . . . . . . . . CB-9.4 THU (p152),
CH-16.5 FRI (p217)
Carreira, Jose . . . . . . . . . . . . CK-P.8 TUE (p104),
CA-9.6 WED (p134)
Carreto, Romain . . . . . . . . CA-11.5 THU (p152)
Carron, Igor . . . . . . . . . . . . . JSIII-3.3 FRI (p185)
Carry, Émile . . . . . . . . . . . . . ED-3.2 MON (p69)
Caruso, Filippo . . . . . . . . . EB-7.1 WED (p115)
Carusotto, Iacopo . . . . . . . . . EC-2.4 FRI (p197)
Carvacho, Gonzalo . . . . . . . . EB-5.3 TUE (p95),
EB-6.1 WED (p109)
Carvalho, Alyson J. A. . ∙CD-P.11 TUE (p100)
Carvalho, João C A . . . . . EA-P.23 THU (p176)
Casabone, Bernardo . . . . . . . EG-5.1 TUE (p92)
Caspani, Lucia . . . . . . . . . . EA-P.22 THU (p175)
Cassagnettes, Cedric . . . . JSII-1.3 MON (p55)
Cassan, Eric . . . . . . . . . . . . . . EB-3.1 MON (p67)
Cassez, Andy . . . . . . . . . . . CH-P.1 WED (p136),
ED-6.6 FRI (p196)
Cassim, Thibaut . . . . . . . . . CJ-3.6 WED (p121)
Castaing, Marc . . . . . . . . . CM-P.25 MON (p78)
Castelló-Lurbe, David . ∙CD-P.22 TUE (p101),∙EF-P.13 WED (p140)
Castiglia, Antonino . . . . . CB-11.6 THU (p168)
Castillejo, Marta . . . . . . . . CD-P.21 TUE (p101)

Casto, Alessandro . . . . . . . . JSVI-1.4 TUE (p89)
Castro-Marin, Pablo . . . . CF-7.6 WED (p121),∙CH-10.4 THU (p153)
Cataluna, Maria Ana . . . . CF-7.2 WED (p117),
CB-7.1 WED (p128), CB-7.6 WED (p134)
Catani, Jacopo . . . . . . . . . . . . CC-4.4 FRI (p184)
Catanzaro, Dominic . . . . EB-11.1 THU (p149)
Catoire, Fabrice . . . . . . . . . CG-4.6 THU (p155),
CG-6.2 THU (p165), CG-P.4 THU (p173)
Cattaneo, Laura . . . . . . . . . . ∙CF-2.5 MON (p63)
Cattaneo, Paolo . . . . . . . . . . . CK-3.4 TUE (p96)Caut, Alexander . . . . . . . . . CK-9.3 THU (p152)
Cavagnetto, Matteo . . . . . . CL-2.5 THU (p153)
Cavaillès, Adrien . . . . . . . . . . EB-4.3 TUE (p87),∙EA-3.3 THU (p150)
Ceballos, Mailyn . . . . . . . . CA-P.20 MON (p75),
CJ-6.2 THU (p143)
Ceccarelli, Francesco . . . . EB-6.1 WED (p109),∙CK-7.1 WED (p128), EA-8.1 FRI (p200)
Cecconi, Vittorio . . . . . . ∙CH-1.1 MON (p53),∙CC-3.5 THU (p169), ED-6.3 FRI (p192)
Ceconello, Chiara . . . . . . . CH-2.1 MON (p58),
CL-6.1 FRI (p189), CD-13.2 FRI (p203)
Cegielski, Piotr . . . . . . . . . . CA-9.3 WED (p130)
Celebrano, Michele . . . . . ∙EG-2.1 MON (p58),∙PD-2.8 THU (p171)
ceneda, Daniele . . . . . . . . . ∙JSVI-2.5 TUE (p99)
Centini, Marco . . . . . . . . . . . CE-3.5 MON (p71),
JSVI-2.4 TUE (p97), JSVI-2.5 TUE (p99)Černeckytė, Augustė . . . . . . CA-P.5 MON (p74)
Cerullo, G. . . . . . . . . . . . . . . . . . EI-2.1 FRI (p188)
Cerullo, Giulio . . . . . . . . . . ED-1.2 MON (p53),
CH-2.1 MON (p58), ED-P.2 MON (p79),
CH-8.4 WED (p133), CL-6.1 FRI (p189),
CL-6.5 FRI (p197), CD-13.2 FRI (p203),
CM-11.3 FRI (p214), EI-4.2 FRI (p212),
EI-4.4 FRI (p214)
Cerutti, Laurent . . . . . . . . . . CB-4.1 TUE (p90),
CB-4.2 TUE (p90)
César Cuello, Jessica . . . . . . ∙CE-9.3 FRI (p192)
Cesca, Tiziana . . . . . . . . . . . JSVI-2.5 TUE (p99)
Cézard, Nicolas . . . . . . . . . . . CJ-6.4 THU (p145)
Chabaud, Ulysse . . . . . . . . EB-12.2 THU (p159)
Chabrol, Gregoire . . . . . . . . CE-1.6 MON (p57)
Chaiwongkhot, Poompong
EB-P.14 THU (p177)
Chakrabarti, Arnab . . . . . . EB-7.2 WED (p117)
Chakraborty, Arup Lal . . EH-P.17 THU (p179)
Chalupa-Gantner, Franziska∙CM-P.17 MON (p78)
Chalus, Olivier . . . . . . . . . ∙CA-P.22 MON (p75)
Chambinaud, Axel . . . . . . . CD-14.2 FRI (p213)
Chambonneau, Maxime ∙CM-2.3 MON (p60),
CM-2.6 MON (p62), CM-P.9 MON (p77)
Chamorovskiy, Alexander . CL-8.1 FRI (p211)
Chan, Christopher C. S. . . EG-P.8 TUE (p107)
Chan, Eng Aik . . . . . . . . . . . PP-1.7 MON (p64),
CH-P.8 WED (p136), CH-12.6 THU (p169)
Chan, Ryan Ka Yan . . . . . . . . ∙EJ-3.5 FRI (p187)
Chanelière, Thierry . . . . . . . EA-9.2 FRI (p210)
Chang, Taeyong . . . . . . . ∙CK-P.10 TUE (p104),∙CH-12.6 THU (p169)
Chang, Xinshuo . . . . . . . . . . . CD-4.6 TUE (p88)
Chang, Young Jun . . . . . . . . CE-7.3 THU (p167)
Chang, Zhenghu . . . . . . . . . . ED-5.5 FRI (p186)
Chapman, Richard T. . . . ∙CF-P.22 TUE (p103)

Authors' Index

Chapman, Robert J. . . . . . . CK-1.1 MON (p66),∙EB-13.1 THU (p163)
Chapron, Nicolas . . . . . . . . . . CA-4.5 TUE (p86)Charczun, Dominik . . . . . . CE-3.2 MON (p67),
ED-4.2 TUE (p83)Charrier, Joël . . . . . . . . . . . CB-10.3 THU (p158)
Charsley, Jake . . . . . . . . . . . . ∙CH-4.5 TUE (p98)
Chartrand, Caitlin . . . . . . . CC-3.2 THU (p165)
Chauhan, Purujit Singh . EB-P.34 THU (p178)
Chausse, Pierre . . . . . . . . . . . CD-6.4 TUE (p96)
Chauveau, Jean-Marc . . . CH-6.6 WED (p120)
Chauveau, Jean-Michel . . . EG-P.5 TUE (p107)
Chaves, Bruno . . . . . . . . . . . . ∙EE-5.3 FRI (p213)
Chebotarev, A. S. . . . . . . . . . ∙CL-7.1 FRI (p201)
Checchinato, Riccardo ∙EB-11.2 THU (p151),
EB-P.24 THU (p177)
Chekhova, Maria . . . . . . . . PD-2.8 THU (p171)
Chellu, Abhiroop . . . . . . . ∙EG-1.4 MON (p56),∙EB-P.12 THU (p177)
Chemnitz, Mario . . . . . . . . . CI-4.6 WED (p135)
Chen, Bowen . . . . . . . . . . . . . . CI-P.4 FRI (p219),∙CI-P.5 FRI (p219)
Chen, Chaobo . . . . . . . . . . . . CM-5.1 TUE (p90)Chen, Chun-Wei . . . . . . . . . . CJ-1.5 TUE (p99),
CJ-6.6 THU (p149)
Chen, Eng Aik . . . . . . . . . . . PP-1.6 MON (p64),
CH-P.4 WED (p136)
Chen, Fu-Der . . . . . . . . . . . . . CL-1.2 MON (p69)Chen, Gaowen . . . . . . . . . . ∙CB-P.17 MON (p76)Chen, Gong . . . . . . . . . . . . . . CE-11.3 FRI (p214)
Chen, Hui . . . . . . . . . . . . . . . . ∙CA-5.5 TUE (p98)
Chen, Hui-Yuan . . . . . . . . ∙EE-1.5 WED (p113)
Chen, Jianping . . . . . . . . . . CK-5.5 WED (p118),
CJ-P.11 FRI (p220)
Chen, Jihan . . . . . . . . . . . . . CK-P.40 TUE (p106)
Chen, Jinghan . . . . . . . . . . . ∙CK-3.3 TUE (p94),
CK-5.4 WED (p118)
Chen, Ming-Chang . . . . . . . CF-2.2 MON (p59)
Chen, Shen-Chen . . . . . . . . CE-P.8 THU (p172)
Chen, Shuyang . . . . . . . . . . . . CL-P.7 FRI (p222)
Chen, Weidong . . . . . . . . . . CA-2.1 MON (p58),
CA-P.18 MON (p75), CA-P.19 MON (p75),∙CH-P.36 WED (p138),∙CA-10.3 THU (p144),∙CA-10.6 THU (p148),∙CH-16.1 FRI (p211), CF-12.5 FRI (p215)
Chen, Xiao . . . . . . . . . . . . . . CG-3.3 THU (p145)
Chen, Yang . . . . . . . . . . . . . . . . CE-8.1 FRI (p180)
Chen, Yi . . . . . . . . . . . . . . . CH-P.30 WED (p138)
Chen, Yu-Hua . . . . . . . . . . . . CL-P.13 FRI (p222)
Chen, Yu-Shao . . . . . . . . . . ∙CK-P.7 TUE (p104),
CE-P.15 THU (p172)
Chen, Yujin . . . . . . . . . . . . CA-10.3 THU (p144)
Cheng, Chia-Sheng . . . . . CK-P.40 TUE (p106)
Cheng, Chuang-Chia . . . . CL-P.19 FRI (p222)
Cheng, Tonglei . . . . . . . . . . . . CJ-7.3 FRI (p184)
Cheng, Weibo . . . . . . . . . . . CM-3.1 MON (p66)
Cheng, Ya . . . . . . . . . . . . . . . . CM-3.1 MON (p66)
Cheng, Yuk Shan . . . . . . . . . ∙ED-6.5 FRI (p196)
Cheng, Zihao . . . . . . . . . . ∙CD-P.27 TUE (p101)
Cherchi, Matteo . . . . . . . . . . . CB-5.5 TUE (p96)
Chergui, Majed . . . . . . . . . JSI-1.4 WED (p112),
EE-1.5 WED (p113)
Chériaux, Gilles . . . . . . . . . . . CF-5.3 TUE (p97)
Chernysheva, Maria . . . . CJ-3.1 WED (p115),
CJ-4.3 WED (p125), CJ-4.5 WED (p127),∙CJ-8.1 FRI (p188)
Cherotchenko, Evgeniia . . CB-9.5 THU (p152)
Chevreuil, Pierre-Alexis . CG-6.1 THU (p163)
Chi, Cheng-Hung . . . . . . ∙CH-6.5 WED (p118)
Chiappini, Andrea . . . . . . . CM-4.2 TUE (p82)
Chiavaioli, Francesco . . . . ∙CL-1.4 MON (p71)
Chichkov, Boris . . . . . . . . . . EG-2.5 MON (p62)
Chichkov, Nikolai . . . . . . . . . . CJ-P.3 FRI (p220)
Chien, Fan-Ching . . . . . CH-P.34 WED (p138),
CH-13.4 FRI (p185), ∙CL-P.19 FRI (p222)
Chien, Ying-Hao . . . . . . . . CG-3.5 THU (p147)
China, Fumihiro . . . . . . . . EA-2.2 THU (p142),
EB-P.9 THU (p176)
Chini, Michael . . . . . . . . . . . . CF-3.2 MON (p67)
Chiriano, Fabrizio . . . . . . ∙CD-14.3 FRI (p215)
Chirico, Giuseppe . . . . . . CM-11.3 FRI (p214)
Chistyakov, Dmitriy . . . . . CB-9.5 THU (p152)
Chlouba, Tomáš . . . . . . . . . EA-4.2 THU (p158),
PD-1.7 THU (p170)
Chmielewski, Krzysztof . CB-P.21 MON (p76)
Chochon, Anaïs . . . . . . . . . . . EA-7.4 FRI (p196)
Choi, Dong J. . . . . . . . . . . . . CK-7.4 WED (p132)
Choi, Duk . . . . . . . . . . . . . CK-11.4 THU (p166)
Choi, Duk-Yong . . . . . . . . . . CE-4.2 TUE (p93),
EH-3.6 THU (p154), CD-12.5 FRI (p197)
Choi, Seungman . . . . . . . . CD-P.13 TUE (p100)
CHOLLET, Clément . . . . CG-P.14 THU (p174)
Chomet, Baptiste . . . . . . ∙CB-10.6 THU (p162)
Choong, Gregory . . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
Chopin, Alexandre . . . . . . . ∙EA-8.5 FRI (p208)
Chordiya, Kalyani . . . . . . . . . CC-P.2 FRI (p218)
Choudhary, Amol . . . . . . . CD-P.6 TUE (p100),∙CD-P.32 TUE (p102), CD-12.3 FRI (p193),
CD-12.4 FRI (p195), CI-7.6 FRI (p208),∙CI-8.6 FRI (p216), CI-P.8 FRI (p219)
Chow, Chang Hoong . . . . EA-P.3 THU (p174),
EB-P.11 THU (p176)
Chow, Weng W. . . . . . . . . . . . . CB-5.6 TUE (p98)
Chowdhury, Sarah . . . . . . CE-P.26 THU (p173)
Christ, Marc . . . . . . . . . . . . . ∙EB-1.4 MON (p57)
Christan-Edwards, Alice EB-P.27 THU (p177)
Christiansen, Rasmus E. . . EG-P.9 TUE (p107)
Christie, Mary L. . . . . . . . PP-2.8 WED (p121),
CL-5.5 FRI (p187), CL-P.2 FRI (p221)
Christodoulides, Demetrios N.
EC-1.5 FRI (p187), EC-P.2 FRI (p223)
Christodoulides, Joseph . . . EI-P.4 FRI (p224)
Christopher, Heike . . . . . . CF-6.5 WED (p113),
CB-11.2 THU (p164)
Christopoulos, Thomas . CK-P.41 TUE (p106)
Chrostek-Mroza, Aneta . . . CM-8.5 FRI (p186)
Chu, Hong . . . . . . . . . . . . . . . CD-P.4 TUE (p100)
Chu, Hongwei . . . . . . . . . . . . CA-3.2 MON (p68)Chu, S. T. . . . . . . . . . . . . . . EF-P.15 WED (p140)
Chu, Sai . . . . . . . . . . . . . . . . . . ED-6.3 FRI (p192),
EE-5.3 FRI (p213)
Chua , Sheon . . . . . . . . . . . . . EA-9.4 FRI (p214)
Chun, Seung-Hyun . . . . . . . . . EI-1.5 FRI (p186)
Chung, Wei . . . . . . . . . . . . . . CL-P.19 FRI (p222)
Churaev, Mikhail . . . . . . . . ∙CE-9.1 FRI (p188),
CK-14.5 FRI (p206)
Churchill, Glenn . . . . . . . . CA-6.3 WED (p110)
Churchill, Glenn M . . . . . . . CE-8.6 FRI (p186),
CE-9.2 FRI (p190)
Chyla, Michal . . . . . . . . . . . . CA-P.1 MON (p74)

Ciappina, Marcelo . . . . . . . CD-7.1 WED (p108)
Cibella, Sara . . . . . . . . . . . . . . CC-4.1 FRI (p180),
CC-4.5 FRI (p186)
Cich, Matthew . . . . . . . . . . CH-5.2 WED (p113)
Cid-Lara, Christofer . . . . CK-P.27 TUE (p105)
Cidrim, Andre . . . . . . . . . . EB-P.35 THU (p178)
Ciers, Anastasiia . . . . . . . ∙EA-3.1 THU (p148),
CK-15.3 FRI (p212)
Ciers, Joachim . . . . . . . . . . . . CB-2.3 MON (p68)
Cimrman, Martin . . . . . . . . CA-P.1 MON (p74)
Cinquanta, Eugenio . . . . . CE-P.10 THU (p172)
Cinquegrana, Paolo . . . . . ∙JSI-P.7 WED (p141)
Cipolato, Oscar . . . . . . . . . . CK-14.2 FRI (p202)
Ciraci, Cristian . . . . . . . . . ∙EH-3.4 THU (p152)
Cirelli, Claudio . . . . . . . . . . JSI-1.4 WED (p112)
Ciriolo, Anna G. . . . . . . . . . CM-6.3 TUE (p94)
Cirmi, Giovanni . . . . . . . . . JSI-P.4 WED (p141),
JSI-5.3 THU (p145)
Citrin, D.S. . . . . . . . . . . . . . . CC-P.10 FRI (p218)
Ciuciulkaite, Agne . . . . . . . EH-2.4 THU (p146)
Clady, Raphaël . . . . . . . . . . CM-3.4 MON (p68),∙CL-4.2 THU (p165)
Clark, Alex . . . . . . . . . . . . . . . EB-2.2 MON (p61)
Clark, Alex S. . . . . . . . . . . . EB-8.5 WED (p127),
CD-13.6 FRI (p209)
Clarke, Edmund . . . . . . . . . PD-1.9 THU (p170)
Clarkson, W. Andrew . . . ∙CA-7.2 WED (p126)
Clarkson, William . . . . . . . . . CJ-P.5 FRI (p220)
Claronino, Peter . . . . . . . . . . . EI-4.2 FRI (p212)
Classen, Anton . . . . . . . . . . . CH-1.5 MON (p57)
Claude, Jean Benoit . . . . . . . EG-5.5 TUE (p96),
PP-2.12 WED (p121), EH-P.16 THU (p179)
Clausen-Schaumann, Hauke
PP-1.9 MON (p64), CM-P.5 MON (p77)
Clemmen, Stephane . . . . . . CD-3.2 MON (p68)
Clerc, Marcel G. . . . . . . . . . . . EF-8.3 FRI (p195),
JSIII-6.5 FRI (p217), EF-10.1 FRI (p211)
Climente, Juan I. . . . . . . . . CE-P.21 THU (p172)
Coates, Michael R. . . . . . . . . . EE-3.2 FRI (p193)
Cobet, Munise . . . . . . . . . . . . CB-2.3 MON (p68)
Codemard, Christophe . CH-11.4 THU (p161)
Coen, Stephane . . . . . . . . . CD-8.5 WED (p120),
CD-9.3 WED (p124),
CD-10.3 WED (p130),
CD-10.4 WED (p132), EF-3.4 THU (p144),
EF-3.6 THU (p148), PD-2.7 THU (p171)
Coffee, Ryan . . . . . . . . . . . . . JSI-4.6 WED (p134)
Cohadon , Pierre-François EA-9.4 FRI (p214)
Cohen, Mathis . . . . . . . . . ∙EB-11.4 THU (p153)
Cohen, Noa E. . . . . . . . . . . . CL-P.14 FRI (p222)
Coish, William . . . . . . . . . . . . EC-2.4 FRI (p197)
Cojocaru, Crina . . . . . . . . CD-P.31 TUE (p102),
CD-7.5 WED (p112), EH-3.5 THU (p152),
EH-P.19 THU (p179)
Colacion, Gabriel . . . . . . . . EF-2.1 WED (p129)
Colaizzi, Lorenzo . . . . . . . . CF-1.3 MON (p57),
CF-3.3 MON (p69), CG-3.2 THU (p143),
EE-3.1 FRI (p189), EE-3.4 FRI (p197)
Colautti, Maja . . . . . . . . . . . EA-4.1 THU (p156)
Cole, Garrett D. . . . . . . . . . . CE-3.2 MON (p67),
CE-6.1 THU (p157)
Collard, Liam . . . . . . . . . . . . CH-15.1 FRI (p201)
Collier, John . . . . . . . . . . . . CA-8.2 WED (p116)
Collini, Maddalena . . . . . . CM-11.3 FRI (p214)
Collombon, Mathieu . . . . . ED-1.1 MON (p53)
Colmbrié, Sylvain . . . . . . . . CD-2.5 MON (p62)230

Colmenares Q., Juan Carlos
JSIV-1.3 WED (p118)
Colombo, Alessandro . . . . JSI-3.1 WED (p122)
Columbo, Lorenzo . . . . . . . . CD-6.5 TUE (p96),
EF-2.4 WED (p133)
Columbo, Lorenzo L. . . . . CB-6.2 WED (p124)
Combrié, Sylvain . . . . . . . . . EA-8.5 FRI (p208),
JSIII-6.2 FRI (p213)
Concetta Canino, Maria . CH-14.2 FRI (p193)
Conci, Claudio . . . . . . . . . . CM-11.3 FRI (p214)
Conejero, J. Alberto . . . . . . EF-P.5 WED (p139)
Conejero, José Alberto . . . EF-6.6 THU (p168)
Conejero Jarque, Enrique CF-1.3 MON (p57),
EE-P.8 WED (p138)
Conforti, Matteo . . . . . . . . . EF-3.3 THU (p144),
PD-2.2 THU (p170), ED-6.6 FRI (p196)
Congar, Antoine . . . . . . . . CB-10.3 THU (p158)
Connelly, Blair C. . . . . . . . ∙CE-6.6 THU (p163)
Conper, Nigel . . . . . . . . . CH-P.33 WED (p138)
Conrad, Johanna . . . . . . . ∙EB-P.20 THU (p177)
Conradt, Frieder . . . . . . . . . . EG-5.4 TUE (p96)
Consolino, Luigi . . . . . . . EF-P.16 WED (p140),
CC-4.4 FRI (p184), CK-13.5 FRI (p196)
Constancias, Christophe
CH-P.22 WED (p137)
Constant, Eric . . . . . . . . . ∙CG-4.6 THU (p155),
CG-6.2 THU (p165), CG-P.4 THU (p173)
Constantin, Florin Lucian∙ED-1.4 MON (p57)
Contestabile, Giampiero . JSIII-3.2 FRI (p183)
Conti, Claudio . . . . . . . . . . CH-2.5 MON (p62),∙PL-2a.1 TUE (p90), CC-6.4 FRI (p206),
EF-10.5 FRI (p215)
Conti, Fabrizio . . . . . . . . . . . EG-2.1 MON (p58)
Coolen, Laurent . . . . . . . . . CK-12.6 FRI (p186)
Cooper, Eric . . . . . . . . . . . . . . . EA-7.3 FRI (p192)
Cooray, Vernon . . . . . . . . . CD-8.1 WED (p114)
Copie, François . . . . . . . . . ∙EF-P.2 WED (p139),∙EF-7.6 FRI (p187), EF-9.5 FRI (p207),
EF-9.6 FRI (p209)
Corbijn van Willenswaard, Lars J.
CK-P.30 TUE (p105), CK-P.33 TUE (p106),
CK-P.38 TUE (p106)
Cordaro, Andrea . . . . . . . . ∙EH-5.1 THU (p162)
Cordier, Martin . . . . . . . . . . . EA-1.2 TUE (p83),∙EA-7.2 FRI (p190), CD-14.2 FRI (p213)
Cordones, Amy A. . . . . . . . . . EE-3.3 FRI (p195)
Coreno, M. . . . . . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Coreno, Marcello . . . . . . . . JSI-2.5 WED (p118)
Corkum, Paul . . . . . . . . . . . . . CF-3.2 MON (p67)
Corkum, Paul B. . . . . . . . . . . CD-4.5 TUE (p86)Cormier, Eric . . . . . . . . . . . . . CJ-8.5 FRI (p196)
Corney, Joel F. . . . . . . . . . . . EB-2.1 MON (p59)
Corni, Stefano . . . . . . . . . . . . . EG-4.2 TUE (p84)
Corre, Yann . . . . . . . . . . . . CM-P.32 MON (p79)
Corrias, Nicola . . . . . . . . . EF-P.16 WED (p140)
Corrielli, Giacomo . . . . . . JSII-P.1 MON (p80),
EB-6.1 WED (p109), EA-8.1 FRI (p200)
Corso Silva, Cassia . . . . . . . CD-13.3 FRI (p205)
Cortes, Emiliano . . . . . ∙JSIV-1.1 WED (p114),
EH-3.2 THU (p150)
Corti, Matteo . . . . . . . . . . . CH-8.4 WED (p133)
Corzo, Daniel . . . . . . . . . . . CE-5.5 THU (p153)
Cossart, Rosa . . . . . . . . . . . CH-P.1 WED (p136)
Costa Lima, Bismarck . . . ∙CJ-P.16 FRI (p220)

Cotrufo, Michele . . . . . . . . EH-3.1 THU (p148)
Couchot, François . . . . . . . PD-2.3 THU (p171)
Coudé du Foresto, Vincent
JSII-3.4 MON (p71)
Couderc, Vincent . . . . . . CD-9.1 WED (p122),
EF-7.4 FRI (p185), EF-7.5 FRI (p187),
CD-13.3 FRI (p205), CD-13.4 FRI (p205),
EE-5.3 FRI (p213)
Couderd, Vincent . . . . . . . . . . EF-7.1 FRI (p181)
Coudevylle, Jean-René . . . . CD-5.5 TUE (p91),
JSIII-6.5 FRI (p217)
Coudreau, Sébastien . . . . . CF-9.3 WED (p131)
Coulais, Corentin . . . . . . . . EH-4.3 THU (p158)
Coulibaly, Saliya . . . . . . . . . . EF-10.1 FRI (p211)
Courjal, Nadège . . . . . . . . . JSII-2.5 MON (p63),
JSII-P.3 MON (p80), ∙CE-5.2 THU (p151)
Courvoisier, Francois . . . CM-3.5 MON (p70),
CM-4.1 TUE (p82), CM-8.6 FRI (p186),∙EE-2.2 FRI (p185)
Couturier, Raphaël . . . . . . . CH-2.4 MON (p60)
Covre da Silva, Saimon . . . . EB-5.3 TUE (p95)
Cox, Emma . . . . . . . . . . . . . . CE-11.4 FRI (p214)
Cox, Joel D. . . . . . . . . . . . . . . . EG-4.5 TUE (p88)
Cozic, Solenn . . . . . . . . . . . . CE-1.5 MON (p57),
CJ-P.3 FRI (p220)
Crego, Aurora . . . . . . . . . . . . CF-3.3 MON (p69),∙CF-9.4 WED (p133), CG-5.3 THU (p159)
Crespi, Andrea . . . . . . . . . ∙CK-6.5 WED (p126),
CK-7.1 WED (p128), EA-8.1 FRI (p200)
Crespo, Helder . . . . . . . . CD-P.18 TUE (p101),
CB-7.6 WED (p134), PD-1.3 THU (p170),
CL-7.4 FRI (p205)
Crespo López-Urrutia, José R.
ED-P.5 MON (p79), CF-8.2 WED (p125),
CG-6.5 THU (p169)
Crippa, Gabriele . . . . . . . . . CM-6.3 TUE (p94),
CE-P.10 THU (p172)
Crisafi, Francesco . . . . . . . . . CL-6.5 FRI (p197)
Cristea, Dana . . . . . . . . . . . . . ∙CK-2.2 TUE (p86)
Cristescu, Simona M. . . CH-P.23 WED (p137),
CH-16.2 FRI (p213)
Cristiani, Ilaria . . . . . . . . . . CK-5.2 WED (p116)
Croitoru, Gabriela . . . . . . . ∙CA-P.4 MON (p74)
Croquette , Michaël . . . . . . . EA-9.4 FRI (p214)
Crotti, Giulia . . . . . . . . . . . . CD-11.2 FRI (p183)
Crouzier, Marius . . . . . . . . ∙CK-P.5 TUE (p104)
Crozier, Daniel . . . . . . . . . . . . CL-7.6 FRI (p209)
Crozier, Kenneth B. . . . . . EH-3.6 THU (p154)
Cruciano, Cristina . . . . . . CH-8.4 WED (p133),
EI-4.2 FRI (p212)
Crump, Paul . . . . . . . . . . ∙CB-11.1 THU (p162),
CB-11.3 THU (p166)
Crut, Aurélien . . . . . . . . . . . JSVI-1.4 TUE (p89)
Cruz, Jose Luis . . . . . . . . . . CH-15.5 FRI (p209)
Cruz, Viviene Dela . . . . . CM-7.5 WED (p112)
Cryan, James . . . . . . . . . . . . JSI-4.6 WED (p134)
Csajbók, Viktória . . . . . . EE-P.12 WED (p139),
PD-1.2 THU (p170)
Csizmadia, Tamas . . . . . . . JSI-2.5 WED (p118)
Csontos, János . . . . . . . . . . . CF-P.6 TUE (p102),
CG-4.1 THU (p149)
Cuadrado-Laborde, Christian
CD-P.22 TUE (p101)
Cubas Heim, Rebecca . . ∙CK-P.15 TUE (p104)
Cubillos, Javier . . . . . . . . . CK-P.27 TUE (p105),
CK-P.31 TUE (p106)

Authors' Index

Cueff, Sébastien . . . . . . . . . CK-15.4 FRI (p214)
Cuenat, Stéphane . . . . . . . . CH-2.4 MON (p60)
Cui, Shuai . . . . . . . . . . . . . . ∙CK-5.3 WED (p116)
Cui, Xiaoqi . . . . . . . . . . . . . . . . ∙EI-P.1 FRI (p223)
Cui, Yihao . . . . . . . . . . . . . ∙JSIII-P.13 FRI (p225)
Cummins, Cian . . . . . . . . ∙CE-P.16 THU (p172)
Currie, Sebastian G. . . . CD-P.34 TUE (p102),
EA-3.5 THU (p152)
Curry, Richard J. . . . . . . . . . . CE-9.4 FRI (p194)
Cutrona, Antonio . . . . . . . CC-3.5 THU (p169),∙ED-6.3 FRI (p192)
Ćutuk, Ana . . . . . . . . . . . . . . CB-P.10 MON (p76)
Cvecek, Kristian . . . . . . . . CD-13.5 FRI (p207)
Czajkowski, Rafal . . . . . . . . CE-5.1 THU (p149)
Czyszanowski, Tomasz . . . . CB-3.2 TUE (p84)

DDabbene, Simone . . . . . ∙CA-10.2 THU (p142)
Dacasa, Hugo . . . . . . . . . . . . CG-4.6 THU (p155)
Dadashi, Khalil . . . . . . . . . . . . CB-3.3 TUE (p86)
Dadenkov, Ivan . . . . . . . . . . . . EJ-P.9 MON (p80)
Daems, Devin . . . . . . . . . . . CH-15.3 FRI (p205)
Dagens, Beatrice . . . . . . . . . CK-P.5 TUE (p104),∙CK-10.3 THU (p158)
Dahlem, Marcus . . . . . . . CE-P.16 THU (p172)
Dahlström, Jan Marcus . . JSI-4.3 WED (p130),
JSI-4.4 WED (p132)
Dai, Lilong . . . . . . . . . . . . . ∙EF-P.20 WED (p140)
Dakovski, Georgi . . . . . . . . JSI-4.6 WED (p134)
Dakovski, Georgi L. . . . . . . . EE-3.3 FRI (p195)
Dal Cin, Sandro . . . . . . . . . ∙CB-P.4 MON (p75),
CB-8.1 THU (p142), CB-8.2 THU (p142)
Dal Conte, Stefano . . . . . . . . EI-4.2 FRI (p212),∙EI-4.4 FRI (p214)
Dalapati, Pradip . . . . . . . . CH-6.6 WED (p120)
D’Alessandro, Giampaolo EH-P.7 THU (p178)
Dalidet, Romain . . . . . . . . ∙EB-2.5 MON (p63),
EB-11.4 THU (p153)
DALLA-BARBA, Gilles . . CA-7.3 WED (p126)
Dallachiesa, Lauren . . . . . . CI-4.2 WED (p131)
Dalloz, Nicolas . . . . . . . . . . EH-4.5 THU (p160)
Damarla, Ganesh . . . . . . . . . . CC-7.3 FRI (p212)
D’Ambrosio, Davide . . . . ∙CH-2.5 MON (p62),
CK-13.5 FRI (p196)
Damzen, Michael . . . . . . . . . PP-1.1 MON (p64),
CA-P.6 MON (p74), CA-6.5 WED (p112)
Damzen, Michael J. . . . . . . CA-6.3 WED (p110)
Danailov, M. B. . . . . . . . . . . JSI-3.5 WED (p126)
Danailov, Miltcho . . . . . . . JSI-2.5 WED (p118),
JSI-P.7 WED (p141)
Danailov, Miltcho B. . . . ∙JSI-2.2 WED (p116),
JSI-4.3 WED (p130)
Danan, Eliezer . . . . . . . . . . . CL-P.14 FRI (p222)
Danan, Yossef . . . . . . . . . . . . CL-P.14 FRI (p222)
Dancus, Ioan . . . . . . . . . . . . CA-P.22 MON (p75)Dang, Ka My . . . . . . . . . . . . . CL-1.2 MON (p69)
Dangel, Roger . . . . . . . . . . . JSIII-4.4 FRI (p197)
Dangoisse , Guillaume . . . . EA-9.4 FRI (p214)
Dania, Lorenzo . . . . . . . . . . PD-2.6 THU (p171)
Danilevičius, Rokas . . . . . CA-11.6 THU (p154)
Danto, Sylvain . . . . . . . . . . . . CE-1.2 MON (p53)Danz, Thomas . . . . . . . . . . . CG-3.5 THU (p147)
Danzl, Johann G. . . . . . . . . ∙CL-1.1 MON (p67)
DARBON, Stéphane . . . . CG-P.14 THU (p174)
Darket, Anne Sofie . . . . . . CK-4.5 WED (p114)

Darmala, Ganesh . . . . . . . . . . CC-7.6 FRI (p216)
Darmawan, Yoshua A. . . . EG-6.3 WED (p110)
Darmo, Juraj . . . . . . . . . . . . . CC-4.2 FRI (p180),
CC-7.2 FRI (p210)
Darquié, Benoit . . . . . . . . . . ED-3.5 MON (p73)
Darras, Tom . . . . . . . . . . . . . . . EB-4.3 TUE (p87)
Darvill, John . . . . . . . . . . . . . JSI-P.4 WED (p141)
Darwich, Dia . . . . . . . . . . . . CJ-5.4 WED (p133),
CJ-8.5 FRI (p196)
Das, Ranjan . . . . . . . . . . . . CK-P.15 TUE (p104),
CK-7.5 WED (p134)
Das, Sambit . . . . . . . . . . . . . . . EE-3.3 FRI (p195)
Dasari, Durga B.R. . . . . . . EB-10.5 THU (p147)
Dasari, Durga Bhaktavatsala Rao
EB-7.1 WED (p115), ∙EB-7.2 WED (p117)
Daskalaki, Christina . . . . . . CC-6.3 FRI (p204)
Datta, Ananga Mohan . . ∙EA-P.16 THU (p175)
Datta, Srijoyee . . . . . . . . . . ∙CM-3.4 MON (p68)
Daudet, Laurent . . . . . . . . . JSIII-3.3 FRI (p185)
Dauliat, Romain . . . . . . . . CD-9.1 WED (p122)
David, C. . . . . . . . . . . . . . . . JSI-3.5 WED (p126)
David, Christin . . . . . . . . . . CD-11.4 FRI (p187)
Davidson, Ian . . . . . . . . . . . ∙CE-2.1 MON (p59),
CI-1.3 WED (p111), CH-10.3 THU (p151)
Davidson, Ian A. . . . . . . . . . CE-2.4 MON (p61),
CE-2.5 MON (p63), CH-10.4 THU (p153),
CJ-9.3 FRI (p204)
Davis, Alex C. . . . . . . . . . . CE-P.30 THU (p173)
Davis, Alex O.C. . . . . . . . ∙CD-14.5 FRI (p217)
Davis, James . . . . . . . . . . . . JSIII-P.13 FRI (p225)
Davis, Lauren . . . . . . . . . . . . CC-1.1 THU (p149)
Davydova, Alisa . . . . . . . . ∙EF-2.3 WED (p133),
EF-3.2 THU (p142)
Dax, Andreas . . . . . . . . . . . CA-11.5 THU (p152)
Day, Richard . . . . . . . . . . . . . CE-5.3 THU (p151)
Day, Timothy . . . . . . . . . . . . . CD-6.5 TUE (p96)
De, Souvaraj . . . . . . . . . . . . CK-P.15 TUE (p104),∙CK-7.5 WED (p134)
de Aldana, Javier Rodríguez Vázquez
CA-9.1 WED (p128), CA-9.4 WED (p132)
De Andres, Aitor . . . . . . . ∙CG-3.6 THU (p149)
De Angelis, Costantino . . EG-2.1 MON (p58),
CK-6.3 WED (p124)
de Araújo, Cid B. . . . . . . . CD-P.16 TUE (p100)
de Boer, Johannes F. . . . . CH-P.3 WED (p136),
CH-12.2 THU (p165)
de Boo, Gabriele G. . . . . . . CE-10.2 FRI (p204)
de Ceglia, Domenico . . . . EH-3.5 THU (p152)
de Coster, George J. . . . . . . CE-6.6 THU (p163)
De Fanis, Alberto . . . . . . . . JSI-P.2 WED (p141)
de Faria Pinto, Tiago . . . . CA-8.2 WED (p116)
De Gendt, Stefan . . . . CM-LIM.3 WED (p117)
De Giovannini, Umberto . CG-1.2 TUE (p85),
CG-5.3 THU (p159)
De La Prida, Liset M . . . . . CH-15.1 FRI (p201)
de las Heras, Alba . . . . . . . ∙CF-2.1 MON (p59),
PD-1.5 THU (p170), ∙EE-3.5 FRI (p197)
De Leon Mayeu, Joël . . . . . . EC-2.4 FRI (p197)
De Luca, Federico . . . . . . . EH-3.4 THU (p152)
De Marinis, Lorenzo . . . . ∙JSIII-3.2 FRI (p183)
de Matteis, Diego . . . . . . . . JSVI-1.2 TUE (p85)
de Mey, Robbe . . . . . . . . . ∙CK-P.20 TUE (p105)
de Michele, Vincenzo . . . . . CM-6.4 TUE (p96)de Nalda, Rebeca . . . . . . . CD-P.21 TUE (p101)
De Natale, Paolo . . . . . . EF-P.16 WED (p140),
CK-13.5 FRI (p196), CH-14.2 FRI (p193)

De Ninno, Giovanni . . . . . JSI-2.5 WED (p118)
de Oliveira, Thales . . . . . . . CC-P.16 FRI (p218)
De Paoli, Greta . . . . . . . . . CM-7.6 WED (p114)
de Riedmatten, Hugues . . . EG-5.1 TUE (p92),
EB-9.1 WED (p129), EB-9.4 WED (p133),
EA-2.1 THU (p142)
De Rossi, Alfredo . . . . . . . . CD-2.5 MON (p62),
JSIII-2.1 THU (p162), EA-8.5 FRI (p208),
JSIII-6.2 FRI (p213)
de Souza Menezes, Leonardo
EI-1.4 FRI (p186)
de Sterke, C. Martijn . . . . EF-P.9 WED (p139)
de Valcárcel, Germán J. . CD-P.19 TUE (p101),
EF-P.17 WED (p140), ∙EF-5.1 THU (p156),∙EA-P.24 THU (p176)
de Vito, Giulio . . . . . . . . . . . JSVI-1.2 TUE (p85)
De Vittorio, Massimo . . . . CH-15.1 FRI (p201)
de Vos, Erik W. . . . . . . . . . . . . CG-2.3 TUE (p99)
De Witte, Jasper . . . . . . . . . . CD-3.2 MON (p68)
Debatin, Markus . . . . . . . . EA-P.18 THU (p175)
Debord, Benoît . . . . . . . . . CM-P.25 MON (p78),
CD-8.3 WED (p118), CJ-4.2 WED (p123),
CD-14.2 FRI (p213)
Deckert, Thomas . . . . . . . . EH-2.4 THU (p146),
CF-11.1 FRI (p201), ∙EI-4.3 FRI (p214)
Decobert, Jean . . . . . . . . . . . . . CB-5.3 TUE (p94)
Deconihout, Bernard . . . . EE-P.5 WED (p138)
Défossez, Florent . . . . . . . . CJ-3.6 WED (p121)
Defrère, Denis . . . . . . . . . . JSII-3.2 MON (p69)
Degout-Charmette, ElodieCL-P.15 FRI (p222)
Deinert, Jan-Christoph . . . CC-P.16 FRI (p218)
Deinhart, Victor . . . . . . . . . EH-5.6 THU (p168)
Deja, Yves . . . . . . . . . . . . . . . ∙CE-5.4 THU (p153)
Deka, Jayanta . . . . . . . . . . . . EJ-P.10 MON (p80)
Dekker, Ronald . . . . . . . . . . . . CB-5.1 TUE (p92)
Dekorsy, Thomas . . . . . . . . CA-P.12 MON (p74)
Del Bene, Filippo . . . . . . . . . . CL-6.2 FRI (p191)
Del Carmen Lozano, Ninfa
CH-P.18 WED (p137)
Del Fatti, Natalia . . . . . . . . . JSVI-1.4 TUE (p89)del Hougne, Philipp . . . . . . CL-3.3 THU (p159)
Del Villar, Ignacio . . . . . . . . CL-1.4 MON (p71)
Delagnes, Jean-Christophe
CL-2.4 THU (p153)
Delarosbil, Jean-luc . . . . . . . CE-1.2 MON (p53)
Delaye, Philippe . . . . . . . . . . CD-3.5 MON (p72)
Delden, Marcel van . . . . . . . CF-12.2 FRI (p211)
Delehaye, Marion . . . . . . . . ED-3.2 MON (p69)
Delgado, Teresa . . . . . . . . . . . CE-4.5 TUE (p99),
CE-10.4 FRI (p206)
Delgado-Pinar, MartinaCH-11.3 THU (p159),∙CH-15.5 FRI (p209)
Del’Haye, Pascal . . . . . . . . . CD-P.9 TUE (p100),
CK-5.1 WED (p114), CD-9.6 WED (p126),
CD-10.5 WED (p132), EF-P.3 WED (p139),
CK-8.1 THU (p142), CK-8.6 THU (p148),
EF-6.3 THU (p166), ED-6.1 FRI (p188)
Deliancourt, Etienne . . ∙CH-P.11 WED (p136)
Deligiannidis, Stavros CH-P.17 WED (p137),
CL-2.2 THU (p151), JSIII-1.1 THU (p156),
EJ-3.4 FRI (p187)
Della Casa, Pietro . . . . . . . . . CB-4.4 TUE (p91),
CF-6.5 WED (p113), CB-11.1 THU (p162)
Della Torre, Alberto . . . . . CK-4.3 WED (p112)
Della Valle, Giuseppe . . . . CD-11.2 FRI (p183)
Delmulle, Maxime . . . . . . . JSIII-6.2 FRI (p213)

231

Delplace, Pierre . . . . . . . . . . . EC-2.2 FRI (p193)
Delpy, Joseph . . . . . . . . . . . ∙EA-P.5 THU (p175)
DelRe, Eugenio . . . . . . . . . . . EF-10.5 FRI (p215)
Demagh, Nacer-E. . . . . . . . . CE-1.6 MON (p57)
Demarchi, Andrea . . . . . . . CK-14.6 FRI (p208)
Demekhin, Philipp V. . . . . JSI-4.3 WED (p130)
Demeridou, Ioanna . . . . . . . . EI-1.2 FRI (p182)
Demesh, Maksim . . . . . . . . . CA-1.1 MON (p52)
Demetriou, Giorgos . . . . . . CA-5.4 TUE (p96)
Demidovich, A. . . . . . . . . . JSI-3.5 WED (p126)
Demidovich, Alexander . JSI-2.5 WED (p118),
JSI-P.7 WED (p141)
Demir, Abdullah . . . . . . . CB-P.20 MON (p76),
CB-3.3 TUE (p86)
Demirbas, Umit . . . . . . . . CA-P.23 MON (p75),
CE-6.4 THU (p161), CC-3.3 THU (p167)
Demircan, Ayhan . . . . . . . . . EJ-2.3 MON (p60),
CF-P.19 TUE (p103), CD-9.4 WED (p124),
EF-P.1 WED (p139), EF-5.3 THU (p158),
EE-5.2 FRI (p211)
Demoli, Nazif . . . . . . . . . . . . . EA-6.2 FRI (p184),
CL-P.5 FRI (p221)
Demongodin, Pierre . . . . ∙CK-5.6 WED (p120)
Demur, Romain . . . . . . . . . ∙CD-1.4 MON (p56),∙CJ-2.5 WED (p115)
Deng, Bo . . . . . . . . . . . . . . . . . ∙EA-9.6 FRI (p216)
Deng, Fu . . . . . . . . . . . . . . . . . CD-1.5 MON (p56)Deng, Hong . . . . . . . . . . . . . . CK-13.2 FRI (p190)
Deng, Hui . . . . . . . . . . . . . . . . ∙CB-3.1 TUE (p82)
Deng, Yunpei . . . . . . . . . . . . JSI-1.2 WED (p110)
Deniel, Lucas . . . . . . . . . . . . . ∙CD-5.1 TUE (p90)
Denisov, Dmitrii . . . . . . . . . CB-9.5 THU (p152)
Denker, Boris . . . . . . . . . . . . CA-1.2 MON (p52)
DENOEUD, Adrien . . . . CG-P.14 THU (p174)
Deo, Vincent . . . . . . . . . . . . JSII-1.3 MON (p55)
Deplace, Pierre . . . . . . . . . . . . EC-2.3 FRI (p195)
DePonte, Dan . . . . . . . . . . . . . EE-3.3 FRI (p195)
Deponte, Daniel . . . . . . . . . JSI-4.6 WED (p134)
Derlikiewicz, Julia . . . . . . . CG-P.8 THU (p174)
Derrien, Thibault . . . . . . . . ∙CM-5.4 TUE (p91)
Derycke, Christophe . . . . CA-P.22 MON (p75)
Desai, Niyati . . . . . . . . . . . . . JSII-3.5 MON (p73)
Deschenes, Jean-Daniel . . ED-3.1 MON (p67)
Deschler, Felix . . . . . . . . . . EH-P.14 THU (p179)
Descrovi, Emiliano . . . . . . . . EI-3.5 FRI (p208),∙CK-15.1 FRI (p210)
Désévédavy, Frédéric . . . . . . CJ-7.3 FRI (p184)
Deshmukh, Chetan . . . . . . . . EG-5.1 TUE (p92)
Despont, Michel . . . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
Destouches, Nathalie . . . ∙EH-4.5 THU (p160)
Devaud, Louisiane . . . . . . . . . EA-9.3 FRI (p212)
Devetta, Michele . . . . . . . . . CM-6.3 TUE (p94),
JSI-5.5 THU (p149), CG-3.2 THU (p143),
CE-P.10 THU (p172)
Dewhurst, J. K. . . . . . . . . . . . CG-1.1 TUE (p83)
Dewhurst, John Kay . . . . . CG-3.5 THU (p147)
Dey, Sibnath . . . . . . . . . . . ∙CK-P.28 TUE (p105)
Dhama, Rakesh . . . . . . . . . . . EG-2.3 MON (p60)
Dhanabalan, Balaji . . . . . . . . CE-4.3 TUE (p95)
Dhar, Himadri . . . . . . . . . . . PD-1.9 THU (p170)
Dhawan, Rajveer . . . . . . . ∙CD-P.6 TUE (p100),
CD-12.3 FRI (p193), CD-12.4 FRI (p195),∙CI-7.6 FRI (p208)
Dhaybi, Ali . . . . . . . . . . . . . . ∙CJ-4.2 WED (p123)
Dhillon, Sukhdeep . . . . . . . CC-2.3 THU (p161)

Di Battista, Giorgio . . . . . . . ∙EI-3.2 FRI (p204)
Di Falco, Andrea . . . . . . . PP-2.11 WED (p121),
CL-4.6 THU (p169), EH-P.1 THU (p178)
Di Fraia, M. . . . . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Di Fraia, Michele . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130), JSI-5.5 THU (p149)
Di Francescantonio, Agostino
EG-2.1 MON (p58)
Di Giano, Niki . . . . . . . . . . CK-7.1 WED (p128)
Di Giulio, Valerio . . . . . . . . EG-P.1 TUE (p106),
EH-2.3 THU (p144)
Di Martino, Giuliana . . . CH-8.3 WED (p131)
Di Noia, Gabriele . . . . . . . . . . CL-6.5 FRI (p197)
Di Palo, Nicola . . . . . . . . . . ∙CF-2.4 MON (p61),
CG-2.2 TUE (p97), PP-2.4 WED (p120),
CG-3.5 THU (p147), CG-P.1 THU (p173),
CG-P.5 THU (p173)
Di Russo, Enrico . . . . . . . . CH-6.6 WED (p120)
di Vora, Robert . . . . . . . . . CD-7.3 WED (p110),
CH-P.19 WED (p137)
Diamanti, Eleni . . . . . . . . . . . EB-5.2 TUE (p93),
EB-13.4 THU (p167)
Dias, Eduardo J. C. . . . . . . . . CK-2.4 TUE (p88)
Dias, Ricardo G. . . . . . . . . . . . EC-P.5 FRI (p223)
Díaz, Francesc . . . . . . . . . . CA-P.19 MON (p75),
CA-P.20 MON (p75), CA-9.1 WED (p128),
CJ-6.2 THU (p143), CE-8.5 FRI (p186)
Diaz, Francisco . . . . . . . . . CK-P.34 TUE (p106)
Díaz Rivas, Daniel . . . . . . ∙CF-P.18 TUE (p103)
Dichiarante, Valentina . . . . . EE-3.4 FRI (p197)
Dick, Anneli . . . . . . . . . . . . . . CL-8.4 FRI (p215)
Didier, Pierre . . . . . . . . . . . ∙CB-9.4 THU (p152),
CI-5.1 FRI (p180)
Didychenko, Denys . . . . . . . ∙CA-4.1 TUE (p82)
Diebel, Laura . . . . . . . . . . . . . . EG-4.3 TUE (p86)
Diego, Michele . . . . . . . . . . . JSVI-1.4 TUE (p89)
Diego-Rucabado, Andrea . CE-1.4 MON (p55)
Dietrich, Christian M. . . . CF-P.19 TUE (p103)
Díez, Antonio . . . . . . . . . . CD-P.22 TUE (p101),
CH-11.3 THU (p159)
Diez Carlon, Andres . . . . . . . EI-4.5 FRI (p216)
Diez Merida, Jaime . . . . . . . . . EI-4.5 FRI (p216)
DiGiovanni, David . . . . . . . . . CJ-1.1 TUE (p93)
Dikande Bitha, Rodrigues . ∙EF-8.5 FRI (p197)
Dikopoldsev, Alexander . . CB-8.3 THU (p144)
Dikopoltsev, Alex . . . . . . ∙CB-8.6 THU (p148),∙EC-3.1 FRI (p201)
Dikopoltsev, Alexander . CB-8.5 THU (p146)
Dilhan, Lucie . . . . . . . . . . . . CE-11.4 FRI (p214)
Dimitriou, Vasilis . . . . . . . . CM-9.6 FRI (p196)
Dimopoulos, Evangelos . . EG-1.1 MON (p52)Din, Amin . . . . . . . . . . . . . ∙CM-P.30 MON (p78)
Dinc, Niyazi Ulas . . . . . . JSIII-1.5 THU (p160)
Ding, Jiaye . . . . . . . . . . . . . . . EB-8.5 WED (p127)
Ding, Lei . . . . . . . . . . . . . . . . . . EC-1.5 FRI (p187)
Ding, Peisheng . . . . . . . . . . . CL-1.2 MON (p69),
CL-1.3 MON (p69)Ding, Xuefei . . . . . . . . . . . . . ∙CC-7.1 FRI (p210)
Ding, Yunhong . . . . . . . . . . . CC-5.5 FRI (p196),
CC-6.2 FRI (p204)
Dinkelaker, Aline N. . . . . JSII-3.4 MON (p71),∙JSII-P.1 MON (p80)
Dirdal, Christopher . . . . . ∙CL-4.4 THU (p167)
Dirin, Dmitry . . . . . . . . . . . CA-9.3 WED (p130)
Dirmeier, Thomas . . . . . . . . EB-2.1 MON (p59)

Authors' Index

Dittel, Christoph . . . . . . . CK-11.3 THU (p166)
Divall, Marta . . . . . . . . . . . . PP-2.2 WED (p120),
CE-P.2 THU (p171)
Divliansky, Ivan . . . . . . . . . CF-P.5 TUE (p102),
CH-7.6 WED (p127)
Diwo-Emmer, Elke . . . . . . . CB-2.5 MON (p72)
Dixneuf, Clément . . . . . . . CJ-5.4 WED (p133)
Dixneuf, Sophie . . . . . . . . . ∙CL-P.15 FRI (p222)
Djordjevic, Ivan B . . . . . . . EB-P.13 THU (p177)
Dmitriev, Alexandre . . . . . . . EG-4.2 TUE (p84)
Doblas-Jimenez, David . . JSI-P.3 WED (p141)
Dobner, Sven . . . . . . . . . . . . EA-4.3 THU (p158)
Docampo, Pablo . . . . . . . . . CE-1.1 MON (p53),
CE-P.11 THU (p172)
Dogadov, Oleg . . . . . . . . . . . CF-P.9 TUE (p103),
EI-4.4 FRI (p214)
Dold, Simon . . . . . . . . . . . . . JSI-P.2 WED (p141)
Dolgaleva, Ksenia . . . . . . . . CE-7.1 THU (p163)
Döll, Nico Lennart . . . . . . EB-P.18 THU (p177)
Dolso, Gian Luca . . . . . . . . . CF-2.4 MON (p61),
CG-2.2 TUE (p97), ∙PP-2.4 WED (p120),∙CG-P.1 THU (p173), CG-P.5 THU (p173)
Dombi, Péter . . . . . . . . . . . . EE-1.6 WED (p115),
EE-P.7 WED (p138), EE-P.12 WED (p139),∙EH-2.2 THU (p144), CC-1.5 THU (p155),
PD-1.2 THU (p170), CE-P.6 THU (p171)
Domeneguetti, Renato R.
PP-1.11 MON (p64), EJ-P.1 MON (p79)
Domínguez Bucio, Thalía CK-P.2 TUE (p104),
CE-8.6 FRI (p186)
Domínguez-Juárez, Jorge Luis
∙CH-8.6 WED (p135)
Domke, Matthias . . . ∙CM-LIM.5 WED (p119)
Domröse, Till . . . . . . . . . . . . EG-3.3 MON (p68)
Donato, Mattia . . . . . . . . . . CH-6.4 WED (p118)
Dong, Gaoneng . . . . . . . . . EG-1.1 MON (p52),∙CB-1.4 MON (p56)
Dong, Liang . . . . . . . . . . . . . . . ∙CJ-1.2 TUE (p95)
Dong, Lulu . . . . . . . . . . . . . CA-10.6 THU (p148)
Dong, Xin . . . . . . . . . . . . . . . CH-15.2 FRI (p205)
Dongare, Pratiksha . . . . . JSIV-1.5 WED (p120)
Donges, Jan Niklas . . . . . . EB-P.32 THU (p178)
D’Onofrio, Luciano Jacopo CG-2.2 TUE (p97)
D’Orazio, Antonella . . . . EH-P.18 THU (p179),
EH-P.19 THU (p179)
Doricchi, Andrea . . . . . . . . CE-P.1 THU (p171)
Doris, Eli A. . . . . . . . . . . . . . JSIII-5.4 FRI (p207)
Dornbusch, Daniel . . . . . . . CC-P.16 FRI (p218)
Doron, Maeva . . . . . . . . . ∙CH-P.22 WED (p137)
Dorosz, Dominik . . . . . . . . ∙CE-1.4 MON (p55)
Dörsam, Jan Helge . . . . . . . PD-1.1 THU (p170)
dos Santos, Luiz F. . . . . . . . CH-P.7 WED (p136)
Dostovalov, Alexandr V. . . CJ-P.20 FRI (p221)
Doty, Matthew F. . . . . . . . CE-P.21 THU (p172)
Douglass, Glen . . . . . . . . . . ∙JSII-3.3 MON (p69)
Doumbia, Yaya . . . . . . . . . ∙CB-7.2 WED (p130)
Downing, James . . . . . . . . . . CE-11.4 FRI (p214)
Drag, Cyril . . . . . . . . . . . . . ∙CD-P.26 TUE (p101)
Dragic, Peter . . . . . . . . . . . . . CE-7.1 THU (p163)
Drake, Tara . . . . . . . . . . . . . ∙EF-2.1 WED (p129)
Dranczewski, Jakub . . . . . . . EF-8.4 FRI (p197),
CK-14.2 FRI (p202)
Drawer, Jens-Christian . . . . . EI-2.6 FRI (p196)
Draxinger, Wolfgang . . . . . . CL-8.4 FRI (p215)
Dréau, Anaïs . . . . . . . . . . . ∙CK-4.1 WED (p108)
Drechsler, Ute . . . . . . . . . . . . CE-9.1 FRI (p188),

CK-14.5 FRI (p206)
Dremin, Viktor . . . . . . . . . . . . CL-6.4 FRI (p197)
Dresler, Christoph . . . . . . . EE-1.4 WED (p113)
Drewes, Jonas . . . . . . . . . . CK-P.19 TUE (p105)
Dris, Stefanos . . . . . . . . . . . . . . EJ-3.4 FRI (p187)
Driver, Taran . . . . . . . . . . . ∙JSI-4.2 WED (p130),
JSI-4.6 WED (p134)
Drmota, P. . . . . . . . . . . . . . . . . ED-5.1 FRI (p180)
Drs, Jakub . . . . . . . . . . . . . . ∙CG-4.4 THU (p153)
Drüeke, Helena . . . . . . . . PP-2.10 WED (p121),
EC-P.1 FRI (p222)
Druon, Frédéric . . . . . . . . . CA-3.2 MON (p68),
CE-4.1 TUE (p93), CE-4.4 TUE (p97),
CF-P.3 TUE (p102), CA-11.3 THU (p150),
CE-P.29 THU (p173)
Du, Haoze . . . . . . . . . . . . . . ∙CE-6.5 THU (p161)
Du, Mengqi . . . . . . . . . . . . . CF-P.15 TUE (p103),
CH-6.1 WED (p114)
Du, Mingde . . . . . . . . . . . . . . . . EI-P.1 FRI (p223)
Du-Burck, Frédéric . . . . . . ED-P.7 MON (p79),
CB-6.4 WED (p126)
Duarte, Carlos . . . . . . . . . CH-P.20 WED (p137)
Dubey, Swadheen . . . . . . . ∙EA-P.2 THU (p174)
Dubietis, Audrius . . . . . . . CD-P.25 TUE (p101)
Dubochet, Olivier . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
Dubois, Maxime . . . . . . . CH-P.22 WED (p137)
Duboisset, Julien . . . . . . . . EG-6.1 WED (p108)
Dubreuil, Nicolas . . . . . . . . CD-3.5 MON (p72)
Dubreuil, Pascal . . . . . . . . CD-P.10 TUE (p100)
Dubroeucq, Romain . . . . ∙ED-2.3 MON (p61),
ED-4.2 TUE (p83)
Dubrovkin, Alexander . . ∙EG-3.2 MON (p66)
DuBurck, Frederic . . . . . . . . ED-3.5 MON (p73)
Ducci, Sara . . . . . . . . . . . . . . EB-6.6 WED (p115)
Duchateau, Guillaume . . . CM-10.4 FRI (p206)
Dudelev, Vladislav . . . . . . . CB-9.5 THU (p152)
Dudley, John M. . . . . . . . . . EF-10.2 FRI (p211),
EF-10.3 FRI (p213)
Dudley, John Michael . . . . . CD-5.3 TUE (p90),
CD-9.2 WED (p122)
Dudovich, Nirit . . . . . . . . EE-P.14 WED (p139),
CG-5.4 THU (p161), ∙CG-6.3 THU (p167)
Duelk, Marcus . . . . . . . . . . CB-11.6 THU (p168)
Dufour, Martin . . . . . . . . . . . EF-9.5 FRI (p207),∙EF-9.6 FRI (p209)
Duivestein, Pim . . . . . . . . . EB-13.2 THU (p165)
Dulieu, Olivier . . . . . . . . . . . ∙EA-7.5 FRI (p196)
Dumeige, Yannick . . . . . . . . CD-4.1 TUE (p82),
CK-3.5 TUE (p96)
Dumergue, Mathieu . . . . . JSI-2.5 WED (p118)
Duò, Lamberto . . . . . . . . . . . EG-2.1 MON (p58)
Duocastella, Marti . . . . . . . . . CL-7.3 FRI (p205)
Dupish, Dupish . . . . . . . . . . . EA-6.3 FRI (p186)
Duplinskiy, Alexander . . CH-12.3 THU (p167)
Dupont, Hippolyte . . . . . . ∙CA-3.2 MON (p68)Duque Gijon, Maria . . . . . . CB-P.8 MON (p76),∙CB-P.19 MON (p76),∙EF-P.21 WED (p140)
Duquennoy, Rocco . . . . . . ∙EA-4.1 THU (p156)
Durán, Vicente . . . . . . . . . . . ED-6.2 FRI (p190)
Durán Gómez, J.S.S. . . . . . CD-14.4 FRI (p215)
Durán-Hernández, Andrés . EB-4.5 TUE (p89)
Durán Retamal, José . . . . . . . EI-3.3 FRI (p204)
Durécu, Anne . . . . . . . . . . . CJ-2.3 WED (p113),
CJ-6.4 THU (p145), CJ-P.1 FRI (p220)

Düsterer, Stefan . . . . . . . . . JSI-5.3 THU (p145),
JSI-5.4 THU (p147)
Dutta, Joydip . . . . . . . . . . . . ∙CI-P.10 FRI (p219)
Dutta Gupta, Bhaswar . . . . ∙CJ-7.4 FRI (p186),
CJ-P.12 FRI (p220)
Duwe, Matthias . . . . . . . . . . CM-2.1 MON (p58)
Dwivedi, Paras . . . . . . . . . . . PD-2.1 THU (p170)
Dyatlov, Mikhail . . . . . . . . ∙CD-3.5 MON (p72)
Dziechciarczyk, Łukasz . . . CA-5.4 TUE (p96)
Dziewior, Jan . . . . . . . . . . . . EA-P.1 THU (p174)

E
E. Christiansen, Rasmus . CK-15.6 FRI (p216)
Eardley, Samuel . . . . . . . ∙CG-P.10 THU (p174)
Ebadi, Kaveh . . . . . . . . . . . . CB-P.20 MON (p76)
Ebendorff-Heidepriem, Heike
CD-2.3 MON (p60)
Eber, Alexander . . . . . . . . CD-7.3 WED (p110),∙CH-P.19 WED (p137)
Ebrahim-Zadeh, Majid . . . CD-6.1 TUE (p92),
CD-P.19 TUE (p101)
Ebrahimzadeh, Saeid . . . ∙CF-8.3 WED (p125)
Eckhof, Patty . . . . . . . . . . . . . CA-3.5 MON (p72)
Edelmann, Marvin . . . . . ∙CF-8.5 WED (p127),
CJ-P.7 FRI (p220), CJ-P.19 FRI (p221)
Eden, J. Gary . . . . . . . . . . . . . . EA-1.1 TUE (p83)
Edvardsen, André W. . . . . ∙CJ-10.4 FRI (p214)
Edwards, Brian . . . . . . . . . . EH-5.1 THU (p162)
Efetov, Dmitri K. . . . . . . . . . . EI-3.3 FRI (p204),
EI-4.5 FRI (p216)
Eggleton, Benjamin J. . . . . CD-12.5 FRI (p197)
Egorov, Anton . . . . . . . . . . . CB-9.5 THU (p152)
Egun, Felix . . . . . . . . . . . . . . JSI-4.6 WED (p134)
Ehlers, Henrik . . . . . . . . . . . JSI-P.6 WED (p141)
Ehlert, Christopher . . . . . . JSI-5.4 THU (p147)
Ehrentraut, Lutz . . . . . . . . . CG-3.4 THU (p145)
Ehrhardt, Max . . . . . . . . . ∙CM-7.3 WED (p110),∙CK-11.3 THU (p166), EC-1.3 FRI (p185),∙EA-8.3 FRI (p204)
Ehrlich, Katjana . . . . . . . . CH-11.2 THU (p159)
Eich, Alexander . . . . . . . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118)
Eichhorn, Marc . . . . . . . . . . CA-3.4 MON (p70),
CA-P.16 MON (p74), ∙CA-P.17 MON (p75),
CJ-10.5 FRI (p214)
Eidam, Tino . . . . . . . . . . . . CF-P.21 TUE (p103),∙CL-8.5 FRI (p215)
Eiermann, Bernd . . . . . . . . . CF-P.4 TUE (p102)
Eigner, Christof . . . . . . . . . EA-4.5 THU (p160),
EA-5.5 THU (p168), CI-5.5 FRI (p186)
Eikema, Kjeld . . . . . . . . . . . ED-1.1 MON (p53),
CF-P.15 TUE (p103)
Eikema, Kjeld S. E. . . . . . CH-6.1 WED (p114),
CG-P.7 THU (p174)
Eikenberry, Stephen . . . ∙JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Eilenberger, Falk . . . . . . . . CD-2.3 MON (p60),
EG-5.3 TUE (p94), CK-P.24 TUE (p105),
CK-P.36 TUE (p106), CK-11.4 THU (p166),
EB-P.32 THU (p178), EI-2.6 FRI (p196)
Eisenbach, Lucas . . . . . . . ∙CF-10.4 THU (p145)
Eisenschreiber, Jan . . . . . . CA-8.4 WED (p118)
Eitner, Madeleine . . . . . . . . CA-3.4 MON (p70)
El, Gennady . . . . . . . . . . . . . . . EF-9.5 FRI (p207)
El Dirani, Houssein . . . . . CK-5.6 WED (p120)

232

El-Ganainy, Ramy . . . . . . . . . CB-3.3 TUE (p86),
EF-8.2 FRI (p193)
El Hassan, Ashraf . . . . . . . ∙CD-1.3 MON (p54)
El Moussawi, Fatima . . . . CH-P.1 WED (p136)
El Sokhen, Rabih . . . . . . . . ∙EC-2.3 FRI (p195)
Elfarash, Ahmed . . . . . . . ∙CE-P.20 THU (p172)
Eliezer, Yaniv . . . . . . . . . . . . . . CJ-1.5 TUE (p99)
Elistratova, Elizaveta . . . . ∙CE-2.4 MON (p61)
Elizarov, Maxim . . . . . . . JSIV-1.4 WED (p118),∙CM-8.4 FRI (p184)
Ellebæk Christiansen, Rasmus
EC-2.5 FRI (p197)
Elliott, Peter . . . . . . . . . . . . . CG-3.5 THU (p147)
Elliott, Robin . . . . . . . . . ∙CH-P.13 WED (p136)
Ellis, Jennifer . . . . . . . . . . . . . ED-3.1 MON (p67)
Elosua Aguado, Cesar . . . CE-5.6 THU (p155)
Elsdon, Michael . . . . . . . . . . . . CI-P.2 FRI (p219)
Elshaari, Ali W. . . . . . . . . . . CK-1.2 MON (p66)
Elu, Ugaitz . . . . . . . . . . . . . . CD-P.5 TUE (p100),
CD-7.1 WED (p108)
Emadi, Ramin . . . . . . . . . . . EA-4.1 THU (p156)
Emeriau, Pierre-EmmanuelEB-6.1 WED (p109)
Emons, Moritz . . . . . . . . . . . . EE-4.3 FRI (p205)
Enbutsu, Koji . . . . . . . . . . . EA-2.2 THU (p142),
EA-2.6 THU (p148), EA-3.6 THU (p154)
Enders, Michael . . . . . . . . . . CD-P.5 TUE (p100)
Endo, Mamoru . . . . . . . . . . EA-2.2 THU (p142),
EA-2.6 THU (p148), EA-3.6 THU (p154)
Endo, Shun . . . . . . . . . . . . . . . CJ-P.10 FRI (p220)
Eng-Johnsson, Per . . . . . . JSI-4.3 WED (p130),
CG-4.6 THU (p155)
Engel, Lena . . . . . . . . . . . . . ∙EA-4.6 THU (p162),
EA-5.1 THU (p162)
Engelsen, Nils J. . . . . . . . . . . ∙EA-9.1 FRI (p210)
Engheta, Nader . . . . . . . . . EH-1.4 WED (p132),
EH-5.1 THU (p162)
Englebert, Nicolas . . . . . . CF-P.14 TUE (p103),
EF-2.2 WED (p131), ∙EF-2.5 WED (p135),
EF-5.5 THU (p160)
Enriquez, Javier . . . . . . . . . CE-P.18 THU (p172)
Enslin, Johannes . . . . . . . . . CB-2.3 MON (p68)
Eom, Joo Beom . . . . . . . . . . . CL-P.17 FRI (p222)
Eppelt, Sebastian . . . . . . . . . . EB-5.1 TUE (p93)
Erben, Benjamin . . . . . . . . CA-6.6 WED (p114)
Erdman, Emily C. . . . . . . ∙CA-8.3 WED (p118)
Erdogan, R. Tufan . . . . . . . . ∙CK-3.1 TUE (p92)Eremeev, Kirill . . . . . . . . . . ∙CA-3.3 MON (p68),
CA-9.4 WED (p132), ∙CA-11.2 THU (p150)
Eriksson, Matias . . . . . . . . ∙CI-1.2 WED (p109),EB-7.3 WED (p117)
Erkintalo, Miro . . . . . . . . . CD-8.5 WED (p120),
CD-9.3 WED (p124),
CD-10.3 WED (p130),
CD-10.4 WED (p132),∙EF-2.2 WED (p131), EF-3.4 THU (p144),
EF-3.6 THU (p148), PD-2.7 THU (p171),
CJ-7.4 FRI (p186), CJ-P.12 FRI (p220)
Ermolaev, Andrei V. . . . . . ∙EF-10.3 FRI (p213)
Ermoleav, Andrei V. . . . . . . EF-10.2 FRI (p211)
Erni, Daniel . . . . . . . . . . . . CH-P.25 WED (p137)
Ernstorfer, Ralph . . . . . . . . CG-3.5 THU (p147)
Ertl, Marie . . . . . . . . . . . . . . . . CC-7.2 FRI (p210)
Ertl, Marie C. . . . . . . . . . . . . . CC-4.2 FRI (p180)
Esan, Ayomikun . . . . . . . . ∙CL-P.11 FRI (p222)
Escale, Marc Reig . . . . . . JSIII-1.6 THU (p162)

Eschen, Wilhelm . . . . . . . CH-6.2 WED (p116),
CH-P.10 WED (p136)
Escoto, Esmerando . . . . ∙CF-10.1 THU (p143),
EE-4.1 FRI (p201)
Esfahani, Reza Nekouie . . . CM-8.5 FRI (p186)
Esguerra, Luisa . . . . . . . . . EB-10.3 THU (p145)
Eskandari-asl, Amir . . . . . . . CG-2.2 TUE (p97)
Esmann, Martin . . . . . . . . . JSVI-1.1 TUE (p83),
EI-2.6 FRI (p196)
Esmiller, Bruno . . . . . . . . . CD-8.1 WED (p114)
Espinosa, Daniel . . . . . . . . . CE-7.1 THU (p163)
Esquivias, Ignacio . . . . . . . CB-7.4 WED (p132)
Esquvias, Ignacio . . . . . . . . CB-P.15 MON (p76)
Esser, Dominik . . . . . . . . . ∙CA-6.6 WED (p114)
Eßer, Jonas . . . . . . . . . . . . . . CA-6.6 WED (p114)
Esser, Stefan . . . . . . . . . . . . . . CA-4.1 TUE (p82),∙CA-10.4 THU (p144)
Esteban-Martín, Adolfo . . CD-6.1 TUE (p92),
CD-P.19 TUE (p101), EF-P.17 WED (p140)
Estébanez, Irene . . . . . . ∙JSIII-1.4 THU (p160),
JSIII-2.2 THU (p164)
Evans, Owen . . . . . . . . . . . . ∙EG-P.4 TUE (p107)
Evlyukhin, Andrey . . . . . . . EG-2.5 MON (p62)
Evrard, Bertrand . . . . . . . . . . ∙EI-4.1 FRI (p210)
Ewers, Benjamin . . . . . . . . CA-P.12 MON (p74)
Ezquerra, Tiberio A. . . . . . CM-9.2 FRI (p190)

F
Fabbri, Riccardo . . . . . . . . . . . EE-4.3 FRI (p205)
Fabert, Marc . . . . . . . . . . . . CD-9.1 WED (p122)
Fabre, Nicolas . . . . . . . . . . ∙EB-7.6 WED (p121)
Fabrizi, Federico . . . . . . . ∙CA-9.3 WED (p130)
Facciala’, Davide . . . . . . . . . CF-2.5 MON (p63),
CM-6.3 TUE (p94), JSI-5.5 THU (p149),
CG-3.2 THU (p143)
Faini, Giulia . . . . . . . . . . . . . . . CL-6.2 FRI (p191)
Fainozzi, Danny . . . . . . . . . JSI-1.4 WED (p112)
Fainsin, David . . . . . . . . . ∙EB-13.4 THU (p167)
Faist, Jérôme . . . . . . . . . . . . JSII-2.2 MON (p61),
EG-3.1 MON (p66), CD-3.3 MON (p68),
CK-6.2 WED (p124), CB-8.3 THU (p144),
CB-8.4 THU (p144), CB-8.5 THU (p146),
CB-8.6 THU (p148), CB-9.1 THU (p148),
CB-9.2 THU (p150), CB-9.3 THU (p150),
CC-4.1 FRI (p180), CC-4.3 FRI (p182),
CC-4.5 FRI (p186), CH-13.2 FRI (p183),
ED-6.4 FRI (p194), EC-3.1 FRI (p201)
Falco, Andrea Di . . . . . . . . EH-4.2 THU (p158),
EH-4.6 THU (p162)
Falcoz, Franck . . . . . . . . . . . CG-P.3 THU (p173)
Fallnich, Carsten . . . . . . . . CF-8.4 WED (p127),
CD-10.1 WED (p128), CH-13.5 FRI (p187)
Falsi, Ludovica . . . . . . . . . . ∙EF-10.5 FRI (p215)
Famà , Francesca . . . . . . . . EA-P.2 THU (p174)
Fan, Guangyu . . . . . . . . . . . . CD-4.5 TUE (p86),
CG-3.2 THU (p143)
Fan, Kezhou . . . . . . . . . . . . . ∙EG-P.8 TUE (p107)
Fan, Tongmiao . . . . . . . . . . . CD-3.4 MON (p70)
Fan, Yizhe . . . . . . . . . . . . . . . . PP-1.3 MON (p64),
CB-P.1 MON (p75), ∙CB-P.3 MON (p75)
Fang, Tianyu . . . . . . . . . . . ∙CH-P.2 WED (p136)
Fantova, Jorge . . . . . . . . . . . ∙CM-6.5 TUE (p96)
Fara, Jan . . . . . . . . . . . . . . . . CA-8.3 WED (p118)
Farace, Bonaventura . . . . CF-10.1 THU (p143)
Fargin, Evelyne . . . . . . . . . . . CE-1.2 MON (p53)

Authors' Index

Farid, Nazar . . . . . . . . . . . CM-P.21 MON (p78)
Farina, Serena . . . . . . . . . . . CH-9.3 THU (p145)
Farkas, Arnold . . . . . . . . . . CG-4.1 THU (p149)
Farooq, Aamir . . . . . . . . . . . . ED-2.6 MON (p63)
Farrel, Carl . . . . . . . . . . . . . CH-10.4 THU (p153)
Farrer, Ian . . . . . . . . . . . . . . . PD-1.9 THU (p170)
Farsari, Maria . . . . . . . . . . . CM-1.1 MON (p52),
CM-1.4 MON (p54), PP-1.8 MON (p64),
CM-3.2 MON (p66), CM-P.2 MON (p77),
CM-P.3 MON (p77), CM-P.4 MON (p77),
CM-P.12 MON (p77), CM-P.31 MON (p78),
CH-12.4 THU (p167), CM-8.5 FRI (p186),
CC-6.3 FRI (p204), CM-11.4 FRI (p214)
Fasano, Matteo . . . . . . . . . . . JSVI-1.4 TUE (p89)
Faßbender, Alexander . . . . CK-15.5 FRI (p214)
Fatome, Julien . . . . . . . . . CD-8.5 WED (p120),
EF-2.2 WED (p131), ∙PD-2.7 THU (p171)
Fattahi, Hanieh . . . . . . . . . . CF-9.3 WED (p131)
Faugier-Tovar, Jonathan . . . CD-6.4 TUE (p96)
Faupel, Franz . . . . . . . . . . . CK-P.19 TUE (p105)
Faure, Nicolas . . . . . . . . . CH-P.18 WED (p137),
CL-P.15 FRI (p222)
Fayard, Nikos . . . . . . . . . . . . . EA-7.4 FRI (p196)
Fedder, Helmut . . . . . . . . . EB-11.6 THU (p155)
Fedeli, Jean-Marc . . . . . . . CK-4.3 WED (p112)
Federico, Michelangelo . . ∙CJ-P.14 FRI (p220)
Federman, Yotam . . . . . . . . CG-5.4 THU (p161)
Fedorov, Sergey A. . . . . . . . . EA-9.1 FRI (p210)
Fedorov, Vladimir Yu. . . . . . EE-2.3 FRI (p187)
Fedoryshyn, Yuriy . . . . . . . CI-3.1 WED (p123)
Fedotov, A. B. . . . . . . . . . . . . . CL-7.1 FRI (p201)
Fedotov, Alexander . . . . . . . ∙EJ-P.9 MON (p80)
Fedotov, Andrei . . . . . . . . . . . CF-5.5 TUE (p99)
Fedotova, Anna . . . . . . . . . . . ∙EG-5.3 TUE (p94)
Fedotova, Olga . . . . . . . . . . . . EJ-P.9 MON (p80)
Fedrizzi, Alessandro . . . . . . EB-5.5 TUE (p97),
EB-9.3 WED (p131), CD-14.3 FRI (p215)
Fehér, Beatrix . . . . . . . . . ∙EE-P.12 WED (p139),
PD-1.2 THU (p170)
Fehrembach, Anne-Laure
CD-P.10 TUE (p100)
Feichtner, Thorsten . . . . . . ∙CK-2.3 TUE (p86),
EH-5.6 THU (p168)
Feifel, R. . . . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Feifel, Raimund . . . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130), JSI-5.4 THU (p147)
Feise, David . . . . . . . . . . . . CB-11.5 THU (p168)
Feist, Armin . . . . . . . . . . . . . EG-3.3 MON (p68),
EG-6.2 WED (p108), EF-9.2 FRI (p203)
Fellinger, Jakob . . . . . . . . . . CF-8.3 WED (p125)
Feneyrou, Patrick . . . . . . . . . CH-4.4 TUE (p96)Feng, Ye . . . . . . . . . . . . . . . . . CF-7.3 WED (p117)
Feng, Zitong . . . . . . . . . . . . . . . CI-8.1 FRI (p210)
Fennel, Thomas . . . . . . . . . JSI-3.1 WED (p122)
Fergestad, Halvor R. . . . . ∙CK-1.3 MON (p68),
CK-P.18 TUE (p105)
Ferhatovic, Adin . . . . . . . . CB-11.6 THU (p168)
Ferlaino, Francesca . . . . . . . . EA-7.1 FRI (p188)
Fermann, Martin . . . . . . . . ED-3.3 MON (p69),∙CD-5.6 TUE (p91)
Fernandes, Russell . . . . . . . CH-16.4 FRI (p215)
Fernandez, Alma . . . . . . . . CH-1.5 MON (p57),∙CL-7.6 FRI (p209)
Fernandez, Arnaud . . . . . . EF-3.3 THU (p144),
PD-2.2 THU (p170)
Fernández, Estrella . . . . . . CH-15.5 FRI (p209)

Fernandez, T. Toney . . . . CM-7.1 WED (p108)
Fernandez, Toney . . . . . . . CJ-4.6 WED (p127),
CJ-7.2 FRI (p182)
Fernandez, Toney Teddy . . CJ-6.1 THU (p143)
Fernandez de Cordoba, Pedro
EF-P.5 WED (p139), EF-6.6 THU (p168)
Fernández-Irigoyen, Joaquín
CL-1.4 MON (p71)
Fernandez-Nuñez, Sara . . CL-4.5 THU (p169)
Fernández-Villoria, Francisco
EE-3.1 FRI (p189)
Féron, Patrice . . . . . . . . . . . . . CK-3.5 TUE (p96)
Ferranti, Giacomo . . . . . . ∙EB-6.2 WED (p109)
Ferrari, Andrea C. . . . . . . . . . CL-6.5 FRI (p197)
Ferrari, Eugenio . . . . . . . . . . CA-P.2 MON (p74)
Ferraro, Mario . . . . . . . . . . . EF-4.4 THU (p154),
EF-7.1 FRI (p181), EF-7.4 FRI (p185),
EF-7.5 FRI (p187), EJ-3.3 FRI (p185)
Ferraro, Rebecca . . . . . . . . CD-1.2 MON (p54)
Ferré, Amélie . . . . . . . . . . . . CL-4.2 THU (p165)
Ferreira, Paulo H.D. . . . . . EB-6.1 WED (p109)
Ferreira, Tiago . . . . . . . . . JSIII-P.14 FRI (p225)
Ferrera, Marzia . . . . . . . . . . PD-2.8 THU (p171)
Ferrier, Alban . . . . . . . . . . . . . EG-5.1 TUE (p92)
Ferrier, Lydie . . . . . . . . . . . . CK-15.4 FRI (p214)
Fersini, Francesco . . . . . . . . . CL-6.3 FRI (p195)
Fertig, Florian . . . . . . . . . . . . EB-5.1 TUE (p93),∙EB-9.2 WED (p131)
Feuerer, Lennart . . . . . . . . . . . EE-5.1 FRI (p211)
Feurer, Thomas . . . . . . . . . JSI-1.2 WED (p110),
JSI-1.4 WED (p112), CC-1.2 THU (p151)
Feurstein, Paul . . . . . . . . . . PP-1.13 MON (p65),
JSIV-P.2 WED (p141)
Février, Sébastien . . . . . . . . CD-13.4 FRI (p205)
Fibrich, Martin . . . . . . . . ∙CA-P.11 MON (p74),
CA-8.4 WED (p118)
Fickler, Robert . . . . . . . . . . CI-1.2 WED (p109),CI-1.4 WED (p113), ∙EB-7.3 WED (p117),
CD-10.2 WED (p130),
EB-12.1 THU (p157), EC-3.4 FRI (p205),
EE-5.4 FRI (p215)
Field, James W. . . . . . . . . . CK-P.12 TUE (p104),
CM-7.4 WED (p112), CE-P.17 THU (p172),
CE-11.5 FRI (p216)
Figueiredo, Jose . . . . . . . . . CK-13.3 FRI (p192),
JSIII-5.5 FRI (p209), ∙JSIII-P.16 FRI (p225)
Filip, Radim . . . . . . . . . . . . . EA-P.7 THU (p175)
Filipkowski, Adam . . . . . . . . . CJ-9.1 FRI (p200)
Filipovich, Matthew . . . . . JSIII-3.3 FRI (p185)
Filippov, Valery . . . . . . . . . . CJ-5.1 WED (p129)
Filler, Thomas . . . . . . . . . . . CH-13.3 FRI (p183)
Filloux, Pascal . . . . . . . . . . . EB-6.6 WED (p115)
Filonenko, Georgy A. . . . . . . CK-3.1 TUE (p92)
Finazzi, Marco . . . . . . . . . . . EG-2.1 MON (p58),
PD-2.8 THU (p171)
Finco, Giovanni . . . . . . . . . CD-1.2 MON (p54),
JSII-2.2 MON (p61), CK-1.1 MON (p66),
EB-13.1 THU (p163), CE-9.5 FRI (p196)
Fink, Franziska . . . . . . . . . . . CF-P.4 TUE (p102)
Finkler, Amit . . . . . . . . . . . . EB-7.2 WED (p117)
Finot, Christophe . . . . . . . CD-9.2 WED (p122),
CE-7.5 THU (p169), EF-10.3 FRI (p213)
Finot, Christphe . . . . . . . . . . EF-10.2 FRI (p211)
Fiorentino, Marco . . . . . . . CK-P.11 TUE (p104)
Fioretto, Dario . . . . . . . . . . . . EB-3.1 MON (p67)Firstenberg, Ofer . . . . . . . . EB-7.1 WED (p115)

Fischer, Anna . . . . . . . . . . . . ∙EF-8.4 FRI (p197),
CK-14.2 FRI (p202)
Fischer, Bennet . . . . . . . . . . CI-4.6 WED (p135)
Fischer, Daniel . . . . . . . . . . . CM-2.1 MON (p58)
Fischer, Ingo . . . . . . . . . . . JSIII-1.4 THU (p160),
JSIII-2.2 THU (p164)
Fischer, Julian . . . . . . . . . . . CG-4.4 THU (p153)
Fischer, Julius . . . . . . . . . . CK-11.5 THU (p168)
Fischer, Peter . . . . . . . . . . . CG-3.6 THU (p149),∙CG-P.13 THU (p174)
Fisicaro, Matteo . . . . . . . . ∙EA-P.11 THU (p175)
Fissore, Matteo . . . . . . . . . . . CE-11.4 FRI (p214)
Fjodorow, Peter . . . . . . . . . ∙CA-1.2 MON (p52)
Flatae, Assegid M. . . . . . . ∙EB-7.5 WED (p119)
Fleischman, Zackery . . . . . CA-3.1 MON (p66)
Flender, Roland . . . . . . . . . . CM-9.5 FRI (p196)
Fletcher, Simon . . . . . . . . CH-10.6 THU (p155)
Fleury, Romain . . . . . . . . . . . . EC-2.2 FRI (p193)
Flimelova, Miroslava . . . CM-P.26 MON (p78)
Flint, Alex I. . . . . . . . . . . ∙CM-7.6 WED (p114),
CJ-5.5 WED (p133), EF-P.11 WED (p140),∙CE-P.30 THU (p173), CD-14.5 FRI (p217)
Flisgen, Thomas . . . . . . . . . CE-P.9 THU (p172)
Flodgren, Vidar . . . . . . . . . ∙JSIII-5.2 FRI (p205)
Floery, Tobias . . . . . . . . . . . . CA-1.5 MON (p56),
CF-12.4 FRI (p215)
Florentin, Raphaël . . . . . . CJ-5.4 WED (p133),∙CJ-5.6 WED (p135), CJ-P.18 FRI (p221)
Flores, Yuri Victorovich . ∙CB-9.6 THU (p154)
Flores Esparza, Sergio Iván
CK-12.4 FRI (p184)
Florez, Jefferson . . . . . . . . . EB-2.2 MON (p61),
EB-8.5 WED (p127), CD-13.6 FRI (p209)
Florian, Camilo . . . . . . . . . CM-2.1 MON (p58),∙CM-4.5 TUE (p86)
Flöry, Tobias . . . . . . . . . . . . . CF-11.6 FRI (p209)
Foglia, Laura . . . . . . . . . . . ∙JSI-1.3 WED (p112),
JSI-1.5 WED (p114), JSI-P.1 WED (p141)
Fokine, Michael . . . . . . . . . CM-1.6 MON (p56),∙CE-11.1 FRI (p210), CJ-P.25 FRI (p221)
Follman, David . . . . . . . . . . CE-6.1 THU (p157)
Folpini, Giulia . . . . . . . . . . CE-P.10 THU (p172)
Foltynowicz, Aleksandra ∙ED-2.4 MON (p61),
ED-2.5 MON (p63), ED-P.4 MON (p79),
ED-4.1 TUE (p83)
Fondell, Mattis . . . . . . . . . . . . EE-3.3 FRI (p195)
Fong, Kin-Chung . . . . . . . . . . EI-3.2 FRI (p204)
Fons, Paul . . . . . . . . . . . . . . . . . EI-P.2 FRI (p224)
Fontaine, Nicolas K. . . . . . . CI-4.2 WED (p131)
Foran, Joseph . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Ford, Bethan . . . . . . . . . . . . . CI-8.5 FRI (p214),
CI-P.2 FRI (p219), ∙CL-P.12 FRI (p222)
Fordell, Thomas . . . . . . . . . . ED-P.3 MON (p79)
Forget, Nicolas . . . . . . . . . . . . CF-5.3 TUE (p97),
CF-6.1 WED (p109), CF-9.3 WED (p131),
CG-3.4 THU (p145), CG-P.16 THU (p174),
CF-12.3 FRI (p213)
Forrer, Andres . . . . . . . . . . . . CC-4.1 FRI (p180),
CC-4.5 FRI (p186), CH-13.2 FRI (p183)
Forrest, Richard . . . . . . . . . . . CB-4.5 TUE (p91)
Forster, Patrick . . . . . . . . . . ∙CJ-10.5 FRI (p214)
Foster, Michael . . . . . . . . . CH-10.3 THU (p151)
Fournel, Thierry . . . . . . . . CM-P.15 MON (p77)
Fournier, Aurélie . . . . . . . . CC-2.3 THU (p161)
Fournier, Corinne . . . . . CH-P.18 WED (p137),

233

CL-P.15 FRI (p222)
Francés, Jorge . . . . . . . . . . CM-P.29 MON (p78)
Francesconi, Saverio . . . . EB-6.6 WED (p115),∙EB-P.22 THU (p177)
Francis, Henry . . . . . . . . . . . CK-P.8 TUE (p104),
CK-4.4 WED (p112), CA-9.6 WED (p134),
PD-1.6 THU (p170)
Franckié, Martin . . . . . . . . CH-13.2 FRI (p183)
Franco, Enar . . . . . . . . . . . . . ∙EJ-P.3 MON (p80),∙CF-4.1 TUE (p83)
Franczyk, Marcin . . . . . . . . . . CJ-9.1 FRI (p200)
Frank, Jernej . . . . . . . . . . ∙CH-12.3 THU (p167)
Frank, Milan . . . . . . . . . . . . . CA-P.1 MON (p74),
CA-P.9 MON (p74)Frankis, Henry . . . . . . . . . CA-9.6 WED (p134)
Franz, Yohann . . . . . . . . . . . CK-6.3 WED (p124)
Frassetto, Fabio . . . . . . . . . JSI-2.5 WED (p118),
CF-9.4 WED (p133), CG-3.2 THU (p143),
CG-5.3 THU (p159)
Fratalocchi, Andrea . . . . . CH-2.2 MON (p58),
JSIV-1.4 WED (p118), CM-8.4 FRI (p184),
JSIII-P.6 FRI (p224), JSIII-P.12 FRI (p225)
Frazer, Jonathan . . . . . . . . EB-6.2 WED (p109),
EB-P.16 THU (p177)
Freeman, Joshua . . . . . . . . . CC-2.3 THU (p161)
Fregoni, Jacopo . . . . . . . . . . . . EG-4.2 TUE (p84)
Freiberg, Katharina . . . . . . CM-2.1 MON (p58)
Freiwang, Peter . . . . . . . . . PP-2.9 WED (p121),
EB-P.1 THU (p176)
Frenz, Martin . . . . . . . . . . . . . CL-P.6 FRI (p221)
Freudenstein, Josef . . . . . ∙CG-5.1 THU (p157)
Freysz, Eric . . . . . . . . . . . . . . CE-10.3 FRI (p206),
CJ-P.15 FRI (p220)
Freysz, Valérian . . . . . . . . . . . CJ-8.5 FRI (p196),
CJ-P.15 FRI (p220)
Fricke, Jörg . . . . . . . . . . . . . . CB-P.5 MON (p75),
CB-P.14 MON (p76), CB-4.4 TUE (p91),
CF-6.5 WED (p113), CB-10.4 THU (p160),
CB-11.2 THU (p164),
CB-11.4 THU (p166), CB-11.5 THU (p168)
Friebel, Patrick . . . . . . . . . . . CF-2.5 MON (p63)Friedrich, Conrad . . . . . . . CH-9.5 THU (p149)
Friedrich, Jochen . . . . . . . EB-10.5 THU (p147)
Friedt, Jean-Michel . . . . . . . ED-3.2 MON (p69)
Frigerio, Jacopo . . . . . . . . . . . CD-5.5 TUE (p91)
Frimmer, Martin . . . . . . . . ∙EB-1.3 MON (p55),∙EA-9.3 FRI (p212)
Fritsch, Kilian . . . . . . . . . . . CD-2.1 MON (p58),
CD-P.30 TUE (p101), CF-P.17 TUE (p103),
CF-6.4 WED (p113), CF-7.4 WED (p119),
CF-10.2 THU (p143), CL-7.5 FRI (p207)
Fritzsche, Alexander . . . . . . ∙EC-1.3 FRI (p185)
Froehly, Luc . . . . . . . . . . . . . . CM-4.1 TUE (p82),
EE-2.2 FRI (p185)
Froh, Jan . . . . . . . . . . . . . . . . CA-6.2 WED (p108)
Frolov, Mikhail . . . . . . . . . . . CA-1.2 MON (p52)
Fruhling, Colton . . . . . . . CE-P.26 THU (p173)
Frühling, Ulrike . . . . . . . . . JSI-5.3 THU (p145)
Frymire, Augustine . . . . . CH-5.2 WED (p113)
Fu, Daiheng . . . . . . . . . . . . ∙CK-P.18 TUE (p105)
Fu, Ming . . . . . . . . . . . . . . . . . PD-1.9 THU (p170)
Fu, Qiang . . . . . . . . . . . . . . . . . CD-6.6 TUE (p98),
CD-7.6 WED (p114), ∙CJ-9.3 FRI (p204)
Fu, Silin . . . . . . . . . . . . . . . . . ∙EF-P.7 WED (p139)
Fu, Xing . . . . . . . . . . . . . . . . . JSIII-P.4 FRI (p224)
Fu, Yuxi . . . . . . . . . . . . . . . . . CF-P.11 TUE (p103)

Fuchsberger, Johannes . . . . CH-3.3 TUE (p86)
Fuenzalida, Jorge . . . . . . . . EB-8.1 WED (p123),
EB-8.2 WED (p123), EB-8.4 WED (p125)
Fuerbach, Alex . . . . . . . . . CM-P.10 MON (p77),
CJ-6.1 THU (p143), ∙CJ-7.2 FRI (p182)
Fuerbach, Alexander . . . . ∙CJ-4.6 WED (p127)
Fuertjes, Pia . . . . . . . . . . . . . . CF-12.6 FRI (p217)
Fuji, Takao . . . . . . . . . . . . . . EG-6.3 WED (p110),∙JSI-2.4 WED (p118), ∙CJ-8.3 FRI (p194),∙CF-12.1 FRI (p211)
Fujii, Shun . . . . . . . . . . . . . CD-P.17 TUE (p101),
CK-P.26 TUE (p105), CI-8.3 FRI (p212)
Fujikata, Jun-ichi . . . . . . . . CC-P.11 FRI (p218)
Fujimoto, Masaki . . . . . . . . JSI-2.4 WED (p118)
Fujimoto, Rintaro . . . . . . . . EB-P.9 THU (p176)
Fujimoto, Yasushi . . . . . . . . . CA-4.4 TUE (p86),
CJ-5.2 WED (p131), CJ-9.2 FRI (p204),
CJ-P.4 FRI (p220)
Fujiwara, Mikio . . . . . . . . . EB-12.4 THU (p161)
Fukuda, Takumi . . . . . . . . . . . ∙EI-P.2 FRI (p224)
Fukui, Kosuke . . . . . . . . . . . EA-2.6 THU (p148)
Fule, Miklos . . . . . . . . . . . . CA-8.5 WED (p120),
CG-P.9 THU (p174)
Fulop, Jozsef . . . . . . . . . . . . . . CC-P.2 FRI (p218)
Fülöp, József A. . . . . . . . . . ∙CC-1.5 THU (p155)
Funken, Sebastian . . . CM-LIM.6 WED (p121)
Furch, Federico . . . . . . . . . CF-10.3 THU (p145)
Furfaro, Luca . . . . . . . . . . . . . CM-4.1 TUE (p82),
CM-8.6 FRI (p186), EE-2.2 FRI (p185)
Furness, Tom . . . . . . . . . . . CH-10.6 THU (p155)
Fürst, Lukas . . . . . . . . . . . ∙CD-7.3 WED (p110),
CH-P.19 WED (p137)
Furukawa, Hideaki . . . . . . . CI-4.1 WED (p129)
Furusawa, Akira . . . . . . . . . EA-2.2 THU (p142),
EA-2.6 THU (p148), EA-3.6 THU (p154)
Furutani, Yuji . . . . . . . . . . . . CF-12.1 FRI (p211)
Fusella, Fabrizio . . . . . . . . . . EF-10.5 FRI (p215)
Fyrillas, Andreas . . . . . . . . EB-6.1 WED (p109)

G
G. Kazansky, Peter . . . . . . . CJ-5.1 WED (p129)
Gaafar, Mahmoud . . . . . . CA-9.6 WED (p134),
PD-1.6 THU (p170)
Gaafar, Mahmoud A. . . . . JSII-2.4 MON (p63),
CK-P.8 TUE (p104), ∙CK-4.4 WED (p112)
Gaal, Benedek . . . . . . . . . . EB-P.33 THU (p178)
Gaal, Peter . . . . . . . . . . . . . ∙CA-8.5 WED (p120)
Gabbrielli, Tecla . . . . . . . ∙EF-P.16 WED (p140)
Gacemi, Djamal . . . . . . . . . . . CH-4.4 TUE (p96)
Gaffney, Kelly J. . . . . . . . . . . . EE-3.3 FRI (p195)
Gagliardi, Gianluca . . . . . . CH-2.5 MON (p62),∙CK-13.5 FRI (p196)
Gagrani, Nikita . . . . . . . . CK-10.5 THU (p160)
Gahlmann, Timo . . . . . . . ∙CK-8.3 THU (p144)
Gaida, Christian . . . . . . . . . CJ-10.3 FRI (p212),
CL-8.5 FRI (p215)
Gaida , John H. . . . . . . . . . . . EG-3.3 MON (p68)
Gailevičius, Darius . . . . . . CE-3.3 MON (p69),∙CM-P.27 MON (p78), CA-4.6 TUE (p88),
CM-6.2 TUE (p92), CK-3.6 TUE (p98),
CE-11.2 FRI (p212)
Gaio, Michele . . . . . . . . . . . . CK-14.2 FRI (p202)
Galagan, Boris . . . . . . . . . . . CA-1.2 MON (p52)
Galán, Marina F. . . . . . . . . . . CF-1.3 MON (p57)
Galán, Marina Fernández

Authors' Index∙EE-P.8 WED (p138)
Galante, Giulia . . . . . . . . . . . ∙CH-4.3 TUE (p96)Gali, Sushma . . . . . . . . . . ∙CE-P.23 THU (p173)
Galiakhmetova, Diana . . . . . CJ-P.9 FRI (p220),
CJ-P.23 FRI (p221)
Galiffi, Emanuele . . . . . . . . EH-1.3 WED (p132)
Galimberti, Marco . . . . . . CF-P.23 TUE (p103),
CA-8.2 WED (p116)
Galindo, Jefferson A. O. CH-P.7 WED (p136),
CE-P.28 THU (p173)
Galland, Christophe . . . . . . EG-3.4 MON (p68)Gallego, Guillermo . . . . . EB-10.3 THU (p145)
Gallego, Sergi . . . . . . . . . . . CM-P.29 MON (p78)
Galler, Anna . . . . . . . . . . . . ∙EE-1.3 WED (p111)
Gallet, Isabelle . . . . . . . . . . CE-7.5 THU (p169)
Galli, Iacopo . . . . . . . . . . . . CH-14.2 FRI (p193)
Galli, Matteo . . . . . . . . . . . . . . EA-8.5 FRI (p208)
Galli, Paola . . . . . . . . . . . . . . CI-3.4 WED (p127)
Gallician, Guillaume . . . . . JSI-4.3 WED (p130)
Gallmann, Lukas . . . . . . . . . ∙CG-2.3 TUE (p99),∙CG-6.1 THU (p163)
Gallo, Katia . . . . . . . . . . . . . . CD-1.3 MON (p54),
CK-1.2 MON (p66), CK-1.3 MON (p68),
CK-1.5 MON (p70), CK-P.18 TUE (p105),
CL-5.4 FRI (p187), CE-9.4 FRI (p194)
Galvanauskas, Karolis . . . . CE-11.2 FRI (p212)
Galzerano, Gianluca . . . . . PD-2.1 THU (p170)
Gammon, Daniel . . . . . . . CE-P.21 THU (p172)
Gandola, Massimo . . . . . . . . EA-6.3 FRI (p186)
Gandolfi, Marco . . . . . . . . . JSVI-1.4 TUE (p89),
CK-6.3 WED (p124)
Ganesh, Sandhya . . . . . . . ∙EA-P.14 THU (p175)
Gangrskaia, Elizaveta . . . . EG-P.2 TUE (p106),∙CF-9.2 WED (p131)
Ganija, Miftar . . . . . . . . . . ∙CA-8.1 WED (p114)
Gannott, Florentina . . . . . CK-5.1 WED (p114)
Ganti, Radhakrishna . . . . . . . CI-7.3 FRI (p204)
Gao, Lei . . . . . . . . . . . . . . . . . . ∙ED-5.5 FRI (p186)
Gao, Ming . . . . . . . . . . . . ∙CD-10.1 WED (p128)
Gao, Yan . . . . . . . . . . . . . . . . ∙CK-1.4 MON (p68),
CD-P.1 TUE (p100)
Gaponenko, Maxim . . . . . . . CF-P.4 TUE (p102)
Garbin, Bruno . . . . . . . . . . . . EF-8.1 FRI (p189),∙CK-14.6 FRI (p208), ∙JSIII-6.2 FRI (p213)
Garcés, Ignacio . . . . . . . . . . . . CI-6.6 FRI (p196)
Garcia, Martin . . . . . . . . . . . CG-3.5 THU (p147)
Garcia, Sebastien . . . . . . . . . . EA-8.2 FRI (p202)
Garcia, Yehudit . . . . . . . . . . . EF-10.5 FRI (p215)
Garcia Arellano, Guadalupe
ED-3.5 MON (p73)
Garcia-Blanco, Sonia . . . CA-9.6 WED (p134),
PD-1.6 THU (p170)
García-Cabrera, Ana . . . . . . ∙EI-2.3 FRI (p192)
García de Abajo, F. Javier EG-1.3 MON (p56),
EG-4.5 TUE (p88), EG-P.1 TUE (p106),
EG-6.5 WED (p112), EH-2.3 THU (p144)
García de Abajo, Javier . . . . CK-2.4 TUE (p88)
Garcia-Garfido, Juan . . . CE-P.18 THU (p172)
Garcia-Mandayo, Gemma . CM-6.5 TUE (p96)
García-Monreal, Javier . ∙EF-P.17 WED (p140)
García-Montero, Maria . . CL-4.5 THU (p169)
García Tijero, José Manuel
CB-P.15 MON (p76), CB-7.4 WED (p132)
Gardes, Frederic Y. . . . . . . CK-P.2 TUE (p104),
CM-7.6 WED (p114), CE-8.6 FRI (p186)
Gardosi, Gabriella . . . . . . . . ∙CK-3.2 TUE (p92)

Garicia-Blanco, Sonia M. CK-4.4 WED (p112)
Garnache, Arnaud . . . . . . CD-8.4 WED (p118),
EF-4.2 THU (p152), EF-4.3 THU (p152),
CB-10.6 THU (p162), EF-5.2 THU (p158)
Garoli, Denis . . . . . . . . . . . . EH-2.4 THU (p146),
CE-P.1 THU (p171)
Garratt, Douglas . . . . . . . . JSI-4.6 WED (p134),
EE-3.3 FRI (p195)
Garrè, Giacomo . . . . . . . . . . . CL-6.3 FRI (p195)
Garreau de Loubresse, FélixEB-5.2 TUE (p93)
Garthoff, Robert . . . . . . . . . . . EB-5.1 TUE (p93)
Garzon, Nuria . . . . . . . . . . . CL-4.5 THU (p169)
Gaspar, Jonathan . . . . . . . CM-P.32 MON (p79)
Gasparini, Leonardo . . . . . . EA-6.3 FRI (p186)
Gates, James C. . . . . . . . . . CK-P.12 TUE (p104),
CM-7.4 WED (p112), CM-7.6 WED (p114),
CA-6.3 WED (p110), CJ-5.5 WED (p133),
EF-P.11 WED (p140), CE-P.17 THU (p172),
CE-P.30 THU (p173), CE-8.6 FRI (p186),
CE-9.2 FRI (p190), CE-11.5 FRI (p216)
Gatkine, Pradip . . . . . . . . . ∙JSII-1.4 MON (p57)
Gatsa, Oleksandr . . . . . . ∙CM-P.26 MON (p78)
Gatti, Davide . . . . . . . . . . . . ED-1.2 MON (p53),
ED-2.6 MON (p63), ED-P.2 MON (p79)
Gatto, Lorenzo . . . . . . . . . ∙CE-P.10 THU (p172)
Gaudillat, Valentine . . . . . . ∙CD-4.1 TUE (p82)
Gaul, Erhard . . . . . . . . . . . CG-P.13 THU (p174)
Gaulke, Marco . . . . . . . . . . . CA-2.4 MON (p62),
CA-2.5 MON (p62), ∙CB-2.1 MON (p66)
Gautam, Naveenta . . . . . . . . ∙CI-P.8 FRI (p219)
Gauthier-Lafaye, OlivierCD-P.10 TUE (p100),∙CK-12.4 FRI (p184)
Gawith, Corin B. E. . . . . CM-7.4 WED (p112),
CA-6.3 WED (p110), CJ-5.5 WED (p133),
EF-P.11 WED (p140), CE-P.17 THU (p172),
CE-8.6 FRI (p186), CE-9.2 FRI (p190),
CE-11.5 FRI (p216)
Gay, Mathilde . . . . . . . . . . . . CD-4.1 TUE (p82),
CJ-2.3 WED (p113)
Gbur, Greg . . . . . . . . . . . . . . . EC-P.12 FRI (p223)
Ge, Li . . . . . . . . . . . . . . . . . . . . . . EF-8.2 FRI (p193)
Gebert, Thomas . . . . . . . . . . . CF-5.1 TUE (p93)
Gebhardt, Martin . . . . . . . . CJ-10.1 FRI (p210),
CJ-10.3 FRI (p212)
Gȩbski, Marcin . . . . . . . . . . . . CB-3.2 TUE (p84)
Geesmann, Fridolin J. . . . CF-P.19 TUE (p103),∙CF-11.3 FRI (p205)
Gehl, Michael . . . . . . . . . . . . . CB-5.6 TUE (p98)
Gehring, Tobias . . . . . . . . PP-1.11 MON (p64),
EJ-P.1 MON (p79)
Geilen, Andreas . . . . . . . . . . . EF-7.3 FRI (p183),∙CD-12.6 FRI (p197)
Geiregat, Pieter . . . . . . . . . . CK-8.4 THU (p144)
Geiselmann, Michael . . . CK-4.4 WED (p112),
CA-9.6 WED (p134), PD-1.6 THU (p170)
Gellesch, Markus . . . . . . . EA-P.10 THU (p175)
Geloni, Gianluca . . . . . . . . ∙JSI-2.1 WED (p114)
Gemmell, Nathan . . . . . . . . . EB-2.2 MON (p61)
Gemmell, Nathan R. . . . . EB-8.5 WED (p127),
CD-13.6 FRI (p209)
Genchi, Luca . . . . . . . . . . ∙CD-P.35 TUE (p102),
CH-P.20 WED (p137)
Genco, Armando . . . . . . . CH-8.4 WED (p133),∙EI-4.2 FRI (p212)
Genest, Jerome . . . . . . . . . . . ED-2.6 MON (p63)
Genier, Etienne . . . . . . . . . . . ED-6.6 FRI (p196)

Gennisson, Jean-Luc . . . . . CL-2.3 THU (p151)
Genovese, Marco . . . . . . . . EB-7.1 WED (p115)
Genty, Goëry . . . . . . . . . . . . . CD-5.3 TUE (p90),
CD-9.2 WED (p122), CJ-4.4 WED (p125),
EF-10.2 FRI (p211), EF-10.3 FRI (p213)
George, Antony . . . . . . . . . CD-2.3 MON (p60)
Georges, Patrick . . . . . . . . . CF-1.4 MON (p57),
CA-3.2 MON (p68), CE-4.1 TUE (p93),
CE-4.4 TUE (p97), CF-P.3 TUE (p102),
CA-11.3 THU (p150), CE-P.29 THU (p173)
Georges, Robert . . . . . . . . . ED-2.3 MON (p61)
Georgiev , Kaloyan . . . . CA-10.5 THU (p146),
CD-11.2 FRI (p183)
Geradot, Brian D. . . . . . . . . . . EB-5.5 TUE (p97)
Gerhardt, Nils C. . . . . . . . . . CB-2.4 MON (p70)
Gerken, Martina . . . . . . . CH-P.15 WED (p137)
Germann, Matthias . . . . . . . ED-2.4 MON (p61)
Gérôme, Frédéric . . . . . . CM-P.25 MON (p78),
CD-8.3 WED (p118), CJ-4.2 WED (p123),
CD-14.2 FRI (p213)
Gerritsma, Kirsten . . . . . . . . CB-5.1 TUE (p92)Gerz, Daniel . . . . . . . . . . . . . CF-P.2 TUE (p102),∙CL-2.1 THU (p149), CL-5.3 FRI (p185)
Getman, Fedor . . . . . . . . . . CH-2.2 MON (p58),
JSIII-P.6 FRI (p224)
Ghadimi, Amir . . . . . . . . . . . . CE-9.3 FRI (p192)
Ghadimi, Amir H. . . . . . . . . . CE-9.6 FRI (p196)
Ghafur, Omair . . . . . . . . . . . CG-4.5 THU (p153)
Ghalanos, George N. . . CD-10.5 WED (p132)
Ghanem, Bernard . . . . . . . . JSIII-P.6 FRI (p224)
Ghawas, Muhammad . . . . . ∙CJ-P.15 FRI (p220)
Ghazaryan, Lilit . . . . . . . CK-11.4 THU (p166)
Ghelfi, Paolo . . . . . . . . . . . . . . . CI-7.1 FRI (p200)
Gheorghe, Lucian-Marian CA-P.4 MON (p74)
Ghezellou, Misagh . . . . . . EB-11.1 THU (p149)
Ghislanzoni, Silvia . . . . . . CH-2.1 MON (p58),
CL-6.1 FRI (p189), CL-6.5 FRI (p197)
Gholam-Mirzaei, Shima . ∙CF-3.2 MON (p67)
Gholipour, Behrad . . . . . CE-P.20 THU (p172),
EI-3.4 FRI (p206), JSIII-P.13 FRI (p225)
Ghorbel, Inès . . . . . . . . . . . CD-2.5 MON (p62),
EA-8.5 FRI (p208)
Ghosh, Alekhya . . . . . . . . ∙CD-9.6 WED (p126),
CK-8.1 THU (p142), CK-8.6 THU (p148),
EF-6.3 THU (p166)
Ghosh, Anirban . . . . . . . . . ∙EC-P.12 FRI (p223)
Ghosh, Debashri . . . . . . . . . . EE-5.2 FRI (p211)
Ghosh, Payel . . . . . . . . . . . ∙EH-P.17 THU (p179)
Ghosh, Somnath . . . . . . . . CK-P.28 TUE (p105)
Giakoumakis, Georges . . . CL-4.2 THU (p165)
Giambra, Marco Angelo . CI-3.4 WED (p127)
Giancola, Silvio . . . . . . . . . . JSIII-P.6 FRI (p224)
Giannessi, L. . . . . . . . . . . . . . JSI-3.5 WED (p126)
Giannessi, Luca . . . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130)
Giannetti, Ambra . . . . . . . . . CL-1.4 MON (p71)
Gibert, Luna . . . . . . . . . . . CM-P.25 MON (p78)
Gibson, Brant C. . . . . . . . . . . CA-5.3 TUE (p96)
Gibson, Graham . . . . . . . . . . EA-6.1 FRI (p180)
Gibson, Graham M. . . . . . EG-6.6 WED (p114)
Gierschke, Philipp . . . . . CF-10.4 THU (p145),
EE-4.2 FRI (p203), CJ-10.1 FRI (p210)
Gierss, Peter . . . . . . . . . . . . . CB-P.10 MON (p76)
Giesberts, Martin . . . . . . . CA-6.6 WED (p114)
Giesen, Steffen . . . . . . . . . . EA-P.18 THU (p175)
Giesz, Valérian . . . . . . . . . . EB-11.4 THU (p153)

234

Gigan, Sylvain . . . . . . . . . . . CI-1.2 WED (p109),
EA-3.3 THU (p150), JSIII-3.3 FRI (p185)
Gigli, Carlo . . . . . . . . . . . . JSIII-1.5 THU (p160)
Gilaberte Basset, Marta . EB-8.2 WED (p123),∙EB-8.4 WED (p125)
Gilaberte Basset, Mata . . . EB-8.1 WED (p123)
Gilbert, Audrey . . . . . . . . . . . . CB-4.1 TUE (p90)
Gili, Valerio Flavio . . . . . . . ∙EA-6.3 FRI (p186)
Gilicze, Barnabás . . . . . . . . CF-P.21 TUE (p103)
Gilinger, Tibor . . . . . . . . . . CA-8.5 WED (p120),
CG-P.9 THU (p174)
Gilles, Hervé . . . . . . . . . . . . CJ-5.6 WED (p135),
CJ-P.18 FRI (p221)
Gillgrass, Sara-Jayne . . . . . . . CB-4.5 TUE (p91)
Gini, Emilio . . . . . . . . . . . . CK-6.2 WED (p124),
CB-9.3 THU (p150)
Ginis, Vincent . . . . . . . . . . ∙EH-5.2 THU (p164)
Ginolas, Arnim . . . . . . . . CB-11.2 THU (p164),
CB-11.3 THU (p166), CB-11.5 THU (p168)
Ginzburg, Vlad . . . . . . . . . CG-P.12 THU (p174)
Gioannini, Mariangela . . . CB-6.2 WED (p124)
Giordano, Luidgi . . . . . . . . CA-3.2 MON (p68),
CE-4.5 TUE (p99), CE-10.4 FRI (p206)
Giordano, Maria Caterina
CK-15.1 FRI (p210)
Giordano, Stefano . . . . . . . . JSVI-1.4 TUE (p89)
Giorgini, Antonio . . . . . . . CH-2.5 MON (p62),
CK-13.5 FRI (p196)
Giovannetti, Gaia . . . . . . . . CG-3.2 THU (p143)
Giovannini, Tommaso . . . ∙EJ-2.2 MON (p60),
EH-P.20 THU (p179)
Giparakis, Miriam . . . . . . . . CC-4.2 FRI (p180)
Giraldo, Andrus . . . . . . . . . . . EF-8.5 FRI (p197)
Girard, Sylvain . . . . . . . . . . CJ-5.6 WED (p135),
CJ-P.18 FRI (p221)
Girardi, Marcello . . . . . . . . CK-1.4 MON (p68),
CD-P.1 TUE (p100), CF-P.7 TUE (p102),
CI-2.2 WED (p119), EF-3.5 THU (p146),∙CK-9.3 THU (p152), ED-6.2 FRI (p190)
Girish, K . . . . . . . . . . . . . . . . . . . CI-8.6 FRI (p216)
Girnghuber, Anna . . . . . . . CG-5.1 THU (p157)
Gisselbrecht, Mathieu . . . . . CF-5.2 TUE (p95),
JSI-4.3 WED (p130), CG-5.2 THU (p159)
Gittinger, Moritz . . . . . . . . . . . EI-2.6 FRI (p196)
Giudici, Massimo . . . . . . ∙CD-8.4 WED (p118),
CB-7.3 WED (p130), EF-4.3 THU (p152),
EF-5.2 THU (p158)
Giust, Remo . . . . . . . . . . . . . . CM-4.1 TUE (p82),
EE-2.2 FRI (p185)
Glaab, Johannes . . . . . . . . . . CB-P.5 MON (p75),
CB-11.2 THU (p164), CB-11.3 THU (p166)
Gladyshev, Andrey . . . . . . . CB-9.5 THU (p152)
Glandorf, Thomas J. . . . . . CL-3.6 THU (p163)
Glauser, Adrian Michael JSII-2.2 MON (p61)
Glebov, Leonid . . . . . . . . . . CF-P.5 TUE (p102),
CH-7.6 WED (p127)
Glicenstein, Simon . . . . . . CL-3.1 THU (p157),∙CL-3.4 THU (p161)
Globisch, Björn . . . . . . . . . CB-P.11 MON (p76),
CC-2.2 THU (p161)
Gloor, Sebastian . . . . . . . . . ∙CC-4.3 FRI (p182),
CC-4.5 FRI (p186)
Gloppe, Arnaud . . . . . . . . . . . . EI-3.1 FRI (p200)
Głowacki, Maciej . . . . . . . . CE-7.4 THU (p169)
Glushkov, Kirill . . . . . . . . CG-P.12 THU (p174)
Głuszek, Aleksander . . . . . CA-2.3 MON (p60),

ED-2.4 MON (p61)
Gnanavel, Abira . . . . . . . . . . EA-4.5 THU (p160)
Gnilitskyi, Iaroslav . . . . ∙CM-P.18 MON (p78),
CM-P.28 MON (p78)
Goavec-Merou, Gwenaël . ED-3.2 MON (p69)
Göb, Madita . . . . . . . . . . . . . . . CL-8.4 FRI (p215)
Göb, Moritz . . . . . . . . . . . . . . . EA-9.6 FRI (p216)
Goda, Keisuke . . . . . . . . . . . . ∙CL-5.1 FRI (p181)
Godfrey, Michael . . . . . . . . CE-5.3 THU (p151)
Godin, Thomas . . . . . . . . . . CA-2.4 MON (p62),
CC-2.4 THU (p163)
Goetschy, Arthur . . . . . . . . . CH-1.2 MON (p53)
Gognau, Alexandre . . . . . . CJ-3.6 WED (p121)
Goldberg, Aaron Z. . . . . . . EB-7.3 WED (p117)
Goldmann, Mirko . . . . . ∙JSIII-2.2 THU (p164)
Goldner, Philippe . . . . . . . . . EG-5.1 TUE (p92)
Golestani, Ali . . . . . . . . . . . . EB-9.5 WED (p133)
Golling, Matthias . . . . . . . . CA-2.4 MON (p62),
CA-2.5 MON (p62), CB-2.1 MON (p66)
Golombek, Adina . . . . . . . . CK-12.5 FRI (p186)
Golyari, Keyhan . . . . . . . . . CF-P.16 TUE (p103)
Gomes, Anderson . . . . . . . . CE-7.1 THU (p163)
Gomes, Anderson S. L. . CD-P.11 TUE (p100),
CD-P.16 TUE (p100)
Gomes, Tiago . . . . . . . . . . . CF-7.2 WED (p117),
CB-7.1 WED (p128)
Gomes, Tiago dos Santos∙CB-7.6 WED (p134)
Gomez, Rodrigo . . . . . . . . EB-11.6 THU (p155),
EB-P.10 THU (p176), EB-P.20 THU (p177)
Gómez de León, Alvaro . . . EC-2.3 FRI (p195)
Gomez-Pedrero, Jose Antonio
CL-4.5 THU (p169)
Gonçalves, P. André D. . . ∙EG-1.3 MON (p56),
EG-6.5 WED (p112)
Gonçalves, Rogéria R. . . . CH-P.7 WED (p136)
Goncharov, Semyon . . . . . . . CF-5.4 TUE (p97),
CD-P.12 TUE (p100),∙CF-P.17 TUE (p103),
CF-10.2 THU (p143), CL-7.5 FRI (p207)
Gong, Jingwen . . . . . . . . . . . . CI-P.11 FRI (p219)
Gonoskov, Arkady . . . . . . . CG-3.6 THU (p149)
Gonoskov, Ivan . . . . . . . . . . EA-P.8 THU (p175)
Gonzales-Ureta, Junior R.
EB-11.2 THU (p151), EB-P.24 THU (p177)
Gonzalez, Anthony . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Gonzalez, Luis . . . . . . . . . . EB-P.10 THU (p176)
Gonzalez-Fernandez, Veronica∙CL-4.5 THU (p169)
Gonzalez-Izquierdo, Bruno
CG-P.13 THU (p174)
Gonzalez Martin del Campo, Luis Javier∙EB-12.6 THU (p163)
González-Vázquez, Jesús . . EE-3.1 FRI (p189)
Goodwin, Melissa . . . . . . . . EG-P.7 TUE (p107)
Goodwin, Melissa J. . . . . CK-P.33 TUE (p106),
CK-P.37 TUE (p106)
Goossen-Schmidt, Nora∙CB-10.4 THU (p160)
Gopinath, Vishaal . . . . . . . JSII-2.3 MON (p61)
Gorbenko, Ilya . . . . . . . . ∙EH-P.12 THU (p179)
Gordon, Iouli E. . . . . . . . . . . ED-2.4 MON (p61)
Gorelova, Daria . . . . . . . . . ∙JSI-3.3 WED (p124)
Gores, Florian . . . . . . . . . . CG-P.16 THU (p174)
Gorza, Simon-Pierre . . . . CF-P.14 TUE (p103),
EF-2.5 WED (p135), EF-5.5 THU (p160),
EF-6.4 THU (p166)

Authors' Index

Goschin, Florian . . . . . . . . . PD-2.6 THU (p171)
Goth, Katharina . . . . . . . . ∙CA-3.4 MON (p70),
CA-P.16 MON (p74)
Goto, Takuma . . . . . . . . . . . EG-6.3 WED (p110)
Götte, Jörg B. . . . . . . . . . . . . . ∙EJ-2.5 MON (p62)
Gotti, Riccardo . . . . . . . . . . ED-1.2 MON (p53),
ED-P.2 MON (p79), CD-6.1 TUE (p92),
CA-10.2 THU (p142)
Goulden, Lachlan . . . . . . . . CD-12.5 FRI (p197)
Gour, Jeetendra . . . . . . . . ∙EH-2.5 THU (p148),
CD-11.3 FRI (p185), ∙CD-11.4 FRI (p187)
Gourgues, Ronan . . . . . . . ∙CH-8.2 WED (p131)
Govdeli, Alperen . . . . . . . ∙CK-13.4 FRI (p194)
Gow, Paul C. . . . . . . . . . . . CM-7.4 WED (p112),
CM-7.6 WED (p114), CE-P.17 THU (p172),
CE-P.30 THU (p173), ∙CE-8.6 FRI (p186),
CE-11.5 FRI (p216)
Grabar, Alexander . . . . . . EF-P.23 WED (p141)
Grábner, Martin . . . . . . . . . . CJ-10.6 FRI (p216)
Grabulosa, Adrià . . . . . . . ∙JSIII-4.5 FRI (p197),
JSIII-6.1 FRI (p211)
Graf, Thomas . . . . . . . . . . . CB-P.10 MON (p76),
CA-4.1 TUE (p82), CA-9.2 WED (p130),
CA-10.4 THU (p144),
CE-P.19 THU (p172), CI-P.4 FRI (p219),
CI-P.5 FRI (p219)
Gräfe, Markus . . . . . . . . . . ∙EB-8.1 WED (p123),
EB-8.2 WED (p123), EB-8.4 WED (p125),
EA-P.19 THU (p175), EB-P.10 THU (p176)
Gräfe, Stefanie . . . . . . . . . . . EA-P.8 THU (p175)
Graffitti, Francesco . . . . . . . EB-5.5 TUE (p97),
CD-14.3 FRI (p215)
Granados, Eduardo . . . . . . . ∙CA-5.1 TUE (p92)Grande, Adrian . . . . . . . . . . . ∙CJ-8.5 FRI (p196)
Grande, Marco . . . . . . . . . . . CH-3.4 TUE (p86),
CB-4.1 TUE (p90), CB-4.2 TUE (p90),
CK-P.6 TUE (p104), CK-P.32 TUE (p106),
CH-P.14 WED (p136),
EH-P.18 THU (p179),
EH-P.19 THU (p179), CH-15.1 FRI (p201)
Grandi, Samuele . . . . . . . . . ∙EG-5.1 TUE (p92),∙EB-9.1 WED (p129), ∙EB-9.4 WED (p133)
Grandjean, Nicolas . . . . . CB-10.3 THU (p158)
Grange, Rachel . . . . . . . . . . CD-1.2 MON (p54),
JSII-2.2 MON (p61), CK-1.1 MON (p66),
EH-4.1 THU (p156), JSIII-1.6 THU (p162),
EB-13.1 THU (p163), CE-9.5 FRI (p196),
CE-9.6 FRI (p196), JSIII-4.3 FRI (p195)
Grant, Thomas . . . . . . . . CH-12.1 THU (p163),∙EC-3.5 FRI (p207)
Grantzioti, Eleni . . . . . . . . CH-16.3 FRI (p215)
Graß, Tobias . . . . . . . . . . . . CD-7.1 WED (p108)
Grassani, Davide . . . . . . . . JSII-2.4 MON (p63),
CD-5.2 TUE (p90)
Grasselli, Federico . . . . . . . EB-9.3 WED (p131)
Grateau, Antonin . . . . . . . . EB-8.3 WED (p125)
Graupeter, Sarina . . . . . . . . . CB-2.3 MON (p68)Gray, David . . . . . . . . . . . . . . PP-1.8 MON (p64),
CM-P.4 MON (p77)
Grebing, Christian . . . . . . CF-P.21 TUE (p103)
Grebnev, Kirill . . . . . . . . . . ∙CJ-4.3 WED (p125)
Greculeasa, Madalin . . . . . . CA-P.4 MON (p74)
Green, Alice . . . . . . . . . . . . . JSI-5.3 THU (p145)
Green, Andrew . . . . . . . . . CH-11.2 THU (p159)
Green, Jonathan T. . . . . . . CA-8.4 WED (p118)
Green, Natalie K. . . . . . . . . CC-1.4 THU (p153),∙CC-3.2 THU (p165), ∙CC-P.8 FRI (p218)
Greentree, Andrew D. . . . . CA-5.3 TUE (p96)
Greetham, Greg M. . . . . . . CF-P.22 TUE (p103)
Greffet, Jean-Jacques . ∙JSIV-2.1 WED (p122),
EA-7.4 FRI (p196)
Gregersen, Niels . . . . . . . . EB-P.33 THU (p178)
Gregory, Thomas . . . . . . . . . . EA-6.1 FRI (p180)
Grelet, Sacha . . . . . . . . . . . . ∙CH-1.3 MON (p55)
Gresch, Tobias . . . . . . . . . . CB-9.2 THU (p150)
Gretzinger, Thomas . . . . . CJ-4.6 WED (p127),∙CJ-6.1 THU (p143)
Griebner, Uwe . . . . . . . . . . . CA-2.1 MON (p58),
CF-10.3 THU (p145), CF-10.5 THU (p147),∙CF-12.6 FRI (p217)
Griesbach, Nele . . . . . . . . . . ED-P.5 MON (p79)
Griesbeck, Michael . . . . . . . CA-3.4 MON (p70)
Grigoletto, Massimo . . . . . . CB-2.3 MON (p68)
Grigorova, Teodora F. . . . . . EE-4.1 FRI (p201)
Grigutis, Robertas . . . . . ∙CD-P.25 TUE (p101)
Grillet, Christian . . . . . . . . CK-4.3 WED (p112)
Grillot, Frederic . . . . . . . . . . CB-5.6 TUE (p98),
CB-9.4 THU (p152), CI-5.1 FRI (p180)
Grinblat, Gustavo . . . . . . . . EH-3.2 THU (p150)
Grineviciute, Lina . . . . . . . ∙CE-3.3 MON (p69),
CK-3.6 TUE (p98), CE-11.2 FRI (p212)
Griol, Amadeu . . . . . . . . . . EG-6.4 WED (p112)
Grisard, Arnaud . . . . . . . . . CD-1.4 MON (p56),
CD-2.5 MON (p62)
Grishina, Diana A. . . . . . . CK-P.33 TUE (p106)
Grobecker, Anja . . . . . . . . . . CJ-6.3 THU (p145)
Gröblacher, Simon . . . . . . EB-13.2 THU (p165)
Gröbmeyer, Sebastian . . CD-7.2 WED (p108),∙CF-6.4 WED (p113), PD-1.4 THU (p170)
Grojo, David . . . . . . . . . . . . . CM-2.2 MON (p58)
Groll, Daniel . . . . . . . . . . . . . . . EI-2.5 FRI (p196)
Grosjean, Lucas . . . . . . . . . . CE-5.2 THU (p151)
Gross, Simon . . . . . . . . . . . JSII-3.2 MON (p69),
JSII-3.3 MON (p69), ∙CM-7.1 WED (p108),
CJ-4.6 WED (p127)
Große-Wortmann, Uwe . . JSI-P.4 WED (p141)
Grosshans, Frédéric . . . . . EB-12.2 THU (p159)
Gruber, Anton . . . . . . . . . CF-P.13 TUE (p103),
CJ-3.4 WED (p119)
Gründeman, Elmer . . . . . . ED-1.1 MON (p53)
Grüneberg, Mario . . . . . . . . . CL-P.9 FRI (p222)
Grünewald, Lorenz . . . . . ∙EG-P.2 TUE (p106),
CF-9.2 WED (p131)
Grychtol, Patrik . . . . . . . . ∙JSI-P.3 WED (p141)
Grzelczak, Marek . . . . . . . . EG-P.6 TUE (p107)
Gstir, Sebastian . . . . . . . . . . . EB-3.2 MON (p67)
Guasoni, Massimiliano . . CK-6.3 WED (p124)
Guccione, Giovanni . . . . . . . . EB-4.3 TUE (p87)
Guérin, Caroline . . . . . . . CH-P.11 WED (p136)
Guérineau, Théo . . . . . . . . . ∙CE-1.2 MON (p53)
Guérit, Stéphanie . . . . . . . CH-10.1 THU (p149)
Guerreiro, Paulo Tiago . CD-P.18 TUE (p101),
PD-1.3 THU (p170), CL-7.4 FRI (p205)
Guery, Leo . . . . . . . . . . . . . . . CF-2.3 MON (p61),
EE-1.1 WED (p109)
Guessoum, Assia . . . . . . . . . CE-1.6 MON (p57)
Guezennec, Tristan . . . . . . . . CJ-P.2 FRI (p220)
Guggenmos, Alexander . . CA-P.22 MON (p75)
Gühr, Markus . . . . . . . . . . . JSI-2.6 WED (p120),
JSI-5.3 THU (p145), JSI-5.4 THU (p147)
Guichard, Florent . . . . . . . . CF-P.3 TUE (p102)
Guidici, Massimo . . . . . . . . EF-4.2 THU (p152)

Guidry, Melissa . . . . . . . . . EB-11.1 THU (p149)
Guidry, Melissa A. . . . . . . . . CD-5.1 TUE (p90),∙EA-2.4 THU (p144)
Guillaume, Olivier . . . . . . . CM-1.2 MON (p52)
Guillemey, Lilian . . . . . . . . CK-12.6 FRI (p186)
Guillemot, Lauren . . . . . . . CA-2.4 MON (p62),
CA-3.2 MON (p68), CA-11.2 THU (p150)
Guillet de Chatellus, Hugues
CH-11.1 THU (p157), CI-P.12 FRI (p219)
Guina, Mircea . . . . . . . . . . . EG-1.4 MON (p56),
CB-2.2 MON (p66), CB-5.5 TUE (p96),
PP-2.3 WED (p120), CE-P.3 THU (p171),
EB-P.12 THU (p177)
Guiramand, Léo . . . . . . . . . CC-2.4 THU (p163)
Guiraud, Germain . . . . . . . CJ-5.4 WED (p133)
Gülmüş, Merve . . . . . . . . . . . . EI-1.4 FRI (p186)
Gumann, Alexander . . . . . CK-5.1 WED (p114)
Gumenyuk, Regina . . . . . . CJ-5.1 WED (p129),
CJ-8.4 FRI (p196)
Gundogdu, Sinan . . . . . . . ∙CK-7.2 WED (p130)
Günther, Axel . . . . . . . . . . . . CE-5.4 THU (p153)
Guntinas-Lichius, Orlando CL-6.5 FRI (p197)
Guo, Chen . . . . . . . . . . . . . . . . CF-5.2 TUE (p95),
CF-P.18 TUE (p103), CG-4.6 THU (p155),
CG-5.2 THU (p159), ∙PD-1.3 THU (p170)
Guo, Hairun . . . . . . . . . . . . EF-P.20 WED (p140)
Guo, Tuan . . . . . . . . . . . . . . . . CL-1.4 MON (p71)
Guo, Zhaoheng . . . . . . . . . ∙JSI-2.3 WED (p116)
Gupta, Abhishek . . . . . . . . . ∙CC-P.2 FRI (p218)
Gupta, Sumanta . . . . . . . . . JSIII-3.2 FRI (p183)
Gupta, Vineet . . . . . . . . . . . . . CC-P.2 FRI (p218)
Gurevich, Svetlana . . . . . . . . EJ-1.3 MON (p56),
CB-P.7 MON (p76), EF-5.2 THU (p158),∙EF-6.5 THU (p168)
Gurevich, Svetlana V. . . . . . EJ-P.2 MON (p79),
EJ-P.8 MON (p80), EF-4.2 THU (p152),
EF-4.3 THU (p152), JSIII-P.15 FRI (p225)
Gushiken, Eiyu . . . . . . . . . . ∙CM-P.8 MON (p77)
Gustave, François . . . . . CH-P.26 WED (p137),
CJ-6.4 THU (p145), CJ-P.1 FRI (p220)
Guth, Lennart . . . . . . . . . . ∙ED-P.5 MON (p79),
CF-8.2 WED (p125), CG-6.5 THU (p169)
Gutierrez, Jaime . . . . . . . . . . EB-P.8 THU (p176)
Gutowski, Piotr . . . . . . . . . CB-P.12 MON (p76),
CB-P.21 MON (p76)
Guttmann, Martin . . . . . . . . CB-2.3 MON (p68)Gutz, Daria . . . . . . . . . . . . . . CL-4.2 THU (p165)
Guyon, Olivier . . . . . . . . . . JSII-1.3 MON (p55),
JSII-3.3 MON (p69)
Guzmán-Silva, Diego . . CK-P.16 TUE (p105),
CK-12.3 FRI (p182)
Gyger, Samuel . . . . . . . . . . . . CK-1.2 MON (p66)

H
Haarlammert, Nicoletta . . . CJ-1.3 TUE (p97),
CJ-2.4 WED (p113), CJ-6.3 THU (p145),
CJ-8.2 FRI (p192)
Haas, Walter . . . . . . . . . . . . CD-8.1 WED (p114)
Haboucha, Adil . . . . . . . . . . . ∙CJ-P.2 FRI (p220)
Hadden, John . . . . . . . . . . . . CK-15.2 FRI (p210)
Hader, Joerg . . . . . . . . . . . . . . . EI-2.4 FRI (p194)
Hadfield, Robert . . . . . . . . . . . EI-3.3 FRI (p204)
Hadji, Emmanuel . . . . . . . . CL-3.1 THU (p157),
CL-3.4 THU (p161)
Haefner, Constantin L. . . . ∙PL-3.1 TUE (p90)235

Haelterman , Marc . . . . . . . . EJ-P.5 MON (p80),
EF-5.6 THU (p162)
Haertelt, Marko . . . . . . . . . . CB-9.6 THU (p154)
Hafermann, Martin . . . . . CK-4.2 WED (p110)
Häfner, Constantin . . . . . CF-10.4 THU (p145)
Hagedorn, Sylvia . . . . . . . . CK-7.2 WED (p130)
Haghighi, Nasibeh . . . . . JSIII-2.4 THU (p166)
Haglund, Åsa . . . . . . . . . . . . ∙CB-2.3 MON (p68)Hahl, Felix . . . . . . . . . . . . . . . . CA-5.3 TUE (p96)
Hahn, Sven . . . . . . . . . . . . . . CA-6.6 WED (p114)
Hahn, Thilo . . . . . . . . . . . . . . . . EI-2.5 FRI (p196)
Hahn-Jose, Thomas . . . . . . PD-1.1 THU (p170)
Haindl, Rudolf . . . . . . . . . . ∙EG-3.3 MON (p68)
Hainer, Felix . . . . . . . . . . . . EH-P.14 THU (p179)
Haines, Jack . . . . . . . . . . . . ∙CK-6.3 WED (p124)
Hajj, Tony . . . . . . . . . . . . . . . ∙CE-1.6 MON (p57)
Hakert, Hubertus . . . . . . . . CJ-3.5 WED (p119)
Hakkarainen, Teemu . . . . . EG-1.4 MON (p56),
EB-P.12 THU (p177)
Hakobyan, Sargis . . . . . . . . CB-9.2 THU (p150)
Halas, Naomi . . . . . . . . . . JSIV-1.5 WED (p120)
Halbhuber, Maike . . . . . . . . . EG-4.3 TUE (p86)
Haldar, Raktim . . . . . . . . . . CD-14.1 FRI (p211),
CD-14.4 FRI (p215), EF-10.4 FRI (p215)
Halder, Arindam . . . . . . . . . . . CJ-9.4 FRI (p206)
Halder, Raktim . . . . . . . . . . . . EE-5.2 FRI (p211)
Hall, Layton . . . . . . . . . . . . . . ∙CF-4.2 TUE (p83)
Hallman, Kent . . . . . . . . . CD-P.31 TUE (p102),
CD-7.5 WED (p112), EH-3.5 THU (p152)
Hallum, Goran E . . . . . . . . CM-10.5 FRI (p208)
Hallum, Goran Erik . . . . ∙CM-P.24 MON (p78)
Halstuch, Aviran . . . . . . . ∙CM-7.2 WED (p108)
Hammani, Kamal . . . . . . . . CE-7.5 THU (p169)
Hamouda, Frederic . . . . . CK-10.3 THU (p158)
Hampel, Hana K. . . . . . . . CK-11.6 THU (p168)
Han, Bo . . . . . . . . . . . . . . . . . . . . EI-2.6 FRI (p196)
Han, Peng . . . . . . . . . . . . . . . . . EE-3.3 FRI (p195)
Han, Sang-Kook . . . . . . . . . . . CI-7.2 FRI (p202)
Han, Sangyoon . . . . . . . . . . CK-7.4 WED (p132)
Han, SeungYun . . . . . . . . . . ∙EC-P.10 FRI (p223)
Hanhijärvi, Kalle . . . . . . . . . ED-P.3 MON (p79)
Hanna, Marc . . . . . . . . . . . . CF-1.4 MON (p57),
CF-P.3 TUE (p102)
Hänsch, Theodor . . . . . . . . . ED-1.3 MON (p55)
Hänsch, Theodor W. . . . . . ED-2.2 MON (p59),
CD-5.1 TUE (p90), CK-7.3 WED (p132),
PD-2.1 THU (p170)
Hänsel, Wolfgang . . . . . . . . CK-1.3 MON (p68)
Hansen, K. . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Hansen, Rasmus Eilkær . . CH-1.4 MON (p55)
Hanson, Ronald K . . . . . . . . ∙CH-4.1 TUE (p92)
Hansson, Tobias . . . . . . . . . . . EF-7.1 FRI (p181)
Hanstorp, Dag . . . . . . . . . . . CG-3.6 THU (p149)
Hanus, Václav . . . . . . . . . EE-P.12 WED (p139),∙PD-1.2 THU (p170)
Hänzi, Pascal . . . . . . . . . . . . CE-7.4 THU (p169)
Haraguchi, Masanobu . . . . CC-P.11 FRI (p218)
Harb, Joelle . . . . . . . . . . . . . ∙CE-3.4 MON (p69),
CM-P.14 MON (p77)
Harbord, Edmund . . . . . . EA-P.20 THU (p175)
Harder, Irina . . . . . . . . . . . CK-5.1 WED (p114),
CK-8.6 THU (p148)
Hariharan, Anand . . . . . . . . . . CJ-1.1 TUE (p93)
Hariton, Victor . . . . . . . . . . CD-2.1 MON (p58),
CD-P.30 TUE (p101), JSI-P.4 WED (p141)
Harjanne, Mikko . . . . . . . . . . CB-5.5 TUE (p96)

Harkhoe, Krishan . . . . . . . . JSIII-P.5 FRI (p224)
Harmon, Nathaniel . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Harouri, Abdelmounaim . . EA-8.1 FRI (p200)
Harren, Frans J. M. . . . . CH-P.23 WED (p137),
CH-16.2 FRI (p213)
Harrington, Joseph . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Harrington, Kerrianne . ∙JSII-2.1 MON (p59),
CD-4.2 TUE (p82), CH-10.2 THU (p151),
CD-14.5 FRI (p217)
Harris, Robert . . . . . . . . . . . JSII-2.1 MON (p59)
Harteveld, Cornelis A. M.
CK-P.33 TUE (p106)
Harth, Anne . . . . . . . . . . . . . PD-1.1 THU (p170)
Hartl, Ingmar . . . . . . . . . . . . CA-P.2 MON (p74),
JSI-2.6 WED (p120), CF-8.3 WED (p125),∙JSI-P.4 WED (p141), JSI-5.3 THU (p145),
CF-10.1 THU (p143), PD-1.1 THU (p170),
CJ-P.7 FRI (p220)
Hartmann, Claas . . . . . . . . . PD-1.1 THU (p170)
Hartmann, Jean-Michel . CK-4.3 WED (p112)
Hartmann, Jens . . . . . . . . . CG-P.13 THU (p174)
Hartwell, Sam . . . . . . . . . . . JSI-P.4 WED (p141)
Hartwell, Samuel . . . . . . . . . CA-P.2 MON (p74)
Harvey, Clarissa M. . . . . . . ∙CJ-P.25 FRI (p221)
Hary, Mathilde . . . . . . . . . . ∙CD-5.3 TUE (p90),∙CD-9.2 WED (p122)
Hase, Eiji . . . . . . . . . . . . . . . . CC-P.11 FRI (p218)
Hase, Muneaki . . . . . . . . . . . . . EI-P.2 FRI (p224)
Hasegawa, Hiroshi . . . . . . . . . CI-6.4 FRI (p194)
Hashimoto, Rei . . . . . . . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76)
Hashizume, Jinpei . . . . . . CK-P.29 TUE (p105)
Hassan, Absar U. . . . . . . . . . . EC-1.5 FRI (p187)
Hassan, Karim . . . . . . . . . . . . . CB-5.3 TUE (p94)
Hassan, Mostafa . . . . . . . . ∙CM-3.5 MON (p70),
CM-4.1 TUE (p82), EE-2.2 FRI (p185)
Hassan, Muhammad T. . . . CE-P.9 THU (p172)
Hassan, Muhammad Tehwar
CB-10.4 THU (p160)
Hassanpour Yesaghi, Ehsan
JSI-3.1 WED (p122)
Hasse, Kore . . . . . . . . . . . . . . CM-6.1 TUE (p92),∙CK-P.3 TUE (p104)
Häßner, Denny . . . . . . . . . . . CJ-1.3 TUE (p97),
CJ-6.3 THU (p145)
Haugg, Stephanie . . . . . . . . CA-9.6 WED (p134)
Häusler, Karl . . . . . . . . . . . . ∙CB-P.5 MON (p75)
Häusler, Samuel . . . . . . . . . EB-13.1 THU (p163)
Havlíček, Jan . . . . . . . . . . . . . CA-P.7 MON (p74)
Hawkes, Steve . . . . . . . . . . . CA-8.2 WED (p116)
Hawkins, Thomas . . . . . . . . . CD-6.2 TUE (p92)
Hawkins, Thomas W. . . . . CD-7.6 WED (p114)
Haxton, Daniel . . . . . . . . . . JSI-4.6 WED (p134)
Hayashi, Kenshi . . . . . . . . . . CE-6.5 THU (p161)
Hayashi, Tetsuya . . . . . . . . . CI-4.2 WED (p131)
Hayat, Alex . . . . . . . . . . . . . . EA-5.3 THU (p166),
EB-13.5 THU (p169), EF-9.4 FRI (p205)
Hayward, Tina . . . . . . . . . . . . CF-4.2 TUE (p83),
CF-P.5 TUE (p102)
He, Hongsen . . . . . . . . . . . . . CF-P.8 TUE (p102)
He, Jijun . . . . . . . . . . . . . . . CK-4.2 WED (p110)
He, Jing . . . . . . . . . . . . . . . . . . . CL-6.5 FRI (p197)
He, Wenbin . . . . . . . . . . . . . . . CD-4.4 TUE (p86),
CD-4.6 TUE (p88)

Authors' Index

He, Zhao . . . . . . . . . . . . . . JSIV-1.4 WED (p118),
JSIII-P.12 FRI (p225)
He, Zhigang . . . . . . . . . . . . . JSI-P.5 WED (p141)
He, Zonglong . . . . . . . . . . . . CD-2.6 MON (p62)
Healy, Noel . . . . . . . . . . . . . ∙CE-1.1 MON (p53),
CE-P.11 THU (p172)
Heathcote, Robert . . . . . . . CA-8.2 WED (p116)
Heber, Michael . . . . . . . . . . JSI-3.4 WED (p126)
Hebling, János . . . . . . . . . . CC-1.5 THU (p155),
CE-P.6 THU (p171), CC-P.5 FRI (p218),
CC-P.9 FRI (p218), CC-P.13 FRI (p218),
CC-P.15 FRI (p218)
Hecht, Bert . . . . . . . . . . . . . . . . CK-2.3 TUE (p86)
Hecht, Linos . . . . . . . . . . . . . JSI-3.1 WED (p122)
Heckelmann, Ina . . . . . . . ∙CB-8.5 THU (p146),
CB-8.6 THU (p148)
Heckl, Oliver H. . . . . . . . . . CE-3.2 MON (p67),
CF-8.3 WED (p125), CE-6.1 THU (p157)
Hedir, Melissa . . . . . . . . . . . . . EF-8.1 FRI (p189)
Heffernan, Jon . . . . . . . . . . . PD-1.9 THU (p170)
Hehl, Gregor . . . . . . . . . . . . . . CF-5.4 TUE (p97),∙CL-7.5 FRI (p207)
Heidrich, Jonas . . . . . . . . . . CA-2.4 MON (p62),
CB-2.1 MON (p66)
Heidt, Alexander M. . . . . . CE-7.4 THU (p169)
Hein, Linus . . . . . . . . . . . . . CK-7.3 WED (p132)
Heindel, Tobias . . . . . . . . . EB-P.32 THU (p178)
Heine, Jan . . . . . . . . . . . . . . . CD-14.4 FRI (p215)
Heiner, Zsuzsanna . . . . . . . ∙CA-1.4 MON (p54)
Heinig, Daniel . . . . . . . . . EB-P.19 THU (p177)
Heiniger, Adam . . . . . . . . . CH-5.2 WED (p113)
Heinrich, Alexander-Cornelius
EE-5.1 FRI (p211)
Heinrich, Arne . . . . . . . . . CA-10.2 THU (p142)
Heinrich, Matthias . . . . . . . EB-2.3 MON (p61),
EB-4.2 TUE (p85), CM-7.3 WED (p110),
PP-2.10 WED (p121),
CK-11.3 THU (p166), CK-12.2 FRI (p180),
EC-1.3 FRI (p185), EC-2.1 FRI (p189),
EA-8.3 FRI (p204), EA-8.4 FRI (p206),
EF-9.1 FRI (p201), EC-P.1 FRI (p222),
EC-P.2 FRI (p223), ∙EC-P.3 FRI (p223)
Heitz, Johannes . . . . . . . . . . ∙CM-9.4 FRI (p194)
Heizenreder, Benedikt . . EA-P.2 THU (p174)
Heizer, Ludovit . . . . . . . . . . . CM-9.5 FRI (p196)
Hejda, Matěj . . . . . . . . . . . ∙JSIII-5.4 FRI (p207),
JSIII-5.5 FRI (p209), JSIII-6.3 FRI (p215)
Helal, Ahmed . . . . . . . . . . CG-P.13 THU (p174)
Held, Marcus . . . . . . . . . . . CH-6.4 WED (p118)
Heldt, Tobias . . . . . . . . . . . . ED-P.5 MON (p79),∙CF-8.2 WED (p125), CG-6.5 THU (p169)
Helfrich, Christof . . . . . ∙CH-10.5 THU (p153)
Helgason, Óskar B. . . . . . . CD-P.1 TUE (p100),
CF-P.7 TUE (p102), CK-P.35 TUE (p106),∙EF-3.5 THU (p146)
Helgason, Oskar Bjarki . . CK-9.3 THU (p152)
Helin , Philippe . . . . . . . . CE-P.16 THU (p172)
Heller, Lukas . . . . . . . . . . . . . EA-2.1 THU (p142)
Hellerer, Thomas . . . . . . . CH-8.1 WED (p129),
CH-P.35 WED (p138)
Hellwig, Tim . . . . . . . . . . . . EA-4.3 THU (p158),
CH-13.5 FRI (p187)
Helm, Manfred . . . . . . . . . . EE-P.3 WED (p138)
Hemsley, Elizabeth . . . . . CD-P.10 TUE (p100),
CH-P.16 WED (p137)
Henaff, Johan . . . . . . . . . . . EA-3.2 THU (p150),∙EB-13.6 THU (p169)
Henderson, Grant W . . . . . EA-2.5 THU (p146)
Hendra, Patrick . . . . . . . . ∙EA-P.19 THU (p175)
Hendry, Ian . . . . . . . . . . . . . . . CJ-7.4 FRI (p186),
CJ-P.12 FRI (p220)
Henke, Jan-Wilke . . . . . . ∙EG-6.2 WED (p108),∙EF-9.2 FRI (p203)
Henkel, Thomas . . . . . . . . . CL-2.1 THU (p149)
Hennin, Geraud . . . . . . . . . . ∙EA-1.3 TUE (p85)
Henning, Andrew J. . . . . . CH-7.2 WED (p123)
Hennrich, Markus . . . . . . EB-11.5 THU (p153),
EB-P.35 THU (p178)
Henrich, Brian . . . . . . . . . . . . CL-7.6 FRI (p209)
Henriksson, Nils . . . . . . . . . EH-2.4 THU (p146)
Henry, Antoine . . . . . . . . . . ∙EB-3.1 MON (p67)
Hensel, Christian . . . . . . . . CD-P.5 TUE (p100)
Hensen, Bas . . . . . . . . . . . . EB-13.2 THU (p165)
Her, Man J. . . . . . . . . . . . . . . CK-7.4 WED (p132)
Herbers, Sofia . . . . . . . . . . . ∙ED-P.3 MON (p79)
Herda, Robert . . . . . . . . . . . ED-3.4 MON (p71),
CH-P.35 WED (p138)
Herkommer, Clemens . . . CD-8.1 WED (p114)
Hermann, Benedikt . . . . . . ∙CM-8.1 FRI (p180)
Hermann, Felix . . . . . . . . . . JSIII-3.1 FRI (p181)
Hernandez, Yves . . . . . . . . . CJ-3.6 WED (p121)
Hernández-García, CarlosCF-1.3 MON (p57),
CF-2.1 MON (p59), CG-1.3 TUE (p87),
EG-P.2 TUE (p106), EE-P.8 WED (p138),
PD-1.5 THU (p170), CI-5.2 FRI (p180),
EJ-3.1 FRI (p181), EI-2.3 FRI (p192),
EE-3.5 FRI (p197)
Hernandez-Gomez, Cristina
CF-P.23 TUE (p103), CA-8.2 WED (p116)
Hernandez-Serrano, Arturo
CC-7.1 FRI (p210)
Herr, Simon . . . . . . . . . . . . . EB-8.6 WED (p127)
Herr, Tobias . . . . . . . . . . . . . JSII-2.4 MON (p63),
CD-5.2 TUE (p90), CK-P.8 TUE (p104),
CK-4.4 WED (p112), CA-9.6 WED (p134),
CK-9.4 THU (p152), CK-9.5 THU (p154),
PD-1.6 THU (p170)
Herrera, Felipe . . . . . . . . . CE-P.18 THU (p172)
Herrfurth, Oliver . . . . . . . . . . CL-8.5 FRI (p215)
Herrmann, Franziska Marie
EB-12.3 THU (p159)
Herrmann, Harald . . . . . . EB-6.3 WED (p111),
EA-5.5 THU (p168)
Herrmann, Paul . . . . . . . . . . . ∙EI-1.3 FRI (p184)
Herter, Alexa . . . . . . . . . . . ∙CD-3.3 MON (p68),
CC-5.1 FRI (p188)
Herth, Etienne . . . . . . . . . . . . CD-5.5 TUE (p91)
Hertlein, Alexander . . . . . EF-6.1 THU (p162),
EF-6.2 THU (p164)
Hertwig, Andreas . . . . . . . . CM-2.1 MON (p58)
Hertzog, Manuel . . . . . . . . EH-P.14 THU (p179)
Hertzsch, Daniel . . . . . . . . . ED-3.4 MON (p71)
Herzog, Thomas . . . . . . . . . EA-4.6 THU (p162)
Hesser, Günter . . . . . . . . . . . . CM-9.4 FRI (p194)
Hesslow, Daniel . . . . . . . . . . JSIII-3.3 FRI (p185)
Hetzel, Sabrina . . . . . . . . . . . EF-P.5 WED (p139)
Heu-Thao, Sylvie . . . . . . . . . . CH-4.3 TUE (p96)
Heuck, Mikkel . . . . . . . . . . . CB-1.3 MON (p54),∙CI-1.5 WED (p115)
Heuermann, Tobias . . . . CF-10.4 THU (p145),
CJ-10.1 FRI (p210), ∙CJ-10.2 FRI (p210),
CJ-10.3 FRI (p212)

Heydarian, Hojjat . . . . . . . . PD-1.4 THU (p170)
Heyl, Christoph M. . . . . . CF-8.3 WED (p125),
JSI-P.3 WED (p141), JSI-P.4 WED (p141),
CF-10.1 THU (p143), PD-1.1 THU (p170),
EE-4.1 FRI (p201), CJ-P.19 FRI (p221)
Heynck, Michael . . . . . . . . CF-P.16 TUE (p103)
Hidalgo-Rojas, Diego . . . . . CF-4.5 TUE (p89),∙CE-P.18 THU (p172)
Hideur, Ammar . . . . . . . . . . CA-2.4 MON (p62),
CA-3.2 MON (p68), CC-2.4 THU (p163)
Hiekkamäki, Markus . . . . CI-1.4 WED (p113),
EB-7.3 WED (p117), ∙EB-12.1 THU (p157)
Hieta, Tuomas . . . . . . . . . . CH-P.6 WED (p136)
Higgins, Gerard . . . . . . . . . EB-11.5 THU (p153)
Higuchi, Reiji . . . . . . . . . . . . . ∙CI-6.4 FRI (p194)
Hijazi, Frederick . . . . . . . EB-13.2 THU (p165)
Hikosaka, Yasumasa . . . . . JSI-2.4 WED (p118)
Hilico, Adèle . . . . . . . . . . . . CJ-5.4 WED (p133)
Hill, Daniel . . . . . . . . . . . . . . CH-13.6 FRI (p187)
Hill, Lewis . . . . . . . . . . . . . . . CD-P.9 TUE (p100),
CD-9.6 WED (p126), EF-P.3 WED (p139),∙EF-6.3 THU (p166), PD-2.7 THU (p171),
ED-6.1 FRI (p188)
Hillbrand, Johannes . . . . . CB-8.1 THU (p142),
ED-6.4 FRI (p194)
Hilmann, Falk . . . . . . . . . . CH-6.2 WED (p116)
Hilska, Joonas . . . . . . . . . . EB-P.12 THU (p177)
Hinkov, Borislav . . . . . . . . . . CH-3.3 TUE (p86)
Hinze, Ulf . . . . . . . . . . . . . . . . . CJ-P.3 FRI (p220)
Hiramoto, Kota . . . . . . . . . CK-5.4 WED (p118)
Hirmer, Eva-Maria . . . . . . . EF-6.3 THU (p166)
Hirosawa, Kenichi . . . . . . . CA-9.5 WED (p132)
Hisano, Daisuke . . . . . . . . . . . CI-6.3 FRI (p192),∙CI-P.1 FRI (p219)
Hisatake, Shintaro . . . . . . . CC-P.11 FRI (p218)
Hjältén, Adrian . . . . . . . . . ED-2.4 MON (p61),
ED-P.4 MON (p79), ED-4.1 TUE (p83)
Hjelme, Dag Roar . . . . . . . . . . EI-3.5 FRI (p208)
Hjort, Filip . . . . . . . . . . . . . . . CB-2.3 MON (p68)
Hlavatsch, Michael . . . . . . . . CC-7.2 FRI (p210)
Ho, Joseph . . . . . . . . . . . . . . . ∙EB-5.5 TUE (p97),
EB-9.3 WED (p131), CD-14.3 FRI (p215)
Ho, Sin-Hang (Enoch) . . . CC-3.2 THU (p165)
Ho, Xuan-Long . . . . . . . . . . . CA-P.3 MON (p74)
Ho, Ying-Lung Daniel . . . CK-P.7 TUE (p104),
CE-P.15 THU (p172)
Hoang, Nhat-Phi . . . . . . . . . CA-P.2 MON (p74)
Hoang, V. T. . . . . . . . . . . . . EF-P.15 WED (p140)
Hoang, Van Thuy . . . . . . EF-P.10 WED (p140),
CD-13.4 FRI (p205), EF-10.4 FRI (p215),
EE-5.3 FRI (p213)
Hoblos, Ayman . . . . . . . . . . CE-5.2 THU (p151)
Hoe Tan, Hark Hoe . . . . CK-10.5 THU (p160)
Hoekman, Marcel . . . . . . . . . CB-5.1 TUE (p92)
Hoekstra, Tom . . . . . . . . . . ∙CK-13.6 FRI (p196)
Hoenl, Simon . . . . . . . . . . . . CK-14.5 FRI (p206)
Hofer, Christina . . . . . . . . . CF-P.2 TUE (p102),
CD-7.2 WED (p108), EF-6.1 THU (p162),
EF-6.2 THU (p164), PD-1.4 THU (p170)
Hofer, Christoph . . . . . . . . . CF-P.4 TUE (p102)
Höfer, Marco . . . . . . . . . . . . CA-6.6 WED (p114)
Hofer, Matthias . . . . . . . . . CH-P.1 WED (p136),
CH-10.1 THU (p149)
Hofer, Tobias . . . . . . . . . . . ∙CF-7.4 WED (p119)
Hoff, Dominik . . . . . . . . . . . ∙CF-5.2 TUE (p95),∙CG-5.2 THU (p159)

236

Hoff, Ulrich . . . . . . . . . . . . . . . EA-9.5 FRI (p214)
Hofferberth, Sebastian . . . CK-15.5 FRI (p214)
Hoffet, Félix . . . . . . . . . . . . . . EB-5.2 TUE (p93),∙EA-2.1 THU (p142)
Hoffmann, Andreas . . . . . . JSI-3.1 WED (p122)
Hoffmann, Franziska . . . . . . CL-6.5 FRI (p197)
Hoffmann, Gerd-A. . . . . . CE-P.24 THU (p173)
Hoffmann, Hans-Dieter . CA-6.6 WED (p114)
Hoffmann, Manuel . . . . . ∙CK-P.13 TUE (p104)
Hoffmann, Martin . . . . . . . CA-2.2 MON (p60),
CF-12.2 FRI (p211)
Höffner, Josef . . . . . . . . . . . CA-6.2 WED (p108)
Höflich, Katja . . . . . . . . . . . EH-5.6 THU (p168)
Höfling, Sven . . . . . . . . . . . CB-8.1 THU (p142),
EB-11.2 THU (p151), EA-5.3 THU (p166),
EA-P.20 THU (p175), EB-P.24 THU (p177),
EF-9.4 FRI (p205)
Hoflund, Maria . . . . . . . . . . CG-4.6 THU (p155)
Hofmann, Martin R. . . . . . . CB-2.4 MON (p70)
Högner, Maximilian . . . . CD-7.2 WED (p108),∙EF-6.1 THU (p162), EF-6.2 THU (p164)
Höing, Dominik . . . . . . . . . . CK-1.6 MON (p72)Holl, Peter . . . . . . . . . . . . . . . . CB-2.5 MON (p72)
Holland, Kayla M. . . . . . . . . . CC-7.5 FRI (p214)
Hollm, Marko . . . . . . . . . . . . . CG-2.3 TUE (p99)
Holmen, Lars G. . . . . . . . . . . CJ-10.4 FRI (p214)
Holmes, Christopher . . . ∙CE-5.3 THU (p151),
CE-P.17 THU (p172), CE-11.5 FRI (p216)
Holtkamp, Hannah U. . . . PP-2.8 WED (p121),
CL-5.5 FRI (p187), CL-P.2 FRI (p221)
Holzmeier, Fabian . . . CM-LIM.3 WED (p117),
EE-3.1 FRI (p189)
Holzwarth, Ronald . . . . . . . CK-1.3 MON (p68),
CD-6.3 TUE (p94)
Hommelhoff, Peter . . . . . . EA-4.2 THU (p158),
PD-1.7 THU (p170)
Hommerich, Uwe . . . . . . . . CA-3.1 MON (p66)
Hondo, Fumihiro . . . . . . . . . . CJ-8.3 FRI (p194)
Hong, Hyun-Gue . . . . . . . . . ED-P.1 MON (p79)
Hong, Myung S. . . . . . . . . . CK-7.4 WED (p132)
Hönninger, Clemens . . . . CM-2.4 MON (p60),
CM-3.6 MON (p72)
Honzátko, Pavel . . . . . . . . . . CJ-P.24 FRI (p221)
Hooten, Sean . . . . . . . . . . . ∙CK-P.11 TUE (p104)
Hoppe, Niklas . . . . . . . . . . CK-11.5 THU (p168)
Horáček, Martin . . . . . . . . CA-8.3 WED (p118),
CA-8.4 WED (p118)
Horák, Michal . . . . . . . . . . . EG-P.3 TUE (p106)
Horak, Peter . . . . . . . . . . . . . CE-2.4 MON (p61),
CE-2.5 MON (p63), CK-P.12 TUE (p104),
CH-10.3 THU (p151), CE-11.5 FRI (p216)
Horn, Katinka . . . . . . . . . . . . . EE-4.1 FRI (p201)
Hornung, Florian . . . . . . . CK-11.5 THU (p168)
Horodynski, Michael . . . . EG-6.6 WED (p114)
Horsley, Simon . . . . . . . . . . EH-4.2 THU (p158),
CL-3.3 THU (p159)
Horst, Folkert . . . . . . . . . . . JSIII-3.1 FRI (p181),
JSIII-4.4 FRI (p197)
Hosaka, Masahito . . . . . . . . JSI-2.4 WED (p118)
Hosni, Mohamed. I . . . . . . . ∙CI-6.5 FRI (p196)
Hou, Lianping . . . . . . . . . . . . PP-1.3 MON (p64),
CB-P.1 MON (p75), CB-P.3 MON (p75)
Hou, Ming-Han . . . . . . . . . . CE-P.8 THU (p172)
Houard, Aurélien . . . . . . . ∙CD-P.7 TUE (p100),∙CD-8.1 WED (p114), EF-P.7 WED (p139)
Houard, Jonathan . . . . . . . . EG-P.5 TUE (p107),

CH-6.6 WED (p120), EE-P.5 WED (p138),
CC-2.4 THU (p163), CC-7.3 FRI (p212),∙CC-7.6 FRI (p216)
Houdré, Romuald . . . . . . . CL-3.1 THU (p157),
CL-3.4 THU (p161)
Houver, Sarah . . . . . . . . . . . PP-2.1 WED (p120),
CC-P.1 FRI (p218)
Høvik, Jens . . . . . . . . . . . . . . . CH-3.1 TUE (p82)
Howlader, Manotosh . . . . . . CI-P.3 FRI (p219)
Hrabina, Jan . . . . . . . . . . . . . . ED-P.7 MON (p79)
Hreb, Vasyl . . . . . . . . . . . . CE-P.12 THU (p172)
Hsieh, Leo Jih-Liang . . ∙JSIII-1.5 THU (p160)
Hsu, Chia Wei . . . . . . . . . . . CH-1.2 MON (p53)
Hu, Guyue . . . . . . . . . . . . . . . EF-5.4 THU (p160),∙CH-15.2 FRI (p205)
Hu, Hongtao . . . . . . . . . . . . . . CG-1.3 TUE (p87)
Hu, Jianqi . . . . . . . . . . . . . . . CI-1.2 WED (p109),
JSIII-P.4 FRI (p224)
Hu, Jiaqi . . . . . . . . . . . . . . . . . . . CB-3.1 TUE (p82)
Hu, Juejun . . . . . . . . . . . . . . . CD-3.5 MON (p72)
Hu, Shui-Ming . . . . . . . . . . . ∙ED-4.3 TUE (p85)
Hu, Xinxin . . . . . . . . . . . . . . . . EA-1.2 TUE (p83)
Hua, Yi . . . . . . . . . . . . . . . . . . JSI-P.4 WED (p141),∙CJ-P.7 FRI (p220)
Huang, Anqi . . . . . . . . . . . . EB-P.14 THU (p177)
Huang, Chung-Che Kevin
CK-P.7 TUE (p104), CE-P.15 THU (p172)
Huang, Dongmei . . . . . . . CD-P.27 TUE (p101),
CF-P.1 TUE (p102), CJ-3.2 WED (p117)
Huang, Guanhao . . . . . . . . EG-6.2 WED (p108),
CK-14.5 FRI (p206), EF-9.2 FRI (p203),
EA-9.1 FRI (p210)
Huang, Jian-Jang . . . . . . . . CH-15.4 FRI (p207)
Huang, Jiasheng . . . . . . . . EA-P.12 THU (p175)
Huang, Jingsheng . . . . . . . . . ED-5.5 FRI (p186)
Huang, Kai . . . . . . . . . . . . . . . . CE-8.1 FRI (p180)
Huang, Ligang . . . . . . . . . . . . ED-5.5 FRI (p186)
Huang, Lujun . . . . . . . . . . . . CD-1.5 MON (p56)Huang, Meng . . . . . . . . . . . . . CD-6.2 TUE (p92),∙CD-7.6 WED (p114)
Huang, Pei . . . . . . . . . . . . . . CF-P.11 TUE (p103)
Huang, Qi . . . . . . . . . . . . . . . . . CD-4.6 TUE (p88)
Huang, Wei-Hong . . . . . . . . CF-12.1 FRI (p211)
Huang, Yen-Chieh . . . . . . ∙CA-P.3 MON (p74),
CC-P.12 FRI (p218)
Huang, Yidong . . . . . . . . . CA-10.3 THU (p144)
Huang, Yung-Chin . . . . . . . CL-P.19 FRI (p222)
Huang, Zhiwei . . . . . . . . . EF-P.18 WED (p140)
Hübener, Hannes . . . . . . . . . CG-1.2 TUE (p85),
CG-5.3 THU (p159)
Huber, Florian . . . . . . . . . . ∙EA-P.1 THU (p174)
Huber, Heinz P. . . . . . . . . . . PP-1.9 MON (p64),
CM-P.5 MON (p77), CM-P.6 MON (p77),∙CM-10.5 FRI (p208)
Huber, Heinz Paul . . . . . . CM-P.24 MON (p78),
CM-10.3 FRI (p204)
Huber, Marinus . . . . . . . . . CL-2.1 THU (p149),
PD-1.4 THU (p170), ∙CH-13.1 FRI (p181),
CL-5.3 FRI (p185)
Huber, Robert . . . . . . . . . . CJ-3.3 WED (p117),
CJ-3.5 WED (p119), CL-8.1 FRI (p211),
CL-8.3 FRI (p213), CL-8.4 FRI (p215)
Huber, Rupert . . . . . . . . . . . . EG-4.3 TUE (p86),
CD-7.2 WED (p108), CG-5.1 THU (p157)
Huberich, Lysander . . . . . . EG-3.5 MON (p70)
Hubin, Norbert . . . . . . . . . . JSII-2.3 MON (p61)

Authors' Index

Hübner, Jens . . . . . . . . . . . . . EE-1.4 WED (p113)
Huby, Elsa . . . . . . . . . . . . . . . JSII-1.3 MON (p55)
Hudzikowski, Arkadiusz . CA-2.3 MON (p60),
ED-2.4 MON (p61)
Huelshoff, Lena . . . . . . . . . . CF-P.4 TUE (p102)
Huet, Hêlio . . . . . . . . . . . . . . . . EA-8.1 FRI (p200)
Hug, Daniel . . . . . . . . . . . ∙CA-11.5 THU (p152)
Huges, Maxime . . . . . . . . . CH-6.6 WED (p120)
Hugger, Florian . . . . . . CM-LIM.4 WED (p119)
HUGONNOT, EmmanuelCA-7.3 WED (p126)
Hugues, Maxime . . . . . . . . . EG-P.5 TUE (p107)
Huh, Chul . . . . . . . . . . . . . . CA-11.4 THU (p152)
Huidobro, Paloma A. . . . . EH-1.3 WED (p132)
Hulin, Sébastien . . . . . . . CH-P.11 WED (p136)
Hulkkonen, Hanna . . . . . . . EG-1.4 MON (p56)
Hülshoff, Lena . . . . . . . . . . . CA-3.5 MON (p72)
Hummel, Thomas . . . . . . . . . . CI-5.5 FRI (p186)
Hünecke, Christian . . . . . . EA-P.8 THU (p175)
Hung, Nguyen Viet . . . . . EF-P.19 WED (p140)
Hunger, David . . . . . . . . . . . . . EG-5.1 TUE (p92)
Hunt, Benjamin D. . . . . . . . . EA-1.1 TUE (p83)
Hunter, Diana E. . . . . . . . . ∙CF-11.5 FRI (p207)
Hunter, Robert I. . . . . . . . . EH-4.2 THU (p158)
Huppert, Simon . . . . . . . . . . . EJ-1.4 MON (p56)
Hurtado, Antonio . . . . . . . JSIII-5.4 FRI (p207),
JSIII-5.5 FRI (p209), JSIII-6.3 FRI (p215)
Hurvitz, Inbar . . . . . . . . . . CD-9.5 WED (p126)
Huser, Thomas . . . . . . . CH-P.28 WED (p137),
CL-P.16 FRI (p222)
Hüttenhofer, Ludwig . . . . CH-8.4 WED (p133)
Hutter, Sarah . . . . . . . . . . . . PD-1.4 THU (p170)
Hutter, Sarah Rebecca . . . ∙ED-3.4 MON (p71)
Huttunen, Mikko . . . . . . . . CE-7.1 THU (p163)
Huttunen, Mikko J. . . . . CD-10.2 WED (p130)
Huwyler, Nicolas . . . . . . . . . CB-2.1 MON (p66)
Huy, K. P. . . . . . . . . . . . . . . EF-P.15 WED (p140)
Huy, Kien Phan . . . . . . . . . . CK-13.1 FRI (p188)
Huyan, Yuheng . . . . . . . . . EA-P.10 THU (p175)
Huyet, Guillaume . . . . . . . . CB-7.3 WED (p130)
Huynh, Jaroslav . . . . . . . . . . CA-P.1 MON (p74)
Hwang, Sheng-Kwang . . . . . . CI-8.4 FRI (p214)
Hytönen, Roosa . . . . . . . . . . EG-1.4 MON (p56)
Hyun, Minji . . . . . . . . . . . . . CA-9.1 WED (p128)
Hyun, Young-Jin . . . . . . . . . . ∙CI-7.2 FRI (p202)

I
Iadanza, Simone . . . . . . . . . . CH-3.2 TUE (p84),
CH-3.4 TUE (p86), CK-P.6 TUE (p104),
CK-P.32 TUE (p106), CH-P.14 WED (p136)
Iazzolino, Antonio . . . . . . . CL-2.4 THU (p153)
Ibrahim, Heide . . . . . . . . . . . . CD-4.5 TUE (p86)
Ibsen, Morten . . . . . . . . . . CH-P.13 WED (p136)
Idlahcen, Said . . . . . . . . . . . CC-2.4 THU (p163)
Ignacchiti, Jim . . . . . . . . . ∙CD-8.3 WED (p118)
Ihlemann, Jürgen . . . . . . . . . CK-P.4 TUE (p104)
Ihn, Yong-sup . . . . . . . . . . . EB-P.26 THU (p177)
IJzerman, Wilbert L . . . . . PP-2.6 WED (p121),
CI-P.13 FRI (p219)
Ikeda, Kazuhiro . . . . . . . . . CK-8.2 THU (p142)
Ikeda, Naoki . . . . . . . . . . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76), CK-P.17 TUE (p105),
EC-P.11 FRI (p223)
Ikeda, Tatsuhiko N. . . . . . . EE-1.2 WED (p109)
Ikonen, Erkki . . . . . . . . . . . CH-P.6 WED (p136)

Ikuta, Rikizo . . . . . . . . . . ∙EB-11.3 THU (p151),
EB-12.4 THU (p161), EB-P.9 THU (p176),∙EB-P.15 THU (p177)
İlday, F. Ömer . . . . . . . . . . . CF-P.10 TUE (p103)
Ilie, Stefan T. . . . . . . . . . . . CM-7.6 WED (p114)
Iliou, Alexander . . . . . . . . . CH-6.2 WED (p116)
Illés, Gergő . . . . . . . . . . . . . . ∙CC-P.9 FRI (p218),
CC-P.13 FRI (p218)
Illienko, Maksym . . . . . ∙CH-P.24 WED (p137),
CH-14.5 FRI (p197)
Ilyakov, Igor . . . . . . . . . . . . . CC-P.16 FRI (p218)
Im, Dong-Gil . . . . . . . . . . . . EB-7.4 WED (p119)
Imamoglu, Atac . . . . . . . . . . . . EI-4.1 FRI (p210)
Imamura, Riku . . . . . . . . . ∙CK-P.26 TUE (p105)
Imamura, Shunsuke . . . . . CA-9.5 WED (p132)
Imani, Aref . . . . . . . . . . . . . ∙CD-2.2 MON (p58),
CF-12.4 FRI (p215)
Imlau, Mirco . . . . . . . . . . . CH-P.5 WED (p136),
CE-P.12 THU (p172)
Imoto, Nobuyuki . . . . . . . . EB-11.3 THU (p151)
Imran, Muhammad . . . . . . . ∙CI-7.1 FRI (p200)
Inagaki, Takuya . . . . . . . . . . CK-8.2 THU (p142)
Indra, Lukáš . . . . . . . . . . . . CA-8.3 WED (p118),∙CA-8.4 WED (p118)
Indra, Win . . . . . . . . . . . . . . . . ∙CI-8.1 FRI (p210)
Inoue, Asuka . . . . . . . . . . . . EA-2.6 THU (p148),∙EA-3.6 THU (p154)
Inoue, Shuichiro . . . . . . . . . PD-2.4 THU (p171)
Intravaia, Francesco . . . . . . . . EJ-4.4 FRI (p195)
Inzani, Giacomo . . . . . . . . . CF-2.4 MON (p61),∙CG-2.2 TUE (p97), PP-2.4 WED (p120),
CG-P.1 THU (p173), ∙CG-P.5 THU (p173)
Inzenhofer, Tobias . . . . . . . . . EG-4.3 TUE (p86)
Iqbal, Muhammad Waqar∙EF-P.23 WED (p141)
Iqbal, Neelam . . . . . . . . . . . . CL-3.5 THU (p161)
Isao , Morohashi . . . . . . . . . . . CI-8.2 FRI (p210)
Isaule, Felipe . . . . . . . . . . . . . . EJ-2.5 MON (p62)Isaza-Monsalve, Mariano
EB-12.3 THU (p159)
Isella, Giovanni . . . . . . . . . . . CD-5.5 TUE (p91)
Ishaaya, Amiel A . . . . . . . . CM-7.2 WED (p108)
Ishi-Hayase, Junko . . . . . . EE-P.11 WED (p139)
Ishii, Osamu . . . . . . . . . . . . . . . CJ-9.2 FRI (p204)
Ishikawa, Kenichi . . . . . . . CM-P.22 MON (p78)
Ishikawa, Kenichi L. . . . . . CM-P.8 MON (p77),
CM-5.2 TUE (p90)Ishizuka, Hiroaki . . . . . . . . . . EI-4.5 FRI (p216)
Islam, Raonaqul . . . . . . . . . . . . EJ-4.5 FRI (p197)
Ismail, I. . . . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Israelsen, Niels Møller . . . CH-1.4 MON (p55)Ito, Isao . . . . . . . . . . . . . . . . . . . CC-P.6 FRI (p218)
Ivanina, Aleksandra . . . . ∙CH-P.3 WED (p136)
Ivanov, Mikhail . . . . . . . . . . . . EC-P.6 FRI (p223)
Ivanov, Misha . . . . . . . . . . . . CG-1.5 TUE (p89),
CG-5.4 THU (p161)
Iyikanat, Fadil . . . . . . . . . . . EG-1.3 MON (p56),
EG-4.5 TUE (p88)
Izquierdo, David . . . . . . . . . . ∙CI-6.6 FRI (p196)
Izquierdo, Manuel . . . . . . . JSI-P.3 WED (p141)
Izumi, Shuro . . . . . . . . . . . . EB-P.23 THU (p177)

J
J. Kbashi, Hani . . . . . . . . . . ED-P.9 MON (p79)
Jacinto, Carlos . . . . . . . . . . . ∙CL-P.10 FRI (p222)

Jackson, Greg . . . . . . . . . . . . CE-2.1 MON (p59)
Jackson, Stuart . . . . . . . . . . . . . CJ-7.2 FRI (p182)
Jacob, Bejoys . . . . . . . . . . . . ∙CK-13.3 FRI (p192)
Jacob, Philip . . . . . . . . . . . . . CH-13.1 FRI (p181)
Jacovi, Ronen . . . . . . . . . . . . EA-5.3 THU (p166)
Jacquemin, Clément . . . . ∙CH-16.5 FRI (p217)
Jacques, Laurent . . . . . . . . CH-10.1 THU (p149)
Jacquet, Pierre-Edouard . . ∙EA-9.4 FRI (p214)
Jacquot, Maxime . . . . . . . . . CH-2.4 MON (p60)
Jagadish, Chennupati . . CK-10.5 THU (p160)
Jäger, Matthias . . . . . . . . . . ∙CE-1.3 MON (p55),
CE-1.4 MON (p55)
Jagerska, Jana . . . . . . . . . . . . ∙CH-3.1 TUE (p82)
Jahnel, Marcus . . . . . . . . . . . CC-P.16 FRI (p218)
Jaidl, Michael . . . . . . . . . . . . ∙CC-4.2 FRI (p180),
CC-7.2 FRI (p210)
Jaison, Gregory T. . . . . . . CH-10.4 THU (p153)
Jalali, Mandana . . . . . . . ∙CH-P.25 WED (p137)
Jamali, Fariba . . . . . . . . . . . ∙CI-3.3 WED (p125)
Jambunathan, Venkatesan∙CA-P.19 MON (p75)
Janner, Davide . . . . . . . . . . . . CJ-6.2 THU (p143)
Jansonas, Gaudenis . . . ∙CD-10.6 WED (p134)
Jaque, Daniel . . . . . . . . . . . . . CL-P.10 FRI (p222)
Jara-Schulz, Gladys . . . . . . . ∙EF-8.3 FRI (p195)
Jargot, Gaëtan . . . . . . . . . . . . . CD-4.5 TUE (p86)
Jarutis, Vygandas . . . . . . . . CD-P.8 TUE (p100)
Jarzyna, Marcin . . . . . . . . . . . CI-P.14 FRI (p219)
Jasim, Ali . . . . . . . . . . . . . . . . . CJ-P.24 FRI (p221)
Jasion, Greg . . . . . . . . . . . . . . CI-1.3 WED (p111)
Jasion, Gregory . . . . . . . . . . . CE-2.1 MON (p59)
Jasion, Gregory T. . . . . . . . . . . CJ-9.3 FRI (p204)
Jastrzȩbski, Marcin . . . ∙EB-10.6 THU (p149),
EA-P.21 THU (p175)
Jauberteau, Raphael . . . . . . . . EJ-3.3 FRI (p185)
Jauk, Thomas . . . . . . . . . . . CK-11.6 THU (p168)
Jáuregui, César . . . . . . . . . . . CJ-1.3 TUE (p97),∙CJ-2.4 WED (p113), CJ-4.1 WED (p123),
CJ-8.2 FRI (p192), CJ-10.1 FRI (p210),
CJ-10.3 FRI (p212), CJ-10.6 FRI (p216)
Jaurigue, Lina . . . . . . . . . . JSIII-2.3 THU (p166)
Javaloyes, Julien . . . . . . . . . . EJ-1.3 MON (p56),
CB-P.7 MON (p76), EJ-P.2 MON (p79),
EJ-P.8 MON (p80), ∙EF-4.2 THU (p152),
EF-4.3 THU (p152), EF-5.2 THU (p158),
EF-6.5 THU (p168), JSIII-P.15 FRI (p225)
Jawaid , Ali M. . . . . . . . . . CD-P.11 TUE (p100),
CD-P.16 TUE (p100)
Jaworski, Piotr . . . . . . . . . . . ED-2.5 MON (p63)
Jayantha, Ayesha . . . . . . . . ∙CE-7.5 THU (p169)
Jayaprakash, Rahul . . . . . . . . . EI-4.2 FRI (p212)
Jedrkiewicz, Ottavia . . . . . . CM-4.2 TUE (p82)
Jedrzejczyk, Daniel . . . . . CA-10.2 THU (p142)
Jeffers, John . . . . . . . . . . . . . . . EB-5.5 TUE (p97)
Jelínek, Michal . . . . . . . . . . ∙CA-P.1 MON (p74),∙CA-P.9 MON (p74), CA-P.10 MON (p74)
Jelínková, Helena . . . . . . . . CA-P.7 MON (p74),
CA-P.8 MON (p74), CA-P.10 MON (p74),
CA-P.11 MON (p74)
Jeng, Shie-Chang . . . . . . . CH-P.30 WED (p138)
Jensen, Lars O. . . . . . . . . . . JSI-P.6 WED (p141)
Jeon, Tae-In . . . . . . . . . . . . . . ∙CC-P.4 FRI (p218)
Jeong, Byung Kyu . . . . . . . . EA-2.2 THU (p142)
Jeong, Tae-In . . . . . . . . . . . ∙EH-P.5 THU (p178)
Jeong, Young Uk . . . . . . . . EE-P.13 WED (p139)
Jeong, Youngjae . . . . . . . . . CK-7.4 WED (p132)

237

Jepsen, Peter U . . . . . . . . . . CC-1.3 THU (p153)
Jepsen, Peter Uhd . . . . . . . . ∙CC-5.5 FRI (p196),
CC-6.2 FRI (p204)
Jeske, Jan . . . . . . . . . . . . . . . . . . CA-5.3 TUE (p96)
Jetter, Michael . . . . . . . . . ∙CB-P.10 MON (p76),
EA-4.6 THU (p162), EA-5.1 THU (p162),
CK-11.5 THU (p168), EA-P.12 THU (p175)
Jewell, Jeffrey . . . . . . . . . . . . JSII-1.4 MON (p57)
Jha, Abhilash . . . . . . . . . . ∙EA-P.10 THU (p175)
Jha, Animesh . . . . . . . . . . . ∙CL-3.5 THU (p161),
CE-P.22 THU (p173)
Jha, Mukund . . . . . . . . . . . . ∙CD-12.3 FRI (p193)
Ji, Guoqing . . . . . . . . . . . . . . . ∙CD-4.4 TUE (p86)
Ji, Kaiwen . . . . . . . . . . . . . . . . . EF-8.1 FRI (p189),∙EF-8.2 FRI (p193)
Ji, Xinru . . . . . . . . . . . . . . . . CK-4.2 WED (p110),∙CK-9.2 THU (p150), CB-10.1 THU (p156),∙CE-8.2 FRI (p180), EC-1.2 FRI (p183),
CK-14.1 FRI (p200)
Jiang, Dapeng . . . . . . . . . . . . CA-P.9 MON (p74)
Jiang, Jie . . . . . . . . . . . . . . . . . ED-3.3 MON (p69)
Jiang, Pisu . . . . . . . . . . . . . . . EB-1.5 MON (p57),
CK-6.4 WED (p126)
Jiang, Xiangqian . . . . . . . . CH-7.2 WED (p123)
Jiang, Xiangqian Jane . . CH-10.6 THU (p155)
Jiang, Xin . . . . . . . . . . . . . . . . CD-4.4 TUE (p86),
CD-4.6 TUE (p88)
Jiang, Xunuo . . . . . . . . . . . . . PP-1.1 MON (p64),
CA-P.6 MON (p74)
Jiang, Yujiao . . . . . . . . . . . . CD-8.2 WED (p116)
Jiang, Yuxao . . . . . . . . . . . . . JSI-P.4 WED (p141)
Jiang, Yuxin . . . . . . . . . . . . . CD-3.4 MON (p70)
Jimenez, Gloria Lesly . . . . . CE-1.4 MON (p55)
Jiménez-Galán, Álvaro . . . . EC-P.6 FRI (p223)
Jin, Duo . . . . . . . . . . . . . . . . . . ∙CA-5.2 TUE (p94)
Jirauschek, Christian . . . . CJ-3.3 WED (p117),
CL-8.3 FRI (p213)
Jiříčková, Bára . . . . . . . . . . . . CJ-9.5 FRI (p208),∙CJ-10.6 FRI (p216)
Jisha, Chandroth P . . . . . ∙CE-6.3 THU (p159),
EC-3.2 FRI (p203), EC-P.7 FRI (p223)
Jöchl, Elsa . . . . . . . . . . . . . . ∙EG-3.1 MON (p66),
CK-6.2 WED (p124)
Joel, Anna-Christin . . . . . . . CM-9.4 FRI (p194)
Joffre, Manuel . . . . . . . . . . . . CF-P.3 TUE (p102)
Joglekar, Yogesh . . . . . . . . . . . EC-1.3 FRI (p185)
Johannes, Hans-H. . . . . . . CE-P.24 THU (p173)
Johanning, Robert . . . . . . . CD-14.1 FRI (p211)
Johnson, Brandon . . . . . . . . CE-11.4 FRI (p214)
Johnson, Brett C. . . . . . . . . . CE-10.2 FRI (p204)
Johnson, Jeremy . . . . . . . . ∙CC-1.1 THU (p149)
Johnson, Jeremy A. . . . . . CC-1.4 THU (p153),
CC-3.2 THU (p165), CC-7.5 FRI (p214),
CC-P.8 FRI (p218)
Johnson, Kerr . . . . . . . . . . CH-10.4 THU (p153)
Johnson, Philip . . . . . . . . . . JSI-1.4 WED (p112)
Johnston, Benjamin . . . . . . CJ-4.6 WED (p127)
Jójárt, Péter . . . . . . . . . . . . . CF-P.21 TUE (p103)
Jolly, Alain . . . . . . . . . . . . . CH-P.11 WED (p136)
Jolly, Spencer W. . . . . . . . . CB-P.13 MON (p76),
CK-P.20 TUE (p105), EF-P.14 WED (p140),
CC-P.15 FRI (p218)
Joly, Yves . . . . . . . . . . . . . . . . CG-3.5 THU (p147)
Jones, Dafydd . . . . . . . . . . . . EG-P.4 TUE (p107)
Jones, David . . . . . . . . . . . . . EF-6.2 THU (p164)
Jones, David J. . . . . . . . . . . . EF-6.1 THU (p162)

Jones, Jonathan . . . . . . . . EA-P.10 THU (p175)
Jones, R. Jason . . . . . . . . . . ∙ED-2.1 MON (p59),
CB-P.9 MON (p76)
Jonin, Christian . . . . . . . . . EH-P.6 THU (p178)
Jonusas, Mindaugas . . . . . . CF-P.3 TUE (p102)
Jonušauskas, Linas . . . . . . ∙CM-11.5 FRI (p216)
Joos, Raphael . . . . . . . . . . CK-11.5 THU (p168),∙EA-P.12 THU (p175)
Jose, Manoj . . . . . . . . . . . . . . CE-5.5 THU (p153)
Josso, Quentin . . . . . . . . . . . CL-P.15 FRI (p222)
Jost, John . . . . . . . . . . . . . . . . CK-9.4 THU (p152)
Josyula, Nitya Kalyani . . . . CH-1.5 MON (p57)
Joulain, Frank . . . . . . . . . . . . . . CJ-P.3 FRI (p220)
Jousselin, Herve . . . . . . . . . CF-9.3 WED (p131)
Jouy, Pierre . . . . . . . . . . . . . CH-13.2 FRI (p183)
Jovanovic, Nemanja . . . . . JSII-1.4 MON (p57)Jóźwiak, Hubert . . . . . . . . . . ED-1.2 MON (p53)
Juchniewicz, Marcin . . . . . CK-P.9 TUE (p104),
CK-P.23 TUE (p105)
Juergens, Peter . . . . . . . . . . . EE-1.1 WED (p109)
Jukna, Vytautas . . . . . . . . . . CM-4.4 TUE (p86),
CD-P.25 TUE (p101), CM-8.3 FRI (p182)
Julien, Pierre . . . . . . . . . . . . . ∙CA-5.4 TUE (p96)
Jullien, Aurélie . . . . . . . . . . . . CF-5.3 TUE (p97)
Julsgaard, Brian . . . . . . . . . CM-10.2 FRI (p204)
Jumbo Nogales, Alba María∙EG-P.6 TUE (p107)
Junaid, Saher . . . . . . . . . . . . . CI-4.6 WED (p135)
Junek, Jiří . . . . . . . . . . . . . . ∙CH-8.5 WED (p133)
Jung, Joonkyo . . . . . . . . . . . CK-P.10 TUE (p104)
Jung, Junha . . . . . . . . . . . . . CF-P.20 TUE (p103),
CE-7.3 THU (p167)
Jung, Natalie . . . . . . . . . . . . . CB-2.4 MON (p70)
Jung, Robert . . . . . . . . . . . . CF-10.6 THU (p149)
Jungbluth, Bernd . . . . . . . . CA-6.2 WED (p108)
Juodagalvis, Tomas . . . . . . CF-11.2 FRI (p203)
Juodkazis, Saulius . . . . . . . . CM-1.1 MON (p52)
Jupé, Marco . . . . . . . . . . . . CD-P.24 TUE (p101),
CE-P.24 THU (p173)
Jureńczyk, Jarosław . . . . . . CK-P.9 TUE (p104)
Jürgens, Peter . . . . . . . . . . . . . CM-6.4 TUE (p96)
Jürgensen, Sabrina . . . . . . . EH-5.6 THU (p168)
Jurkevicius, Jonas . . . . . . . CF-P.13 TUE (p103)
Jurkus, Karolis . . . . . . . . . . . CF-11.2 FRI (p203)
Juska, Gediminas . . . . . . . . EA-4.4 THU (p160)
Just, Florian . . . . . . . . . . . . . . . CL-8.5 FRI (p215)
Juste-Dolz, Augusto . . . . . CH-15.5 FRI (p209)
Jusza, Anna . . . . . . . . . . . . . . CK-P.9 TUE (p104),
CH-11.6 THU (p163), CE-10.5 FRI (p208)
Jutas, Rokas . . . . . . . . . . . . . ∙CA-1.5 MON (p56),
CF-12.4 FRI (p215)

KK. Efetov, Dmitri . . . . . . . . . . EI-3.2 FRI (p204)
K. Sivan, Aswathi . . . . . . . . JSVI-1.2 TUE (p85)
K. Y. Wong, Kenneth . . . . . EF-5.4 THU (p160)
Kaakinen, Mika . . . . . . . . . . CL-1.5 MON (p73)
Kabouraki, Elmina . . . . . CM-P.31 MON (p78),∙CM-8.5 FRI (p186)
Kachorovskii, Valentin . EH-P.12 THU (p179)
Kaczmarek, Malgosia . . . . EH-P.7 THU (p178)
Kadan, Viktor . . . . . . . . . . . ∙CM-2.5 MON (p62)
Kadiwala, Moinuddin . . ∙CF-10.2 THU (p143)
Kadowaki, Takuya . . . . . . . CE-6.5 THU (p161)
Kaertner, Franz . . . . . . . . . . PD-1.6 THU (p170)

Authors' Index

Kaertner, Franz X. . . . . . . . . CJ-P.19 FRI (p221)
Kafesaki, Maria . . . . . . . . . CM-1.4 MON (p54),
PP-1.8 MON (p64), CM-P.4 MON (p77),
CC-6.3 FRI (p204), CM-11.4 FRI (p214)
Kahaei, Mohammad Hossein
CI-4.2 WED (p131)
Kahaly, Mousumi . . . . . . . . . CC-P.2 FRI (p218)
Kahle, Hermann . . . . . . . . . EG-1.4 MON (p56),∙CB-2.2 MON (p66)
Kainz, Martin A. . . . . . . . . . . CC-4.2 FRI (p180)
Kaiser, Benjamin . . . . . . . . . . . EI-4.4 FRI (p214)
Kaiser, Florian . . . . . . . . . EB-10.5 THU (p147)
Kaji, Takahiro . . . . . . . . . . . . CC-P.11 FRI (p218)
Kaksis, Edgar . . . . . . . . . . . . CA-1.5 MON (p56),
CD-2.2 MON (p58), CF-9.2 WED (p131),
CF-11.6 FRI (p209), CF-12.4 FRI (p215)
Kakuno, Tsutomu . . . . . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76)
Kalafatakis, Ilias . . . . . . . . . CD-13.1 FRI (p201)
Kalashnikov, Mikhail . . . . CG-P.3 THU (p173)
Kalashnikov, Vladimir. L. CA-1.1 MON (p52)
Kalavrouziotis, Dimitrios . . EJ-3.4 FRI (p187)
Kale, Yogeshwar . . . . . . . . EA-P.10 THU (p175)
Kalganova, Arina . . . . . . ∙CM-P.20 MON (p78)
Kalinin, Nikolay . . . . . . . . . . EB-2.1 MON (p59)
Kallega, Rakshitha . . . . . . CK-P.14 TUE (p104)
Kallinger, Birgit . . . . . . . . . EB-10.5 THU (p147)
Kallioniemi, Leevi . . . . . . . . . EG-4.4 TUE (p86)
Kalot, Ghadir . . . . . . . . . . . . CL-2.3 THU (p151)
Kalusniak, Sascha . . . . . . . . CA-3.5 MON (p72),
CA-6.1 WED (p108)
Kamel, Ayman N. . . . . . . . . ∙EG-P.9 TUE (p107)
Kamiński, Jerzy Z. . . . . . . . CG-P.8 THU (p174)
Kamp, Martin . . . . . . . . . . . EA-P.20 THU (p175)
Kamrádek, Michal . . . . . . . . CJ-9.1 FRI (p200),
CJ-9.5 FRI (p208)
Kamynin, Vladimir . . . . . EB-P.14 THU (p177)
Kanda, Natsuki . . . . . . . . . . ∙CC-5.4 FRI (p196),
CC-P.6 FRI (p218)
Kane, Deb M. . . . . . . . . . . ∙CM-P.10 MON (p77)
Kaneko, Kei . . . . . . . . . . . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76)
Kaneyasu, Tatsuo . . . . . . . . JSI-2.4 WED (p118)
Kang, Bong Joo . . . . . . . . EE-P.13 WED (p139),∙CC-1.2 THU (p151)
Kang, Guseon . . . . . . . . . . . . ∙CC-5.3 FRI (p194)
Kang, Jiqiang . . . . . . . . . . . . CH-15.2 FRI (p205)
Kaniyar Prasanna Kumar, Shreelakshmi∙CE-8.3 FRI (p182)
Kanneworff, Kirsten . . . ∙EB-P.25 THU (p177)
Kanno, Atsushi . . . . . . . . . . CC-P.11 FRI (p218)
Kansal, Ishu . . . . . . . . . . . . . . . . CJ-1.1 TUE (p93)
Kantartzis, Nikolaos V. . . . . EC-P.2 FRI (p223)
Kante, Boubacar . . . . . . . . . . ∙CB-3.4 TUE (p86)
Kantner, Markus . . . . . . . . . ∙CB-P.6 MON (p75)
Kapaklis, Vassilios . . . . . . . EH-2.4 THU (p146)
Kaplan, Ali Emre . . . . . . . . CK-5.2 WED (p116)
Kaplanis, Stefanos-Ioannis
CD-13.1 FRI (p201)
Kappert, F. Jasmin . . . . . . EG-6.2 WED (p108),EF-9.2 FRI (p203)
Kapsalidis, Filippos . . . . . CB-8.3 THU (p144),
CB-9.1 THU (p148), CB-9.3 THU (p150)
Kapteyn, Henry C. . . . . . . . . CF-2.1 MON (p59)
Kar, Goutam . . . . . . . . . . . . . . CL-6.5 FRI (p197)
Karachinsky, Leonid . . . . . CB-9.5 THU (p152)

Karagogeos, Domna . . . . . CD-13.1 FRI (p201)
Karam, Charbel . . . . . . . . . . . EA-7.5 FRI (p196)
Karam, Michella . . . . . . . . . ∙CC-7.3 FRI (p212),
CC-7.6 FRI (p216)
Kardaś, Tomasz . . . . . . . . . . CE-7.4 THU (p169)
Karhu, Juho . . . . . . . . . . . . CH-5.3 WED (p115),∙CH-P.6 WED (p136)
Kariman, Behjat Sadat . . . CM-11.3 FRI (p214)
Karlen, Lauriane . . . . . . . . . . CF-P.4 TUE (p102)
Karlsson, Magnus . . . . . . . CD-2.6 MON (p62),
CF-P.7 TUE (p102), CK-9.3 THU (p152)
Karmakar, Subhajit . . . . . . EH-P.8 THU (p178)
Karnieli, Aviv . . . . . . . . . . . CD-9.5 WED (p126)
Karnok, Mate . . . . . . . . . . . CA-8.5 WED (p120),
CG-P.9 THU (p174)
Karpa, Leon . . . . . . . . . . . . . . . EA-7.5 FRI (p196)
Karpf, Sebastian . . . . . . . . CF-P.13 TUE (p103),
CJ-3.4 WED (p119), CJ-3.5 WED (p119),
CL-8.2 FRI (p211)
Karpiński, Michał . . . . . . . EB-9.5 WED (p133),
EB-12.5 THU (p161), ∙EB-P.21 THU (p177)
Karpov, Maxim . . . . . . . . . . CK-9.4 THU (p152)
Karpowicz, Nicholas . . . . . CA-2.3 MON (p60),
CF-P.2 TUE (p102), CF-P.16 TUE (p103),
CD-7.2 WED (p108)
Karst, Maximilian . . . . . . . . ∙EE-4.2 FRI (p203)
Kartashov, Daniil . . . . . . . . EA-P.8 THU (p175)
Kartashov, Yaroslav . . . . . . EF-P.5 WED (p139),
EF-6.6 THU (p168)
Kartashov, Yaroslav V. . . . . . EJ-3.3 FRI (p185),
EF-9.1 FRI (p201)
Kärtner, Franz . . . . . . . . . . . . CF-5.1 TUE (p93),
CA-9.6 WED (p134), CE-6.4 THU (p161)
Kärtner, Franz X. . . . . . . . . CF-3.4 MON (p71),
CA-P.23 MON (p75), CK-P.8 TUE (p104),
CK-4.4 WED (p112), CD-8.2 WED (p116),
CF-8.5 WED (p127), CG-4.3 THU (p151),
CC-3.3 THU (p167), PD-1.1 THU (p170),
CC-P.5 FRI (p218), CJ-P.7 FRI (p220)
Karunakaran, Anamika nair
∙CK-P.35 TUE (p106)
Karuseichyk, Ilya . . . . . . . EB-8.3 WED (p125)
Karuseichyk, Sopfy . . . . ∙EF-P.12 WED (p140)
Karvinen, Pertri . . . . . . . . . EG-1.4 MON (p56)
Karvounis, Artemios . . . . CD-1.2 MON (p54),
EH-4.1 THU (p156)
Kaselouris, Evaggelos . . . . . CM-9.6 FRI (p196)
Kasemann, Raphael . . . . . CA-6.6 WED (p114)
Kashiwazaki, Takahiro . . EA-2.2 THU (p142),∙EA-2.6 THU (p148), EA-3.6 THU (p154)
Kasik, Ivan . . . . . . . . . . . . . . . . CJ-9.1 FRI (p200)
Kasparian, Jérôme . . . . . . . CD-8.1 WED (p114)
Kassab, Hadil . . . . . . . . . . ∙CD-7.2 WED (p108)
Kassamakov, Ivan . . . . . . CH-12.4 THU (p167)
Kassi, Samir . . . . . . . . . . . . . . ED-2.3 MON (p61)
Kasztelanic, Rafal . . . . . . . ∙CE-5.1 THU (p149)
Kato, Takashi . . . . . . . . . . ∙CH-7.3 WED (p125)
Katoh, Masahiro . . . . . . . . . JSI-2.4 WED (p118)
Katopodis, Christos . . . . . ∙CL-P.18 FRI (p222)
Katow, Hiroki . . . . . . . . . . ∙CM-P.22 MON (p78)
Katrukha, V.A. . . . . . . . . . . . . CL-7.1 FRI (p201)
Katsantonis, Ioannis . . . . . . CC-6.3 FRI (p204)
Katsipoulaki, Eirini . . . . . . . ∙EI-1.2 FRI (p182)
Katsuragawa, Hiroya . . . . . . . CJ-9.2 FRI (p204)
Katsuragawa, Masayuki ∙EF-P.22 WED (p140)
Katzer, Manuel . . . . . . . . . . . . . EI-4.4 FRI (p214)

Kaufmann, Fabian . . . . . . . JSII-2.2 MON (p61),
CK-1.1 MON (p66), JSIII-1.6 THU (p162),
EB-13.1 THU (p163), ∙CE-9.5 FRI (p196),
JSIII-4.3 FRI (p195)
Kaur, Yashpreet . . . . . . . . . JSVI-1.2 TUE (p85)
Kausas, Arvydas . . . . . . . . ∙CA-P.24 MON (p75)
Kaushalram, Archana . . . . . . CI-P.9 FRI (p219)
Kaushik, Chahat . . . . . . . . . EC-P.12 FRI (p223)
Kawamoto, Yuki . . . . . . . . ∙CK-P.29 TUE (p105)
kawanishi, Satoki . . . . . . . . . . CI-8.3 FRI (p212)
Kawano, Isao . . . . . . . . . . . . . CJ-P.10 FRI (p220)
Kawasaki, Akito . . . . . . . . . ∙EA-2.2 THU (p142)
Kawazoe, Tadashi . . . . . . . . CE-6.5 THU (p161)
Kawohl, Jan . . . . . . . . . . . . . . ED-P.3 MON (p79)
Kazakevičius, Aivaras . . ∙CA-11.6 THU (p154)
Kazakov, Dmitry . . . . . . . . . ∙CD-6.5 TUE (p96),
EF-2.4 WED (p133), CB-8.2 THU (p142)
Kazakov, Georgy . . . . . . . . EA-P.2 THU (p174)
Kazama, Takushi . . . . . . . . EA-2.2 THU (p142),
EA-2.6 THU (p148), EA-3.6 THU (p154)
Kazansky, Peter . . . . . . . . . . . CM-4.3 TUE (p84)
Kazasky, Peter . . . . . . . . . . . CH-7.4 WED (p125)
Kazemi, Mehdi . . . . . . . . . . . CA-P.2 MON (p74),
JSI-P.4 WED (p141)
Kažukauskas, Evaldas . . . . ∙CM-8.3 FRI (p182)
Kbashi, Hani . . . . . . . . . . . . EF-P.18 WED (p140)
Kbashi, Hani J. . . . . . . . . . . . ∙ED-5.4 FRI (p186)
Ke, Xinjian . . . . . . . . . . . . . . . . CE-8.1 FRI (p180)
Keathley, Philip . . . . . . . . . . . CF-5.1 TUE (p93)
Kefalogianni, Maria . . . . . ∙CD-13.1 FRI (p201)
Kehagias, Nikolaos . . . . . CM-P.31 MON (p78)
Keil, Denise . . . . . . . . . . . . . CA-P.12 MON (p74)
Keil, Robert . . . . . . . . . . . . . . EB-3.2 MON (p67)
Keizo , Inagaki . . . . . . . . . . . . . CI-8.2 FRI (p210)
Keller, Kilian R. . . . . . . . . . . . ∙EF-9.3 FRI (p205)
Keller, Ursula . . . . . . . . . . . . CA-2.4 MON (p62),
CA-2.5 MON (p62), CB-2.1 MON (p66),
CG-2.3 TUE (p99), CF-7.1 WED (p115),
CF-9.1 WED (p129), CC-2.2 THU (p161),
CG-6.1 THU (p163)
Kellert, Martin . . . . . . . . . CA-P.23 MON (p75),
CE-6.4 THU (p161), PD-1.1 THU (p170),
CJ-P.19 FRI (p221)
Kellner, Jost . . . . . . . . . . . . . CK-1.1 MON (p66),
JSIII-4.3 FRI (p195)
Kelly, Thomas . . . . . . . . . . . . CE-2.1 MON (p59),∙CH-10.3 THU (p151)
Kelly, Thomas W. . . . . . . . . CE-2.4 MON (p61),
CE-2.5 MON (p63)
Kelmanson, I. V. . . . . . . . . . . . CL-7.1 FRI (p201)
Keloth, Akshay . . . . . . . . . . CK-P.14 TUE (p104)
Kemiche, Malik . . . . . . . . . . . EA-7.4 FRI (p196)
Kemlin, Vincent . . . . . . . . . CE-5.2 THU (p151)
Kemp, Alan . . . . . . . . . . . . . . . CA-5.4 TUE (p96)
Kempf, Hannes . . . . . . . . . . ∙CF-3.1 MON (p67),
ED-3.4 MON (p71)
Kenanakis, George . . . . . . CM-P.12 MON (p77)
Kenchingotn Goldsmith, Harry-Dean∙JSII-1.3 MON (p55)
Kennedy, Brendan . . . . . . . . . CL-7.2 FRI (p203)
Kerantzopoulos, Constantinos
CC-6.3 FRI (p204)
Kerdilès, Sébastien . . . . . . CK-5.6 WED (p120)
Kermene, Vincent . . . . . . . . EF-10.4 FRI (p215)
Kerridge-Johns, William PP-2.5 WED (p121),
CG-P.2 THU (p173)

238

Kerridge-Johns, William R.
∙CJ-5.2 WED (p131)
Kershaw, Stephen V. . . . . . EG-P.8 TUE (p107)
Kervazo, Ronan . . . . . . . . . CB-10.3 THU (p158)
Kfir, Ofer . . . . . . . . . . . . . . . . EG-6.2 WED (p108)
Khajavikhan, Mercedeh . . . EC-1.5 FRI (p187),
EC-P.2 FRI (p223)
Khalili, Mohsen . . . . . . . . . CC-2.1 THU (p157),∙CC-P.7 FRI (p218)
Khan, Imran . . . . . . . . . . . . . EB-6.4 WED (p113)
Khan, Muhammad Shaukat
CE-5.5 THU (p153), CL-P.9 FRI (p222)
Khan, Sana . . . . . . . . . . . . . . ∙CE-3.6 MON (p73)
Khanda, Ankita . . . . . . . . . CK-P.39 TUE (p106)
Khatri, Dipendra . . . . . . . . . CF-3.2 MON (p67)
Khatua, Saumyakanti . . . EH-P.17 THU (p179)
Khazaee, Sara . . . . . . . . . . . . CD-2.3 MON (p60)
Khazanov, Efim . . . . . . . . CG-P.12 THU (p174)
Khodabakhsh, Amir . . . CH-P.23 WED (p137),
CH-16.2 FRI (p213)
Khodadad Kashi, Anahita
CD-9.1 WED (p122),∙EA-P.22 THU (p175), CD-14.1 FRI (p211)
Khodakovskiy, Nikita . . . CF-10.1 THU (p143)
Khramova, Y.V. . . . . . . . . . . . . CL-7.1 FRI (p201)
Khudyakov, Dmitriy . . . . . CJ-5.3 WED (p131)
Khurana, Ankur . . . . . . . . . ∙EB-1.5 MON (p57)
Kiani, Fatemeh . . . . . . . . . . PP-1.13 MON (p65),∙JSIV-1.2 WED (p116),
JSIV-P.2 WED (p141)
Kibler, Bertrand . . . . . . . . . PD-2.7 THU (p171),
CJ-7.3 FRI (p184)
Kidd, Connor . . . . . . . . . . . CC-2.3 THU (p161)
Kiedrowski, Kevin . . . . . . CD-P.24 TUE (p101)
Kiel, Thomas . . . . . . . . . . . . . . . EJ-4.4 FRI (p195)
Kieleck, Christelle . . . . . . . CA-3.4 MON (p70),
CA-P.16 MON (p74), CJ-10.5 FRI (p214)
Kielpinski, Mark . . . . . . . . . CL-2.1 THU (p149)
Kiessling, Jens . . . . . . . . . . EB-8.6 WED (p127),
CL-5.2 FRI (p183)
Kiewiet, Max . . . . . . . . . . . . CD-12.5 FRI (p197)
Kildishev, Alexander V. . CE-P.26 THU (p173)
Kilic, Max . . . . . . . . . . . . . . . CE-5.4 THU (p153)
Kilinc, Muharrem . . . . . . ∙CA-P.23 MON (p75)
Kim, Byunggi . . . . . . . . . . . CD-P.13 TUE (p100)
Kim, Danbi . . . . . . . . . . . . . . CC-P.14 FRI (p218)
Kim, Dong-Hyun . . . . . . . . CF-9.5 WED (p133)
Kim, Dong U. . . . . . . . . . . ∙CK-7.4 WED (p132)
Kim, Dongkyu . . . . . . . . . . EB-P.26 THU (p177)
Kim, Doyeong . . . . . . . . . . . CG-3.3 THU (p145)
Kim, Jungwon . . . . . . . . . . CA-9.1 WED (p128),
ED-5.2 FRI (p182)
Kim, Kanghae . . . . . . . . . . . ∙CL-P.17 FRI (p222)
Kim, Kap-Jin . . . . . . . . . . . . CF-9.5 WED (p133)
Kim, Kwanghyun . . . . . . . . . . ∙EI-3.4 FRI (p206)
Kim, Myungshik . . . . . . . . . . EB-2.2 MON (p61)
Kim, Myungshik S. . . . . . . CD-13.6 FRI (p209)
Kim, San . . . . . . . . . . . . . . . . . EH-P.5 THU (p178)
Kim, Sehyeon . . . . . . . . . . . . EH-P.5 THU (p178)
Kim, Seung-Woo . . . . . . CD-P.13 TUE (p100),CM-8.2 FRI (p180), CC-5.3 FRI (p194)
Kim, Seungchul . . . . . . . . . . EH-P.5 THU (p178)
Kim, Taewon . . . . . . . . . . . . CD-P.13 TUE (p100)
Kim, U-Shin . . . . . . . . . . . . EB-7.4 WED (p119),∙EB-10.1 THU (p143)
Kim, Yeong Gwang . . . . . . . CE-7.3 THU (p167)

Kim, Yoon-Ho . . . . . . . . . . EB-7.4 WED (p119),
EB-10.1 THU (p143)
Kim, Yosep . . . . . . . . . . . . . . EB-7.4 WED (p119)
Kim, Young-Jin . . . . . . . . . CD-P.13 TUE (p100),CM-8.2 FRI (p180), CC-5.3 FRI (p194)
Kim, Young-Ryeul . . . . . . . . CM-8.2 FRI (p180)
Kimura, Shogo . . . . . . . . . . . CK-8.2 THU (p142)
King, Ben . . . . . . . . . . . . . . CB-11.1 THU (p162),
CB-11.3 THU (p166)
Kini Manjeshwar, SushanthEA-3.1 THU (p148), CK-15.3 FRI (p212)
Kinoshita, Yutaro . . . . . . . EE-P.11 WED (p139)
Kinsey, Nathaniel . . . . . . . . CE-7.1 THU (p163)
Kioseoglou, George . . . . . . . . EI-1.2 FRI (p182),
EI-P.4 FRI (p224)
Kip, Detlef . . . . . . . . . . . . . . . CM-6.1 TUE (p92),
CK-P.3 TUE (p104)
Kippenberg, Tobias . . . . . . . CK-3.4 TUE (p96),
CB-5.4 TUE (p96), PP-2.2 WED (p120),
EF-3.1 THU (p142), EF-3.2 THU (p142),
CB-10.1 THU (p156), CE-P.2 THU (p171),
EC-1.2 FRI (p183), CE-9.1 FRI (p188)
Kippenberg, Tobias J. . . CK-4.2 WED (p110),
EG-6.2 WED (p108), ∙CB-6.1 WED (p122),
EF-2.3 WED (p133), CK-9.2 THU (p150),
CE-8.1 FRI (p180), CE-8.2 FRI (p180),
CK-14.1 FRI (p200), CK-14.5 FRI (p206),
EF-9.2 FRI (p203), EA-9.1 FRI (p210)
Kira, Mackillo . . . . . . . . . . . CG-5.1 THU (p157)
Kiraly, Csaba . . . . . . . . . . . . CA-8.5 WED (p120)
Kirchner, Adrian . . . . . . . CD-7.3 WED (p110),
CH-P.19 WED (p137)
Kirsch, Dennis C. . . . . . . . ∙CJ-3.1 WED (p115),
CJ-8.1 FRI (p188)
Kirsch, Marco Steffen . . . . . ∙EF-9.1 FRI (p201)
Kirsche, Alexander . . . . . . CH-6.2 WED (p116)
Kirste, Lutz . . . . . . . . . . . . . CE-P.13 THU (p172)
Kishikawa, Hiroki . . . . . . . . CC-P.11 FRI (p218)
Kiss, Bálint . . . . . . . . . . . . . . . CM-9.5 FRI (p196)
Kiss, Zsolt G. . . . . . . . . . . . . EE-P.7 WED (p138)
Kistenev, Yury . . . . . . . . . . . . . EJ-P.4 MON (p80)
Kitagawa, Hitoshi . . . . . . . CK-P.29 TUE (p105)
Kitamura, Kyoko . . . . . . . . CK-P.29 TUE (p105)
Kitzler-Zeiler, Markus . . . . CF-11.6 FRI (p209)
Kivshar, Yuri . . . . . . . . . . . CK-11.4 THU (p166)
Klas, Robert . . . . . . . . . . . . CH-6.2 WED (p116),
EE-4.2 FRI (p203), CJ-10.1 FRI (p210)
Klauck, Friederike . . . . . . . ∙EB-2.3 MON (p61)
Kleefoot, Max-Jonathan
CM-LIM.6 WED (p121)
Kleem, Götz . . . . . . . . . . . . . . . CI-P.4 FRI (p219)
Klein, Jürgen . . . . . . . . . . . . CA-6.6 WED (p114)
Klein, Lukáš . . . . . . . . . . ∙CH-P.12 WED (p136)
Klein, Maciej . . . . . . . . . . . CK-10.4 THU (p160)
Klein, Sarah . . . . . . . . . . . . . CA-6.6 WED (p114)
Kleine, Carlo . . . . . . . . . . . . . . EE-3.3 FRI (p195)
Kleine-Ostmann, Thomas
CK-P.15 TUE (p104), CK-7.5 WED (p134)
Kleis, Sebastian . . . . . . . . . . EB-P.6 THU (p176)
Klenen, Jan . . . . . . . . . . . . . CH-P.5 WED (p136),∙CE-P.12 THU (p172)
Klenke, Arno . . . . . . . . . . . . CJ-2.2 WED (p111),
CJ-2.4 WED (p113), CJ-8.2 FRI (p192)
Klimczak, Mariusz . . . . . . ∙CE-7.4 THU (p169)
Klimmer, Sebastian . . . . . . . . EI-1.3 FRI (p184),∙EI-2.2 FRI (p190)

Authors' Index

Kling, Matthias F. . . . . . . . . CK-1.6 MON (p72),
CF-P.16 TUE (p103)
Klingebiel, Sandro . . . . . . CF-10.6 THU (p149)
Klini, Argyro . . . . . . . . . . . . PP-1.8 MON (p64),
CM-P.4 MON (p77), ∙CM-P.12 MON (p77),
CE-5.6 THU (p155)
Klinner-Teo, Teresa . . . . . JSII-3.3 MON (p69)
Klitis, Charalambos . . . . . . CD-14.4 FRI (p215)
Klufts, Marie . . . . . . . . . . . . . ∙CL-8.1 FRI (p211),
CL-8.3 FRI (p213)
Knefz, Nico . . . . . . . . . . . . CK-11.6 THU (p168)
Kneissl, Michael . . . . . . . . . CB-2.3 MON (p68)
Kneller, Omer . . . . . . . . . ∙EE-P.14 WED (p139),∙CG-5.4 THU (p161)
Knigge, Andrea . . . . . . . . . . CB-P.5 MON (p75),
CB-P.14 MON (p76), CB-4.4 TUE (p91),
CF-6.5 WED (p113), CB-10.4 THU (p160),
CB-11.1 THU (p162),∙CB-11.2 THU (p164),
CB-11.3 THU (p166),
CB-11.4 THU (p166), CB-11.5 THU (p168)
Knight, Jonathan C. . . . . . . CE-2.2 MON (p59),
CD-4.2 TUE (p82)
Knighton, Brittany . . . . . . . CC-1.1 THU (p149)
Knips, Lukas . . . . . . . . . . . . PP-2.9 WED (p121),
EA-P.1 THU (p174), EB-P.1 THU (p176)
Knopp, Gregor . . . . . . . . . . JSI-1.2 WED (p110),∙JSI-1.4 WED (p112), JSI-3.2 WED (p124),
JSI-4.1 WED (p128)
Knorr, Andreas . . . . . . . . . . . . EI-4.4 FRI (p214)
Knorr, Matthias . . . . . . . . CD-7.2 WED (p108),CG-5.1 THU (p157)
Knötig, Hedwig . . . . . . . . . . . CI-5.1 FRI (p180)
knottnerus, ivo . . . . . . . . . . . EA-P.9 THU (p175)
Knurr, Jonas . . . . . . . . . . . . JSI-1.2 WED (p110),
JSI-3.2 WED (p124), JSI-4.1 WED (p128)
Ko, Do-Kyeong . . . . . . . . CH-P.21 WED (p137),
CC-P.14 FRI (p218)
Ko, Dong-Woo . . . . . . . . ∙CK-P.12 TUE (p104),
CE-11.5 FRI (p216)
Kobayashi, Nobuaki . . . . . PD-2.4 THU (p171)
Kobayashi, Toshiki . . . . . EB-11.3 THU (p151),
EB-12.4 THU (p161), ∙EB-P.9 THU (p176)
Kobayashi, Yohei . . . . . . . . . . CC-P.6 FRI (p218)
Kobelke, Jens . . . . . . . . . . . . . CE-1.3 MON (p55)Koch, Elias R. . . . . . . . . . . . . ∙EJ-P.2 MON (p79),∙EJ-P.8 MON (p80)
Koch, Stephan W . . . . . . . . . . . EI-2.4 FRI (p194)
Koch, Thomas . . . . . . . . . CM-P.17 MON (p78)
Koch, Timea . . . . . . . . . . . . . CL-3.6 THU (p163)
Koch, Ueli . . . . . . . . . . . . . . . CI-3.1 WED (p123)
Kochanneck, Leif . . . . . . . ∙JSI-P.6 WED (p141)
Kochanowicz, Marcin . . . . . CE-1.4 MON (p55)
Kočica, Jernej Jan . . . . . . . . . CL-8.6 FRI (p217)
Kodde, Felix . . . . . . . . . . . . CH-P.5 WED (p136),
CE-P.12 THU (p172)
Koenig, Tilman . . . . . . . . . . . ED-3.4 MON (p71)
Koeninger, Anna . . . . . . . . . . CB-4.3 TUE (p91)
Koepfli, Stefan M. . . . . . . . . CI-3.1 WED (p123)
Koester, Jan-Philipp . . . . CB-P.14 MON (p76),∙CB-4.4 TUE (p91), CB-11.4 THU (p166)
Koeth, Johannes . . . . . . . . . CB-8.1 THU (p142),
CI-5.1 FRI (p180)
Koganei, Ayaka . . . . . . . . . . . ∙CJ-9.2 FRI (p204)
Kogure, Satoshi . . . . . . . . . . . CJ-P.10 FRI (p220)
kogure, Soma . . . . . . . . . . . . . . CI-8.3 FRI (p212)

Kohlhaas, Robert B. . . . . . CC-2.2 THU (p161)
Kohutych, Anton . . . . . . . EF-P.23 WED (p141)
Koilpillai, David . . . . . . . . . . . CI-7.3 FRI (p204)
Koilpillai, R. David . . . . . . . . CI-6.1 FRI (p188)
Kokh, Stepan . . . . . . . . . . . . CG-6.5 THU (p169)
Kokkinakis, Emmanouil . PD-2.8 THU (p171)
Kokkinidis, Nikolaos . . . . ∙CE-P.7 THU (p171)
Kolarczik, Mirco . . . . . . . . EB-11.6 THU (p155)
Kolatschek, Sascha . . . . . . EA-4.6 THU (p162),
CK-11.5 THU (p168), EA-P.12 THU (p175)
Kolatzki, Katharina . . . . . . JSI-3.1 WED (p122)
Kolb, Jan Philip . . . . . . . . . . CJ-3.5 WED (p119)
Kolbe, Tim . . . . . . . . . . . . . . CB-2.3 MON (p68),
CK-7.2 WED (p130)
Kolenda, Jonas . . . . . . . . . . . CA-1.5 MON (p56)
Kolesnichenko, Pavel . . ∙EH-P.14 THU (p179)
Kolis, Joseph . . . . . . . . . . . . . . . CJ-1.2 TUE (p95)
Kolodzie, Niklas . . . . . . . . . ∙PP-1.4 MON (p64),∙CB-P.2 MON (p75)
Koltashev, Vasily . . . . . . . . . CA-1.2 MON (p52)
Kolytcheff, Chloé . . . . . . . . . CL-P.15 FRI (p222)
Komagata, Kenichi . . . . . . . CB-8.4 THU (p144)
Komagata, Kenichi N. . . . . ∙ED-6.4 FRI (p194)
Komar, Andrei . . . . . . . . . . . CD-11.5 FRI (p187)
Komis, Ioannis . . . . . . . . . . ∙EF-P.8 WED (p139)
Konecny, Ales . . . . . . . . . . . . CB-P.4 MON (p75)
König, Lorenzo . . . . . . . . . ∙JSII-3.5 MON (p73)
Konotop, Vladimir . . . . . . . . . EF-9.1 FRI (p201)
Konstantaki, Maria . . . . . . CE-5.6 THU (p155),∙CH-16.3 FRI (p215)
Konstantakis, Panagiotis . . ∙EE-2.3 FRI (p187)
Kontenis, Gabrielius . . . . . . ∙CA-4.6 TUE (p88)
Koompai, Natnicha . . . . . . . . CD-5.5 TUE (p91)
Koong, Zhe Xian . . . . . . . . . . . EB-5.5 TUE (p97)
Kopf, Lea . . . . . . . . . . . . . . . . . ∙EE-5.4 FRI (p215)
Kopidakis, George . . . . . . . . . EI-1.2 FRI (p182)
Kopinski-Grünwald, Oliver
CM-1.2 MON (p52)
Kopp, Yasmin . . . . . . . . . . . . . ∙CF-5.4 TUE (p97)
Korakas, Nikolaos . . . . . . . . CE-P.7 THU (p171)
Kordas, Antonis . . . . . . . . . ∙CM-P.2 MON (p77)
Kordts, Arne . . . . . . . . . . . . . CK-1.3 MON (p68),
CD-6.3 TUE (p94)korichi, Oussama . . . . . . . ∙CI-1.4 WED (p113)
Koritsoglou, Olga . . . . . . . CM-10.4 FRI (p206)
Korn, Georg . . . . . . . . . . . . CG-P.13 THU (p174)
Kornienko, Vladimir . . . . ∙EG-2.4 MON (p62),∙EB-P.29 THU (p178)
Korostelin, Yuri . . . . . . . . . . CA-1.2 MON (p52)
Koschny, Thomas . . . . . . . . EH-3.3 THU (p150)
Kosevich, Yury . . . . . . . . . ∙JSVI-1.3 TUE (p87),
JSVI-2.2 TUE (p95)
Koshelev, Kiril . . . . . . . . . CK-11.4 THU (p166)
Kosheleva, Valeriia . . . . . EH-P.10 THU (p179)
Koskinen, Tomi . . . . . . . . . . EG-2.4 MON (p62)
Kotra, Pavan . . . . . . . . . . . . . CE-5.4 THU (p153)
Kouadou, Tiphaine . . . . . . EA-3.2 THU (p150)
Kouichi , Akahane . . . . . . . . . CI-8.2 FRI (p210)
Koulouklidis, Anastasios CM-11.4 FRI (p214)
Kountouris, George . . . . ∙CK-4.5 WED (p114),
EJ-4.6 FRI (p197)
Kourmoulakis, George . . . . ∙EI-P.4 FRI (p224)
Kovacs, Attila P. . . . . . . . . CA-8.5 WED (p120),∙CG-P.9 THU (p174)
Kovács, Katalin . . . . . . . . . . CG-4.5 THU (p153)
Kovalenko, Maksym . . . . . CA-9.3 WED (p130)

Kovalenko, Nazar . . . . . . . ∙CD-2.1 MON (p58),
CD-P.30 TUE (p101)
Kovalev, Anton . . . . . . . . . CB-7.3 WED (p130),
EF-P.24 WED (p141)
Kovalev, Fedor . . . . . . . . . . ∙EH-P.3 THU (p178)
Kovalev, Sergey . . . . . . . . . . CC-P.16 FRI (p218)
Koviarov, Aleksandr . . . . . . . CJ-P.9 FRI (p220),∙CJ-P.23 FRI (p221)
Kovylina, Miroslavna . . . . EG-6.4 WED (p112)
Kowalczyk, Kasia . . . . . . . . JSI-4.6 WED (p134)
Kowalczyk, Katarzyna . . . . CG-1.4 TUE (p87),
EE-4.6 FRI (p209)
Kowalczyk, Katarzyna M. CG-3.1 THU (p143)
Kowalczyk, Maciej . . . . . . . CA-2.3 MON (p60),
PD-1.4 THU (p170)
Kowalewski, Markus . . . . . . . EE-3.2 FRI (p193)
Kowalsky, Wolfgang . . . . . CE-5.4 THU (p153),
CE-P.24 THU (p173)
Koyama, Hiromi . . . . . . . . CB-P.16 MON (p76),
CK-P.17 TUE (p105)
Koyama, Hiromo . . . . . . . . . EC-P.11 FRI (p223)
Koyama, Masatsugu . . . . . CK-7.3 WED (p132)
Koyama, Yuya . . . . . . . . . . . . . . CJ-P.4 FRI (p220)
Kozlovsky, Vladimir . . . . . . CA-1.2 MON (p52)
Kozon, Marek . . . . . . . . . ∙CK-P.25 TUE (p105),∙CK-P.30 TUE (p105),∙CK-11.2 THU (p164)
Kozuno, Tadashi . . . . . . . . . . . CI-P.1 FRI (p219)
Kracht, Dietmar . . . . . . . . . CA-P.15 MON (p74)
Kraft, Fabio Aldo . . . . . ∙CH-P.15 WED (p137)
Krahne, Roman . . . . . . . . . . ∙CE-4.3 TUE (p95),
CE-P.1 THU (p171)
Krajewska, Katarzyna . . . . CG-P.8 THU (p174)
Krakofsky, Jonas . . . . . . . . ∙EH-3.1 THU (p148)
Krämer, Ria G . . . . . . . . . . . ∙CM-9.3 FRI (p192)
Kränkel, Christian . . . . . . . CA-3.5 MON (p72),
CF-P.4 TUE (p102), CK-P.3 TUE (p104),
CA-6.1 WED (p108), CA-11.1 THU (p148),
CA-11.2 THU (p150)
Křápek, Vlastimil . . . . . . . . EG-P.3 TUE (p106)
Kraus, Peter . . . . . . . . . . . . . EE-1.1 WED (p109)
Kraus, Peter M. . . . . . . . . . . . CF-2.3 MON (p61)
Kraus, Stefanie . . . . . . . . . . PD-1.7 THU (p170)
Krause, Benedikt L. . . . . . . ∙CC-5.2 FRI (p192)
Krause, Michael . . . . . . . . . CH-6.2 WED (p116)
Krauskopf, Bernd . . . . . . . . . . EF-8.5 FRI (p197)
Krausz, Ferenc . . . . . . . . . . . CA-2.3 MON (p60),
CD-7.2 WED (p108), CF-6.4 WED (p113),
CF-9.6 WED (p135), CL-2.1 THU (p149),
PD-1.4 THU (p170), CH-13.1 FRI (p181)
Krawczyk, Bartosz . . . . . . . . ∙CD-4.3 TUE (p84)
Kraych, Adrien E. . . . . . . . ∙PD-2.3 THU (p171)
Krebbers, Roderik . . . . ∙CH-P.23 WED (p137),∙CH-16.2 FRI (p213)
Kreidl, Bastian . . . . . . . . . . ∙PP-1.9 MON (p64),∙CM-P.5 MON (p77)
Kremer, Mark . . . . . . . . . . . . . EC-P.3 FRI (p223)
Kretschmar, Martin . . . . . JSI-3.1 WED (p122),
CG-6.4 THU (p169)
Kreutzmann, Sabrina . . . CB-11.3 THU (p166),
CB-11.5 THU (p168)
Kriezis, Emmanouil . . . . CK-P.41 TUE (p106)
Krishnaiah, Kummara Venkata
CH-14.4 FRI (p197)
Kristensen, Philip T. . . . . . EG-P.9 TUE (p107),
CK-4.5 WED (p114)

239

Kristensen, Philip Trøst . . . ∙EJ-4.4 FRI (p195),
EJ-4.6 FRI (p197)
Krizsán, Gergő . . . . . . . . . . CE-P.6 THU (p171),∙CC-P.5 FRI (p218), CC-P.13 FRI (p218)
Kroh, Tobias . . . . . . . . . . . . . . CC-P.5 FRI (p218)
Kroner, Martin . . . . . . . . . . . . . EI-4.1 FRI (p210)
Krstić, Aleksa . . . . . . . . . . . ∙EA-5.6 THU (p168)
Krueger, Michael . . . . . . . . CG-5.4 THU (p161)
Krüger, Jörg . . . . . . . . . . . . . CM-2.1 MON (p58)
Krüger, Michael . . . . . . . . EE-P.14 WED (p139)
Krupa, Katarzyna . . . . . . . . . EF-7.5 FRI (p187),∙CD-13.3 FRI (p205)
Kruse, Björn . . . . . . . . . . . . . JSI-3.1 WED (p122)
Krušič, Š. . . . . . . . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Krutzik, Markus . . . . . . . . . . EB-1.4 MON (p57)
Krylow, Sergej . . . . . . . . . . . CG-3.5 THU (p147)
Krzakala, Florent . . . . . . . . JSIII-3.3 FRI (p185)
Krzempek, Karol . . . . . . . . . ED-2.4 MON (p61),
ED-2.5 MON (p63)Kržič , Andrej . . . . . . . . . . EB-P.10 THU (p176),
EB-P.18 THU (p177), EB-P.19 THU (p177)
Ktena, Niki . . . . . . . . . . . . . . CD-13.1 FRI (p201)
Kubeček, Václav . . . . . . . . . CA-P.1 MON (p74),
CA-P.9 MON (p74), CA-P.10 MON (p74)
Kubullek, Maximilian . . . ∙CF-3.4 MON (p71),
CG-4.3 THU (p151)
Kuchinskii, Vladimir . . . . . CB-9.5 THU (p152)
Kudlinski, Alexandre . . . . . CD-4.3 TUE (p84),
ED-6.6 FRI (p196)
Kudo, Tetsuhiro . . . . . . . . ∙EG-6.3 WED (p110)
Kuehn, Sergei . . . . . . . . . . . . JSI-2.5 WED (p118)
Kues, Michael . . . . . . . . . . . . EJ-2.3 MON (p60),
CD-9.1 WED (p122), EA-P.22 THU (p175),
EB-P.5 THU (p176), EJ-4.3 FRI (p193),
CD-14.1 FRI (p211), CD-14.4 FRI (p215),
EF-10.4 FRI (p215), EE-5.2 FRI (p211)
Kuhlmann, Marion . . . . . . JSI-5.3 THU (p145),
JSI-5.4 THU (p147)
Kühlthau, Tim . . . . . . . . . . . . ∙CI-P.4 FRI (p219),
CI-P.5 FRI (p219)
Kuhn, Stefan . . . . . . . . . . . . . . CJ-1.3 TUE (p97),
CJ-2.4 WED (p113), CJ-6.3 THU (p145),
CJ-8.2 FRI (p192)
Kuhn, Tilmann . . . . . . . . . . . . . EI-2.5 FRI (p196)
Kühnemann, Frank . . . . . EB-8.6 WED (p127),
CL-5.2 FRI (p183)
Kuk, Natalia . . . . . . . . . . . ∙EB-11.5 THU (p153),
EB-P.35 THU (p178)
Kulkarni, Anagha S. . . . . CE-P.21 THU (p172)
Kullock, Rene . . . . . . . . . . . . . CK-2.3 TUE (p86)
Kumar, Ankit . . . . . . . . . . . . EA-5.3 THU (p166)
Kumar, Praveen . . . . . . . . . . . . CI-5.4 FRI (p186)
Kumar, Rupesh . . . . . . . . . EB-P.16 THU (p177)
Kumar, Subith . . . . . . . . . . . . EC-P.12 FRI (p223)
Kumar , Vijay . . . . . . . . . . . . . CI-P.6 FRI (p219)
Kumar, Vivek . . . . . . . . . . . . CH-1.1 MON (p53)
Kumari, Sneha . . . . . . . . . ∙CK-P.14 TUE (p104)
kumazaki, Hajime . . . . . . . . . CI-8.3 FRI (p212)
Kumi-Barimah, Eric . . . ∙CE-P.22 THU (p173)
Kunihashi, Yoji . . . . . . . . . . . CF-2.2 MON (p59)
Kunkel, Philipp . . . . . . . . . . . EA-7.3 FRI (p192)
Kunnus, Kristjan . . . . . . . . . . EE-3.3 FRI (p195)
Kuno, Takuma . . . . . . . . . . . . . CI-6.4 FRI (p194)
Kunz, Jachin . . . . . . . . . . . . ∙EB-8.6 WED (p127)
Kuo, Cang-He . . . . . . . . . . . . CC-P.12 FRI (p218)

Kuo, Shiao-Wei . . . . . . . . . . CE-3.1 MON (p67)
Kupnik, Mario . . . . . . . . . . . PD-1.1 THU (p170)
Kuppadakkath, Athira . . CK-P.24 TUE (p105),∙CK-11.4 THU (p166)
Kurdi, Gabor . . . . . . . . . . . . JSI-P.7 WED (p141)
Kurdiumov, Sergei . . . . . ∙CH-12.1 THU (p163)
Kuriakose, Akhil . . . . . . . . . ∙CM-4.2 TUE (p82)
Kurihara, Taishu . . . . . . . . . . CJ-P.10 FRI (p220)
Kurizki, Gershon . . . . . . . ∙EB-7.1 WED (p115),
EB-7.2 WED (p117)
Kuroda, Takashi . . . . . . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76), CK-P.17 TUE (p105),
EC-P.11 FRI (p223)
Kurosu, Takayuki . . . . . . . . . ∙CI-6.2 FRI (p190)
Kürschner, Dorian . . . . . . CM-P.24 MON (p78)
Kurth, Florens . . . . . . . . . . CE-P.24 THU (p173)
Kurtsiefer, Christian . . . . . EA-P.3 THU (p174),
EB-P.4 THU (p176), EB-P.11 THU (p176)
Kurzyna, Stanisław . . . . . EB-10.6 THU (p149),∙EA-P.21 THU (p175)
Kusaba, Satoshi . . . . . . . . . EE-1.2 WED (p109),
PP-2.13 WED (p121), EI-P.6 FRI (p224)
Kusama, Shota . . . . . . . . . . . CF-12.1 FRI (p211)
Kusch, Justine . . . . . . . . . . . . CD-1.2 MON (p54)
Kuse, Naoya . . . . . . . . . . . . . . CC-P.11 FRI (p218)
Kutkan, Seda . . . . . . . . . . . . . . CE-4.3 TUE (p95)
Kutnyakhov, Dmytro . . . . JSI-3.4 WED (p126)
Kutscher, Tonio . . . . . . . . . ∙CJ-3.4 WED (p119),
CJ-3.5 WED (p119)
Kutscher, Tonio F. . . . . . . CF-P.13 TUE (p103)
Kutscher, Tonio Franz . . . . . CL-8.2 FRI (p211)
Kuttruff, Joel . . . . . . . . . . . . EG-3.5 MON (p70),
EG-4.2 TUE (p84), CE-P.1 THU (p171)
Kuula, Joel . . . . . . . . . . . . . . CH-P.6 WED (p136)
Kuyken, Bart . . . . . . . . . . . . . CD-3.2 MON (p68)Kużmicz, Aleksandr . . . . CB-P.12 MON (p76),
CB-P.21 MON (p76)
Kuzmin, Igor . . . . . . . . . . . CG-P.12 THU (p174)
Kuznetsov, Alexey G. . . . . . CJ-P.20 FRI (p221)
Kuznetsov, Nikolai . . . . . . . EF-2.3 WED (p133)
Kwaśny, Alicja . . . . . . . . . . . CD-P.3 TUE (p100)
Kwon, Suh-young . . . . . . ∙CF-P.20 TUE (p103),
CE-7.3 THU (p167)
Kwon, Taeg Yong . . . . . . . . ∙ED-P.1 MON (p79)
Kyriakakis, Apostolos . . . . CM-3.2 MON (p66)

L
Labadie, Lucas . . . . . . . . . . JSII-3.2 MON (p69),
JSII-3.4 MON (p71)
Labat, Damien . . . . . . . . . . CH-P.1 WED (p136)
Labazuy, Philippe . . . . . . CH-P.22 WED (p137)
Lablanquie, P. . . . . . . . . . . . JSI-4.5 WED (p132)
Lablonde, Laurent . . . . . . CB-10.3 THU (p158)
Labonté, Laurent . . . . . . . . . EB-2.5 MON (p63),
EB-11.4 THU (p153)
Labranche, Phillipe . . . . . . . CE-1.2 MON (p53)
Lacava, Cosimo . . . . . . . . . . CK-P.2 TUE (p104),∙CK-5.2 WED (p116), CK-6.3 WED (p124)
Lachman, Lukáš . . . . . . . . . . EA-P.7 THU (p175)
Laçin, Mesut . . . . . . . . . . . ∙CF-P.10 TUE (p103)
Lackmann, Nick . . . . . . . . . ED-P.5 MON (p79),
CF-8.2 WED (p125), CG-6.5 THU (p169)
Lackner, Lukas . . . . . . . . . . . . . EI-2.6 FRI (p196)
Lacour, Sylvestre . . . . . . . . JSII-1.3 MON (p55),∙JSII-3.1 MON (p67)

Authors' Index

Lacourt, Pierre-Ambroise ∙CM-8.6 FRI (p186)
Lacroûte, Clément . . . . . . . . ED-3.2 MON (p69)
Ladaci, Ayoub . . . . . . . . . . CM-P.32 MON (p79)
Ladika, Dimitra . . . . . . . . . CM-1.1 MON (p52),∙PP-1.8 MON (p64), ∙CM-P.4 MON (p77),
CH-12.4 THU (p167)
Ladouce, Mathieu . . . . . . . PP-1.10 MON (p64),∙CB-P.18 MON (p76), CB-P.22 MON (p76),
EF-P.4 WED (p139)
Ladugin, Maksim . . . . . . . . CB-9.5 THU (p152)
LAFARGUE, Léa . . . . . . . ∙CA-7.3 WED (p126)
Laffont, Guillaume . . . . . CM-P.32 MON (p79),
CH-P.11 WED (p136)
Lafforgue, Christian . . . . . . . CD-6.4 TUE (p96)
Lafiosca, Piero . . . . . . . . . . . . EJ-2.2 MON (p60),
EH-P.20 THU (p179)
Lagendijk, Ad . . . . . . . . . . . CH-1.6 MON (p57),
CK-P.37 TUE (p106), EG-P.7 TUE (p107),
CH-P.29 WED (p137),
CK-11.2 THU (p164)
Lago-Rivera, Dario . . . . . . EB-9.1 WED (p129),
EB-9.4 WED (p133)
Lagoudakis, Pavlos G . . . CM-P.20 MON (p78)
LaGrange, Thomas . . . . . . . . CK-3.4 TUE (p96)Lai, Choon Kong . . . . . . . . . CD-12.5 FRI (p197)
Lai, Jian-Zong . . . . . . . . . ∙CH-P.34 WED (p138)
Lai, Kun-Yu . . . . . . . . . . . . . CH-13.4 FRI (p185)
Laliotis, Athanasios . . . . . . ED-3.5 MON (p73)Lall, Brejesh . . . . . . . . . . . . . . . CI-P.8 FRI (p219)
Lallement, Manon . . . . . . . JSII-1.3 MON (p55)
Lallier, Eric . . . . . . . . . . . . . . CD-1.4 MON (p56),
CJ-2.5 WED (p115), CI-7.5 FRI (p206)
Lamers, Jacob . . . . . . . . . . . ∙JSIII-P.9 FRI (p225)
Lamich, Tomáš . . . . . . . . . . . EA-P.7 THU (p175)
Lammertyn, Jeroen . . . . . . CH-15.3 FRI (p205)
Lamminger, Philipp . . . . CF-P.13 TUE (p103),
CJ-3.4 WED (p119), ∙CJ-3.5 WED (p119),
CL-8.2 FRI (p211)
Lamour, Tobias . . . . . . . . . . CF-7.3 WED (p117)
Lampen, Jacob . . . . . . . . . . . ∙ED-3.3 MON (p69)Lampert, Yazan . . . . . . . . ∙CC-3.4 THU (p167),
CC-5.1 FRI (p188)
Lamperti, Alessio . . . . . . . . . CG-2.2 TUE (p97)Lamperti, Marco . . . . . . . . ∙ED-1.2 MON (p53),
ED-2.6 MON (p63), ∙ED-P.2 MON (p79),∙EB-P.28 THU (p178)
Lance, Romain . . . . . . . . . . JSIII-P.1 FRI (p224),∙JSIII-P.3 FRI (p224)
Lancry, Matthieu . . . . . . . . CM-3.5 MON (p70)
Landais, David . . . . . . . . . . . . . CJ-P.2 FRI (p220)
Landau, Nadav . . . . . . . . . . . . ∙EF-9.4 FRI (p205)
Landsiedel, Justus . . . CM-LIM.5 WED (p119)
Lang, Tino . . . . . . . . . . . . . . ∙CA-P.2 MON (p74),
JSI-P.4 WED (p141), PD-1.1 THU (p170)
Langbehn, Bruno . . . . . . . . JSI-3.1 WED (p122)
Langbein, Wolfgang . . . . . EG-P.4 TUE (p107),
CL-4.1 THU (p163)
Lange, Christoph . . . . . . . . . . EG-4.3 TUE (p86)Lange, Holger . . . . . . . . . . . . CK-1.6 MON (p72)Lange, Simon . . . . . . . . . . . . CC-1.3 THU (p153)
Lange, Simon Jappe . . . . . . . CC-5.5 FRI (p196)
Lanin, A. A. . . . . . . . . . . . . . . . CL-7.1 FRI (p201)
Lanin, Aleksandr . . . . . . . . . . CF-5.5 TUE (p99)
Lanzavecchia, German . . . CE-P.1 THU (p171)
Lanzillotti-Kimura, Norberto Daniel∙JSVI-1.1 TUE (p83)

Laplanche, Lucas . . . . . . . CH-P.16 WED (p137)
Lapointe, Jerome . . . . . . . . . CE-1.2 MON (p53)
Lappas, Alexandros . . . . . . CE-5.6 THU (p155)
Lapre, Coraline . . . . . . . . . ∙CH-1.4 MON (p55),
CD-9.2 WED (p122)
Laptenok, Sergey . . . . . . ∙CH-P.20 WED (p137)
Laptenok, Sergey P. . . . . . CD-P.35 TUE (p102)
Larciprete, Maria CristinaCE-3.5 MON (p71),
JSVI-2.4 TUE (p97), JSVI-2.5 TUE (p99)
Lardschneider, Anna . . . . . . . CI-5.1 FRI (p180)
Larger, Laurent . . . . . . . . . . . CM-8.6 FRI (p186)
Larnimaa, Santeri . . . . . . CH-5.3 WED (p115),∙CH-14.3 FRI (p195)
Laroche, Mathieu . . . . . . . CJ-5.4 WED (p133),
CJ-5.6 WED (p135), ∙CJ-P.18 FRI (p221)
Larochelle, Patrick . . . . . . . CE-1.2 MON (p53)
Larsen, Benjamin L. . . . . ∙EB-P.23 THU (p177)
Larsen, Kirk . . . . . . . . . . . . . JSI-4.6 WED (p134)
Larsson, Anders . . . . . . . . . CK-9.3 THU (p152)
Lartigue, Olivier . . . . . . . CH-P.22 WED (p137)
Lasfargues, Gilles . . . . . . CH-P.22 WED (p137)
Lassonde, Philippe . . . . . . . CD-4.5 TUE (p86)
Latkowski, Sylwester . . . . . . CB-5.2 TUE (p92)
Latour, Gaël . . . . . . . . . . . . . . . CH-4.3 TUE (p96)Lau, Kinran . . . . . . . . . . CM-LIM.1 WED (p115)
Laudert, Benjamin . . . . . . . . EG-5.3 TUE (p94),∙CK-P.36 TUE (p106)
Laudyn, Urszula A. . . . . . CD-P.29 TUE (p101)
Launay, Julien . . . . . . . . . . . JSIII-3.3 FRI (p185)
Laurat, Julien . . . . . . . . . . . . . EB-4.3 TUE (p87),
EB-5.2 TUE (p93), EA-2.3 THU (p144),
EA-7.4 FRI (p196)
Laurell, Fredrik . . . . . . . . . CM-1.6 MON (p56),
CD-2.4 MON (p60)
Lauria, Simone . . . . . . . . . ∙CK-8.5 THU (p146)
Laurindo Jr, Vanderli . . . EB-P.27 THU (p177)
Law, Nicholas . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Le, Truong-Son Dinh . . . . . CM-8.2 FRI (p180)
Le, Van Doan . . . . . . . . . . . . EH-4.5 THU (p160)
Le Blanc, Catherine . . . . CA-11.3 THU (p150)
Le Coq, David . . . . . . . . . . . . CM-6.6 TUE (p98)
Le Corre, Kilian . . . . . . . . . CJ-5.4 WED (p133),
CJ-5.6 WED (p135), CJ-P.18 FRI (p221)
Le Gouët, Julien . . . . . . . . . . . . CJ-P.1 FRI (p220)
Le Gratiet, Luc . . . . . . . . . . . JSVI-1.1 TUE (p83)
Le Jeannic, Hanna . . . . . . . . . EB-4.3 TUE (p87)
Le Kernec, Arnaud . . . . . . . . . CI-7.5 FRI (p206)
Le Mignon, Quentin . . . . . . ED-2.3 MON (p61)
Le Pallec, Jean-Christophe
CH-P.11 WED (p136)
Le Pays Du Teilleul, Paul . CE-1.5 MON (p57)
Le Phu, Thien . . . . . . . . . . . . ∙CM-6.6 TUE (p98)
Leach, Jonathan . . . . . . . . CH-10.2 THU (p151)
Leahu, Grigore . . . . . . . . . . . CE-3.5 MON (p71),
JSVI-2.4 TUE (p97)
Leblanc, Olivier . . . . . . . . CH-10.1 THU (p149)
Lecler, Sylvain . . . . . . . . . . . . CE-1.6 MON (p57)
Lecomte, Steve . . . . . . . . . . . CF-P.4 TUE (p102)
Lecourt, Jean-Bernard . . . ∙CJ-3.6 WED (p121)
Lederer, Maximilian . . . . . . . EE-4.3 FRI (p205)
Ledingham, Patrick . . . . ∙EB-10.4 THU (p145)
Ledingham, Patrick M . . EB-P.27 THU (p177)
Lee, Bong Jae . . . . . . . . . . . . JSVI-2.2 TUE (p95)
Lee, Chao-Kuei . . . . . . . . . . CE-3.1 MON (p67),
CH-P.30 WED (p138)

Lee, Chung-Hyun . . . . . . . ∙EB-7.4 WED (p119)
Lee, Heon . . . . . . . . . . . . . . . EH-2.4 THU (p146)
Lee, In Hak . . . . . . . . . . . . . . CE-7.3 THU (p167)
Lee, Jacob . . . . . . . . . . . . . . . JSI-4.6 WED (p134)
Lee, Jae Hoon . . . . . . . . . . . . ED-P.1 MON (p79)
Lee, Jae-Wung . . . . . . . . . . . . . CB-5.5 TUE (p96)
Lee, Jaewon . . . . . . . . . . . . EB-11.2 THU (p151),
EB-P.24 THU (p177)
Lee, Jinho . . . . . . . . . . . . . . . . . . CJ-7.2 FRI (p182)
Lee, Ju Han . . . . . . . . . . . . . CF-P.20 TUE (p103),
CE-7.3 THU (p167)
Lee, Kevin . . . . . . . . . . . . . . . . CD-5.6 TUE (p91)
Lee, Kyung-Jin . . . . . . . . . . . CF-9.5 WED (p133)
Lee, Kyungtaek . . . . . . . . . CF-P.20 TUE (p103),∙CE-7.3 THU (p167)
Lee, Ming-Chang . . . . . . . ∙CK-P.40 TUE (p106)
Lee, Sang-Bum . . . . . . . . . . . ED-P.1 MON (p79)
Lee, SangLok . . . . . . . . . . . . . ED-P.1 MON (p79)
Lee, Sunghun . . . . . . . . . . . . . . EI-1.5 FRI (p186)
Lee, Timothy . . . . . . . . . CH-P.13 WED (p136),∙CH-P.32 WED (p138),
CH-10.6 THU (p155), CE-5.3 THU (p151)
Lee, Wendy S. L. . . . . . . . . EH-3.6 THU (p154)
Lee, Yong-Tak . . . . . . . . . . . . CE-P.4 THU (p171)
Lee, Younggeun . . . . . . . . . . CM-8.2 FRI (p180)
Leemans, Wim P. . . . . . . . CF-10.1 THU (p143),
PD-1.1 THU (p170)
Lefebvre, Denis . . . . . . . . . . EG-P.5 TUE (p107)
Légaré, François . . . . . . . . . . CD-4.5 TUE (p86)
Legero, Thomas . . . . . . . . . . ED-P.3 MON (p79)
Leggio, Luca . . . . . . . . . . . . CM-P.15 MON (p77)
Legoffic, Olivier . . . . . . . . . . . CJ-P.2 FRI (p220)
Leguay, Lucie . . . . . . . . . . . EB-P.12 THU (p177)
Lehmann, Kevin K. . . . . . . ED-P.4 MON (p79),
ED-4.1 TUE (p83)
Lehotai, Levente . . . . . . . . ∙CF-P.6 TUE (p102),
CG-4.1 THU (p149), CG-P.3 THU (p173)
Lehoux, Pauline . . . . . . . . . . . CA-4.5 TUE (p86)
Lei, Fuchuan . . . . . . . . . . . . . CK-1.4 MON (p68),∙CD-P.1 TUE (p100), CF-P.7 TUE (p102),
EF-3.5 THU (p146)
Lei, Yuhao . . . . . . . . . . . . . . . CM-4.3 TUE (p84),∙CH-7.4 WED (p125), CJ-5.1 WED (p129)
Leich, Martin . . . . . . . . . . . . CE-1.3 MON (p55),
CE-1.4 MON (p55)
Leipe, Markus . . . . . . . . . . . EB-P.20 THU (p177)
Leitenstorfer, Alfred . . . . EG-3.6 MON (p72),
CF-3.1 MON (p67), ED-3.4 MON (p71),
EG-5.4 TUE (p96), PD-1.4 THU (p170),
EE-5.1 FRI (p211)
Lekosiotis, Athanasios . . . ∙CD-5.4 TUE (p91),
EE-4.5 FRI (p207)
Lelit, Marcin . . . . . . . . . . . . CK-P.9 TUE (p104),∙CK-P.23 TUE (p105)
Lemaitre, Aristide . . . . . . . EG-2.1 MON (p58),
JSVI-1.1 TUE (p83), EB-6.1 WED (p109),EB-6.6 WED (p115), EA-8.1 FRI (p200)
Lemang, Mathilde . . . . . . EB-13.2 THU (p165)
Lemberger, Nick . . . . . . . . . CH-13.5 FRI (p187)
Lemcke, Deniz . . . . . . . . . ∙CD-P.17 TUE (p101)
Lemme, Max C. . . . . . . . . . CA-9.3 WED (p130)
Lemme, Max Christian . . . CE-3.6 MON (p73)
Lendl, Bernhard . . . . . . . . CK-P.32 TUE (p106),
CH-P.14 WED (p136)
Leng, Yu-Chen . . . . . . . . . . . . CE-4.3 TUE (p95)
Lengeling, Sebastian . . . . . . . CI-5.5 FRI (p186)

240

Lennon, Joe M . . . . . . . . . . EA-P.20 THU (p175)
Lenski, Mathias . . . . . . . . CF-10.4 THU (p145),
CJ-10.1 FRI (p210), CJ-10.2 FRI (p210),∙CJ-10.3 FRI (p212)
Lenstra, Daan . . . . . . . . . . . . JSIII-P.7 FRI (p224)
Leo, Francois . . . . . . . . . . . . . EJ-P.5 MON (p80),
CF-P.14 TUE (p103), EF-2.2 WED (p131),
EF-2.5 WED (p135), EF-5.5 THU (p160),
EF-5.6 THU (p162), EF-6.4 THU (p166)
Leo, Giuseppe . . . . . . . . . . . EG-2.1 MON (p58),
EH-3.5 THU (p152)
Leo, Jacopo . . . . . . . . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
Leo Tsui, Hei Chit . . . . . . CE-P.11 THU (p172)
León-Torres, Josué R. . . . ∙EB-8.2 WED (p123)
León-Torres, Josué Ricardo
EA-P.19 THU (p175)
Leonardi, Claudio . . . . . . CM-P.18 MON (p78)
Leonhardt, Christina . . . CF-P.13 TUE (p103),
CJ-3.4 WED (p119)
Leonhardt, Miriam . . . . . . . EF-2.2 WED (p131)
Leonov, Stanislav . . . . . . . . . CA-1.2 MON (p52)
Lepers, Maxence . . . . . . . . . . EA-7.5 FRI (p196)
Lepukhov, Evgenii . . . . . . PP-2.3 WED (p120),
CE-P.3 THU (p171)
Lerner, Alexandre . . . . . ∙CM-P.32 MON (p79),
CH-P.11 WED (p136)
Leshin, Jason . . . . . . . . . . . . . . EC-1.5 FRI (p187)
Lesina, Antonio Calà . . . . . . . EJ-4.3 FRI (p193)
Leskowschek, Michael . . CF-8.3 WED (p125)
Lesniak, Magdalena . . . . . . CE-1.4 MON (p55)Leszczyński, Adam . . . . . . EB-10.2 THU (p143)
Letartre, Xavier . . . . . . . . . . CK-15.4 FRI (p214)
Letsou, Theodore . . . . . . . . . CD-6.5 TUE (p96)
Lettau, Thomas . . . . . . . . . . . . EI-1.3 FRI (p184)
Lettner, Thomas . . . . . . . . . . CK-1.2 MON (p66)
Leuchs, Gerd . . . . . . . . . . . ∙EB-2.1 MON (p59),
EB-6.4 WED (p113), EA-6.1 FRI (p180)
Leuthold, Juerg . . . . . . . . . ∙CI-3.1 WED (p123),
EH-4.1 THU (p156)
Leuthold, Jürg . . . . . . . . . . . CD-1.2 MON (p54)
Levchenko , Andrey . . . . . . CJ-5.3 WED (p131)
Levenson, Ariel . . . . . . . . . . . EA-7.4 FRI (p196)
Levenson, Juan Ariel . . . . . . . EF-8.1 FRI (p189)
Lévêque, Samuel . . . . . . . . . JSII-2.3 MON (p61)
Leveque, Simon . . . . . . . . . . . . CI-7.5 FRI (p206)
Lever, Fabiano . . . . . . . . . . . JSI-5.3 THU (p145),
JSI-5.4 THU (p147)
Leviandier, Luc . . . . . . . . . . CD-1.4 MON (p56),
CJ-2.5 WED (p115)
Levitov, Leonid S. . . . . . . . . . . EI-4.5 FRI (p216)
Levy, Yoann . . . . . . . . . . . . . . CM-5.4 TUE (p91),
CM-9.6 FRI (p196)
Lewenstein, Maciej . . . . . . ∙EB-3.3 MON (p69),
CD-7.1 WED (p108)
Lewis, Steffan . . . . . . . . . . . . JSII-2.3 MON (p61)
Leyendecker, Marius . . . . CA-6.6 WED (p114)
Leykam, Daniel . . . . . . . . . . EC-P.14 FRI (p223)
Leyzner, Maxim . . . . . . . . . CB-P.10 MON (p76)
L’Huillier, Anne . . . . . . . . . . . CF-5.2 TUE (p95),
CF-P.18 TUE (p103), CG-4.6 THU (p155),
CG-5.2 THU (p159), PD-1.3 THU (p170)
Lhuillier, Jérémy . . . . . . . . CK-5.6 WED (p120)
Li, Chen . . . . . . . . . . . . . . . . . JSI-P.4 WED (p141)
Li, Dechun . . . . . . . . . . . . . . . CA-3.2 MON (p68)
Li, Feng . . . . . . . . . . . . . . . . CD-P.27 TUE (p101),

CF-P.1 TUE (p102), CJ-3.2 WED (p117)
Li, Gaoyuan . . . . . . . . . . . ∙JSII-2.2 MON (p61),
CE-9.6 FRI (p196)
Li, Jianfeng . . . . . . . . . . . . . . . CL-1.2 MON (p69)
Li, Jianxiong . . . . . . . . . . . . . JSI-2.5 WED (p118)
Li, Jiaqi . . . . . . . . . . . . . . . . . ∙CJ-4.4 WED (p125)
Li, Jinxiang . . . . . . . . . . . . . . . EG-2.2 MON (p58)
Li, Kaiwei . . . . . . . . . . . . . . . . CL-1.4 MON (p71)
Li, Kang . . . . . . . . . . . . . . . CH-P.33 WED (p138)
Li, Ming . . . . . . . . . . . . . . . . EA-P.24 THU (p176)
Li, Ning . . . . . . . . . . . . . . . JSIV-1.4 WED (p118),
CM-8.4 FRI (p184), ∙JSIII-P.12 FRI (p225)
Li, Peng . . . . . . . . . . . . . . . . . . ED-3.3 MON (p69)
Li, Qian . . . . . . . . . . . . . . . . CA-10.1 THU (p142)
Li, Qingfeng . . . . . . . . . . . . . CM-2.3 MON (p60)
Li, Qiuyang . . . . . . . . . . . . . . . . EI-4.4 FRI (p214)
Li, Shaoxian . . . . . . . . . . . . . CC-1.5 THU (p155)
LI, Taige . . . . . . . . . . . . . . . . ∙CH-14.4 FRI (p197)
Li, Tiantong . . . . . . . . . . . . ∙CK-1.5 MON (p70),
CK-P.18 TUE (p105)
Li, Wei . . . . . . . . . . . . . . . . . . ∙CH-2.3 MON (p60)
Li, Weiwei . . . . . . . . . . . . . . . . CK-1.6 MON (p72)
Li, Xiaoshen . . . . . . . . . . . . . JSI-P.5 WED (p141)
Li, Yewen . . . . . . . . . . . . . . . . PP-1.7 MON (p64),
CH-P.8 WED (p136)
Li, Yu . . . . . . . . . . . . . . . . . . ∙CK-P.22 TUE (p105)
Li, Yu-Wei . . . . . . . . . . . . . . . CL-P.19 FRI (p222)
Li, Yujia . . . . . . . . . . . . . . . . . ∙CF-P.1 TUE (p102),
CJ-3.2 WED (p117)
Li, Yujian . . . . . . . . . . . . . . . . . . CL-P.7 FRI (p222)
Li, Zhengze . . . . . . . . . . . . . . EA-2.3 THU (p144)
Li, Zhuo . . . . . . . . . . . . . . . . . EG-P.8 TUE (p107)
Li, Zihan . . . . . . . . . . . . . . . . PP-2.2 WED (p120),
CE-P.2 THU (p171), ∙CE-8.1 FRI (p180)
Li, Zongda . . . . . . . . . . . . . ∙CD-9.3 WED (p124),
EF-3.4 THU (p144)
Li Voti, Roberto . . . . . . . . . . CE-3.5 MON (p71),∙JSVI-2.4 TUE (p97), JSVI-2.5 TUE (p99)
Liang, Dong . . . . . . . . . . . . . . CI-P.11 FRI (p219)
Liang, Meizhen . . . . . . . . . ∙CA-6.5 WED (p112)
Liang, Shih Lun . . . . . . . . . . EG-1.1 MON (p52)
Liang, Sijing . . . . . . . . . . . . . . CD-6.6 TUE (p98)
Liang, Yu-Cheng . . . . . . ∙CH-P.30 WED (p138)
Liao, Wenjun . . . . . . . . . . . . . CL-P.3 FRI (p221),
CL-P.4 FRI (p221)
Liapis, Andreas . . . . . . . . . CA-9.6 WED (p134)
Liapis, Andreas C. . . . . . . . . . . EI-P.1 FRI (p223)
Liberal, Iñigo . . . . . . . . . . . . EH-5.3 THU (p166)
Liberale, Carlo . . . . . . . . . ∙CM-1.5 MON (p56),
CD-P.35 TUE (p102), CH-P.1 WED (p136),
CH-P.20 WED (p137)
Lidzey, David G. . . . . . . . . CH-8.4 WED (p133),
EI-4.2 FRI (p212)
Liebermeister, Lars . . . . . . CC-2.2 THU (p161)
Liebich, Marlene . . . . . . . . CG-5.1 THU (p157)
Lienau, Christoph . . . . . . . . . . EI-2.6 FRI (p196)
Liero, Armin . . . . . . . . . . . CB-11.2 THU (p164)
Ligato, Nadia . . . . . . . . . . . . CI-3.4 WED (p127)
Ligeti, Gábor . . . . . . . . . . . . EE-P.7 WED (p138)
Lihachev, Grigory . . . . . . . . . CB-5.4 TUE (p96),
CB-10.1 THU (p156), CK-14.1 FRI (p200)
Likam Wa, Patrick . . . . . . . . EC-1.5 FRI (p187)
Likhachev, Grigorii . . . . . . CK-14.5 FRI (p206)
Likhachev, Mikhail . . . . . . ∙CJ-5.3 WED (p131)
Likhachev, Mikhail E. . . . CJ-3.1 WED (p115)
Lim, Charles C.-W. . . . . . . . . EB-5.1 TUE (p93)

Authors' Index

Lim, Dohoon . . . . . . . . . . . ∙EB-P.26 THU (p177)
Lim, Geunweon . . . . . . . . . . CE-7.3 THU (p167)
Lim, Min G. . . . . . . . . . . . . . CK-7.4 WED (p132)
Lim, Soon Wei D. . . . . . . . CK-11.6 THU (p168)
Lima Moura, André . . . . . . CJ-P.16 FRI (p220)
Limbacher, Benedikt . . . . . CC-4.2 FRI (p180),
CC-7.2 FRI (p210)
Liméry, Anasthase . . . . . . . . ∙CJ-P.1 FRI (p220)
Limpert, Jens . . . . . . . . . . . CF-P.21 TUE (p103),∙CJ-2.1 WED (p109), CJ-2.2 WED (p111),
CJ-2.4 WED (p113), CH-6.2 WED (p116),
CJ-4.1 WED (p123), CH-P.10 WED (p136),
CF-10.4 THU (p145), CJ-8.2 FRI (p192),
EE-4.2 FRI (p203), CJ-10.1 FRI (p210),
CJ-10.2 FRI (p210), CJ-10.3 FRI (p212),
CL-8.5 FRI (p215)
Lin, Gong-Ru . . . . . . . . . . . . . CE-3.1 MON (p67)
Lin, Guoping . . . . . . . . . . . ∙CD-12.2 FRI (p191)
Lin, Haifeng . . . . . . . . . . . . CA-10.6 THU (p148)
Lin, Miao-Ling . . . . . . . . . . . . CE-4.3 TUE (p95)
Lin, Ming-Fu . . . . . . . . . . . . JSI-4.6 WED (p134)
Lin, Yan-Jou . . . . . . . . . . . . . CC-P.12 FRI (p218)
Lin, Yu-Chieh . . . . . . . . . . . . ∙CF-4.3 TUE (p85)
Lin, Zhang-Lang . . . . . . . CA-10.3 THU (p144),
CA-10.6 THU (p148)
Lindemann, Markus . . . . . . CB-2.4 MON (p70)
Linden, Stefan . . . . . . . . . . . CK-15.5 FRI (p214)
Lindenblatt, Hannes . . . . . JSI-5.2 THU (p145)
Lindinger, Florian . . . . . . . CL-2.1 THU (p149),
CL-5.3 FRI (p185)
Lindner, Chiara . . . . . . . . . EB-8.6 WED (p127),
CL-5.2 FRI (p183)
Lindner, Florian . . . . . . . . . CJ-5.1 WED (p129)
Lindner, Lukas . . . . . . . . . . . ∙CA-5.3 TUE (p96)
Lindvall, Thomas . . . . . . . . . ED-P.3 MON (p79)
Lingos, Panos . . . . . . . . . . . . . CM-9.1 FRI (p188)
Linke, Norbert M. . . . . . . . . ∙EB-4.4 TUE (p87)
Linovskiy, G. P. . . . . . . . . . . . . CL-7.1 FRI (p201)
Lipatov, Denis . . . . . . . . . . . CJ-5.3 WED (p131)
Lipnickas, Mykolas . . . . . . CA-P.14 MON (p74)
Lipsanen, Harri . . . . . . . . . . . EG-4.4 TUE (p86)
Lisauskas, Alvydas . . . . . . . . CC-6.1 FRI (p200)
Liscidini, Marco . . . . . . . . . EB-6.1 WED (p109)
Little, B. . . . . . . . . . . . . . . . . EF-P.15 WED (p140)
Little, Brent . . . . . . . . . . . . . . ED-6.3 FRI (p192),
EE-5.3 FRI (p213)
Little, Douglas J. . . . . . . . . CM-P.10 MON (p77)
Littmann, Jan-H. . . . . . . . EB-11.2 THU (p151),∙EB-P.24 THU (p177)
Litzel, Julian . . . . . . . . . . . . . PD-1.7 THU (p170)
Liu, Ai . . . . . . . . . . . . . . . . . . . . ED-5.5 FRI (p186)
Liu, Chang . . . . . . . . . . . . ∙CH-6.2 WED (p116),
CH-P.10 WED (p136), CL-6.2 FRI (p191)
Liu, Chunxin . . . . . . . . . . . . . CE-11.1 FRI (p210)
Liu, Fang . . . . . . . . . . . . . . . . . . ∙EI-1.1 FRI (p180)
Liu, Hui-Yun . . . . . . . . . . . . . CB-4.5 TUE (p91)
Liu, Jie . . . . . . . . . . . . . . . . PP-2.12 WED (p121),
EH-P.16 THU (p179)
Liu, Junqiu . . . . . . . . . . . . . CK-4.2 WED (p110),
EG-6.2 WED (p108), CK-14.5 FRI (p206)
Liu, Junwei . . . . . . . . . . . . . . . EG-P.8 TUE (p107)
Liu, Mingkai . . . . . . . . . . . . . CD-11.5 FRI (p187)
Liu, Ningwu . . . . . . . . . . . CH-P.23 WED (p137)
Liu, Peng . . . . . . . . . . . . . . . . . CL-1.4 MON (p71)
Liu, Qi . . . . . . . . . . . . . . . . . . . JSI-P.5 WED (p141)
Liu, Qiang . . . . . . . . . . . . . . . JSIII-P.4 FRI (p224)

Liu, Shande . . . . . . . . . . . . . CA-10.6 THU (p148)
Liu, Tongjun . . . . . . . . . . . . ∙EG-2.2 MON (p58),
CH-6.5 WED (p118), EH-1.2 WED (p130)
Liu, Wei . . . . . . . . . . . . . . . . . JSI-P.5 WED (p141)
Liu, Weiwen . . . . . . . . . . . . CE-P.21 THU (p172)
Liu, Weiyong . . . . . . . . . . . EF-P.22 WED (p140)
Liu, Xiaolong . . . . . . . . . . . . CM-3.1 MON (p66)
Liu, Xiaomeng . . . . . . . . . . CH-6.1 WED (p114)
Liu, Xinyang . . . . . . . . . . . . . . ∙CJ-8.4 FRI (p196)
Liu, Xueming . . . . . . . . . . . CE-P.14 THU (p172)
Liu, Yang . . . . . . . . . . . . . . ∙CK-4.2 WED (p110),
CK-9.2 THU (p150), CD-12.5 FRI (p197),∙CK-14.1 FRI (p200)
Liu, Yangyang . . . . . . . . . . . . CF-3.2 MON (p67)
Liu, Yicheng . . . . . . . . . . . . CA-10.6 THU (p148)
Liu, Yizhou . . . . . . . . . . . . . . . CJ-P.19 FRI (p221)
Liu, Yuzhou G. N. . . . . . . . . . EC-1.5 FRI (p187)
Liu, Zhenghao . . . . . . . . . . EB-P.30 THU (p178)
Llauze, Thomas . . . . . . . . . . . ∙CI-7.4 FRI (p204)
Llopis, Olivier . . . . . . . . . . . EF-3.3 THU (p144),
PD-2.2 THU (p170)
Lo, Guo-Qiang . . . . . . . . . . . CL-1.2 MON (p69)
Loas, Goulc’hen . . . . . . . . . . CA-4.2 TUE (p82),
CA-4.5 TUE (p86)
Lobo-Ploch, Neysha . . . . . CB-2.3 MON (p68)
Lochocki, Benjamin . . . . . CH-P.3 WED (p136)
Locquet, Alexandre . . . . . . CC-P.10 FRI (p218)
Lodi, Dario W. . . . . . . . . . . . CG-3.2 THU (p143)
Loetgering, Lars . . . . . . . . CH-6.2 WED (p116)
Löffler, Wolfgang . . . . . . . EA-P.11 THU (p175),
EA-P.13 THU (p175), EB-P.25 THU (p177)
Lognathan, Sarath K . . . . . CL-3.5 THU (p161)
Lohse, Olga . . . . . . . . . . . . . CK-5.1 WED (p114),
CK-8.6 THU (p148)
Loiko, Pavel . . . . . . . . . . . . . ∙CA-2.4 MON (p62),
CA-3.2 MON (p68), CA-3.3 MON (p68),
CA-P.18 MON (p75), CA-4.5 TUE (p86),
CA-6.4 WED (p112), ∙CA-9.4 WED (p132),
CA-10.3 THU (p144),
CA-10.6 THU (p148), CJ-6.2 THU (p143),
CA-11.2 THU (p150), CE-8.5 FRI (p186)
Loiseau, Pascal . . . . . . . . . . . . CE-4.4 TUE (p97)
Lokar, Žiga . . . . . . . . . . . . . . . . CL-8.6 FRI (p217)
Lombard, Laurent . . . . . . . CJ-2.3 WED (p113),∙CJ-6.4 THU (p145), CJ-P.1 FRI (p220)
Lombardi, Pietro . . . . . . . . . EA-4.1 THU (p156)
Lombosi, Csaba . . . . . . . . . . CC-1.5 THU (p155)
Loncar, Marko . . . . . . . . . . ∙CD-3.1 MON (p66),
CD-3.3 MON (p68), CC-5.1 FRI (p188)
Long, David . . . . . . . . . . . . ∙CH-5.2 WED (p113)
Long, Jiaxuan . . . . . . . . . . . . . CJ-P.11 FRI (p220)
Long, Sophia . . . . . . . . . . . . . CI-8.5 FRI (p214),∙CI-P.2 FRI (p219), CL-P.12 FRI (p222)
Longa, Adrien . . . . . . . . . . . . ∙CD-4.5 TUE (p86)Longobucco, Mattia . . . . EF-P.19 WED (p140)
Lopez, John . . . . . . . . . . . . . CM-2.4 MON (p60),
CM-3.6 MON (p72)
Lopez, Lisa . . . . . . . . . . . . . . . CE-4.1 TUE (p93),
CE-4.4 TUE (p97), ∙CE-4.4 TUE (p97),
CE-P.29 THU (p173), CI-8.5 FRI (p214)
Lopez, Thomas . . . . . . . . . . . CK-P.5 TUE (p104)
Lopez-Aviles, Helena E. . . . EC-1.5 FRI (p187)
Lopez-Galmiche, Gisela . . . EC-1.5 FRI (p187)
Lopez Garcia, Inaki . . . . . CH-14.2 FRI (p193)
López-Querol, Pablo . . . ∙CB-P.15 MON (p76),
CB-7.4 WED (p132)

López-Ripa, Miguel . . . . . . . ∙CF-4.4 TUE (p87)
Lopez-Torres, Diego . . . . . CE-5.6 THU (p155)
Lopushenko, Ivan . . . . . . . CL-4.3 THU (p167),∙EJ-4.2 FRI (p191)
Lorbeer, Raoul-Amadeus∙CA-P.12 MON (p74)
Lord, Marie-Pier . . . . . . . . ∙CJ-6.5 THU (p147)
Lorenz, Adrian . . . . . . . . . . . CE-1.3 MON (p55)
Lorenz, Dominik . . . . . . . . . CJ-10.5 FRI (p214)
Lorenz, Martin . . . . . . . . . . . CE-1.4 MON (p55)
Lorenz, Virginia O. . . . . . . . . EA-1.1 TUE (p83)
Lorenzen, Jan . . . . . . . . . . . . CK-P.8 TUE (p104),
CK-4.4 WED (p112), CA-9.6 WED (p134),
PD-1.6 THU (p170)
Los, Johannes W. N. . . . . . . EB-P.7 THU (p176)
Losev, Sergey . . . . . . . . . . . . CB-9.5 THU (p152)
Lott, James . . . . . . . . . . . . JSIII-2.4 THU (p166),
JSIII-6.1 FRI (p211)
Lotz, Simon . . . . . . . . . . . . . CJ-3.5 WED (p119),
CL-8.1 FRI (p211), CL-8.3 FRI (p213),∙CL-8.4 FRI (p215)
Louca, Charalambos . . . . . . . EI-4.2 FRI (p212)
Louchet-Chauvet, Anne . CL-2.3 THU (p151),
CI-7.4 FRI (p204), ∙EA-9.2 FRI (p210)
Loukakos, Panagiotis . . . . PP-1.8 MON (p64),
CM-P.4 MON (p77)
Lourenço, João . . . . . . . . . JSIII-P.16 FRI (p225)
Lourenco-Martins, Hugo EG-6.2 WED (p108)
Lousteau, Joris . . . . . . . . . . CA-P.20 MON (p75),
CJ-6.2 THU (p143)
Lovász, Béla . . . . . . . . . . . . ∙EE-1.6 WED (p115)
Loveridge, Tegan . . . . . . . . . . EA-1.1 TUE (p83)
Low, Irene . . . . . . . . . . . . . . . PP-2.8 WED (p121),
CL-5.5 FRI (p187), CL-P.2 FRI (p221)
Lowinski, Jan . . . . . . . . . . . . EA-2.1 THU (p142)
Lozano, Magali . . . . . . . . . . CD-P.7 TUE (p100),
CD-8.1 WED (p114)
Lozano-Mendez, Karen . . ∙EB-2.4 MON (p63),
EB-P.10 THU (p176)
Lu, Chao . . . . . . . . . . . . . . . . CD-P.27 TUE (p101)
Lu, Guan-Ting . . . . . . . . . . . . ∙CI-8.4 FRI (p214)
Lu, Jiafeng . . . . . . . . . . . . . . . CM-3.5 MON (p70)
Lu, Jinsheng . . . . . . . . . . . . . EH-5.2 THU (p164)
Lu, Liangjun . . . . . . . . . . . . CK-5.5 WED (p118)
Lu, Mei-Ju . . . . . . . . . . . . . . CK-P.40 TUE (p106)
Lu, Yuerui . . . . . . . . . . . . . . . . . EG-5.3 TUE (p94)
Lu, Zhiwei . . . . . . . . . . . . . . . . CA-5.2 TUE (p94),
CA-5.5 TUE (p98)
Luan, Yigong . . . . . . . . . . . . PD-2.8 THU (p171)
Lubianskii, Iaroslav . . . . . . . CC-4.6 FRI (p186)
Lucas, D. M. . . . . . . . . . . . . . . ∙ED-5.1 FRI (p180)
Lucas, Erwan . . . . . . . . . . . . PD-2.7 THU (p171)
Lucchini, Matteo . . . . . . . . . CF-1.3 MON (p57),
CF-2.4 MON (p61), CF-3.3 MON (p69),
CG-2.2 TUE (p97), PP-2.4 WED (p120),
CF-9.4 WED (p133), ∙CG-5.3 THU (p159),
CG-P.1 THU (p173), CG-P.5 THU (p173),
EE-3.1 FRI (p189), EE-3.4 FRI (p197)
Lüdge, Kathy . . . . . . . . . . ∙JSIII-2.3 THU (p166)
Ludlow, Daisy J.H. . . . . . ∙CC-1.4 THU (p153),
CC-3.2 THU (p165), ∙CC-7.5 FRI (p214)
Ludwig, Arne . . . . . . . . . . . . EA-5.1 THU (p162)
Ludwig, Markus . . . . . . . . ∙JSII-2.4 MON (p63),
EG-3.6 MON (p72), CD-5.2 TUE (p90),
CK-4.4 WED (p112), CK-9.5 THU (p154),
EF-9.3 FRI (p205)

241

Lugiato, Luigi . . . . . . . . . . . . . CD-6.5 TUE (p96)
Lugnan, Alessio . . . . . . . . . ∙JSIII-3.5 FRI (p187)
Lühder, Tilman . . . . . . . . . . . . CJ-1.4 TUE (p97)
Luis, Ruben . . . . . . . . . . . . . ∙CI-4.1 WED (p129)
Lukashchuk, Anton . . . . . CK-4.2 WED (p110)
Łukasik, Sara . . . . . . . . . . . . CE-7.4 THU (p169)
Lukeš, Jakub . . . . . . . . . . . ∙CD-P.28 TUE (p101)
Lukin, Daniil . . . . . . . . . . ∙EB-11.1 THU (p149)
Lukin, Daniil M. . . . . . . . . . . CD-5.1 TUE (p90),
EA-2.4 THU (p144)
Lukonin, Vasily . . . . . . . . . . . . CJ-1.1 TUE (p93)
Lukosiunas, Ignas . . . . . . . . ∙CK-3.6 TUE (p98)
Lumeau, Julien . . . . . . . . . . EF-3.3 THU (p144),
PD-2.2 THU (p170)
Luna, Esperanza . . . . . . . . EB-P.12 THU (p177)
Lundeen, Jeff S. . . . . . . . . CH-P.27 WED (p137)
Luntadila Lufungula, Isaac
CD-3.2 MON (p68)
Lunzer, Markus . . . . . . . . . CM-P.17 MON (p78)Luo, Chih-Wei . . . . . . . . . . . CF-12.1 FRI (p211)
Luo, Ching-Lung . . . . . . . CH-13.4 FRI (p185),
CL-P.19 FRI (p222)
Luo, Jiaqi . . . . . . . . . . . . . . . . JSI-P.5 WED (p141)
Luo, Kai-Hong . . . . . . . . . . ∙EB-6.3 WED (p111)
Luo, Tingpeng . . . . . . . . . . . . CA-5.3 TUE (p96)
Luo, Xianshu . . . . . . . . . . . . . CL-1.2 MON (p69)
Lüpken, Niklas M. . . . . . CD-10.1 WED (p128),∙EA-4.3 THU (p158)
Lupo, Alessandro . . . . . ∙JSIII-1.3 THU (p158),∙JSIII-P.17 FRI (p225)
Luque Merino, Rafael . . . . . ∙EI-3.3 FRI (p204),
EI-4.5 FRI (p216)
Lustig, Eran . . . . . . . . . . . . . . . EC-2.1 FRI (p189)
Lutetskiy, Andrey . . . . . . . . CB-9.5 THU (p152)
Lutz, Matthew J. . . . . . . . . . CC-3.2 THU (p165)
Lvovsky, A. I. . . . . . . . . . . . CH-12.3 THU (p167)
Lyasota, Alexey . . . . . . . . . ∙CE-10.2 FRI (p204)
Lydick, Nathan . . . . . . . . . . . . CB-3.1 TUE (p82)Łyszczek, Renata . . . . . . . . . CE-10.5 FRI (p208)
Lyu, Weimin . . . . . . . . . . . . . . ∙CL-P.7 FRI (p222)
Lyu, Zhouping . . . . . . . . ∙CH-12.2 THU (p165)

M
M. Dorney, Kevin . . . . CM-LIM.3 WED (p117)
M. Harvey, Clarissa . . . . . . CM-1.6 MON (p56)
Ma, Hongfeng . . . . . . . . . . . EH-4.5 THU (p160)
Ma, Jinyong . . . . . . . . . . . . ∙CD-3.4 MON (p70),∙EG-5.2 TUE (p92), CK-10.2 THU (p158)
Ma, Ping . . . . . . . . . . . . . . . . . CI-3.1 WED (p123)
Ma, Tammy . . . . . . . . . . . . . . . . PL-3.1 TUE (p90)
Ma, Yue . . . . . . . . . . . . . . . . . . EB-2.2 MON (p61),
CD-13.6 FRI (p209)
Maansson, Erik . . . . . . . . . CG-3.2 THU (p143)
Maaßdorf, Andre . . . . . . . . . CB-4.4 TUE (p91),
CF-6.5 WED (p113), CB-10.4 THU (p160),
CB-11.2 THU (p164),
CB-11.3 THU (p166), CB-11.5 THU (p168)
Maaßdorf, Andreas . . . . . . . CB-P.5 MON (p75)
Mabed, Mehdi . . . . . . . . . . ∙EF-10.2 FRI (p211),
EF-10.3 FRI (p213)
Macaluso, Roberto . . . . . . . JSVI-2.5 TUE (p99)
Maccaferri, Nicolò . . . . . . . ∙EG-4.2 TUE (p84),∙EH-2.1 THU (p142), ∙EH-2.4 THU (p146),∙CE-P.1 THU (p171)
Maccarone, Tom . . . . . . . . JSII-1.2 MON (p55),

PP-1.12 MON (p65), JSII-P.2 MON (p80)
MacDonald, Kevin . . . . . . . EG-2.2 MON (p58),
PP-1.6 MON (p64), CH-6.5 WED (p118),∙EH-1.2 WED (p130), CH-P.4 WED (p136),
CH-12.1 THU (p163)
MacDonald, Kevin F. . . . . . ED-5.3 FRI (p184),
EC-3.5 FRI (p207)
Mach, Lam . . . . . . . . . . . . . . . CF-P.5 TUE (p102),
CH-7.6 WED (p127)
Machnikowski, Paweł . . . . . . EI-2.5 FRI (p196)
Machorro-Ortiz, Aleida JSIV-1.5 WED (p120)
Machu, Yohann . . . . . . . . . . . . EB-4.5 TUE (p89)
Mackenzie, Jacob. I. . . . . . CA-9.2 WED (p130)
Mackonis, Paulius . . . . . . . ∙CA-P.5 MON (p74),
CD-P.14 TUE (p100)
Mackosz, Krzysztof . . . . . . EH-5.6 THU (p168)
Maćkowski, Sebastian . . . CE-P.26 THU (p173)
MacLachlan, David G. . . . JSII-3.4 MON (p71)
Maclot, Sylvain . . . . . . . . . JSI-4.3 WED (p130),
CG-4.6 THU (p155)
Macnaughtan, Matthew . . EF-3.6 THU (p148)
Maconi, Göran . . . . . . . . . CH-12.4 THU (p167)
Maczewsky, Lukas . . . . . . . . EC-1.3 FRI (p185),
EC-2.1 FRI (p189), EC-P.3 FRI (p223)
Maczewsky, Lukas J. . . . . . . EC-P.2 FRI (p223)
Madaras, Scott . . . . . . . . . . . . CB-5.6 TUE (p98)
Madden, Stephen J. . . . . . . CD-12.5 FRI (p197)
Madeikis, Karolis . . . . . . . . CA-P.14 MON (p74)
Madeleine, Tristan . . . . . . ∙EH-P.7 THU (p178)
Madhav, Kalaga . . . . . . . . . JSII-3.4 MON (p71),
JSII-P.1 MON (p80)
Madrid-Wolff, Jorge . . . . ∙CM-1.3 MON (p54)Mady, Franck . . . . . . . . . . CH-11.5 THU (p161)
Maeda, Tomohiro . . . . . . ∙CH-7.1 WED (p123)
Maeder, Andreas . . . . . . . . JSII-2.2 MON (p61),∙CK-1.1 MON (p66), CE-9.5 FRI (p196),
JSIII-4.3 FRI (p195)
Magalhães, Tiago . . . . . . . . . CL-7.4 FRI (p205)
Magat, Germain . . . . . . . . CH-P.22 WED (p137)
Magno, Giovanni . . . . . . . . CK-P.5 TUE (p104),
CK-P.6 TUE (p104), ∙EH-P.18 THU (p179)
Magro, Valentin . . . . . . . . . . . EA-8.2 FRI (p202)
Magunia, Alexander . . . . . JSI-5.2 THU (p145)
Mahapatra, Saroj K. . . . . . . . CI-P.3 FRI (p219)
Mahapatra, Sukanya . . . . . . . EA-7.4 FRI (p196)
Mahdy, Ahmed F. M. EL . . CE-3.1 MON (p67)
Mahieu, Benoit . . . . . . . . . . CD-P.7 TUE (p100),
CD-8.1 WED (p114), EF-P.7 WED (p139)
Mahiou, Rachid . . . . . . . . . . . CE-4.4 TUE (p97)
Mahmudlu, Hatam . . . . . ∙CD-14.1 FRI (p211),
CD-14.4 FRI (p215)
Mahnke, Christoph . . . . . . JSI-P.4 WED (p141)
Maho, Anaëlle . . . . . . . . . . . . . CI-7.5 FRI (p206)
Mai, Lorenzo . . . . . . . . . . . . . CF-1.3 MON (p57),
CF-9.4 WED (p133)
Mai, Sebastian . . . . . . . . . . . EG-P.2 TUE (p106),
CF-9.2 WED (p131)
Maibohm, Christian . . . ∙CD-P.18 TUE (p101),
CL-7.4 FRI (p205), JSIII-P.2 FRI (p224)
Maidment, Luke . . . . . . . . . CD-P.5 TUE (p100)
Maier, Andreas R. . . . . . . . CF-10.6 THU (p149)
Maier, Stefan . . . . . . . . . . . . . EG-1.2 MON (p54)
Maier, Stefan A. . . . . . . . . EH-1.3 WED (p132),
CH-8.4 WED (p133), CH-P.7 WED (p136),
EH-3.2 THU (p150), EI-1.4 FRI (p186),
EI-P.3 FRI (p224)

Authors' Index

Mailis, Sakellaris . . . . . . . CM-P.20 MON (p78)
Maillard, Martin . . . . . . . . ∙CE-10.3 FRI (p206)
Mailliet, Max . . . . . . . . . . . . PD-2.3 THU (p171)
Main, D. . . . . . . . . . . . . . . . . . . ED-5.1 FRI (p180)
Maingot, Benjamin . . . . . . . ∙CF-5.3 TUE (p97)
Mainz, Roland . . . . . . . . . . . . . CF-5.1 TUE (p93)
Mainz, Roland E. . . . . . . . . . CF-3.4 MON (p71),
CG-4.3 THU (p151)
Maioli, Paolo . . . . . . . . . . . . JSVI-1.4 TUE (p89)
Mairesse, Yann . . . . . . . . . . . JSI-5.5 THU (p149)
Maison, Gregory . . . . . . . . . CB-9.4 THU (p152)
Maisons, Gregory . . . . . . . . CH-16.5 FRI (p217)
Maithani, Sanchi . . . . . . . . ∙CF-9.6 WED (p135)
Maître, Agnès . . . . . . . . . . . . . EJ-1.4 MON (p56)
Maitre, Florian . . . . . . . . . . CM-1.3 MON (p54)
Maity, Abhijit . . . . . . . . . . CF-9.6 WED (p135),∙PD-1.4 THU (p170)
Maiwald, Martin . . . . . . . . CB-P.14 MON (p76),
CH-13.3 FRI (p183)
Major, Balázs . . . . . . . . . . . ∙CG-4.5 THU (p153)
Mak, Ka Fai . . . . . . . . . . . . . . CA-2.3 MON (p60),
CF-6.4 WED (p113)
Makarenko, Maksim . . . . . CH-2.2 MON (p58),∙JSIII-P.6 FRI (p224)
Makarov, Vadim . . . . . . . . EB-P.14 THU (p177)
Makino, Kotaro . . . . . . . . . . . . EI-P.2 FRI (p224)
Makos, Ioannis . . . . . . . . . . JSI-2.5 WED (p118)
Makris, Konstantinos . . . ∙EJ-1.2 MON (p54),∙EF-7.2 FRI (p181), ∙EC-P.8 FRI (p223)
Makris, Konstantinos G.
CM-P.11 MON (p77), CM-P.23 MON (p78),
EF-P.8 WED (p139), EC-3.6 FRI (p209)
Maksimenka, Raman . . . . CG-3.4 THU (p145),∙CG-P.16 THU (p174), CF-12.3 FRI (p213)
Maksimov, Roman . . . . . . . . CA-3.3 MON (p68)
Malach, Miroslawa . . . . . . CB-P.11 MON (p76)
Malakzadeh, Abdollah . . . CG-P.3 THU (p173)
Malara, Pietro . . . . . . . . . . . CH-2.5 MON (p62),
CK-13.5 FRI (p196)
Malekmohamadi, Sedigheh∙CJ-P.19 FRI (p221)
Malhouitre, Stephane . . . . . . CB-5.3 TUE (p94)
Malica, Tushar . . . . . . . . . . CB-7.2 WED (p130)
Malik, Pooja . . . . . . . . . . . . . . EB-5.1 TUE (p93),
EB-9.2 WED (p131)
Malinauskas, Mangirdas ∙CM-1.1 MON (p52),∙CE-11.2 FRI (p212)
Malinowski, Marina . . . . . CL-3.5 THU (p161)
Malinverni, Marco . . . . . ∙CB-11.6 THU (p168)
Mallard, Frédéric . . . . . . . . . CL-P.15 FRI (p222)
Mallick, Sadman . . . . . . . CH-12.5 THU (p169)
Mallweger, Marion . . . . . EB-11.5 THU (p153),∙EB-P.35 THU (p178)
Malomed, Boris . . . . . . . . EF-P.19 WED (p140)
Mamaikin, Mikhail . . . . . . CF-P.16 TUE (p103)
Mamann, Hadriel . . . . . . . . . ∙EB-5.2 TUE (p93)
Mamyrbayev, Talgat . . . . . JSI-1.4 WED (p112)
Manavaimaran, Balaji . . . . . CC-4.6 FRI (p186)
Mandal, Avik . . . . . . . . . . . CE-P.20 THU (p172)
Mandalawi, Younus . . . . . CK-7.5 WED (p134),
CI-6.5 FRI (p196)
Mandel, Oliver . . . . . . . . . . CF-7.3 WED (p117)
Manegatti, Francesco . . . . CK-14.6 FRI (p208)
Manek-Hönninger, Inka ∙CM-2.4 MON (p60),
CM-3.6 MON (p72)
Manetta, Angelo . . . . . . . . CK-P.35 TUE (p106)

Manetti, Francesco . . . . . ∙CH-2.1 MON (p58),
CL-6.1 FRI (p189), CD-13.2 FRI (p203)
Manfredda, M. . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Manfredda, Michele . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130)
Manganas, Phanee . . . . . . . CM-P.2 MON (p77)
Mangeney, Juliette . . . . . . . CC-2.3 THU (p161)
Mangini, Fabio . . . . . . . . . . EF-4.4 THU (p154),∙EF-7.1 FRI (p181), EF-7.4 FRI (p185),
EF-7.5 FRI (p187), EJ-3.3 FRI (p185)
Maniewski, Pawel . . . . . . . . CM-1.6 MON (p56)Mann, Sander A. . . . . . . . . EH-3.1 THU (p148)
Mano, Atsushi . . . . . . . . . . . JSI-2.4 WED (p118)
Mano, Takaaki . . . . . . . . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76), EC-P.11 FRI (p223)
Manousidaki, Maria . . . . ∙CM-3.2 MON (p66),
EE-2.3 FRI (p187), CC-6.3 FRI (p204)
Manrique-Nieto, Nicolas ∙CB-2.4 MON (p70)
Mansourzadeh, Samira . CC-2.1 THU (p157),
CC-3.1 THU (p163), ∙CC-P.3 FRI (p218),
CC-P.7 FRI (p218)
Månsson, Erik . . . . . . . . . . . . CK-1.6 MON (p72)
Mansuryan, Tigran . . . . . . . . EF-7.5 FRI (p187),
CD-13.3 FRI (p205)
Mäntynen, Henrik . . . . . . . . . EG-4.4 TUE (p86)
Manuylovich, Egor . . . . . . . . . CJ-P.9 FRI (p220)
Manuzzato, Enrico . . . . . . . . EA-6.3 FRI (p186)
Manwar, Nilesh . . . . . . . ∙JSIV-1.3 WED (p118)
Manwaring, Tanner . . . . . . . CC-7.5 FRI (p214)
Manzoni, Cristian . . . . . ∙CH-8.4 WED (p133),
CG-3.2 THU (p143)
Mao, Bojang . . . . . . . . . . . . . . . CL-6.5 FRI (p197)
Maquieira, Ángel . . . . . . . . CH-15.5 FRI (p209)
Maragkaki, Stella . . . . . . . . . CM-9.5 FRI (p196)
Maragkakis, George . . . . . . . EI-P.4 FRI (p224)
Marangon, Davide . . . . . . . . . CI-5.3 FRI (p182)
Marangoni, Marco . . . . . . . ED-1.2 MON (p53),
ED-2.6 MON (p63), ED-P.2 MON (p79)
Marangos, Jon . . . . . . . . . . . . . CG-1.4 TUE (p87)
Marangos, Jon P. . . . . . . . . CG-3.1 THU (p143),
EE-4.6 FRI (p209)
Marangos, Jonathan . . . . CG-P.10 THU (p174)
Marangos, Jonathan P . . . JSI-4.6 WED (p134)
Marceau, Alice . . . . . . . . . . ∙CD-2.5 MON (p62)
Marcellino, Jeremiah . . . . . . CL-6.5 FRI (p197)
Marchevsky, Andrey . . . . . EG-P.9 TUE (p107)
Marco, David . . . . . . . . . . . . . ∙CI-5.2 FRI (p180)
Marconi, Mathias . . . . . . . CD-8.4 WED (p118),
CB-7.3 WED (p130), EF-4.2 THU (p152),
EF-4.3 THU (p152), EF-5.2 THU (p158)
Marcoux, Pierre . . . . . . . . . . CL-3.1 THU (p157)
Marcoux, Pierre R . . . . . . . CL-3.4 THU (p161)
Marcucci, Niccolò . . . . . . . CK-15.1 FRI (p210)
Mardan Dezfouli, Ali . . . . . . CL-P.5 FRI (p221)
Maria Solé, Rosa . . . . . . . . CA-P.19 MON (p75)
Marianne, Julien . . . . . . . CH-P.22 WED (p137)
Marin-Palomo, Pablo . . . PP-1.10 MON (p64),
CB-P.13 MON (p76), CB-P.18 MON (p76),∙CB-P.22 MON (p76), CB-6.3 WED (p126),∙CI-4.5 WED (p133), EF-P.4 WED (p139)
Marinelli, Agostino . . . . . . JSI-4.6 WED (p134)
Maring, Nicolas . . . . . . . . . EB-6.1 WED (p109)
Marini, Mario . . . . . . . . . . . CM-11.3 FRI (p214)
Markel, Vadim . . . . . . . . . . EH-1.5 WED (p134)
Markham, Damian . . . . . . EB-12.2 THU (p159)

Marklund, Mattias . . . . . . . CG-3.6 THU (p149)
Markmann, Sergej . . . . . . . CB-9.3 THU (p150),
CH-13.2 FRI (p183)
Marmalyuk, Aleksandr . . . CB-9.5 THU (p152)
Marmolejo, Javier . . . . . . . CG-3.6 THU (p149)
Marmuse, Florian . . . . . . . CD-P.26 TUE (p101)
Maroju, Praveen Kumar ∙JSI-2.5 WED (p118),
CG-5.2 THU (p159)
Maron, Gabriele . . . . . . . . . . . EA-1.2 TUE (p83)
Marotta, Andrea . . . . . . . . . CI-4.2 WED (p131)
Marquardt, Christoph . . . . . EB-5.6 TUE (p99),
EB-6.4 WED (p113)
Marques, Anselmo M. . . . . . EC-P.5 FRI (p223)
Márquez, Andrés . . . . . . . CM-P.29 MON (p78)
Marris-Morini, Delphine . . CD-5.5 TUE (p91)
Marš, Matevž . . . . . . . . . . . . . CJ-P.13 FRI (p220)
Marsal, Nicolas . . . . . . . . . EF-P.23 WED (p141)
Marschick, Georg . . . . . . . . . CH-3.3 TUE (p86)
Marsh, John . . . . . . . . . . . . . . PP-1.3 MON (p64),
CB-P.1 MON (p75), CB-P.3 MON (p75)
Marsi, Marino . . . . . . . . . . . . CF-1.4 MON (p57)
Marsik, Premysl . . . . . . . . . EE-1.5 WED (p113)
Martel, Théo . . . . . . . . . . . . ∙CK-12.1 FRI (p180)
Martin, Anthony . . . . . . . . . EB-2.5 MON (p63),
EB-9.6 WED (p135), EB-11.4 THU (p153),
EB-P.2 THU (p176)
Martin, Aude . . . . . . . . . . . . . CH-4.4 TUE (p96)
Martin, Bruno . . . . . . . . . . . . ∙CH-4.4 TUE (p96)
Martin, Cecilia . . . . . . . . . CH-P.20 WED (p137)
Martin, Denis . . . . . . . . . . CB-11.6 THU (p168)
Martin, Dominik . . . . . . . CB-11.1 THU (p162),
CB-11.3 THU (p166)
Martin, Fernando . . . . . . . . . . EE-3.1 FRI (p189)
Martin, Guillermo . . . . . . JSII-1.3 MON (p55),
JSII-2.5 MON (p63), ∙JSII-P.3 MON (p80)
Martin, Haydn . . . . . . . . . . CH-7.2 WED (p123)
Martin, Ines . . . . . . . . . . . . ∙CF-6.1 WED (p109)
Martin, Nazario . . . . . . . . . . . EE-3.1 FRI (p189)
Martin-Garcia, Beatriz . . . . CE-4.3 TUE (p95)
Martín-Hernández, Rodrigo∙CG-1.3 TUE (p87), EG-P.2 TUE (p106)
Martinez, Alejandro . . . . . EG-6.4 WED (p112)
Martinez, Anna . . . . . . . . ∙CC-2.4 THU (p163)
Martinez de Velasco, AndrésED-1.1 MON (p53)
Martínez-Matos, Óscar . . . EJ-P.3 MON (p80),
CF-4.1 TUE (p83)
Martínez Vázquez, Rebeca∙CM-6.3 TUE (p94), CG-3.2 THU (p143),∙CM-11.3 FRI (p214)
Martinod, Marc-Antoine . JSII-3.3 MON (p69)
Martins, João . . . . . . . . . . . CD-P.18 TUE (p101)
Márton, István . . . . . . . . . . . CC-1.5 THU (p155)
Márton, Zsuzsanna . . . . . . CC-1.5 THU (p155)
Martyanov, Mikhail . . . . CG-P.12 THU (p174)
Martynov, G. N. . . . . . . . . . . . CL-7.1 FRI (p201)
Maruta, Akihiro . . . . . . . . . CI-4.3 WED (p131),
CI-6.3 FRI (p192), CI-P.1 FRI (p219)
Marx, Jan . . . . . . . . . . . . . . CH-12.4 THU (p167)
Mas Arabí, Carlos . . . . . . . EF-2.5 WED (p135),∙EF-5.5 THU (p160), EF-6.4 THU (p166)
Masciovecchio, Claudio . JSI-1.5 WED (p114),
JSI-P.1 WED (p141)
Masłowski, Piotr . . . . . . . . . ED-1.2 MON (p53),
CE-3.2 MON (p67), ED-4.2 TUE (p83)
Masoller, Cristina . . . . . . . . CB-P.8 MON (p76),

242

CB-P.19 MON (p76), EF-P.21 WED (p140)
Masominia, Amir . . . . . . . . JSIII-6.5 FRI (p217)
Masominia, Amir Hossein∙JSIII-6.4 FRI (p215)
Mason, Paul . . . . . . . . . . . . ∙CA-8.2 WED (p116)
Masoudi, Ali . . . . . . . . . . ∙CH-10.6 THU (p155)
Massar, Serge . . . . . . . . . . JSIII-1.3 THU (p158),
JSIII-2.6 THU (p168), JSIII-P.17 FRI (p225)
Massaro, Loredana Maria JSIII-6.2 FRI (p213)
Masselin, Pascal . . . . . . . . . . CM-6.6 TUE (p98)
Massella, Damiano . . . . . . CK-P.34 TUE (p106)
Masters, Luke . . . . . . . . . . . . . EA-1.2 TUE (p83)
Matalla, Oliver . . . . . . . . . CB-11.5 THU (p168)
Mateos, Xavier . . . . . . . . . . CA-P.18 MON (p75),
CA-P.19 MON (p75), CA-P.20 MON (p75),
CA-9.1 WED (p128), CA-9.4 WED (p132),
CA-10.3 THU (p144),
CA-10.6 THU (p148), CJ-6.2 THU (p143),
CE-8.5 FRI (p186)
Matha, Robin . . . . . . . . . ∙CH-P.26 WED (p137)
Matheis, Luis . . . . . . . . . . . . ∙EB-3.2 MON (p67)
Mathews, Garrett . . . . . . . CH-5.2 WED (p113)
Mathijssen, Jan . . . . . . . . . ∙CG-P.7 THU (p174)
Mathurin, Carl . . . . . . . . . . CH-5.2 WED (p113)
Matias, Ignacio R. . . . . . . . . CL-1.4 MON (p71)
Matlis, Nichola H. . . . . . . . . . CC-P.5 FRI (p218)
Matlis, Nicholas H. . . . . . . CC-3.3 THU (p167)
Matsuda, Nobuyuki . . . . . . CK-8.2 THU (p142)
Matsui, Yuuki . . . . . . . . . . . . . ∙CJ-P.4 FRI (p220)
Matsumoto, Atsushi . . . . . CI-3.2 WED (p125),∙CB-10.5 THU (p160)
Matsumura, Yudai . . . . . . . CC-P.11 FRI (p218)
Matsunaga, Ryusuke . . . . . . CC-5.4 FRI (p196),
CC-P.6 FRI (p218)
Matsushita, Saya . . . . . . . . . . CJ-P.10 FRI (p220)
Matsuyama, Toru . . . . . . . . . . CF-5.1 TUE (p93)
Matsuzaki, Korenobu . . . ∙CH-9.1 THU (p143)
Mattana, Francesco . . . . . ∙EA-4.4 THU (p160)
Mattei, Giovanni . . . . . . . . . JSVI-2.5 TUE (p99)
Matthes, Jonas . . . . . . . . . . CE-P.24 THU (p173)
Matthews, Jonathan . . . . EB-P.16 THU (p177)
Matthews, Jonathan C. F. EB-6.2 WED (p109),EB-6.5 WED (p113), CH-9.2 THU (p145)
Matthews, Mary . . . . . . . . . . CG-1.4 TUE (p87),∙CG-3.1 THU (p143),
CG-P.10 THU (p174), EE-4.6 FRI (p209)
Matusko, Martina . . . . . . . ∙ED-3.2 MON (p69)
Maucher, Fabian . . . . . . . . EF-4.2 THU (p152),∙EA-7.1 FRI (p188)
Mauclair, Cyril . . . . . . . . ∙CH-P.18 WED (p137)
Mauer, Alsu . . . . . . . . . . . . . CA-6.2 WED (p108)
Maulini, Richard . . . . . . . . CB-9.2 THU (p150)
Maurice, Olivier . . . . . . . . CD-8.1 WED (p114)
Maurin, Isabelle . . . . . . . . . . ED-3.5 MON (p73)
Mauritsson, Johan . . . . . . . JSI-2.5 WED (p118)
Mavridou, Kalliopi . . . . . . . EE-P.3 WED (p138)
Mawet, Dimitri . . . . . . . . . . JSII-1.4 MON (p57),
JSII-3.5 MON (p73)
Maxwell, Innes L. . . . . . . . . EG-P.7 TUE (p107)
Mayer, Aline. S . . . . . . . . . . CF-8.3 WED (p125)
Mayer, Dennis . . . . . . . . . . ∙JSI-5.3 THU (p145),∙JSI-5.4 THU (p147)
Mayer, Nicola . . . . . . . . . . . . ∙CG-1.5 TUE (p89)
Mayer Martins, Jonas . . ∙JSIII-P.15 FRI (p225)
Maynard, Cobi . . . . . . . . . . ∙CK-15.2 FRI (p210)
Mayzlin, Yuriy . . . . . . . . . . . . CC-6.5 FRI (p208)

Mazauric, Serge . . . . . . . . . . CK-15.4 FRI (p214)
Mazelanik, Mateusz . . . ∙EB-10.2 THU (p143),
EB-10.6 THU (p149), EA-P.21 THU (p175),
EA-6.4 FRI (p186)
Maznev, Alexei . . . . . . . . . . JSI-1.4 WED (p112)
Mazur, Mikael . . . . . . . . . . . CI-4.2 WED (p131)
Mazza, Tommaso . . . . . . . . JSI-P.2 WED (p141),
JSI-5.3 THU (p145), JSI-5.4 THU (p147)
Mbithi, Nelson . . . . . . . . . . CE-P.6 THU (p171),
CC-P.13 FRI (p218)
McCallum, Jeffrey C. . . . . . CE-10.2 FRI (p204)
McCauley, John . . . . . . . . . . ED-2.1 MON (p59)
McCourt, Peter . . . . . . . . CH-P.28 WED (p137)
McCracken, Richard . . . . . CF-7.3 WED (p117)
McCracken, Richard A. . . . EJ-P.7 MON (p80),
CF-11.4 FRI (p205), CF-11.5 FRI (p207)
McCutcheon, Dara P S . . EA-P.20 THU (p175)
McGhee, Kirsty . . . . . . . . . CH-8.4 WED (p133)
McGoverin, Cushla . . . . . . CL-P.11 FRI (p222)
McIntosh, Rohin . . . . . . . . ∙CH-1.2 MON (p53)
McKay, Jason . . . . . . . . . . . . . CA-3.1 MON (p66)
McMillan, Alex . . . . . . . . . . CH-9.2 THU (p145)
Mears, Robbie . . . . . . . . . . . . . CD-4.2 TUE (p82)
Mecozzi, Antonio . . . . . . . . CI-4.2 WED (p131)
Medaglia, PierGianni . . CM-P.18 MON (p78)
Medeghini, Fabio . . . . . . . . CF-2.4 MON (p61),
CF-9.4 WED (p133), CG-5.3 THU (p159)
Medina, Eli . . . . . . . . . . . . . CG-P.13 THU (p174)
Meetei, Toijam Sunder . CH-P.21 WED (p137),∙CE-P.4 THU (p171)
Meethale Palakkool, Nadira∙CE-P.15 THU (p172)
Meglinski, Igor . . . . . . . . . . CL-1.5 MON (p73),∙EJ-P.4 MON (p80), EJ-P.6 MON (p80),
CL-4.3 THU (p167), CL-4.4 THU (p167),
CL-6.4 FRI (p197), EJ-4.2 FRI (p191)
Méhaignerie, Paul . . . . . . . . ∙EB-4.5 TUE (p89)
Mehew, Jake Dudley . . . . . . . ∙EI-4.5 FRI (p216)
Mei, Chao . . . . . . . . . . . . . . . CF-6.2 WED (p109),∙CF-10.5 THU (p147)
Meier, Janosch . . . . . . . . . . . . . CI-6.5 FRI (p196)
Meier, Jessica . . . . . . . . . . . . . . CK-2.3 TUE (p86)
Meier, Joachim . . . . . . . . . . . . EE-4.3 FRI (p205)
Meierhofer, Manuel . . . . . . CG-5.1 THU (p157)
Meinecke, Jasmin D. A. . . EA-P.1 THU (p174)
Mekhael, Madona . . . . . ∙CD-10.2 WED (p130)
Mekhail, Simon . . . . . . . . . . . EA-6.1 FRI (p180)
Melchert, Oliver . . . . . . . . . . EJ-2.3 MON (p60),∙CD-9.4 WED (p124), EF-P.1 WED (p139),
EF-5.3 THU (p158), EE-5.2 FRI (p211)
Melissinaki, Vasileia . . . . . CM-1.1 MON (p52),∙CM-P.31 MON (p78),
CH-12.4 THU (p167)
Melli, Federico . . . . . . . . . . ∙CE-2.3 MON (p61)
Melninkaitis, Andrius . . CM-P.31 MON (p78)
Melo-Luna, Carlos A. . . ∙EB-P.19 THU (p177)
Melo Luna, Carlos Andres
EB-P.10 THU (p176)
Memeo, Roberto . . . . . . . . CK-6.5 WED (p126)
Mendoza-Castro, Jesus Hernan
CH-3.4 TUE (p86), ∙CK-P.32 TUE (p106),
CH-P.14 WED (p136)
Menezes, Leonardo de S.
∙CH-P.7 WED (p136),∙CE-P.28 THU (p173), EI-P.3 FRI (p224)
Meng, Bo . . . . . . . . . . . . . . . . CB-9.3 THU (p150)

Authors' Index

Meng, Chao . . . . . . . . . . . . . . CL-4.4 THU (p167)
Meng, Fanchao . . . . . . . . . . CD-9.2 WED (p122)
Mennea, Paolo L. . . . . . . . CA-6.3 WED (p110),
CE-P.17 THU (p172), CE-9.2 FRI (p190)
Menon, Rajesh . . . . . . . . . . . . CF-4.2 TUE (p83),
CF-P.5 TUE (p102)
Mense, Thorben . . . . . . . . . CA-6.2 WED (p108)
Menyuk, Curtis R. . . . . . . . ED-P.8 MON (p79),
EJ-4.5 FRI (p197)
Menzel, Henning . . . . . . . CE-P.24 THU (p173)
Mer, Ewan . . . . . . . . . . . . . CM-7.5 WED (p112)
Meretska, Maryna L. . . . . CK-11.6 THU (p168)
Merghem, Kamel . . . . . . . . . CB-5.3 TUE (p94)
Mergo, Paweł . . . . . . . . . . . . . CE-10.5 FRI (p208)
Merkle, Larry . . . . . . . . . . . . CA-3.1 MON (p66)
Merklein, Moritz . . . . . . . . ∙CD-12.5 FRI (p197)
Merlo, Sabina . . . . . . . . . . . PP-2.7 WED (p121),
CL-2.6 THU (p155), CL-P.1 FRI (p221)
Mermillod-Blondin, Alexandre
CM-6.4 TUE (p96)
Meron, Omri . . . . . . . . . . . . . ∙EE-5.5 FRI (p215)
Merten, André . . . . . . . . . . . CB-9.6 THU (p154)
Mertenskötter, Lutz . . . . . . . CB-P.6 MON (p75)
Merzuk, Barbara . . . . . . . . . JSI-2.5 WED (p118)
Mesaritakis, Charis . . ∙CH-P.17 WED (p137),∙CL-2.2 THU (p151),
JSIII-1.1 THU (p156), JSIII-3.4 FRI (p187),
EJ-3.4 FRI (p187)
Meschede, Marcus J. . . . PP-2.10 WED (p121),
EC-P.1 FRI (p222)
Messaddeq, Younès . . . . . . . CE-1.2 MON (p53)
Messerschmidt, John P. . ∙CD-8.2 WED (p116)
Messner, Leon . . . . . . . . . . EB-10.3 THU (p145)
Messner, Manuel . . . . . . . CA-10.2 THU (p142)
Mestre Torà, Blanca . . . . . . ∙CL-7.3 FRI (p205)
Metais, Samuel . . . . . . . . . . CF-6.1 WED (p109)
Metrangolo, Pierangelo . . . . EE-3.4 FRI (p197)
Metzger, Thomas . . . . . . . CD-8.1 WED (p114),
CF-10.6 THU (p149)
Meucci, Marco . . . . . . . . . . . . CC-4.4 FRI (p184)
Mevel, Eric . . . . . . . . . . . . . CG-4.6 THU (p155),
CG-P.4 THU (p173)
Mevert, Robin . . . . . . . . . . CF-P.19 TUE (p103),
CF-11.3 FRI (p205)
Meyer, Eric . . . . . . . . . . . . . . EA-P.1 THU (p174)
Meyer, Johann Gabriel . ∙CD-P.12 TUE (p100),∙CC-3.6 THU (p169)
Meyer, M. . . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Meyer, Marco . . . . . . . . . . . . . CM-9.4 FRI (p194)
Meyer, Michael . . . . . . . . . JSI-4.3 WED (p130),
JSI-P.2 WED (p141), EE-4.3 FRI (p205)
Meyer, Rudolf . . . . . . . . . . . CF-10.4 THU (p145)
Meyer, Stefan . . . . . . . . . . . . . ∙CL-8.2 FRI (p211)
Meyer-Zedler, Tobias . . . . . . CL-8.5 FRI (p215)
Meyer zum Alten Borgloh, Mara
EA-7.5 FRI (p196)
Meylahn, Fabian . . . . . . . . ∙EA-5.2 THU (p164)
Mhibik, Oussama . . . . . . . . CF-P.5 TUE (p102),
CH-7.6 WED (p127)
Miao, Ting . . . . . . . . . . . . . CH-P.33 WED (p138)
Michaelis, David J. . . . . . . CC-3.2 THU (p165),
CC-7.5 FRI (p214)
Michaelis de Vasconcellos, Steffen
EI-2.5 FRI (p196)
Michail, Antonis . . . . . . . . . . . EI-P.4 FRI (p224)
Michailovas, Andrejus . . . CA-1.5 MON (p56),

CA-P.14 MON (p74), CA-11.6 THU (p154)
Michailovas, Kirilas . . . . . . CA-1.5 MON (p56)Michal, Kwaśny . . . . . . . . ∙CD-P.29 TUE (p101)
Michalak, Krzysztof . . . . CB-P.21 MON (p76)
Michalzik, Rainer . . . . . . . . CB-2.4 MON (p70)Michel, Knut . . . . . . . . . . . . CD-8.1 WED (p114)
Micheletti, Paolo . . . . . . . . ∙CC-4.1 FRI (p180),
CC-4.3 FRI (p182), CC-4.5 FRI (p186)
Michelletti, Paolo . . . . . . . CB-8.6 THU (p148),
EC-3.1 FRI (p201)
Michler, Peter . . . . . . . . . . . CB-P.10 MON (p76),
EA-4.6 THU (p162), EA-5.1 THU (p162),
CK-11.5 THU (p168), EA-P.12 THU (p175)
Mididoddi, Chaitanya . . . CL-3.3 THU (p159)
Midorikawa, Katsumi . . . . . . CF-4.3 TUE (p85)
Mignet, Nathalie . . . . . . . . . CL-2.3 THU (p151)
Mihelič, A. . . . . . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Mika, Jaromír . . . . . . . . . . . ∙EA-P.7 THU (p175)
Mikaelsson, Sara . . . . . . . . . . CF-5.2 TUE (p95),
CG-5.2 THU (p159)
Mikami, Yuya . . . . . . . . . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118)
Mikhailov, Dmitriy . . . . . . CB-9.5 THU (p152)
Mikhailov, Egor . . . . . . . . . . CJ-5.3 WED (p131)
Mikhailov, Stepan . . . . . . . . JSI-P.6 WED (p141)
Miki, Shigehito . . . . . . . . . . EA-2.2 THU (p142),
EB-P.9 THU (p176)
Mikkelsen, Anders . . . . . . . JSIII-5.2 FRI (p205)
Mikkonen, Tommi . . . . . . CH-P.6 WED (p136)
Mikołajczyk, Michał . . . . . EB-9.5 WED (p133)
Mildren, Rich . . . . . . . . . . . . CE-7.1 THU (p163)
Mildren, Richard Paul . . . . . CA-5.5 TUE (p98)
Milian, Carles . . . . . . . . . . . EF-P.5 WED (p139),
EJ-3.3 FRI (p185)
Milián Enrique, Carles . . ∙EF-6.6 THU (p168)
Milla, Maria Jose . . . . . . . CM-P.25 MON (p78)
Millar-Blanchaer, Maxwell
JSII-3.5 MON (p73)
Miller, Lucius . . . . . . . . . . . . CB-9.1 THU (p148)
Miller, Vincent . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Millo, Jacques . . . . . . . . . . . ED-3.2 MON (p69)
Millon, Celia . . . . . . . . . . . ∙PP-2.1 WED (p120),CC-2.1 THU (p157), ∙CC-P.1 FRI (p218)
Mills, Arthur K. . . . . . . . . . EF-6.1 THU (p162),
EF-6.2 THU (p164)
Milne, Alasdair . . . . . . . . ∙CH-10.2 THU (p151)
Minár, Ján . . . . . . . . . . . . . . . CM-P.6 MON (p77)
Minassian, Ara . . . . . . . . . . CA-6.5 WED (p112)
Mincigrucci, Riccardo . . ∙JSI-1.5 WED (p114),
JSI-P.1 WED (p141)
Minkevičius, Justinas . . . . CM-4.4 TUE (p86)
Minoshima, Kaoru . . . . . ∙CH-5.1 WED (p109),
CH-7.3 WED (p125)
Minovich, Alexander . . CK-10.1 THU (p156)
Mintert, Florian . . . . . . . . . PD-1.9 THU (p170)
Mir, Sameer Ahmad . . . . . . . . CI-6.1 FRI (p188)
Mir, Umair . . . . . . . . . . . . . . CD-11.3 FRI (p185)
Miranda, Miguel . . . . . . . CD-P.18 TUE (p101),
PD-1.3 THU (p170), CL-7.4 FRI (p205)
Mirasso, Claudio R. . . . . JSIII-2.2 THU (p164)
Mirgorodskiy, Ivan . . . . . . . PP-1.4 MON (p64),
CB-P.2 MON (p75)
Mirian, N. . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Mirkes, Holger . . . . . . . . . . CL-2.1 THU (p149),∙CL-5.3 FRI (p185)
Miron, Catalin . . . . . . . . . . JSI-4.3 WED (p130)
Mironov, Sergey . . . . . . . . CG-P.12 THU (p174)
Miroshnichenko, Andrey CD-1.5 MON (p56),
CK-10.5 THU (p160)
Mirza, Inam . . . . . . . . . . . . . ∙CM-9.6 FRI (p196)
Misdanitis, Konstantinos CM-3.2 MON (p66)
Misera, Mattias . . . . . . . . . . . ED-P.3 MON (p79)
Mishina, Ken . . . . . . . . . . . . CI-4.3 WED (p131),
CI-6.3 FRI (p192), CI-P.1 FRI (p219)
Mishra, Pawan . . . . . . . . . . . . . CB-4.5 TUE (p91)
Missbach-Guentner, Jeannine
CL-3.6 THU (p163)
Missori, Mauro . . . . . . . . . . . ∙CC-6.4 FRI (p206)
Mister, Samuel T . . . . . . . ∙EA-P.20 THU (p175)
Mitchell, Arnan . . . . . . . . . CK-4.3 WED (p112)
Mitchell, Morgan . . . . . . . . . . EA-1.6 TUE (p89)
Mitchell, Toby . . . . . . . . . . . CF-7.6 WED (p121)
Mitra, Chayan . . . . . . . . . . . CH-16.4 FRI (p215)
Mitryakhin, Victor . . . . . . . . ∙EI-2.6 FRI (p196)
Mittenzwey, Henry . . . . . . . . EI-4.4 FRI (p214)
Mitzner, Rolf . . . . . . . . . . . . . . EE-3.3 FRI (p195)
Miyamoto, Katsuhiko . . . . . CM-4.6 TUE (p88)
Miyauchi, Kotaro . . . . . . EE-P.11 WED (p139)
Mizaikoff, Boris . . . . . . . . . . . CC-7.2 FRI (p210)
Mlynek, Alexander . . . . . . . . CL-8.1 FRI (p211)
Mocci, Daniele . . . . . . . . . . . CF-1.3 MON (p57),
EE-3.1 FRI (p189), ∙EE-3.4 FRI (p197)
Mocek, Tomáš . . . . . . . . . . . CA-P.1 MON (p74),
CA-P.19 MON (p75)
Moczko, Loïc . . . . . . . . . . . . . . EI-3.1 FRI (p200)
Modsching, Norbert . . . . . CG-4.4 THU (p153)
Moehl, Charles . . . . . . . . . . CK-14.5 FRI (p206)
Moeller, Stefan . . . . . . . . . . JSI-4.6 WED (p134)
Moerk, Jesper . . . . . . . . . . . ∙EG-1.1 MON (p52),
CK-15.6 FRI (p216)
Mohácsi, Árpád . . . . . . . . . CG-4.1 THU (p149)
Mohajan, Shubho . . . . . . . . CL-2.4 THU (p153)
Mohamad, Habib . . . . . . . . . CE-11.4 FRI (p214)
Mohammadi, Maryam . . . . CE-3.6 MON (p73)
Möhl, Charles . . . . . . . . . . . EF-2.3 WED (p133),
CE-9.1 FRI (p188)
Mohr, Christian . . . . . . . . . JSI-P.4 WED (p141)
Mohr, Dominik . . . . . . . . . . CA-6.6 WED (p114)
Moille, Gregory . . . . . . . . . . ED-P.8 MON (p79),
EF-2.2 WED (p131)
Moio, Bruno . . . . . . . . . . . . . CF-2.4 MON (p61),
CG-2.2 TUE (p97)
Moldovan, Simona . . . . . . EG-P.5 TUE (p107),
CH-6.6 WED (p120), EE-P.5 WED (p138)
Molkens, Korneel . . . . . . . . CK-8.4 THU (p144)
Molle, Alessandro . . . . . . . . . CG-2.2 TUE (p97)
Möller, Friedrich . . . . . . . . . . CJ-1.3 TUE (p97),∙CJ-1.4 TUE (p97)
Möller, Marcel . . . . . . . . . . . . EG-3.3 MON (p68)Møller, Søren H. . . . . . . . CM-P.19 MON (p78),
CM-10.2 FRI (p204)
Möller, Thomas . . . . . . . . . . JSI-3.1 WED (p122)
Molodtsov, Serguei . . . . . . JSI-P.3 WED (p141)
Moloney, Jerome V . . . . . . ∙CB-P.9 MON (p76),∙EI-2.4 FRI (p194)
Monat, Christelle . . . . . . . CK-4.3 WED (p112),
CK-5.6 WED (p120)
Monberg, Eric . . . . . . . . . . . . . CJ-1.1 TUE (p93)
Money, Alain . . . . . . . . . . . . . . CE-9.3 FRI (p192)
Monfared, Mohammed . . . . . EI-1.3 FRI (p184)

243

Monge Barolome, Laura . . . CB-4.2 TUE (p90)
Monge Bartolomé, Laura . . CB-4.1 TUE (p90)
Monika, Monika . . . . . . . . . . . EC-3.2 FRI (p203)
Monmayrant, Antoine . . CD-P.10 TUE (p100),
CH-P.16 WED (p137), CK-12.4 FRI (p184)
Monney, Alain . . . . . . . . . . . . ∙CE-9.6 FRI (p196)
Monroy-Ruz, Jorge . . . . . . EB-6.5 WED (p113),
CH-9.2 THU (p145)
Monsalve, Mariano I. . . . EB-P.17 THU (p177)
Monsel, Juliette . . . . . . . . . . EA-3.1 THU (p148)
Monserud, Nils . . . . . . . . . . JSI-3.1 WED (p122)
Montagnese, Matteo . . . . . . CL-P.9 FRI (p222)
Montague, Patrick . . . . . . CK-P.35 TUE (p106)
Montague, Patrick Bowen CH-1.3 MON (p55)Montanaro, Alberto . . . . . . CI-3.4 WED (p127)
Montano, Jacobo . . . . . . . . JSI-P.2 WED (p141),
EE-4.3 FRI (p205)
Montemezzani, Germano
EF-P.23 WED (p141)
Montesinos Ballester, Miguel∙CK-6.2 WED (p124), CB-8.5 THU (p146)
Monteville, Achille . . . . . . . . . CJ-P.2 FRI (p220)
Montfray, Stéphane . . . . . . . EB-3.1 MON (p67)
Montvernay, Régis . . . . . . . . CL-P.15 FRI (p222)
Monvoisin, Natan . . . . . ∙CH-P.16 WED (p137)
Moog, Bruno . . . . . . . . . . . . CE-5.3 THU (p151)
Mooshammer, F. . . . . . . . . . . . EI-2.1 FRI (p188)
Mor, Chen . . . . . . . . . . . . . . EE-P.14 WED (p139)
Mor , Ori . . . . . . . . . . . . . . . EB-P.27 THU (p177)
Morad, Viktoriia . . . . . . . . CA-9.3 WED (p130)
Moraitis, Christina . . . . . . JSII-1.2 MON (p55),∙PP-1.12 MON (p65), ∙JSII-P.2 MON (p80)
Morand, Alain . . . . . . . . . . . JSII-2.5 MON (p63)
Morandi, Andrea . . . . . . . . JSIII-4.3 FRI (p195)
Morandotti, R. . . . . . . . . . EF-P.15 WED (p140)
Morandotti, Roberto . . . . CI-4.6 WED (p135),
ED-6.3 FRI (p192), EE-5.3 FRI (p213)
Morassi, Martina . . . . . . . . EG-2.1 MON (p58),
JSVI-1.1 TUE (p83), EB-6.1 WED (p109),EB-6.6 WED (p115)
Moratis, Kimon . . . . . . . . . . CK-14.6 FRI (p208)
Morawiec, Seweryn . . . . . . . ∙CL-7.2 FRI (p203)
Moreau, Antonin . . . . . . . . EF-3.3 THU (p144),
PD-2.2 THU (p170)
Moreau, Paul-Antonie . . . . . EA-6.1 FRI (p180)
Moreira, Felipe . . . . . . . . . JSIII-P.14 FRI (p225)
Moreira, Raoni S N . . . . . EA-P.23 THU (p176)
Morel, Benoit . . . . . . . . . . . . . . EE-2.2 FRI (p185)
Morency, Steeve . . . . . . . . . . CE-1.2 MON (p53)
Moreno, David . . . . . . . . . . CD-P.17 TUE (p101)
Moreno, Ignacio . . . . . . . . . . . CI-5.2 FRI (p180)
Moreno, Jorge . . . . . . . . . . . . ED-1.3 MON (p55)
Moreno, Pablo . . . . . . . . . . . . CM-9.2 FRI (p190)
Moreno, Victor . . . . . . . . . . CD-8.1 WED (p114)
Moret, Michel . . . . . . . . . . . CD-8.1 WED (p114)
Moretti, Gianni Q. . . . . . . ∙EH-3.2 THU (p150)
Moretti, Luca . . . . . . . . . . . ∙ED-2.6 MON (p63),
ED-P.2 MON (p79)
Morgner, Uwe . . . . . . . . . . . . EJ-2.3 MON (p60),
CF-P.19 TUE (p103), CD-9.4 WED (p124),
EF-P.1 WED (p139), EF-5.3 THU (p158),
CF-11.3 FRI (p205), EE-5.2 FRI (p211)
Mori, Yojiro . . . . . . . . . . . . . . . CI-6.4 FRI (p194)
Morichika, Ikki . . . . . . . . . CF-7.5 WED (p119),∙EE-P.2 WED (p138), EE-5.6 FRI (p217)
Morillo-Candas, Ana Sofia∙JSI-1.2 WED (p110), JSI-1.4 WED (p112),
JSI-3.2 WED (p124)
Morillo-Candas, Ana Sophia
JSI-4.1 WED (p128)
Morimoto, Katsuki . . . . . . ∙EE-P.9 WED (p139)
Mørk, Jesper . . . . . . . . . . . . . CB-1.3 MON (p54),
CB-1.4 MON (p56), EG-P.9 TUE (p107),
CK-4.5 WED (p114), CB-10.2 THU (p158),
EJ-4.6 FRI (p197)
Mornhinweg, Joshua . . . . . . ∙EG-4.3 TUE (p86)
Morohashi, Takuya . . . . . . . . CA-4.3 TUE (p84)
Morrell, Jane M. . . . . . . . . . . CL-5.4 FRI (p187)
Morrison, Christopher . . . CD-14.3 FRI (p215)
Morrison, Christopher L. . . EB-5.5 TUE (p97)
Mortensen, N. Asger . . . . . . EG-4.5 TUE (p88)
Morzyński, Piotr . . . . . . . . . CE-3.2 MON (p67),
EA-P.9 THU (p175)
Mosca, Mauro . . . . . . . . . . . JSVI-2.5 TUE (p99)
Moselund, Kirsten . . . . . . . . EF-8.4 FRI (p197),
CK-14.2 FRI (p202)
Moser, Christophe . . . . . . CM-1.3 MON (p54),
JSIII-1.5 THU (p160),
JSIII-1.6 THU (p162), CM-11.2 FRI (p212)
Moshammer, Robert . . . . . JSI-5.2 THU (p145)
Mosley, Peter J. . . . . . . . . . CE-P.30 THU (p173),
CD-14.5 FRI (p217)
Moss, D. J. . . . . . . . . . . . . . . EF-P.15 WED (p140)
Moss, David . . . . . . . . . . . . . . ED-6.3 FRI (p192),
EE-5.3 FRI (p213)
Mostajabi, Amirhossein . CD-8.1 WED (p114)
Motomura, Takumi . . . . . . ∙CI-4.3 WED (p131)
Motorin, Evgenii . . . . . . . . . CJ-5.1 WED (p129)
Mou, Chengbo . . . . . . . . . EF-P.18 WED (p140),
EF-P.20 WED (p140)
Mouchel, Roman . . . . . . . EB-P.19 THU (p177)
Mouchliadis, Leonidas . . CD-13.1 FRI (p201),
EI-P.4 FRI (p224)
Moughames, Johnny . . . . JSIII-4.5 FRI (p197),
JSIII-6.1 FRI (p211)
Mouhanna, Hippolyte . . . ∙ED-3.5 MON (p73)
Moune, Séverine . . . . . . . CH-P.22 WED (p137)
Mourkioti, Georgia . . . . . CA-9.2 WED (p130)
Mousavi, Faezeh . . . . . . . . . . EB-5.4 TUE (p97)
Mousavi, Seyedmohammad Abokhamis
CH-10.3 THU (p151)
Mouskeftaras, Alexandros∙CM-10.4 FRI (p206)
Mrokon, Alexander . . . . ∙CE-P.13 THU (p172)
Mu, Sin-Yuan . . . . . . . . . . . CK-P.40 TUE (p106)
Mu, Xin . . . . . . . . . . . . . . . . . ∙CL-1.2 MON (p69)
Mueller, Sebastian . . . . . . . . ED-P.6 MON (p79)
Mueller , Thomas . . . . . . . CH-8.3 WED (p131)
Mühlnickel, Lukas . . . . . . JSIII-2.3 THU (p166)
Mukherjee, Rick . . . . . . . . . PD-1.9 THU (p170)
Mukhin, Ivan . . . . . . . . . . ∙CG-P.12 THU (p174)
Mukhopadhyay, Shroddha
CD-P.31 TUE (p102), ∙EH-3.5 THU (p152)
Mulder, Bert L . . . . . . . . . . PP-2.6 WED (p121),
CI-P.13 FRI (p219)
Müller, André . . . . . . . . . . . CB-P.14 MON (p76),∙CB-11.4 THU (p166)
Muller, Antoine . . . . . . . . . CB-9.2 THU (p150)
Müller, Kilian . . . . . . . . . . . EA-3.3 THU (p150),∙JSIII-3.3 FRI (p185)
Müller, Marcel . . . . . . . . . . . CL-P.16 FRI (p222)
Müller, Michael . . . . . . . . . . CG-4.4 THU (p153)

Authors' Index

Müller, Robert . . . . . . . . . . CE-1.3 MON (p55),
CE-1.4 MON (p55)
Müller, Sebastian . . . . . . . . . ∙CC-6.5 FRI (p208)
Mullins, Terence . . . . . . . . . . . EE-4.3 FRI (p205)
Mullins, Terry . . . . . . . . . . ∙JSI-P.2 WED (p141)
Munch, Jesper . . . . . . . . . . . CA-8.1 WED (p114)
Munj, Abdul-Haseeb . . . ∙PP-2.5 WED (p121),∙CG-P.2 THU (p173)
Munk, Alexander . . . . . . . . CA-6.2 WED (p108)
Munkhbat, Battulga . . . . EB-P.33 THU (p178)
Munkueva, Zhibzema . . . . ∙CJ-P.20 FRI (p221)
Munns, Joseph Hugh Daekin
EB-12.3 THU (p159)
Munro, William J . . . . . . . . . EJ-2.4 MON (p62),
EA-3.5 THU (p152)
Munss, Joseph H. D. . . . . EB-P.17 THU (p177)
Münzenmaier, Yannick . . . CL-2.1 THU (p149)
Mur, Jaka . . . . . . . . . . . . . . . . . ∙CL-8.6 FRI (p217)
Muraviev, Andrey . . . . . . . . CF-3.1 MON (p67)
Murdoch, Stuart . . . . . . . . CD-8.5 WED (p120),
EF-3.4 THU (p144), ∙EF-3.6 THU (p148)
Murdoch, Stuart G. . . . . . CD-9.3 WED (p124),
CD-10.3 WED (p130),
CD-10.4 WED (p132), PD-2.7 THU (p171)
Murnane, Margaret M. . . . . CF-2.1 MON (p59)
Murphy, Leah R. . . . . . . . . ∙CE-2.2 MON (p59),
CD-4.2 TUE (p82)
Murphy, Stephen L. . . . . . . CI-3.3 WED (p125)
Murray, Robert . . . . . . . . . . . . CD-4.3 TUE (p84)
Murray, Robert T . . . . . . . . CL-3.2 THU (p159),
CD-13.6 FRI (p209)
Murta, Gláucia . . . . . . . . . . EB-9.3 WED (p131)
Murzyn, Kevin . . . . . . . . . . . ∙CF-2.3 MON (p61)Musch, Thomas . . . . . . . . . . CF-12.2 FRI (p211)
Muschet, Alexander . . . . . CG-3.6 THU (p149)
Musgrave, Ian . . . . . . . . . . . CF-P.23 TUE (p103)
Musha, Mitsuru . . . . . . . . . . . CJ-P.10 FRI (p220)
Muskens, Otto . . . . . . . . . . . EH-5.4 THU (p166)
Musslimani, Ziad H. . . . . . EF-P.8 WED (p139)
Mussot, Arnaud . . . . . . . . . EF-3.3 THU (p144),
PD-2.2 THU (p170), ED-6.6 FRI (p196)
Myllylä, Teemu . . . . . . . . . . . CL-1.5 MON (p73)Mylnikov, V. Yu. . . . . . . . . . ∙EA-1.4 TUE (p87)
Myronyuk, Oleksiy . . . . . CM-P.33 MON (p79)
Mysyrowicz, André . . . . . . CD-P.7 TUE (p100),
CD-8.1 WED (p114), EF-P.7 WED (p139)

N
N. Casses, Laura . . . . . . . . . CK-15.6 FRI (p216)
N. Neshev, Dragomir . . . . CD-3.4 MON (p70)
Na, Hong Ryeol . . . . . . . . . . . . EI-1.5 FRI (p186)
Na, Yongjin . . . . . . . . . . . . . . ∙ED-5.2 FRI (p182)
Nabekawa, Yasuo . . . . . . . . . . CF-4.3 TUE (p85)
Nabialek, Josie . . . . . . . . . . . . CB-4.5 TUE (p91)
Nacius, Ernestas . . . . . . . . . ∙CM-4.4 TUE (p86)
Nadlinger, D. P. . . . . . . . . . . . ED-5.1 FRI (p180)
Nafria, Vijay . . . . . . . . . . . ∙EB-P.13 THU (p177)
Nagai, Kohei . . . . . . . . . . . . ∙CF-1.2 MON (p55),
CF-2.2 MON (p59), EE-1.2 WED (p109)
Nagl, Nathalie . . . . . . . . . . . . CA-2.3 MON (p60)
Nagy, Oliver . . . . . . . . . . . . . . CC-5.5 FRI (p196)
Nagy, Roland . . . . . . . . . . . EB-10.5 THU (p147)
Nagy, Tamas . . . . . . . . . . . . . CM-6.4 TUE (p96),
CF-6.2 WED (p109), JSI-3.1 WED (p122),∙CF-10.3 THU (p145), CG-6.4 THU (p169)

Nagyilles, Balint . . . . . . . . . CA-8.5 WED (p120)
Nagymihaly, Roland . . . . . CA-8.5 WED (p120)
Nagymihály, Roland S. . . . . CF-P.6 TUE (p102)
Nagymihály, Roland Sándor
CG-4.1 THU (p149), ∙CG-P.3 THU (p173)
Nahon, Laurent . . . . . . . . . . JSI-5.5 THU (p149)
Najafidehaghani, Emad . . CD-2.3 MON (p60)
Nájar, Guillem . . . . . . . . . . CM-P.29 MON (p78)
Nakagawa, Mayuri . . . . . . . . CC-5.4 FRI (p196),∙CC-P.6 FRI (p218)
Nakajima, Shinya . . . . . . . . CI-3.2 WED (p125),
CB-10.5 THU (p160)
Nakashima, Ayata . . . . . . CD-P.17 TUE (p101),
CK-P.26 TUE (p105)
Nakatani, Asuka . . . . . . . . . . . CJ-7.3 FRI (p184)
Nam, Han Ku . . . . . . . . . . . . . CM-8.2 FRI (p180)
Namekata, Naoto . . . . . . . ∙PD-2.4 THU (p171)
Namiki, Shu . . . . . . . . . . . . . . . CI-6.2 FRI (p190)
Nanda, Abhishek . . . . . . . . . . ∙EJ-4.3 FRI (p193)
Nandi, Saikat . . . . . . . . . . . ∙JSI-4.3 WED (p130)
Nandy, Biplob . . . . . . . . . . . CG-3.5 THU (p147)
Naoktatsu , Yamamoto . . . . . CI-8.2 FRI (p210)
Narayanan, T. N. . . . . . . . . . EC-P.15 FRI (p223)
Nardi, Alberto . . . . . . . . . . . EF-2.3 WED (p133)
Nardini, Alessandra . . . . . CM-11.3 FRI (p214)
Narożnik, Mateusz . . . . . . . CE-3.2 MON (p67)
Narváez Castañeda, Emmanuel∙CK-P.39 TUE (p106)
Nasari, Hadiseh . . . . . . . . . . . EC-1.5 FRI (p187)
Nashashibi, Shadi . . . . . . . . CI-3.1 WED (p123)
Nasi, Luis . . . . . . . . . . . . . . . . CC-P.13 FRI (p218)
Nasir, Abdul . . . . . . . . . . . . . . CK-3.3 TUE (p94)
Natile, Michele . . . . . . . . . . CF-1.4 MON (p57),∙CF-P.3 TUE (p102)
Nattress, Brian . . . . . . . . . . CL-3.5 THU (p161)
Nauta, Janko . . . . . . . . . . . . . ED-P.5 MON (p79),
CF-8.2 WED (p125), CG-6.5 THU (p169)
Navajas, David . . . . . . . . . ∙EH-5.3 THU (p166)
Navarrete-Benlloch, Carlos
EA-P.24 THU (p176)
Nawrath, Cornelius . . . . CK-11.5 THU (p168),
EA-P.12 THU (p175)
Nayak, Abani S. . . . . . . . . . JSII-3.4 MON (p71),
JSII-P.1 MON (p80)
Naylon, Jack A. . . . . . . . . . CA-8.3 WED (p118),
CA-8.4 WED (p118)
Nazymbekov, Gabit . . . . . . . . CC-P.9 FRI (p218)
N’diaye, Fatoumata . . . . . . . . CC-7.5 FRI (p214)
Neb, Sergej . . . . . . . . . . . . . . . . CG-2.3 TUE (p99)
Neef, Vera . . . . . . . . . . . . . . . . ∙EB-4.2 TUE (p85)
Neegaard-Nielsen, Jonas EB-P.30 THU (p178)
Néel, Delphine . . . . . . . . . . . . CB-5.3 TUE (p94)
Neergaard-Nielsen, Jonas S.
EB-P.23 THU (p177)
Neergaard-Nielsen, Jonas SchouPP-1.11 MON (p64), EJ-P.1 MON (p79)
Negro, Matteo . . . . . . . . . . . . ∙CL-6.5 FRI (p197)
Nehemya, Snir . . . . . . . . . . . . . EE-5.5 FRI (p215)
Nejezchleb, Karel . . . . . . . . . CA-P.7 MON (p74)
Nelson, Alexander J. M. . . CH-4.2 TUE (p94)
Nelson, Keith . . . . . . . . . . . . JSI-1.4 WED (p112)
Němec, Michal . . . . . . . . . . . CA-P.7 MON (p74),
CA-P.8 MON (p74)
Nemec, Tadeas . . . . . . . . . . CG-6.2 THU (p165)
Neoričić, Lana . . . . . . . . . . JSI-4.3 WED (p130)
Neshev, Dragomir . . . . . . . CD-1.5 MON (p56),

CK-10.5 THU (p160), CE-7.1 THU (p163),
PD-2.9 THU (p171), CD-11.2 FRI (p183),
CD-11.5 FRI (p187)
Neshev, Dragomir N. . . . . EH-3.6 THU (p154),
CK-10.2 THU (p158)
Nespola, Antonino . . . . . . CI-4.2 WED (p131)
Neufeld, Ofer . . . . . . . . . . . . . CG-1.2 TUE (p85),
EE-1.3 WED (p111)
Neuhaus, Josefine . . . . . . . . . . EI-2.4 FRI (p194)
Neumann, Jörg . . . . . . . . . . CA-P.15 MON (p74)
Neuwirth, Julia . . . . . . . . . . . . EB-5.3 TUE (p95)
Newbury, Nathan R. . . . . . . ED-3.1 MON (p67)
Newman, Marcus R. A. . . . EG-P.9 TUE (p107)
Nezamalhosseini, S. Alireza
CI-4.2 WED (p131)
Ng, Boon Long . . . . . . . . . . ∙EA-P.3 THU (p174)
Ng, Vincent . . . . . . . . . . . CD-10.3 WED (p130),∙CD-10.4 WED (p132)
Ng, Wai Kit . . . . . . . . . . . . ∙CK-8.4 THU (p144),∙CK-14.3 FRI (p204)
Ngaha, Jacob . . . . . . . . . . . . . ∙EA-1.5 TUE (p87)
Ngo, Gia Quyet . . . . . . . . . ∙CD-2.3 MON (p60)
Nguyen, Hai Son . . . . . . . . . CK-15.4 FRI (p214)
Nguyen, Thi Anh Nguyet∙CH-13.4 FRI (p185)
Nguyen, Thi Hao Nhi . . . . . CD-5.5 TUE (p91)
NIbbering, Erik T. J. . . . . . . EE-3.2 FRI (p193),
EE-3.3 FRI (p195)
Nichol, B. C. . . . . . . . . . . . . . . ED-5.1 FRI (p180)
Nicholson, Jeffrey . . . . . . . . . ∙CJ-1.1 TUE (p93)
Nicoli, Luca . . . . . . . . . . . . . . EJ-2.2 MON (p60),∙EH-P.20 THU (p179)
Nie, Zhonghui . . . . . . . . . . . CF-2.3 MON (p61),∙EE-1.1 WED (p109)
Nieddu, Thomas . . . . . . . . . . . EB-5.2 TUE (p93)
Nieder, Jana . . . . . . . . . . . . . . CK-13.3 FRI (p192)
Nieder, Jana B. . . . . . . . . . ∙JSIII-P.2 FRI (p224)
Nieder, Jana Berit . . . . . . CD-P.18 TUE (p101),
CL-7.4 FRI (p205)
Niedermayr, Arthur . . . . . . . CG-2.3 TUE (p99)
Niehren, Stefan . . . . . . . . . . . PP-1.9 MON (p64),
CM-P.5 MON (p77)
Nielsen, Sissel . . . . . . . . . . . . . EA-9.5 FRI (p214)
Nielson, Anna . . . . . . . . . . . CL-3.5 THU (p161)
Nielson, Megan . . . . . . . . . . CC-1.1 THU (p149)
Nielson, Megan F. . . . . . . . CC-3.2 THU (p165),
CC-P.8 FRI (p218)
Niemi, Tapio . . . . . . . . . . . . . EG-1.4 MON (p56)
Nieuwoudt, Michel K. . . . PP-2.8 WED (p121),
CL-5.5 FRI (p187), CL-P.2 FRI (p221)
Niewelt, Bartosz . . . . . . . . EB-10.6 THU (p149),
EA-P.21 THU (p175)
Nigmatulin, Fedor . . . . . . . . . EI-P.1 FRI (p223)
Niki, Kaori . . . . . . . . . . . . . . JSI-3.4 WED (p126)
Nikitina, Julianija . . . . . . . CE-3.3 MON (p69),
CK-3.6 TUE (p98)
Nikkhah, Vahid . . . . . . . . . EH-5.1 THU (p162)
Nikl, Martin . . . . . . . . . . . . . . CA-P.7 MON (p74)
Nikodem, Michal . . . . . . CH-P.31 WED (p138)
Nikolov, Ivaylo . . . . . . . . . . JSI-P.7 WED (p141)
Nilforoushan, Niloufar . . ∙CC-2.3 THU (p161)
Ning Wang, Rui . . . . . . . . CB-10.1 THU (p156),
CK-14.5 FRI (p206)
Ninno, G. De . . . . . . . . . . . . JSI-3.5 WED (p126)
Nishida, Kohei . . . . . . . . . . . . ∙CI-6.3 FRI (p192)
Nishijima, Yoshiaki . . . . ∙EH-P.13 THU (p179)

244

Nisoli, Mauro . . . . . . . . . . . . CF-1.3 MON (p57),
CF-2.4 MON (p61), CF-3.3 MON (p69),
CG-2.2 TUE (p97), PP-2.4 WED (p120),
CF-9.4 WED (p133), CG-5.3 THU (p159),
CG-P.1 THU (p173), CG-P.5 THU (p173),
EE-3.1 FRI (p189), EE-3.4 FRI (p197)
Nitanai, Sho . . . . . . . . . . . . . CF-6.6 WED (p115),
EA-3.4 THU (p152)
Noda, Susumu . . . . . . . . . . . ∙CB-1.1 MON (p52)Nold, Johannes . . . . . . . . . . . CJ-1.3 TUE (p97),
CJ-2.4 WED (p113), CJ-8.2 FRI (p192)
Nölleke, Christian . . . . . . . . PP-1.4 MON (p64),
CB-P.2 MON (p75), CB-5.1 TUE (p92)Nolte, Stefan . . . . . . . . . . . . CM-2.3 MON (p60),
CM-2.6 MON (p62), CM-P.9 MON (p77),
EH-2.5 THU (p148), CL-3.6 THU (p163),
CE-6.3 THU (p159), CD-11.3 FRI (p185),
CD-11.4 FRI (p187), CM-9.3 FRI (p192),
EC-3.2 FRI (p203), EC-P.7 FRI (p223)
Nolvi, Anton . . . . . . . . . . . CH-12.4 THU (p167)
Nomura, Junia . . . . . . . . . . ∙CA-9.5 WED (p132)
Nomura, Kenya . . . . . . . . . . PD-2.4 THU (p171)
Nomura, Masahiro . . . . . . JSVI-1.3 TUE (p87),
JSVI-2.2 TUE (p95)
Noordzij, Niels . . . . . . . . . . . EB-P.7 THU (p176)
Noori, Narwan Kabir . . . . . . CC-5.5 FRI (p196)
Norihiko , Sekine . . . . . . . . . . CI-8.2 FRI (p210)
Normani, Simone . . . . . . ∙CA-P.18 MON (p75)
Norris, Barnaby . . . . . . . . . . JSII-3.3 MON (p69)
Norrman, Andreas . . . . . . . . EB-1.3 MON (p55)
Northup, Tracy E. . . . . . . . . PD-2.6 THU (p171)
NOURRY-MARTIN, Maxime
CG-P.14 THU (p174)
Nousios, Georgios . . . . . . CK-P.41 TUE (p106)
Novák, Jakub . . . . . . . . . . . CA-8.3 WED (p118)
Novák, Ondřej . . . . . . . . . . . CA-P.1 MON (p74)
Novikov, Innokenty . . . . . . CB-9.5 THU (p152)
Novotny, Lukas . . . . . . . . . . EB-1.3 MON (p55),
EA-9.3 FRI (p212)
Nowak, Michał P. . . . . . . . CE-P.26 THU (p173)
Nowosielski, Jan . . . . . . . . EB-10.6 THU (p149),
EA-P.21 THU (p175)
Nubbemeyer, Thomas . . . . CK-1.6 MON (p72)
Nugraha, Priyo S. . . . . . . . . CC-1.5 THU (p155)
Numkam Fokoua, Eric . . . CI-1.3 WED (p111)
Nunes Faria, Lucas . . . . . ∙EB-P.30 THU (p178)
Nussbaum-Lapping, AlexanderCA-2.5 MON (p62), CF-7.1 WED (p115)
Nutz, Thomas . . . . . . . . . . . EA-P.20 THU (p175)
Nwatu, Daniel . . . . . . . . . . . ∙CM-6.1 TUE (p92)
Nyga, Piotr . . . . . . . . . . . . ∙CE-P.26 THU (p173)
Nyga, Sebastian . . . . . . . . . CA-6.6 WED (p114)
Nyman, Robert A. . . . . . . . PD-1.9 THU (p170)

O
Oberhausen, Wolfhard . . . ∙CC-4.6 FRI (p186)
Oberli, Solene . . . . . . . . . . . JSI-4.1 WED (p128)
Obreja, Paula . . . . . . . . . . . . . . CK-2.2 TUE (p86)Obrzud, Ewelina . . . . . . . . JSII-2.4 MON (p63),
CD-5.2 TUE (p90)
Occhipinti, Tommaso . . . EB-P.22 THU (p177)
O’Connor, Gerard M. . ∙CM-P.21 MON (p78)
Odaci, Cem . . . . . . . . . . . . ∙CE-5.5 THU (p153),∙CL-P.9 FRI (p222)
Odagawa, Tomofumi . . . . ∙CK-8.2 THU (p142)

Odelius, Michael . . . . . . . . . . EE-3.2 FRI (p193),
EE-3.3 FRI (p195)
Oelmann, Jan-Hendrik . . . ED-P.5 MON (p79),
CF-8.2 WED (p125), ∙CG-6.5 THU (p169)
O’Faolain, Liam . . . . . . . . . . CH-3.2 TUE (p84),
CH-3.4 TUE (p86), CB-4.1 TUE (p90),
CB-4.2 TUE (p90), CK-P.6 TUE (p104),
CK-P.32 TUE (p106), CH-P.14 WED (p136)
Offrein, Bert . . . . . . . . . . . . ∙JSIII-3.1 FRI (p181)
Offrein, Bert J. . . . . . . . . . . . JSIII-4.4 FRI (p197)
Oguchi, Kenichi . . . . . . . . ∙CF-6.6 WED (p115),
EA-3.4 THU (p152)
Ogura, Yusuke . . . . . . . . . JSIII-2.5 THU (p168)
Oguri, Katsuya . . . . . . . . . . . CF-1.2 MON (p55),
CF-2.2 MON (p59), CG-P.15 THU (p174)
Oguz, Ilker . . . . . . . . . . . . JSIII-1.5 THU (p160),
JSIII-1.6 THU (p162)
Oh, Eon Taek . . . . . . . . . . . . . . EI-1.5 FRI (p186)
Oh, Jung Hyun . . . . . . . . . . CF-9.5 WED (p133)
Ohae, Chiaki . . . . . . . . . . . EF-P.22 WED (p140)
Ohata, Nobuo . . . . . . . . . . . CA-9.5 WED (p132)
Ohishi, Yasukate . . . . . . . . . . . CJ-7.3 FRI (p184)
Ohno, Hiroshi . . . . . . . . . . . CB-P.16 MON (p76)
Ohrt, Alexander . . . . . . . . . . CC-6.2 FRI (p204)
Ohshima, Takeshi . . . . . . . . . CA-5.3 TUE (p96),
EB-11.1 THU (p149)
Ohtsu, Motoichi . . . . . . . . . CE-6.5 THU (p161)
Oi, Daniel K. L. . . . . . . . . . . . . EB-5.5 TUE (p97)
Ojanen, Samu-Pekka . . . . PP-2.3 WED (p120),
CE-P.3 THU (p171)
Okamoto, Takuya . . . . . . . . CF-1.2 MON (p55),∙CF-2.2 MON (p59)
Okamura, Yasuhiro . . . . . . CC-P.11 FRI (p218)
Okano, Makoto . . . . . . . . . . CK-8.2 THU (p142)
Okano, Yasuaki . . . . . . . . . . JSI-2.4 WED (p118)
Okazaki, Daiki . . . . . . . . . . ∙CF-7.5 WED (p119)
Oki, Yuji . . . . . . . . . . . . . . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118), CE-6.5 THU (p161)
Okubo, Ken-ichi . . . . . . . JSIII-2.5 THU (p168)
Okuma, Shinji . . . . . . . . . . . . CB-1.5 MON (p56)
Olaizola, Santiago M. . . . . . CM-6.5 TUE (p96)
Olariu, Tudor . . . . . . . . . . . . . CC-4.5 FRI (p186)
Oliveira, Murilo H. . . . . . EB-11.5 THU (p153)
Oliveira, Taynara . . . . . . . . . ∙CH-3.4 TUE (p86)oliverio, lucas . . . . . . . . . . ∙JSIII-P.10 FRI (p225)
Olivero, Massimo . . . . . . . ∙CL-2.5 THU (p153),∙CH-11.5 THU (p161)
Olivier, Thomas . . . . . . . CH-P.18 WED (p137),
CL-P.15 FRI (p222)
Olivieri, Luana . . . . . . . . . . CH-1.1 MON (p53),
CC-3.5 THU (p169), ED-6.3 FRI (p192)
Olivo, Malini . . . . . . . . . . . . . CL-P.3 FRI (p221),
CL-P.4 FRI (p221)
Ollmann, Zoltán . . . . . . . . . CC-1.5 THU (p155)
Olofsson, Edvin . . . . . . . . JSI-4.3 WED (p130),∙JSI-4.4 WED (p132)
Olyaeefar, Babak . . . . . . . . . . ∙CB-3.3 TUE (p86)
Omatsu, Takashige . . . . . . . CM-4.6 TUE (p88),
CA-4.3 TUE (p84), CA-4.4 TUE (p86),
CJ-5.2 WED (p131), CI-5.4 FRI (p186)
Omoumi, Anahita . . . . . . . ∙CF-1.4 MON (p57)
Oneal, Jordan . . . . . . . . . . . . JSI-4.6 WED (p134)
Ong, George . . . . . . . . . . . CH-P.32 WED (p138)
Ookuma, Shinji . . . . . . . . . CB-P.16 MON (p76)
Oolman, Kathleen . . . . . . . . . EA-1.1 TUE (p83)
Opacak, Nikola . . . . . . . . . . CB-P.4 MON (p75),

Authors' Index∙EF-2.4 WED (p133), CB-8.1 THU (p142),
CB-8.2 THU (p142)
Opatrný, Tomáš . . . . . . . . . EB-7.1 WED (p115)
Oppo, Gian-Luca . . . . . . . . CD-P.9 TUE (p100),
CD-9.6 WED (p126), EF-P.3 WED (p139),∙EA-2.5 THU (p146), EF-6.3 THU (p166),
PD-2.7 THU (p171)
Orain, Mikael . . . . . . . . . . . CE-10.3 FRI (p206)
Ordonez-Miranda, Jose . . JSVI-1.3 TUE (p87),∙JSVI-2.2 TUE (p95)
Orenstein, Gal . . . . . . . . . . . CG-5.4 THU (p161)
Oriekhov, Taras . . . . . . . . . CE-11.1 FRI (p210)
Orlov, Sergej . . . . . . . . . . . . . CM-4.4 TUE (p86),
EC-P.13 FRI (p223)
Ornigotti, Marco . . . . . . . . . . EG-4.4 TUE (p86),
EB-12.1 THU (p157), EC-3.4 FRI (p205)
Orrit, Michel . . . . . . . . . . . . CH-14.1 FRI (p189)
Ortiz, Omar . . . . . . . . . . . . . JSVI-1.1 TUE (p83)
Ortkrass, Henning . . . . ∙CH-P.28 WED (p137)
Ortolani, Michele . . . . . . . . EH-3.4 THU (p152)
Osawa, Shuto . . . . . . . . . . . EB-13.3 THU (p167)
Osellame, Roberto . . . . . . JSII-P.1 MON (p80),
CM-6.3 TUE (p94), EB-6.1 WED (p109),
CK-6.5 WED (p126), CK-7.1 WED (p128),
CG-3.2 THU (p143), EA-8.1 FRI (p200),
CM-11.3 FRI (p214)
Osewski, Paweł . . . . . . . . . . . CE-3.5 MON (p71)
Osipov, Vladimir . . . . . . . . . CA-3.3 MON (p68)
Osnabrugge, Gerwin . . . . . CH-2.3 MON (p60)
Osório, Jonas . . . . . . . . . . . . CJ-4.2 WED (p123)
Ososkov, Yan . . . . . . . . . . . . . . CJ-7.2 FRI (p182)
Ospelkaus, Silke . . . . . . . . . . . EA-7.5 FRI (p196)
Ossiander, Marcus . . . . . ∙CK-11.6 THU (p168)
Ostapenko, Hanna . . . . . ∙CF-7.3 WED (p117),∙CF-7.6 WED (p121)
Osterhoff, Jens . . . . . . . . . . CF-10.1 THU (p143)
Osvay, Károly . . . . . . . . . . . . CF-P.6 TUE (p102),
CA-8.5 WED (p120), CG-4.1 THU (p149),
CG-P.9 THU (p174)
Otero, Eva . . . . . . . . . . . . . ∙EH-P.19 THU (p179)
Otobe, Tomohito . . . . . . . . . CM-5.5 TUE (p91),
EE-P.6 WED (p138)
Otomo, Akira . . . . . . . . . . . . CC-P.11 FRI (p218)
Otsu, Toshio . . . . . . . . . . . . . . CC-P.6 FRI (p218)
Ott, Christian . . . . . . . . . . JSI-1.2 WED (p110),
JSI-5.2 THU (p145)
Ou, Jun-Yu . . . . . . . . . . . . . . EG-2.2 MON (p58),
PP-1.6 MON (p64), CH-6.5 WED (p118),
EH-1.2 WED (p130), CH-P.4 WED (p136),
EH-5.4 THU (p166), CH-12.1 THU (p163),
ED-5.3 FRI (p184)
Ou, Xin . . . . . . . . . . . . . . . . . . . CE-8.1 FRI (p180)
Ouahioune, Nedjma . . . . . CG-5.2 THU (p159)
Oujja, Mohamed . . . . . . . ∙CD-P.21 TUE (p101)
Oulton, Rupert . . . . . . . . . . . EB-2.2 MON (p61)
Oulton, Rupert F. . . . . . . . EB-8.5 WED (p127),
PD-1.9 THU (p170), CD-13.6 FRI (p209)
Oulton, Ruth . . . . . . . . . . . EA-P.20 THU (p175)
Ourjoumtsev, Alexei . . . . . . ∙EA-8.2 FRI (p202)
Ouzit, Zakarya . . . . . . . . . . . CK-12.6 FRI (p186)
Ovcharenko, Yevheniy . . . JSI-P.2 WED (p141)
Ovsianikov, Aleksandr . ∙CM-1.2 MON (p52),
CM-P.17 MON (p78)
Owen-Newns, Dafydd . . ∙JSIII-6.3 FRI (p215)
Oxenløwe , Leif . . . . . . . . . ∙CK-9.1 THU (p148)
Ozawa, Akira . . . . . . . . . . . . ED-1.3 MON (p55),

CK-7.3 WED (p132), ∙PD-2.1 THU (p170)
Ozawa, Tomoki . . . . . . . . . . CK-12.3 FRI (p182)
Ozeki, Yasuyuki . . . . . . . . . CF-6.6 WED (p115),
EA-3.4 THU (p152), JSIII-4.2 FRI (p193)

P
P, Venkatachalam . . . . . . . CE-P.23 THU (p173)
P. Epping, Jörn . . . . . . . . . . CD-14.1 FRI (p211)
P. H. Sidiropoulos, Themistoklis
CD-7.1 WED (p108)
P. Mildren, Richard . . . . . . . . CA-5.2 TUE (p94)
Pablos-Marín, José Miguel ∙EJ-3.1 FRI (p181)
Pache, Lucas . . . . . . . . . . . . . . . EA-1.2 TUE (p83)
Pacheco-Peña, Victor . . . . EG-P.3 TUE (p106),∙EH-1.4 WED (p132)
Pacher, Christoph . . . . . . . EB-6.4 WED (p113)
Paciorek, Karolina . . . . . . . EB-P.3 THU (p176),
EB-P.18 THU (p177)
Paczos, Jerzy . . . . . . . . . . . . . . CI-P.14 FRI (p219)
Padberg, Laura . . . . . . . . . . . EA-4.5 THU (p160)
Padgett, Miles . . . . . . . . . . . . ∙EA-6.1 FRI (p180)
Padilha, Lazaro . . . . . . . . . . CE-7.1 THU (p163)
Padron-Brito, Auxiliadora
EA-2.1 THU (p142)
Pagadala, Karthik . . . . . . . CE-P.26 THU (p173)
Pagliuca, Vincent . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Paipulas, Domas . . . . . . . CM-P.27 MON (p78),
CM-6.2 TUE (p92), CM-8.3 FRI (p182)
Pajer, Viktor . . . . . . . . . . . . . CF-P.6 TUE (p102),
CG-P.3 THU (p173)
Pakhomov, Anton . . . . . . . CK-P.24 TUE (p105)
Pal, Arghadeep . . . . . . . . . ∙CK-8.1 THU (p142)
Pal, N. . . . . . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Pal, Soubhik . . . . . . . . . . . . . . . CJ-P.6 FRI (p220)
Pal, Vishwa . . . . . . . . . . . . . EF-P.12 WED (p140)
Palacios, Alicia . . . . . . . . . . . . EE-3.1 FRI (p189)
Palatnick, Skyler . . . . . . . . . JSII-3.5 MON (p73)
Palau, Anna . . . . . . . . . . . . . CD-7.1 WED (p108)
Palaudoux, J. . . . . . . . . . . . . JSI-4.5 WED (p132)
Paligora, David . . . . . . . . . . EF-2.2 WED (p131)
Palma-Vega, Gonzalo . . . . . ∙CJ-1.3 TUE (p97)
Palmer, Bruce Wayne . . . . CC-3.2 THU (p165)
Palmer, Quinn . . . . . . . . . . EA-3.5 THU (p152)
Palmer, Quinn M B . . . . . . . ∙EJ-2.4 MON (p62)
Palomar Davidson, Noelia
CA-6.3 WED (p110), ∙CE-9.2 FRI (p190)
Palomo, José . . . . . . . . . . . . . EB-6.6 WED (p115)
Palosz, Witold . . . . . . . . . . . . CA-3.1 MON (p66)
Palutke, Steffen . . . . . . . . . . JSI-5.3 THU (p145)
Pammi, V. Anirudh . . . . . . . EF-10.1 FRI (p211)
Pan, Biwei . . . . . . . . . . . . . . CE-P.16 THU (p172)
Pan, Jiahe . . . . . . . . . . . . . . . EG-6.2 WED (p108)
Pan, Zhongben . . . . . . . . . . CA-2.1 MON (p58),
CA-3.2 MON (p68)
Panah-Pour, Ali . . . . . . . . CD-10.2 WED (p130)
Panda, Janmey Jay . . . . . . . ∙EC-P.15 FRI (p223)
Pandit, Himangi J. . . . . . . . . ∙CI-P.6 FRI (p219)
Pang, Meng . . . . . . . . . . . . . . . CD-4.4 TUE (p86),
CD-4.6 TUE (p88)
Panitzek, Dieter . . . . . . . . . . CJ-10.5 FRI (p214)
Panna, Dmitry . . . . . . . . . . EA-5.3 THU (p166),
EF-9.4 FRI (p205)
Pantzas, Konstantinos . . CD-8.4 WED (p118),
EF-4.3 THU (p152), CK-14.6 FRI (p208),

JSIII-6.2 FRI (p213), JSIII-6.5 FRI (p217)
Panzas, Konstantinos . . . . . CD-2.5 MON (p62)
Pápa, Zsuzsanna . . . . . . . . EE-1.6 WED (p115),
EE-P.7 WED (p138), EE-P.12 WED (p139),
EH-2.2 THU (p144), PD-1.2 THU (p170),
CM-9.5 FRI (p196), CM-9.5 FRI (p196)
Papadaki, Helen . . . . . . . . . . CM-9.6 FRI (p196)
Papagelis, Konstantinos . . . EI-P.4 FRI (p224)
Papalazarou, Evangelos . . CF-1.4 MON (p57)
Papamakarios, Savvas . . . CM-1.4 MON (p54),∙CM-11.4 FRI (p214)
Paparella, Michele . . . . . . . . CB-4.1 TUE (p90),∙CB-4.2 TUE (p90)
Paparelle, Iris . . . . . . . . . . . . ∙EB-5.4 TUE (p97)
Paparo, Domenico . . . . . . . CC-2.4 THU (p163)
Papasimakis, Nikitas . . . CH-12.1 THU (p163),
CH-12.6 THU (p169), EJ-4.1 FRI (p189),
EC-P.9 FRI (p223)
Papazoglou, Dimitrios G. CM-3.2 MON (p66)
Papazoglou, Dimitris . . . . . CL-P.18 FRI (p222)
Papazoglou, Dimitris G.CM-P.11 MON (p77),
CM-P.23 MON (p78),
CM-P.31 MON (p78), EC-3.6 FRI (p209)
Pappas, Georgios A. . . . . . CE-5.6 THU (p155)
Parashar, Virendra K. . . . . CM-11.2 FRI (p212)
Pardo, Claudio . . . . . . . . . . . . . EB-5.3 TUE (p95)
Pargon, Erwine . . . . . . . . . . . CD-6.4 TUE (p96)
Parida, Debashis . . . . . . . . . CD-P.6 TUE (p100),
CI-7.6 FRI (p208)
Parigi, Valentina . . . . . . . . EA-3.2 THU (p150),
EB-12.2 THU (p159), EB-13.4 THU (p167),
EB-13.6 THU (p169)
Parihar, Reena . . . . . . . . . . CD-12.3 FRI (p193),∙CD-12.4 FRI (p195), CI-8.6 FRI (p216)
Paris, Matteo . . . . . . . . . . . . . . EB-5.4 TUE (p97)
Park, Byeongchan . . . . . CH-P.21 WED (p137),
CE-P.4 THU (p171)
Park, Byong-Guk . . . . . . . . CF-9.5 WED (p133)
Park, JongCheol . . . . . . . . . . ED-P.1 MON (p79)
Park, Junho . . . . . . . . . . . . ∙EE-P.13 WED (p139)
Park, Kyungdeuk . . . . . . . . EB-P.26 THU (p177)
Park, Mun-Won . . . . . . . . . . . CC-P.4 FRI (p218)
Park, Myeongkee . . . . . . . EE-P.13 WED (p139)
Park, Sang Eon . . . . . . . . . . . ED-P.1 MON (p79)
Park, Sehyun . . . . . . . . . . . . . . EA-1.1 TUE (p83)
Park, Sung Huem . . . . . . . . CC-P.14 FRI (p218)
Park, Tae Gwan . . . . . . . . EE-P.13 WED (p139),∙EI-1.5 FRI (p186)
Park, Young J. . . . . . . . . . . . CK-7.4 WED (p132)
Parke, Harry . . . . . . . . . . . EB-11.5 THU (p153),
EB-P.35 THU (p178)
Parker, Helen E. . . . . . . . . CH-10.2 THU (p151)
Parniak, Michał . . . . . . . . EB-10.2 THU (p143),
EB-10.6 THU (p149), EA-P.21 THU (p175),
EA-6.4 FRI (p186)
Parra-Rivas, Pedro . . . . . . . . EJ-P.5 MON (p80),∙EF-P.5 WED (p139), EF-4.4 THU (p154),
EF-5.5 THU (p160), EF-5.6 THU (p162),
EF-6.4 THU (p166), EF-7.1 FRI (p181),
EF-7.4 FRI (p185), EJ-3.3 FRI (p185)
Parriaux, Alexandre . . . . . CB-8.4 THU (p144),
ED-6.4 FRI (p194)
Parry, Charlotte . . . . . . . . . CD-14.5 FRI (p217)
Parry, Matthew . . . . . . . . . . CD-3.4 MON (p70),
EH-3.6 THU (p154)
Parthasarathy, Shravan Kumar

245∙EB-10.5 THU (p147)
Parthenios, John . . . . . . . . . . . EI-P.4 FRI (p224)
Parvitte, Bertrand . . . . . . . CH-16.5 FRI (p217)
Paschke, Katrin . . . . . . . . . CB-11.5 THU (p168)
Pascual, Inmaculada . . . . CM-P.29 MON (p78)
Pashkin, Alexej . . . . . . . . . . EE-P.3 WED (p138)
Pasiskevicius, Valdas . . . . . CM-1.6 MON (p56)
Pasquazi, Alessia . . . . . . . . CH-1.1 MON (p53),
CC-3.5 THU (p169), ED-6.3 FRI (p192)
Pastier, Florian . . . . . . . . . EB-11.4 THU (p153)
Patchkovski, Serguei . . . . . CG-5.4 THU (p161)
Patchkovskii, Serguei . . . EE-P.14 WED (p139)
Patel, Raj B. . . . . . . . . . . . . . CM-7.5 WED (p112)
Patil, Sanket . . . . . . . . . . . . CH-6.4 WED (p118)
Patsalas, Panagiotis . . . . . . . . EI-1.2 FRI (p182)
Pattathil, Rajeev . . . . . . . . . CA-8.2 WED (p116)
Paul, Pallabi . . . . . . . . . . . CK-P.24 TUE (p105),
EE-P.12 WED (p139), EH-2.5 THU (p148),
PD-1.2 THU (p170)
Paul, Pierre-Mary . . . . . . . . CG-P.3 THU (p173)
Pavel, Nicolaie . . . . . . . . . . . . CA-P.4 MON (p74)
Pavitt, Sue . . . . . . . . . . . . . . . CL-3.5 THU (p161)
Pavlov, Ihor . . . . . . . . . . . . . . CM-2.5 MON (p62)
Pavłov, Krystian . . . . . . . . . . CK-P.9 TUE (p104)
Pavlov, Nikolay . . . . . . . . . . CK-9.4 THU (p152)
Pavlova, Svitlana . . . . . . . . . CM-2.5 MON (p62)
Pavlovic Tucakovic, Natasa∙EB-P.3 THU (p176)
Pavlyuk, Anatoly . . . . . . . . CA-6.4 WED (p112)
Pawlak, Dorota Anna . . . . . CE-3.5 MON (p71)
Pazzagli, Sofia . . . . . . . . . . . CK-7.2 WED (p130)
Peacock, Anna C. . . . . . . . . . CD-6.2 TUE (p92),
CD-7.6 WED (p114)
Pearce, Emma . . . . . . . . . . . ∙EB-2.2 MON (p61),∙EB-8.5 WED (p127), ∙CD-13.6 FRI (p209)
Pearl, Shaul . . . . . . . . . . . . . CD-9.5 WED (p126)
Peccianti, Marco . . . . . . . . CH-1.1 MON (p53),
CC-3.5 THU (p169), ED-6.3 FRI (p192)
Pecile, Vito.F . . . . . . . . . . . . CF-8.3 WED (p125)
Pedretti, Ettore . . . . . . . . . JSII-3.4 MON (p71),
JSII-P.1 MON (p80)
Pedrueza-Villalmanzo, Esteban
EG-4.2 TUE (p84)Peh, Justin Yu Xiang . . . ∙EB-P.11 THU (p176)
Peixoto, Rui . . . . . . . . . . . . . CH-15.1 FRI (p201)
Pejchal, Jan . . . . . . . . . . . . . . . CA-P.7 MON (p74)
Péjot, Clément . . . . . . . . . . . CG-P.4 THU (p173)
Pelekanidis, Antonios . . . CF-P.15 TUE (p103),∙CH-6.1 WED (p114)
PELET, YOANN . . . . . . . . . EB-9.6 WED (p135),∙EB-P.2 THU (p176)
Pelini, Jacopo . . . . . . . . . . . ∙CH-14.2 FRI (p193)
Pellerin, Félix . . . . . . . . . . . . ∙EC-2.4 FRI (p197)
Pelucchi, Emanuele . . . . . . EA-4.4 THU (p160)
Penagos Molina, Daniel S.
CH-6.2 WED (p116),∙CH-P.10 WED (p136)
Penco, Giuseppe . . . . . . . . . JSI-2.5 WED (p118)
Pendry, John B. . . . . . . . . . . EH-1.3 WED (p132)
Penent, F. . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Pentangelo, Ciro . . . . . . . . CK-7.1 WED (p128)
Peralle, Cindy . . . . . . . . . . . EA-3.1 THU (p148),∙CK-15.3 FRI (p212)
Peralta Amores, Albert . . ∙CE-7.2 THU (p167)
Perdana, Nanda . . . . . . . . ∙CK-P.19 TUE (p105)
Perego, Auro . . . . . . . . . . . . EF-3.3 THU (p144),

PD-2.2 THU (p170)
Perego, Auro M. . . . . . . . . CD-P.15 TUE (p100),
CD-P.20 TUE (p101), ED-5.4 FRI (p186)
Perego, Auro Michele . . . ∙CI-1.1 WED (p109),
EF-5.1 THU (p156)
Perenzoni, Matteo . . . . . . . . . EA-6.3 FRI (p186)
Perepelitsa, Galina . . . . . . . EF-10.5 FRI (p215)
Perestjuk, Marko . . . . . . . . CK-4.3 WED (p112)
Pérez, Andrés . . . . . . . . . . . CM-P.29 MON (p78)
Perez de Juan, Emilio . . . . EF-2.1 WED (p129)
Pérez-Escudero, José M. . EH-5.3 THU (p166)
Perez-Leija, Armando . . . EA-P.16 THU (p175)
Pérez Prieto, Lucía . . . . . . CA-6.6 WED (p114)
Pérez-Serrano, Antonio CB-P.15 MON (p76),
CB-7.4 WED (p132)
Pergament, Mikhail . . . . . CA-P.23 MON (p75),
CF-8.5 WED (p127), ∙CE-6.4 THU (p161),
CC-3.3 THU (p167), PD-1.1 THU (p170),
CJ-P.19 FRI (p221)
Perin, Georges . . . . . . . . . . . . CK-3.5 TUE (p96),
CB-10.3 THU (p158)
Periwal, Avikar . . . . . . . . . . . . EA-7.3 FRI (p192)
Perminov, Boris . . . . . . . . . ∙CJ-4.5 WED (p127)
Perner, Lucas. W . . . . . . . . CF-8.3 WED (p125)
Perner, Lukas W. . . . . . . . . . CE-3.2 MON (p67),∙CE-6.1 THU (p157)
Pernice, Wolfram . . . . . . . ∙JSIII-5.1 FRI (p201)
Pernice, Wolfram H. P. . . JSIII-3.5 FRI (p187)
Perosa, Giovanni . . . . . . . . JSI-1.5 WED (p114)
Perrakis, George . . . . . . . . . CM-9.1 FRI (p188)
Perron, Nicolas . . . . . . . . . ∙CI-4.6 WED (p135)
Perrone, Guido . . . . . . . . . . CJ-6.2 THU (p143),
CL-2.5 THU (p153), CH-11.5 THU (p161)
Persano Adorno, Dominique
JSVI-2.5 TUE (p99)
Persheyev, Saydulla . . . . PP-2.11 WED (p121),
EH-4.6 THU (p162), EH-P.1 THU (p178)
Persson, Lars . . . . . . . . . . . . . CB-2.3 MON (p68)
Pertoldi, Andrea . . . . . . . . . ∙CJ-P.22 FRI (p221)
Pertot, Yoann . . . . . . . . . . . . ∙CF-12.3 FRI (p213)
Pertsch, Thomas . . . . . . . . . . EG-5.3 TUE (p94),
CE-4.2 TUE (p93), CK-10.1 THU (p156),
CK-10.2 THU (p158),
CK-10.6 THU (p162),
CK-11.4 THU (p166), EB-P.34 THU (p178),
EA-6.3 FRI (p186), EI-2.2 FRI (p190)
Perumangatt, ChithrabhanuCI-5.3 FRI (p182)
Pervak, Vladimir . . . . . . . . CA-2.3 MON (p60),
CF-6.4 WED (p113)
Peschel, Jasper . . . . . . . . . JSI-4.3 WED (p130),
CG-4.6 THU (p155)
Peschel, Ulf . . . . . . . . . . . . . EH-2.5 THU (p148),
EA-5.6 THU (p168), EA-P.8 THU (p175),
EI-1.3 FRI (p184), EC-3.2 FRI (p203)
Pessoa, Allison R. . . . . . . . CH-P.7 WED (p136),
CE-P.28 THU (p173)
Pessoa Chaves, Bruno . . . EF-P.10 WED (p140)
Petelin, Jaka . . . . . . . . . . . . . . CL-8.6 FRI (p217),
CJ-P.13 FRI (p220)
Peterka, Pavel . . . . . . . . . . . . CJ-9.1 FRI (p200),
CJ-9.5 FRI (p208), CJ-10.6 FRI (p216)
Peters, Luke . . . . . . . . . . . . . CH-1.1 MON (p53),
CC-3.5 THU (p169), ED-6.3 FRI (p192)
Petersen, Christian R. . . . . . . CJ-P.8 FRI (p220)
Petersen, Christian Rosenberg
CH-1.4 MON (p55), CD-P.23 TUE (p101),

Authors' Index∙CJ-7.5 FRI (p186)
Petersen, John . . . . . . . CM-LIM.3 WED (p117)
Petersen, Paige K. . . . . . . . . . CC-7.5 FRI (p214)
Peterson, Paige . . . . . . . . . . CC-3.2 THU (p165)
Petit, Laeticia . . . . . . . . . . . ∙CE-10.1 FRI (p200)
Petit, Stéphane . . . . . . . . . . ∙CL-2.4 THU (p153)
Petit, Yannick . . . . . . . . . . . CE-3.4 MON (p69),
CM-P.14 MON (p77)
Petit-Etienne, Camille . . . . CD-6.4 TUE (p96)
Petkovšek, Rok . . . . . . . . . . . CL-8.6 FRI (p217),
CJ-P.13 FRI (p220)
Petremand, Yves . . . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
Petrik, Péter . . . . . . . . . . . . . EH-2.2 THU (p144)
Petronijevic, Emilija . . . . ∙CE-3.5 MON (p71),
JSVI-2.4 TUE (p97)
Petropoulos, Periklis . . . . CK-P.2 TUE (p104),
CK-6.3 WED (p124), CE-8.6 FRI (p186)
Petrov, Lyuben . . . . . . . . . ∙CA-10.5 THU (p146)
Petrov, Valentin . . . . . . . . . ∙CA-2.1 MON (p58),
CA-P.18 MON (p75), CA-10.3 THU (p144),
CA-10.6 THU (p148)
Petrovic, Jovana . . . . . . . . . . CK-P.1 TUE (p104)
Petrozza, Annamaria . . . . CE-P.10 THU (p172)
Petrulėnas, Augustinas . ∙CD-P.14 TUE (p100)
Petscharnig, Stefan . . . . . . EB-6.4 WED (p113)
Pett, Christian . . . . . . . . . . . . ED-2.4 MON (p61)
Peucheret, Christophe . . . . . CD-4.1 TUE (p82)
Pezzilli, Riccardo . . . . . . . CM-P.18 MON (p78)
Pfaff, Yanik . . . . . . . . . . . . ∙CF-10.6 THU (p149)
Pfaller, Pauline . . . . . . . . . . . . EE-4.2 FRI (p203)
Pfeifer, Hannes . . . . . . . . . . CK-15.5 FRI (p214)
Pfeifer, Thomas . . . . . . . . . . ED-P.5 MON (p79),
JSI-1.2 WED (p110), CF-8.2 WED (p125),
JSI-5.2 THU (p145), CG-6.5 THU (p169)
Pfeiffer, Adrian N. . . . . . . ∙CG-3.3 THU (p145)
Pfeiffer, Tom . . . . . . . . . . . . . . CL-8.1 FRI (p211)
Pfleghar, Christian . . . . . . . CJ-4.1 WED (p123)
Pfuhl, Oliver . . . . . . . . . . . . ∙JSII-2.3 MON (p61)
Pham, Cecil . . . . . . . . . . . . . JSII-1.3 MON (p55)
Phan Huy, Kien . . . . . . . . . . CH-9.4 THU (p147)
Phillips, Chris . . . . . . . . . . . . EB-2.2 MON (p61)
Phillips, Chris C. . . . . . . . . EB-8.5 WED (p127),
CD-13.6 FRI (p209)
Phillips, Christopher . . . . CF-7.1 WED (p115),∙CF-9.1 WED (p129)
Phillips, Christopher R. . . CA-2.5 MON (p62),
CC-2.2 THU (p161)
Phillips, David B. . . . . . . . EG-6.6 WED (p114),
CH-10.2 THU (p151), CL-3.3 THU (p159)
Phillips, Jonathan . . . . . . . CA-8.2 WED (p116)
Phillips, Mark . . . . . . . . . . . . ED-2.1 MON (p59)
Piacentini, Fabrizio . . . . . EB-7.1 WED (p115)
Piacentini, Simone . . . . . . JSII-P.1 MON (p80),
CK-7.1 WED (p128)
Piasecka, Aleksandra . . . . . . CB-3.2 TUE (p84)
Picard, Emmanuel . . . . . . CL-3.1 THU (p157),
CL-3.4 THU (p161)
Piccardo, Marco . . . . . . . . . . CD-6.5 TUE (p96),
EF-2.4 WED (p133), CB-8.1 THU (p142),
EH-5.2 THU (p164)
Piccino, Giuliano . . . . . . . . . CD-6.1 TUE (p92)
Piccioli, Francesco S. . . . PP-2.10 WED (p121),
EC-P.1 FRI (p222)
Picciuto, Rose . . . . . . . . . . . . ∙EE-4.6 FRI (p209)
Picco, Enrico . . . . . . . . . . ∙JSIII-2.6 THU (p168)

Picconi, David . . . . . . . . . . . JSI-5.3 THU (p145),
JSI-5.4 THU (p147)
Pichon, Pierre . . . . . . . . . . . . CE-4.1 TUE (p93),
CE-4.4 TUE (p97), ∙CJ-2.3 WED (p113),
CA-11.3 THU (p150)
Picken, Stephen J. . . . . . . . . . CK-3.1 TUE (p92)
Pickston, Alexander . . . . . EB-9.3 WED (p131)
Pickwell-MacPherson, Emma
CC-7.1 FRI (p210)
Picollo, Federico . . . . . . . . . . CM-4.2 TUE (p82)
Picon, Antonio . . . . . . . . . . JSI-4.1 WED (p128)
Picot, Corentin . . . . . . . . . CG-4.6 THU (p155),∙CG-6.2 THU (p165)
Picqué, Nathalie . . . . . . . . . ED-2.2 MON (p59),
CD-5.1 TUE (p90)
Pidishety, Shankar . . . . . . . . . EC-P.9 FRI (p223)
Pieczarka, Maciej . . . . . . . . . ∙CB-3.2 TUE (p84)
Pieniak, Katarzyna . . . . . . CB-P.12 MON (p76)
Pieplow, Gregor . . . . . . . . EB-12.3 THU (p159),∙EB-P.17 THU (p177)
Pierangeli, Davide . . . . . . . CH-2.5 MON (p62),
EF-10.5 FRI (p215)
Pierre, Christophe . . . . . . CM-P.25 MON (p78)Pierścińska, Dorota . . . . . CB-P.12 MON (p76),∙CB-P.21 MON (p76), CK-P.9 TUE (p104)
Pierściński, Kamil . . . . . ∙CB-P.12 MON (p76),
CB-P.21 MON (p76), CK-P.9 TUE (p104)
Pikhtin, Nikita . . . . . . . . . . . CB-9.5 THU (p152)
Pilat, Florian . . . . . . . . . . . . . CB-P.4 MON (p75),
EF-2.4 WED (p133), CB-8.1 THU (p142),∙CB-8.2 THU (p142)
Pilger, Christian . . . . . . . . . . CL-P.16 FRI (p222)
Pilozzi, Laura . . . . . . . . . . . . . CC-6.4 FRI (p206)
Pincha, Jose . . . . . . . . . . . . . . . . CJ-1.1 TUE (p93)
Pines, Ehud . . . . . . . . . . . . . . . EE-3.3 FRI (p195)
Pingale, Poonam . . . . . . . . . CH-16.4 FRI (p215)
Pini, Marta . . . . . . . . . . . . . . . CF-1.3 MON (p57),∙CF-3.3 MON (p69)
Pinilla, Elena . . . . . . . . . . . EG-6.4 WED (p112)
Pinoteau, Thomas . . . . . . CG-P.16 THU (p174)
Pinske, Julien . . . . . . . . . . . . . . EB-4.2 TUE (p85)
Pinto, Nelson . . . . . . . . . . ∙CK-P.34 TUE (p106)
Pintor, Juan . . . . . . . . . . . . . . CK-12.6 FRI (p186)
Piotrowski, Mikolaj . . . . . . ∙CH-3.3 TUE (p86)
Piotrowski, Piotr . . . . . . . . . CE-3.5 MON (p71)
Piramidowicz, Ryszard . . . . CB-5.2 TUE (p92),∙CK-P.9 TUE (p104), CK-P.23 TUE (p105),
CH-11.6 THU (p163), CE-10.5 FRI (p208)
Pirzio, Federico . . . . . . . . . . CD-6.1 TUE (p92),
CA-10.2 THU (p142)
Pisanello, Ferruccio . . . . . . CH-15.1 FRI (p201)
Pisano, Filippo . . . . . . . . . . ∙CH-15.1 FRI (p201)
Pisanty, Emilio . . . . . . . . . . . . CG-1.5 TUE (p89)
Pisignano, Dario . . . . . . . . . CK-14.2 FRI (p202)
Pissadakis, Stavros . . . . . ∙CE-5.6 THU (p155),
CE-P.7 THU (p171), CH-16.3 FRI (p215)
Pittalis, Stefano . . . . . . . . . . . CG-2.2 TUE (p97)
Pizzurro, Sara . . . . . . . . . . . . . CD-6.1 TUE (p92)
Plach, Marius . . . . . . . . . . . . CG-4.6 THU (p155)
Plaja, Luis . . . . . . . . . . . . . . . . CF-2.1 MON (p59),
CG-1.3 TUE (p87), PD-1.5 THU (p170),
EI-2.3 FRI (p192), EE-3.5 FRI (p197)
Plamadeala, Cristina . . . . . . CM-9.4 FRI (p194)
Plaskocinski, Tomasz . . ∙PP-2.11 WED (p121),
EH-4.6 THU (p162), CL-4.6 THU (p169),∙EH-P.1 THU (p178)

Plekan, O. . . . . . . . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Plekan, Oksana . . . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130), JSI-5.5 THU (p149)
Plosz, Balazs . . . . . . . . . . . . . . CD-5.4 TUE (p91),∙EE-4.5 FRI (p207)
Plotnichenko, Victor . . . . . CA-1.2 MON (p52)
Plotnik, Yonatan . . . . . . . . . . EC-2.1 FRI (p189)
Plum, Eric . . . . . . . . . . . . . . . PP-1.6 MON (p64),
CH-P.4 WED (p136), CH-12.1 THU (p163),
EC-3.5 FRI (p207)
Poborska, Julita . . . . . . . . . . . EC-P.6 FRI (p223)
Pochechuev, M. S. . . . . . . . . . CL-7.1 FRI (p201)
Põder, Kristjan . . . . . . . . . . CF-10.1 THU (p143)
Poderini, Davide . . . . . . . . . . . EB-5.3 TUE (p95)
Podgaetskiy, Konstantin . CB-9.5 THU (p152)
Podivilov, Evgeniy . . . . . . . . CJ-P.17 FRI (p221)
Podoleanu, Adrian . . . . . . CH-1.3 MON (p55),
CL-8.1 FRI (p211)
Podoliak, Nina . . . . . . . . . . . EH-P.7 THU (p178)
Podrazký, Ondřej . . . . . . . . . CJ-P.24 FRI (p221)
Pohl, David . . . . . . . . . . . . . . JSII-2.2 MON (p61)Pohl, Thomas . . . . . . . . . . . . ∙EJ-2.1 MON (p58),
EA-7.1 FRI (p188)
Poizat, Jean-Philippe . . . . . EA-9.2 FRI (p210)
Pokorný, Jan . . . . . . . . . . . . . . . CJ-9.5 FRI (p208)
Pokorny, Morgan R. . . . . . PP-2.8 WED (p121),
CL-5.5 FRI (p187), CL-P.2 FRI (p221)
Połatyński, Andrzej . . . . . . CK-P.9 TUE (p104)
Poletti, Francesco . . . . . . . . CE-2.1 MON (p59),
CE-2.4 MON (p61), CD-6.6 TUE (p98),∙CI-1.3 WED (p111), CH-10.3 THU (p151),
CH-10.4 THU (p153), CJ-9.3 FRI (p204)
Poletto, Luca . . . . . . . . . . . . . CM-6.3 TUE (p94),
JSI-2.5 WED (p118), CF-9.4 WED (p133),
CG-3.2 THU (p143), CG-5.3 THU (p159)
Poli, Federica . . . . . . . . . . . . . CJ-P.14 FRI (p220)
Poli, Iacopo . . . . . . . . . . . . . . JSIII-3.3 FRI (p185)
Policht, Veronica . . . . . . . . . CF-P.9 TUE (p103),
EI-4.4 FRI (p214)
Polino, Emanuele . . . . . . . . . . EB-5.3 TUE (p95)
Politi, Claudia . . . . . . . . . . . . . EA-7.1 FRI (p188)
Polli, Dario . . . . . . . . . . . . . . ED-1.2 MON (p53),
CH-2.1 MON (p58), ED-P.2 MON (p79),
CL-6.1 FRI (p189), CD-13.2 FRI (p203)
Pollmann, René . . . . . . . . . . EA-4.5 THU (p160)
Polman, Albert . . . . . . . ∙JSIV-2.4 WED (p126),
EH-2.3 THU (p144), EH-5.1 THU (p162)
Poloczek, Michael . . . . . . . PD-2.8 THU (p171)
Polónyi, Gyula . . . . . . . . . . CE-P.6 THU (p171),
CC-P.5 FRI (p218), ∙CC-P.13 FRI (p218)
Polynkin, Pavel . . . . . . . . . . CA-1.5 MON (p56),∙CM-3.1 MON (p66), CF-12.4 FRI (p215)
Polyushkin , Dmitry . . . . CH-8.3 WED (p131)
Polzik, Eugene S. . . . . . . . . ∙EB-1.1 MON (p53)
Pomerleau, Antoine . . . . . . . CD-4.5 TUE (p86)
Ponomaryov, Alexey . . . . . CC-P.16 FRI (p218)
Ponosova, Anastasiya . . . EB-P.14 THU (p177)
Pont, Mathias . . . . . . . . . . ∙EB-6.1 WED (p109),
EA-8.1 FRI (p200)
Poon, Joyce . . . . . . . . . . . . . . CL-1.3 MON (p69),∙CK-6.1 WED (p122)
Poon, Joyce K. S. . . . . . . . . . CL-1.2 MON (p69),
CK-13.4 FRI (p194)
Popelova, Dominika . . . . . . CA-P.8 MON (p74)
Popenda, Maciej . . . . . . . . CM-P.25 MON (p78)

246

Popminchev, Tenio . . . . . CA-10.5 THU (p146)
Popmintchev, Dimitar . . . CD-2.2 MON (p58),
PD-1.5 THU (p170)
Popmintchev, Tenio . . . . . CD-2.2 MON (p58),∙PD-1.5 THU (p170), EE-3.5 FRI (p197)
Popoff, Youri . . . . . . . . . . . . . CE-9.1 FRI (p188),
CK-14.5 FRI (p206)
Popov, Evgueni . . . . . . . . . CD-P.10 TUE (p100)
Popov, Victor . . . . . . . . . . . . JSI-P.6 WED (p141)
Popova-Gorelova, Daria . JSI-3.4 WED (p126)
Popp, Alexandra . . . . . . . . . ∙EB-5.6 TUE (p99)
Popp, Jürgen . . . . . . . . . . . . CL-2.1 THU (p149),
CL-8.5 FRI (p215)
Porat, Gil . . . . . . . . . . . . . . . . CF-8.3 WED (p125)
Portalupi, Simone L. . . . . . EA-4.6 THU (p162),
CK-11.5 THU (p168)
Portalupi, Simone Luca . ∙EA-5.1 THU (p162),
EA-P.12 THU (p175)
Porte, Xavier . . . . . . . . . . JSIII-2.4 THU (p166),
JSIII-4.5 FRI (p197), JSIII-6.1 FRI (p211),
JSIII-P.1 FRI (p224), JSIII-P.3 FRI (p224)
Portosi, Vincenza . . . . . . . . . CE-1.5 MON (p57)
Posseckardt, Juliane . . . . . . CE-1.4 MON (p55)
Possmayer, Thomas . . . . . . . ∙EI-P.3 FRI (p224)
Potamianos, Dionysios . . . PD-1.4 THU (p170)
Potashin, S. O. . . . . . . . . . . . . . EA-1.4 TUE (p87)
Poudel, Purushottam . . CK-10.1 THU (p156)
Pouille, Quentin . . . . . . . . CM-P.32 MON (p79)
Poulain, Samuel . . . . . . . . . . CE-1.5 MON (p57),
CJ-P.3 FRI (p220)
Poulton, Christopher G. . CD-12.5 FRI (p197)
Poumellec, Bertrand . . . . . CM-3.5 MON (p70)
Pousa, Roberto G. . . . . . . . . . EB-5.5 TUE (p97)
Powis, Ivan . . . . . . . . . . . . . . JSI-5.5 THU (p149)
Powley, Chris . . . . . . . . . . . . . CM-8.5 FRI (p186)
Prada-Rodrigo, Javier . . . . CM-9.2 FRI (p190)
Pradhan, Monica . . . . . . ∙EH-P.15 THU (p179),∙CI-P.3 FRI (p219)
Pradhan, Somarpita . . . . . ∙CE-2.5 MON (p63)
Prakash, Roopa . . . . . . . . . ∙CJ-5.4 WED (p133),
CJ-5.6 WED (p135)
Prakash, Vindhiya . . . . . . . . ∙EA-1.6 TUE (p89)
Prat, Eduard . . . . . . . . . . . . JSI-1.2 WED (p110),
JSI-4.1 WED (p128)
Prati, Franco . . . . . . . . . . . . . CD-6.5 TUE (p96),
EF-2.4 WED (p133), EF-5.1 THU (p156)
Pratiwi, Arni C. . . . . . . . . . . CE-1.3 MON (p55)
Pravdova, Lenka . . . . . . . . . . ED-P.7 MON (p79)
Prawdziak, Sylvain . . . . . . ∙CG-P.4 THU (p173)
Predojević, Ana . . . . . . . . EB-11.2 THU (p151),
EB-P.24 THU (p177)
Pregnolato, Tommaso . . CK-P.21 TUE (p105),
CK-7.2 WED (p130), EB-12.3 THU (p159)
Prelat, Leila . . . . . . . . . . . . . . ∙CK-2.4 TUE (p88)Prencipe, Alessandro . . . ∙CK-1.2 MON (p66),
CK-1.3 MON (p68), CK-1.5 MON (p70),
CK-P.18 TUE (p105), ∙CE-9.4 FRI (p194)
Presi, Marco . . . . . . . . . . . . . . . CI-7.1 FRI (p200)
Pressacco, Federico . . . . . . JSI-P.4 WED (p141)
Prestopino, Giuseppe . . CM-P.18 MON (p78)
Preu, Sascha . . . . . . . . . . . . . . CC-5.2 FRI (p192)
Preuß, Johann A. . . . . . . . . . . EI-2.5 FRI (p196)
Prieto, Ivan . . . . . . . . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
Primot, Jérome . . . . . . . . . . . CL-4.2 THU (p165)
Prince, K. C. . . . . . . . . . . . . JSI-4.5 WED (p132)

Prince, Kevin C. . . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130)
Prince, Kevin Charles . . . . JSI-5.5 THU (p149)
Prinicpi, Alessandro . . . . . . . EI-3.2 FRI (p204)
Prinz, Maximilian . . . . . . . ∙CE-3.2 MON (p67),
CE-6.1 THU (p157)
Priya, Priya . . . . . . . . . . . . . . JSVI-1.1 TUE (p83)
Priyadarshi, Shekhar . . . . ∙EE-1.4 WED (p113)
Proccopio, Lorenzo . . . . . . EB-3.1 MON (p67)
Prodanov, Aleksander . . . PD-1.5 THU (p170)
Produit, Thomas . . . . . . . . CD-8.1 WED (p114)
Prokop, Nando . . . . . . . . . . . CB-2.3 MON (p68)
Prokopeva, Ludmila J. . . CE-P.26 THU (p173)
Pronin, Oleg . . . . . . . . . . . . . CD-2.1 MON (p58),
CF-5.4 TUE (p97), CD-P.12 TUE (p100),
CD-P.30 TUE (p101), CF-P.17 TUE (p103),
CF-7.4 WED (p119), CF-10.2 THU (p143),
CC-3.6 THU (p169), CL-7.5 FRI (p207)
Protte, Maximilian . . . . . . . . . CI-5.5 FRI (p186)
Provino, Laurent . . . . . . . . . . . CJ-P.2 FRI (p220)
Prucnal, Paul R. . . . . . . . . . JSIII-5.4 FRI (p207)
Prudenzano, Francesco . . CE-1.5 MON (p57),
CE-5.3 THU (p151)
Pruy, Pascal . . . . . . . . . . . . . EA-P.12 THU (p175)
Psaltis, Demetri . . . . . . . JSIII-1.5 THU (p160),
JSIII-1.6 THU (p162), EF-7.2 FRI (p181),
EC-P.8 FRI (p223)
Psilodimitrakopoulos, Sotiris
CD-13.1 FRI (p201), EI-P.4 FRI (p224)
Pu, Minhao . . . . . . . . . . . . . CK-P.35 TUE (p106),
CE-7.1 THU (p163)
Puchegger, Stephan . . . . . . CE-6.1 THU (p157)
Puchhammer, Jakob . . . . CM-P.17 MON (p78)
Pudelko, Jonas . . . . . . . . . . ∙EB-6.4 WED (p113)
Puerto, Daniel . . . . . . . . . ∙CM-P.29 MON (p78)
Pugliese, Diego . . . . . . . . . CA-P.20 MON (p75),
CJ-6.2 THU (p143)
Pugzlys, Audrius . . . . . . . . . CA-1.5 MON (p56),
CD-2.2 MON (p58), CF-9.2 WED (p131),
EF-P.19 WED (p140), CF-11.6 FRI (p209),
CF-12.4 FRI (p215)
Pujol-Closa, Pilar . . . . . . . . ∙EC-3.3 FRI (p205)
Punzel, Eric . . . . . . . . . CM-LIM.4 WED (p119)
Pupeikis, Justinas . . . . . . ∙CF-7.1 WED (p115),
CF-9.1 WED (p129), CC-2.2 THU (p161)
Pupeza, Ioachim . . . . . . . . . CF-P.2 TUE (p102),
CD-7.2 WED (p108), CF-9.6 WED (p135),
CL-2.1 THU (p149), EF-6.1 THU (p162),
EF-6.2 THU (p164), PD-1.4 THU (p170),
CH-13.1 FRI (p181), CL-5.3 FRI (p185)
Puppe, Thomas . . . . . . . . . ∙ED-P.6 MON (p79),
CH-P.35 WED (p138), CC-6.5 FRI (p208)
Pusch, Tobias . . . . . . . . . . . . . CB-2.4 MON (p70)
Püschel, Stefan . . . . . . . . . . CK-P.3 TUE (p104),∙CA-11.1 THU (p148)
Pushkarsky, Michael . . . . . . CD-6.5 TUE (p96)
Puts, Lukas . . . . . . . . . . . . . ∙JSIII-P.7 FRI (p224)
Puttnam, Benjamin . . . . . . CI-4.1 WED (p129)
Pylypenko, Uliana . . . . . . . . . EA-6.4 FRI (p186)
Pyrialakos, Georgios G. . . . EC-P.2 FRI (p223)
Pyrlik, Christoph . . . . . . . CB-10.4 THU (p160)
Pysz, Dariusz . . . . . . . . . . . . CE-5.1 THU (p149),
CJ-9.1 FRI (p200)

Q

Authors' Index

Qasim, Muhammad . . . . . CF-P.16 TUE (p103)
Qian, Jiangrui . . . . . . . . . . . CK-P.22 TUE (p105)
Qiang, Yun Long . . . . . . . . ∙EF-P.9 WED (p139)
Qiao, Jie . . . . . . . . . . . . . . . . ∙CE-11.3 FRI (p214)
Qiao, Tian . . . . . . . . . . . . . . . CF-P.8 TUE (p102),∙CF-P.12 TUE (p103)
Qiu, Zheru . . . . . . . . . . . . . CK-4.2 WED (p110),
EG-6.2 WED (p108), ∙PP-2.2 WED (p120),
CK-9.2 THU (p150), CB-10.1 THU (p156),∙CE-P.2 THU (p171), CE-8.2 FRI (p180),
CK-14.1 FRI (p200), EF-9.2 FRI (p203)
Quanz, Sascha Patrick . . . JSII-2.2 MON (p61)
Quay, Rüdiger . . . . . . . . . . . . . CA-5.3 TUE (p96)
Quentel, Alain . . . . . . . . . . . CK-14.2 FRI (p202)
Quet, Aurélie . . . . . . . . . . CH-P.11 WED (p136)
Quevedo, Hernan . . . . . . . CG-P.13 THU (p174)
Quevedo-Galán, Clara . . CB-P.15 MON (p76),∙CB-7.4 WED (p132)
Quidant, Romain . . . . . . . . . . CL-6.2 FRI (p191)
Quimby, Robert . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Quinn, Liam . . . . . . . . . . . ∙CD-8.5 WED (p120)
Quintero Dominguez, Dario A.
CD-P.34 TUE (p102), EA-3.5 THU (p152)
Quintero-Torres, Rafael . CH-8.6 WED (p135)
Quirce, Ana . . . . . . . . . . . . . CB-P.8 MON (p76),
EB-P.8 THU (p176)
Quiring, Viktor . . . . . . . . . EA-5.5 THU (p168),
CI-5.5 FRI (p186)
Quiroz-Juárez , Mario A. CH-8.6 WED (p135)
Qureshi, Pierce C. . . . . ∙CD-10.3 WED (p130),
CD-10.4 WED (p132)

R
R. Kerridge-Johns, William
CA-4.3 TUE (p84), CA-4.4 TUE (p86)
Raab, Ann-Kathrin . . . . . CF-P.18 TUE (p103),
PD-1.3 THU (p170)
Rachidi, Farhad . . . . . . . . . CD-8.1 WED (p114)
Rácz, Péter . . . . . . . . . . . . . . EE-P.7 WED (p138),
CE-P.6 THU (p171)
Rademacher, Georg . . . . . . CI-4.1 WED (p129)
Rader, Claire . . . . . . . . . . . . CC-1.1 THU (p149),
CC-1.4 THU (p153), CC-3.2 THU (p165),
CC-P.8 FRI (p218)
Radulovic, Marija . . . . . ∙CD-P.34 TUE (p102)
Rafailov, Edik . . . . . . . . . CM-P.31 MON (p78),
CJ-P.3 FRI (p220), CJ-P.9 FRI (p220),
CJ-P.23 FRI (p221)
Raghavan, Srinivasan . . . . . CE-8.3 FRI (p182)
Raghunathan, Varun . . . . . EJ-P.10 MON (p80)
Ragni, Andrea . . . . . . . . . . . . . CL-6.5 FRI (p197)
Rahman, Mujeeb . . . . . . . . . . CL-6.5 FRI (p197)
Rahmani, Mohsen . . . . . . . CD-1.5 MON (p56),
CK-10.5 THU (p160), CD-11.2 FRI (p183)
Raimond, Jean-Michel . . . . . EB-4.5 TUE (p89)
Raimondi, Manuela Teresa
CM-11.3 FRI (p214)
Raineri, Fabrice . . . . . . . . . EB-6.6 WED (p115),
EA-7.4 FRI (p196), EF-8.2 FRI (p193),
EA-8.5 FRI (p208), CK-14.6 FRI (p208),
JSIII-6.2 FRI (p213)
Raj, Manthan . . . . . . . . . . . . CC-P.16 FRI (p218)
Raj, Piyush . . . . . . . . . . . . . . . . CI-8.6 FRI (p216)
Raja, Arslan . . . . . . . . . . . . . . . CK-3.4 TUE (p96)

Raja, Arslan S. . . . . . . . . . . EG-6.2 WED (p108),EF-9.2 FRI (p203)
Rajabali, Shima . . . . . . . . . . EG-3.1 MON (p66),
CC-3.4 THU (p167), CC-5.1 FRI (p188)
Rajala, Patrik . . . . . . . . . . . . . CB-2.2 MON (p66)
Rajalakshmi, G. . . . . . . . . . . EC-P.15 FRI (p223)
Rajeshirke, Yashwant . . . . CH-16.4 FRI (p215)
Rajhans, Supriya . . . . . . . CF-10.1 THU (p143),
EE-4.1 FRI (p201)
Rakic, Mario . . . . . . . . . . . . . . CL-P.5 FRI (p221)
Rakonjac, Jelena V. . . . . . . EB-9.1 WED (p129),
EB-9.4 WED (p133)
Rakovich, Yury . . . . . . . . . . . EG-P.6 TUE (p107)
Ramaz, François . . . . . . . . . CL-2.3 THU (p151)
Ramdane, Abderrahim . . CB-7.3 WED (p130)
Ramesh, Prashant R. . . . ∙CE-P.21 THU (p172)
Ramez, Valentin . . . . . . . . . . CB-5.3 TUE (p94)
Ramirez, Hanz Y. . . . . . . . CE-P.21 THU (p172)
Ramirez, Joan Manel . . . . . . CB-5.3 TUE (p94)
Ramirez, Manuel G. . . . . CM-P.29 MON (p78)
Rammelt, Laura . . . . . . . . . . . CM-6.4 TUE (p96)
Ramos, Carlos . . . . . . . . . . . . EB-3.1 MON (p67)
Rampp, Michael . . . . . . . . CF-10.6 THU (p149)
Randerson, Sam . . . . . . . . . . . . EI-4.2 FRI (p212)
Randoux, Stéphane . . . . . . EF-P.2 WED (p139),
EF-7.6 FRI (p187), EC-2.3 FRI (p195),∙EF-9.5 FRI (p207), EF-9.6 FRI (p209)
Ranella, Anthi . . . . . . . . . . . CM-P.2 MON (p77),
CM-P.3 MON (p77)
RANI, SWETA . . . . . . . . . ∙CE-P.31 THU (p173)
Ranjbar Jahromi, Iman . . . EA-4.4 THU (p160)
Rao, A. Srinivasa . . . . . . . . . ∙CA-4.3 TUE (p84)
Rao, Allam Srinivasa . . . . . CJ-5.2 WED (p131)
Rao, Han . . . . . . . . . . . . . . . ∙CF-P.19 TUE (p103)
Rao, Pavithra . . . . . . . . . . . . ∙CH-3.5 TUE (p88)
Rarity, John G. . . . . . . . . . . . CK-P.7 TUE (p104),
EB-6.5 WED (p113), CE-P.15 THU (p172),
EA-P.20 THU (p175)
Raskatla, Venugopal . . . . . EG-2.2 MON (p58),
EH-1.2 WED (p130), CI-P.6 FRI (p219)
Rasmussen, Mattias . . . . . . . CC-5.5 FRI (p196)
Rastelli, Armando . . . . . . . . . EB-5.3 TUE (p95)
Rates, Alfredo . . . . . . . . . . ∙CH-1.6 MON (p57),∙PP-2.6 WED (p121), ∙CI-P.13 FRI (p219)
Rattunde, Marcel . . . . . . . . CB-2.5 MON (p72),
CA-5.3 TUE (p96)
Rauschenbeutel, Arno . . . . . EA-1.2 TUE (p83),
EA-7.2 FRI (p190)
RAVASIO, Alessandra . . CG-P.14 THU (p174)
Ravet-Senkans, Muriel . . . CG-P.3 THU (p173)
Ravi, Koustuban . . . . . . . . . CC-3.3 THU (p167)
Ravi Kumar, Resmi . . . . . . . . ∙EJ-4.1 FRI (p189)
Ray, Paulami . . . . . . . . . . . . . . ∙CJ-P.3 FRI (p220)
Ray, Tridib . . . . . . . . . . . . . ∙EA-2.3 THU (p144),
EA-7.4 FRI (p196)
Raymond, Arnault . . . . . . . EB-6.6 WED (p115)
Raziman, T. V. . . . . . . . . . . . EG-1.2 MON (p54),
CK-8.4 THU (p144), EF-8.4 FRI (p197),∙CK-14.2 FRI (p202)
Re, Michele . . . . . . . . . . . . . CK-5.2 WED (p116)
Real, Bastián . . . . . . . . . . ∙CK-P.16 TUE (p105),
CK-12.3 FRI (p182)
Reale, Hailey . . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Rebholz, Marc . . . . . . . . . . JSI-1.2 WED (p110),∙JSI-5.2 THU (p145)

Rebollar, Esther . . . . . . . . . . ∙CM-9.2 FRI (p190)
Rebolledo-Salgado, Israel CF-P.7 TUE (p102),∙CI-2.2 WED (p119), ∙ED-6.2 FRI (p190)
Reboud, Vincent . . . . . . . . CK-4.3 WED (p112)
Rech, Ivan . . . . . . . . . . . . . . . CH-9.3 THU (p145)
Reddy, Innem . . . . . . . . . . . . CM-1.5 MON (p56)
Redeker, Kai . . . . . . . . . . . . . . . EB-5.1 TUE (p93)
Redivo Cardoso, Fernando
EB-11.2 THU (p151)
Redka, David . . . . . . . . . . . ∙CM-P.6 MON (p77),
CM-10.5 FRI (p208)
Redmann, Andreas . . . . . ∙PD-1.8 THU (p170)
Redolat, Javier . . . . . . . . . ∙EG-6.4 WED (p112)
Redondo, Javier . . . . . . . . . . EF-5.1 THU (p156)
Reduzzi, Maurizio . . . . . . . CF-1.3 MON (p57),
CF-3.3 MON (p69), CF-9.4 WED (p133),
CG-3.5 THU (p147), EE-3.1 FRI (p189),
EE-3.4 FRI (p197)
Rees, Albert van . . . . . . . . . CD-14.1 FRI (p211)
Regan, David . . . . . . . . . . . . CL-4.1 THU (p163)
Régis, Edouard . . . . . . . . . CH-P.22 WED (p137)
Rego, Laura . . . . . . . . . . . . . JSI-4.6 WED (p134),
EE-P.1 WED (p138)
Rehbock, Christoph . CM-LIM.1 WED (p115)
Rehman, Sobia . . . . . . . . . . . CJ-4.6 WED (p127)
Reich, Stephanie . . . . . . . . . EH-5.6 THU (p168)
Reichel, Volker . . . . . . . . . . . CJ-5.1 WED (p129)
Reichenberger, Sven . CM-LIM.1 WED (p115),
CM-10.3 FRI (p204)
Reid, Derryck . . . . . . . . . . . . CH-4.5 TUE (p98),
ED-6.5 FRI (p196)
Reid, Derryck T. . . . . . . . . . . EJ-P.7 MON (p80),
CH-4.2 TUE (p94), CF-7.3 WED (p117),
CF-7.6 WED (p121), CH-10.4 THU (p153)
Reigue, Antoine . . . . . . . . CD-8.3 WED (p118),
CD-14.2 FRI (p213)
Reimann, Rene . . . . . . . . . . . EB-1.3 MON (p55)
Reinert, Friedrich . . . . . . . JSI-3.4 WED (p126)
Reinhardt, Carsten . . . . . . . . CE-8.4 FRI (p184)
Reislöhner, Jan . . . . . . . . . . CG-3.3 THU (p145)
Reitzenstein, Stephan . . JSIII-2.4 THU (p166),
EB-P.32 THU (p178), JSIII-6.1 FRI (p211)
Rekola, Heikki . . . . . . . . . . . EG-1.4 MON (p56)Remis, Andres . . . . . . . . . . . ∙CB-4.1 TUE (p90),
CB-4.2 TUE (p90)
Ren, Haonan . . . . . . . . . . . . CD-7.6 WED (p114)
Ren, Jinliang . . . . . . . . . . . . . . EG-5.2 TUE (p92)
Ren, Wei . . . . . . . . . . . . . . . . . CH-14.2 FRI (p193)
Renaud, Nicolas . . . . . . . . . CK-P.38 TUE (p106)
Rendón-Barraza, CarolinaPP-1.6 MON (p64),
CH-P.4 WED (p136)
Rennhack, Nils . . . . . . . . . . JSI-P.2 WED (p141)
Rentschler, Christian . . . ∙CC-3.3 THU (p167)
Renz, Franz . . . . . . . . . . . . . . CE-5.4 THU (p153)
Repgen, Paul . . . . . . . . . . . . CF-P.10 TUE (p103)
Resan, Bojan . . . . . . . . . . . CA-11.5 THU (p152)
Resch, Gregory . . . . . . . . . . CL-3.1 THU (p157),
CL-3.4 THU (p161)
Reschke, Felix . . . . . . . . . . . . . CC-5.2 FRI (p192)
Ressel, B. . . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Ressel, Peter . . . . . . . . . . . . CB-11.5 THU (p168)
Restaino, Lorenzo . . . . . . . . . EE-3.2 FRI (p193)
Reuner, Marvin . . . . . . . . . . JSI-3.4 WED (p126)
Reuschel, Philipp . . . . . . . . EB-7.5 WED (p119)
Rezaie, Daniel . . . . . . . . . . CE-P.15 THU (p172)
Ribeiro, Ana Filipa . . . . . ∙CF-7.2 WED (p117),247∙CB-7.1 WED (p128)
Ribeiro, Maria Leonor . . CD-P.18 TUE (p101),∙CL-7.4 FRI (p205)
Ribeiro, Sidney J. L. . . . . . CE-P.28 THU (p173)
Ribeiro, Vitor . . . . . . . . . . CD-P.15 TUE (p100),
CD-P.20 TUE (p101), CI-1.1 WED (p109)
Ribezzo, Domenico . . . . . EB-P.22 THU (p177)
Ribič, P. R. . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Ribič, P. Rebernik . . . . . . . . JSI-4.5 WED (p132)
Ribic, Primoz Rebernik . . JSI-2.5 WED (p118)
Richard, Cyril . . . . . . . . . . . . ED-2.4 MON (p61)
Richard, Cyrille . . . . . . . . . . CE-10.4 FRI (p206)
Richardson, David . . . . . . . . CE-2.1 MON (p59)
Richardson, David J. . . . . . . CD-6.6 TUE (p98),
CH-10.4 THU (p153), CJ-9.3 FRI (p204)
Richter, Daniel . . . . . . . . . . . CM-9.3 FRI (p192)
Richter, Lukas Janos . . . . . ∙CK-P.4 TUE (p104)
Richter , Shachar . . . . . . . . . . . EI-P.5 FRI (p224)
Ricken, Raimund . . . . . . . . EA-5.5 THU (p168)
Rico, María Luisa . . . . . . . CD-P.33 TUE (p102)
Ridente, Enrico . . . . . . . . . . CF-P.16 TUE (p103)
Riedhauser, Annina . . . . . . . CE-9.1 FRI (p188),
CK-14.5 FRI (p206)
Riedl, Thomas . . . . . . . . . . . CA-9.3 WED (p130)
Riegel, Harald . . . . . . . CM-LIM.6 WED (p121)
Riek, Claudius . . . . . . . . . . . CF-9.3 WED (p131)
Rieker, Gregory . . . . . . . . . CH-5.2 WED (p113)
Riemensberger, Johann . . . CB-5.4 TUE (p96),
CK-4.2 WED (p110), EF-2.3 WED (p133),
EF-3.2 THU (p142), CB-10.1 THU (p156),
CE-8.1 FRI (p180), EC-1.2 FRI (p183),
CE-9.1 FRI (p188), CK-14.1 FRI (p200),
CK-14.5 FRI (p206)
Riepl, Josef . . . . . . . . . . . . . . . . EG-4.3 TUE (p86)
Rigneault, Hervé . . . . . . . . CF-6.1 WED (p109),
CH-P.1 WED (p136), CH-10.1 THU (p149),
CH-12.2 THU (p165)
Rigutti, Lorenzo . . . . . . . . . EG-P.5 TUE (p107),
CH-6.6 WED (p120)
Rikers, Marijn . . . . . . . . . . . . ∙CE-4.2 TUE (p93)
Rikimi, Shuichiro . . . . . . CH-10.3 THU (p151)
Riley, Joseph A. . . . . . . . . . . ∙EG-P.3 TUE (p106)
Rimlinger, Matthieu . . . . . . EB-1.3 MON (p55)
Rimoldi, Cristina . . . . . . . ∙CB-6.2 WED (p124)
Risdonne, Valentina . . . . . . . CH-4.5 TUE (p98)
Ristau, Detlev . . . . . . . . . . CD-P.24 TUE (p101),
JSI-P.6 WED (p141), CE-P.24 THU (p173)
Ritcher, Robert . . . . . . . . . . . EE-3.1 FRI (p189)
Ritzkowsky, Felix . . . . . . . . . ∙CF-5.1 TUE (p93)
Rivas, Daniel . . . . . . . . . . . . CG-3.5 THU (p147)
Rivas, Daniel. E . . . . . . . . . . . EE-4.3 FRI (p205)
Rizzo, Lorenzo . . . . . . . . . . CM-P.18 MON (p78)
Robarts, Sebastian C. . . . . . ∙EJ-P.7 MON (p80)
Robb, Gordon R M . . . . . . . EA-2.5 THU (p146)
Robert, Bruno . . . . . . . . . . . CE-5.2 THU (p151)
Robert, Hadrien M.L. . . . . . ∙CL-6.2 FRI (p191)
Robert, Laurent . . . . . . . . JSII-2.5 MON (p63),
JSII-P.3 MON (p80)
Roberti, Giacomo . . . . . . . . . EF-9.5 FRI (p207)
Robertson, Duncan A. . . . EH-4.2 THU (p158)
Robertson, Elizabeth . . ∙EB-10.3 THU (p145),∙JSIII-P.1 FRI (p224)
Robertson, Joshua . . . . . . . JSIII-5.4 FRI (p207),
JSIII-6.3 FRI (p215)
Robertson, Scott . . . . . . . . . PD-2.3 THU (p171)
Robin, Thierry . . . . . . . . . . CJ-5.4 WED (p133),

CJ-5.6 WED (p135), CJ-P.18 FRI (p221)
Robinet, Laurianne . . . . . . . . CH-4.3 TUE (p96)
Robinson, Kenneth . . . . . . CL-3.2 THU (p159)
Robinson, Matthew . . . . . . JSI-5.4 THU (p147)
Roccia, Emanuele . . . . . . . . . . EB-5.3 TUE (p95)
Rocco, Davide . . . . . . . . . . . . EG-2.1 MON (p58)
Rochat, Etienne . . . . . . . . . CH-9.4 THU (p147)
Rochette, Martin . . . . . . . . . . ∙CJ-7.1 FRI (p180)
Rock i Carceller, Carles . EB-P.30 THU (p178)
Rockenstein, Sabine . . . . . CG-3.2 THU (p143)
Rockstuhl, Carsten . . . . . . CK-P.19 TUE (p105)
Rodari, Giovanni . . . . . . . . . ∙EB-5.3 TUE (p95)
Roddaro, Stefano . . . . . . . . JSVI-1.4 TUE (p89)
Rodin, Aleksej . . . . . . . . . . CD-P.14 TUE (p100)
Rodin, Aleksej M. . . . . . . . . CA-P.5 MON (p74),∙CM-P.33 MON (p79)
Rodrigo, José A. . . . . . . . . . . EJ-P.3 MON (p80),
CF-4.1 TUE (p83)
Rodriguez, Ainara . . . . . . . . CM-6.5 TUE (p96)
Rodriguez, Anne . . . . . . . . . JSVI-1.1 TUE (p83)
Rodriguez, Etienne . . . . . . . CH-4.4 TUE (p96)
Rodriguez, Jean-Baptiste . . CB-4.1 TUE (p90),
CB-4.2 TUE (p90)
Rodríguez, Laura . . . . . . . ∙CD-7.5 WED (p112)
Rodriguez, Victor R. . . . . EB-13.4 THU (p167)
Rodriguez-Beltrán, René I.
CM-9.2 FRI (p190)
Rodriguez Cuevas, Alberto∙ED-P.9 MON (p79)
Rodríguez Echarri, Álvaro ∙EG-4.5 TUE (p88)
Rodriguez-Suné, Laura . . EH-3.5 THU (p152)
Roeder, Franz . . . . . . . . . . . ∙EA-4.5 THU (p160)
Roeland, Ganaël . . . . . . . ∙EB-12.2 THU (p159)
Roelkens, Gunther . . . . . . . CD-3.2 MON (p68),
CE-P.16 THU (p172), CK-13.2 FRI (p190)
Roerig, Aljoscha . . . . . . . . . JSI-P.2 WED (p141)
Rogach, Andrey L. . . . . . . . . EG-P.8 TUE (p107)
Rogall, Kevin . . . . . . . . . . . CK-P.19 TUE (p105)
Roger, Thomas . . . . . . . . . . . . ∙CI-5.3 FRI (p182)
Rogge, Sven . . . . . . . . . . . . . . CE-10.2 FRI (p204)
Rohit, . . . . . . . . . . . . . . . . . . ∙CH-15.4 FRI (p207)
Rohrbach, David . . . . . . . . CC-1.2 THU (p151)
Röhrer, Christian . . . . . . . . . . CI-P.5 FRI (p219)
Roider, Clemens . . . . . . . . . CD-13.5 FRI (p207)
Roiz, Mikhail . . . . . . . . . . ∙CH-5.3 WED (p115),
CH-14.3 FRI (p195)
Rojas, Ricardo . . . . . . . . . . CE-P.18 THU (p172)
Rojas-Aedo, Ricardo . . . . . . CF-4.5 TUE (p89),
EF-9.3 FRI (p205)
Roldán, Eugenio . . . . . . . EF-P.17 WED (p140)
Rolland, Antoine . . . . . . . . . ED-3.3 MON (p69)
Romagnoli, Marco . . . . . . . CI-3.4 WED (p127)
Roman, Joris . . . . . . . . . . . . . CA-1.5 MON (p56),∙CF-12.4 FRI (p215)
Román-Cortés, Diego . . ∙CK-P.27 TUE (p105)
Romanelli, Marco . . . . . . . . . EG-4.2 TUE (p84),
CI-2.3 WED (p121), CB-7.5 WED (p132)
Romanet, Maxime . . . . . ∙CH-9.4 THU (p147),
CK-13.1 FRI (p188)
Romano, Clément . . . . . . . . CJ-10.5 FRI (p214)
Romano, Valerio . . . . . . . . . CE-7.4 THU (p169)
Romeira, Bruno . . . . . . . . . CK-13.3 FRI (p192),
JSIII-5.5 FRI (p209), JSIII-P.2 FRI (p224)
Romeo, Michelangelo . . . . . . EI-3.1 FRI (p200)
Romer, Miguel . . . . . . . . . . . . . CF-4.2 TUE (p83)
Romero, Carolina . . . . . . . CA-9.1 WED (p128),

Authors' Index

CA-9.4 WED (p132)
Romero, Rosa . . . . . . . . . . CD-P.18 TUE (p101),
PD-1.3 THU (p170), CL-7.4 FRI (p205)
Rompotis, Dimitrios . . . . . . . EE-4.3 FRI (p205)
Ronchetti, Daniele . . . . . . . ED-1.2 MON (p53)
Roncin, Vincent . . . . . . . . . ∙ED-P.7 MON (p79),
CB-6.4 WED (p126)
Ronco, Giuseppe . . . . . . . . . . EB-5.3 TUE (p95),
EA-4.4 THU (p160)
Rondepierre, Fabien . . . . ∙EG-6.1 WED (p108)
Ronning, Carsten . . . . . . . CK-4.2 WED (p110)
Ronquist, K. Göran . . . . . . . CL-5.4 FRI (p187)
rontani, damien . . . . . . . . JSIII-P.10 FRI (p225)
Rooney, William . . . . . . . . . . CL-7.6 FRI (p209)
Ropagnol, Xavier . . . . . . . . CC-2.4 THU (p163)
Ropers, Claus . . . . . . . . . . . . EG-3.3 MON (p68),∙CG-2.1 TUE (p93), EG-6.2 WED (p108),EG-6.5 WED (p112), CG-3.5 THU (p147),
EF-9.2 FRI (p203)
Rosa, Lorenzo . . . . . . . . . . . CE-2.3 MON (p61)
Rosado, Alejandro . . . . . . . CB-7.4 WED (p132)
Rosales-Garcia, Andrea . . . . CJ-1.1 TUE (p93)
Rosanov, Nikolay . . . . . . . . EE-P.4 WED (p138)
Rosenfeld, Lawrence M . . CK-6.4 WED (p126)
Rosenfeld, Wenjamin . . . . . . EB-5.1 TUE (p93)
Roshanghias, Ali . . . . . . . . CE-5.5 THU (p153),
CL-P.9 FRI (p222)
Rosiek, Christian Anker . . . EC-2.5 FRI (p197)
Rosina, Andrea . . . . . . . . . ∙ED-P.4 MON (p79),
ED-4.1 TUE (p83)
Roskos, Hartmut . . . . . . . . . ∙CC-6.1 FRI (p200)
Rösner, B. . . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Ross, Aaron . . . . . . . . . . . . . . CF-P.9 TUE (p103),
EI-4.4 FRI (p214)
Ross, Calum A. . . . . . . . . . . JSII-3.4 MON (p71)
Ross-Adams, Andrew . . . CM-7.1 WED (p108)
Rossetti, Andrea . . . . . . . . . ∙EG-3.6 MON (p72)
Rossetti, Marco . . . . . . . . . CB-11.6 THU (p168)
Rossi, Giulio . . . . . . . . . . . . . . . CF-5.1 TUE (p93)
Rossi, Giulio M. . . . . . . . . . CD-8.2 WED (p116)
Rossi, Giulio Maria . . . . . . CF-3.4 MON (p71),∙CG-4.3 THU (p151)
Rossnagel, Kai . . . . . . . . . . . JSI-3.4 WED (p126)
Rost, Marcel . . . . . . . . . . . . EA-P.11 THU (p175)
Rostami, Habib . . . . . . . . . . . . EI-2.2 FRI (p190)
Rota, Michele . . . . . . . . . . . . . EB-5.3 TUE (p95),
EA-4.4 THU (p160)
Rotermund, Fabian . . . . . CA-9.1 WED (p128),
CF-9.5 WED (p133), EE-P.13 WED (p139),
EI-1.5 FRI (p186)
Roth, Bernhard . . . . . . . . . . CE-5.4 THU (p153),
CE-8.4 FRI (p184)
Roth, Charlaine . . . . . . . . . . ED-1.1 MON (p53)
Roth, Diane J. . . . . . . . . . . . . EG-2.5 MON (p62)
Roth, Friedrich . . . . . . . . . . JSI-3.4 WED (p126)
Roth, Lynn . . . . . . . . . . . . . . . . CL-P.6 FRI (p221)
Roth, Martin M. . . . . . . . . . JSII-3.4 MON (p71),
JSII-P.1 MON (p80)
Rothhardt, Jan . . . . . . . . . . CH-6.2 WED (p116),
CH-P.10 WED (p136), EE-4.2 FRI (p203),
CJ-10.1 FRI (p210)
Rotter, Stefan . . . . . . . . . . . EG-6.6 WED (p114),∙EC-1.5 FRI (p187), JSIII-4.3 FRI (p195)
Rouan, Daniel . . . . . . . . . . . JSII-1.3 MON (p55)
Roul, Julien . . . . . . . . . . . . . . EF-3.3 THU (p144),
PD-2.2 THU (p170)

Rousseau, Loïc . . . . . . . . . . . CC-7.3 FRI (p212)
Rout, Dipak . . . . . . . . . . . . . . CH-3.5 TUE (p88),
CE-P.23 THU (p173)
Rouvière, Clémentine . . . ∙EB-8.3 WED (p125)
Rouzé, Bastien . . . . . . . . . . . CJ-2.3 WED (p113)
Rouzée, Arnaud . . . . . . . . . JSI-3.1 WED (p122),
EE-3.2 FRI (p193)
Rowe, Jasper . . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Rowley, Maxwell . . . . . . . . . . ED-6.3 FRI (p192)
Roy, Anirban . . . . . . . . . . . ∙CH-16.4 FRI (p215)
Roy, Olivier . . . . . . . . . . . . . . CG-P.3 THU (p173)
Roy, Philippe . . . . . . . . . . . CD-9.1 WED (p122)
Roy, Prithu . . . . . . . . . . . . . . ∙EG-5.5 TUE (p96),∙PP-2.12 WED (p121),∙EH-P.16 THU (p179)
Roy, Sanjib K. . . . . . . . . . . . . . CI-P.3 FRI (p219)
Roy Chowdhury, Dibakar EH-P.8 THU (p178)
Rozzi, Carlo Andrea . . . . . . . CG-2.2 TUE (p97)
Rübeling, Philip . . . . . . . . . . EJ-2.3 MON (p60),∙EB-P.5 THU (p176), EE-5.2 FRI (p211)
Rubinstein, Marcos . . . . . . CD-8.1 WED (p114)
Rubio, Angel . . . . . . . . . . . . . CG-1.2 TUE (p85),
EE-1.3 WED (p111), CG-5.3 THU (p159),
EH-P.10 THU (p179)
Rudenko, Anton . . . . . . . . . CM-3.1 MON (p66)
Rudenkov, Alexander . . . . ∙CA-1.1 MON (p52)
Ruiz de Galarreta, CarlotaCM-P.1 MON (p77)
Rukh, Lala . . . . . . . . . . . . . . . EF-2.1 WED (p129)
Runcorn, Timothy . . . . . . . . CD-4.3 TUE (p84)
Runcorn, Timothy H . . . . . CL-3.2 THU (p159)
Runkel, Manuel . . . . . . . . . CA-9.3 WED (p130)
Rupp, Daniela . . . . . . . . . . ∙JSI-3.1 WED (p122)
Rupp, Marius . . . . . . . . . . . . CA-3.4 MON (p70),∙CA-P.16 MON (p74)
Rus, Bedřich . . . . . . . . . . . . CA-8.3 WED (p118),
CA-8.4 WED (p118)
Rußbüldt, Peter . . . . . . . . . CF-10.4 THU (p145)
Rüsseler, Anna K. . . . . . . ∙CE-P.24 THU (p173)
Russell, Philip . . . . . . . . . . . . CD-4.4 TUE (p86),
CD-12.1 FRI (p189)
Russmann, Christoph . . . . CL-3.6 THU (p163)
Rutkauskas, Marius . . . . . . . CH-4.5 TUE (p98)
Rutkowski, Lucile . . . . . . . . ED-1.2 MON (p53),
ED-2.3 MON (p61), ED-P.2 MON (p79),
ED-P.4 MON (p79), ED-4.1 TUE (p83),∙ED-4.2 TUE (p83)
Rutsch, Matthias . . . . . . . . . PD-1.1 THU (p170)
Rutz, Nadja . . . . . . . . . . . . . . . . CL-6.2 FRI (p191)
Ruzhitskaya, Daria . . . . . . EB-P.14 THU (p177)
Ryabchikov, Yury V. . . . . ∙CM-P.16 MON (p77)
Ryczkowski, Piotr . . . . . . . . CJ-4.4 WED (p125)
Ryf, Roland . . . . . . . . . . . . . . CI-4.2 WED (p131)
Ryger, Ivan . . . . . . . . . . . . . . . ED-3.2 MON (p69)
Ryland, Elizabeth . . . . . . . . . . EE-3.3 FRI (p195)
Rytz, Daniel . . . . . . . . . . . . . . . CE-4.5 TUE (p99)
Ryu, Janghyun . . . . . . . . . . . CF-P.20 TUE (p103)

S
S J, Sreeraj . . . . . . . . . . . . . . . ∙CI-6.1 FRI (p188),∙CI-7.3 FRI (p204), CI-P.10 FRI (p219)
Saadi, Chirine . . . . . . . . . . . ∙CK-15.4 FRI (p214)
Saalfrank, Peter . . . . . . . . . . JSI-5.4 THU (p147)
Saavedra-Becerril, Valeria . EG-4.2 TUE (p84)
Sabatini, Bernardo L . . . . . CH-15.1 FRI (p201)

Sabbah, Mohammad . . . . . . EE-4.5 FRI (p207)
Sabbah, Mohammed . . . . . ∙CD-4.2 TUE (p82),∙EE-4.4 FRI (p205)
Sabzehparvar, Milad . . . . ∙PP-1.13 MON (p65),∙JSIV-P.2 WED (p141)
Sacher, Wesley . . . . . . . . . . . . CL-1.3 MON (p69)
Sacher, Wesley D. . . . . . . . . CL-1.2 MON (p69),
CK-13.4 FRI (p194)
Sader, Lynn . . . . . . . . . . . . ∙CD-9.1 WED (p122),
EF-P.10 WED (p140), CD-13.4 FRI (p205),∙EF-10.4 FRI (p215)
Safaei, Reza . . . . . . . . . . . . . . . CD-4.5 TUE (p86)
Safioui, Jassem . . . . . . . . . . . CM-8.6 FRI (p186)
Sagnes, Isabelle . . . . . . . . . CD-2.5 MON (p62),
JSVI-1.1 TUE (p83), EB-6.1 WED (p109),
CD-8.4 WED (p118), EF-P.12 WED (p140),
EF-4.2 THU (p152), EF-4.3 THU (p152),
CB-10.6 THU (p162), EF-5.2 THU (p158),
EF-8.2 FRI (p193), EA-8.1 FRI (p200),
CK-14.6 FRI (p208), JSIII-6.2 FRI (p213),
JSIII-6.5 FRI (p217)
Sagona-Stophel, Steven EB-10.4 THU (p145),
EB-12.5 THU (p161)
Sahin, Ramazan . . . . . . . . . EH-P.9 THU (p179)
Sahm, Alexander . . . . . . . CB-11.5 THU (p168)
Sahre, Mario . . . . . . . . . . . . . CM-2.1 MON (p58)
Sahu, Jayanta . . . . . . . . . . . . . . CJ-8.4 FRI (p196)
Sahu, Jayanta K. . . . . . . . . . . . CJ-9.4 FRI (p206)
Saini, Than S. . . . . . . . . . . . CD-7.6 WED (p114)
Saini, ThanSingh . . . . . . . . . . CD-6.2 TUE (p92)
Saito, Shinji . . . . . . . . . . . . . ∙CB-1.5 MON (p56),
CB-P.16 MON (p76)
Saito, Yuta . . . . . . . . . . . . . . . . . EI-P.2 FRI (p224)
Saive, Rebecca . . . . . . . . ∙JSIV-2.3 WED (p124)
Sakaguchi, Jun . . . . . . . . . . . CI-4.1 WED (p129)
Sakaino, Kazuki . . . . . . . . . CK-8.2 THU (p142)
Sakaizawa, Daisuke . . . . . . CA-9.5 WED (p132)
Sako, Tokuei . . . . . . . . . . . . . PD-2.4 THU (p171)
Sakoda, Kazuaki . . . . . . . . . CB-1.5 MON (p56),∙CB-P.16 MON (p76),∙CK-P.17 TUE (p105), ∙EC-P.11 FRI (p223)
Sakr, Hesham . . . . . . . . . . . . CE-2.4 MON (p61),
CI-1.3 WED (p111)
Salaj, Jehona . . . . . . . . . . . . . . CH-3.1 TUE (p82)
Saldutti, Marco . . . . . . . . . . EG-1.1 MON (p52),∙CB-10.2 THU (p158)
Saleh, Mohammed F. . . . . . CK-8.5 THU (p146)
Salehi, Elham . . . . . . . . . . . . JSI-2.4 WED (p118)
Salem, Noor . . . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Sales, Tasso Oliveira . . . . . . CL-P.10 FRI (p222)
Salim, Shalina . . . . . . . . . . . EB-P.35 THU (p178)
Salimon, Igor . . . . . . . . . . . CM-P.20 MON (p78)
Salinas, Ignacio . . . . . . . . . CK-P.27 TUE (p105),
CK-P.31 TUE (p106), CK-12.3 FRI (p182)
Sallah Atri, Simon . . . . . . . . . EI-P.5 FRI (p224)
Salman, Sarper . . . . . . . . . . CF-8.3 WED (p125)
Salman, Sarper H. . . . . . . . PD-1.1 THU (p170)
Salmela, Lauri . . . . . . . . . . . . CD-5.3 TUE (p90),
EF-10.2 FRI (p211)
Salmon, Estelle . . . . . . . . . . EH-P.6 THU (p178)
Salter, Patrick . . . . . . . . . . . . CM-2.2 MON (p58)
Salut, Roland . . . . . . . . . . . . JSII-2.5 MON (p63),
JSII-P.3 MON (p80), CE-5.2 THU (p151)
Sam, Rhea T. . . . . . . . . . . . . . ∙ED-5.3 FRI (p184)
Samad, Yarjan . . . . . . . . . . . . . CL-6.5 FRI (p197)

248

Samanta, Goutam Kumar . EC-P.12 FRI (p223)
Samartzis, Nikolaos . . . . . . CH-16.3 FRI (p215)
Samsonas, Danielius . . . . . CM-1.1 MON (p52)
San Román, Julio . . . . . . . . . CF-1.3 MON (p57),
CF-2.1 MON (p59), EE-P.8 WED (p138),
EI-2.3 FRI (p192)
Sanada, Haruki . . . . . . . . . . CF-1.2 MON (p55),
CF-2.2 MON (p59), CG-P.15 THU (p174)
Sanaee, Maryam . . . . . . . . . ∙CL-5.4 FRI (p187),
CE-9.4 FRI (p194)
Sánchez, Luis Alberto . ∙CH-11.3 THU (p159)
Sánchez-Baena, Juan . . . . . . EA-7.1 FRI (p188)
Sánchez-López, María del Mar
CI-5.2 FRI (p180)
Sánchez-Soto, Luis L. . . . . EB-2.1 MON (p59),
EB-7.3 WED (p117)
Sandberg, Elin . . . . . . . . . . . . . CL-5.4 FRI (p187)
Sanders, Charlotte E. . . . . CF-P.22 TUE (p103)
Sandik, Gal . . . . . . . . . . . . . . CK-12.5 FRI (p186)
Sandner, Fabian . . . . . . . . . CG-5.1 THU (p157)
Sándor, Péter . . . . . . . . . . . . EE-1.6 WED (p115),
PD-1.2 THU (p170)
Sandoz, Patrick . . . . . . . . . . CH-2.4 MON (p60)
Sanner, Nicolas . . . . . . . . . . CM-3.4 MON (p68)Sano, Yuki . . . . . . . . . . . . . . . EA-3.4 THU (p152)
Sansavini, Francesca . . . . ∙EA-3.2 THU (p150),
EB-13.6 THU (p169)
Sansone, Giuseppe . . . . . . . JSI-2.5 WED (p118)
Santagata, Rosa . . . . . . . . . . . ED-6.6 FRI (p196)
Santamaría, Enrique . . . . . . CL-1.4 MON (p71)
Santandrea, Matteo . . . . . EB-6.3 WED (p111),
EA-5.5 THU (p168)
Santano Rivero, Desiree . . CL-1.4 MON (p71)
Santarelli, Giorgio . . . . . . CJ-5.4 WED (p133),
CJ-5.6 WED (p135)
Santek, Christopher . . . . . CA-P.12 MON (p74)
Santiago-Cruz, Tomas . . . PD-2.8 THU (p171)
Santos, Alan . . . . . . . . . . . . EB-P.35 THU (p178)
Santos, Elkin . . . . . . . . . . . . EB-8.4 WED (p125)
Santos, Elkin A. . . . . . . . . . ∙EA-5.4 THU (p166)
Santos, José . . . . . . . . . . . . . . . . EE-3.1 FRI (p189)
Santra, Sayantani . . . ∙CM-LIM.3 WED (p117)
Sanzaro, Mirko . . . . . . . . . . . . CI-5.3 FRI (p182)
Sapienza, Riccardo . . . . . . . EG-1.2 MON (p54),
EH-1.3 WED (p132), CK-8.4 THU (p144),
JSIII-4.3 FRI (p195), EF-8.4 FRI (p197),
CK-14.2 FRI (p202), CK-14.3 FRI (p204)
Sapozhnik, Alexey . . . . . . . . CK-3.4 TUE (p96)
Saraceno, Clara . . . . . . . . . . CA-2.2 MON (p60),∙CC-2.1 THU (p157)
Saraceno, Clara J. . . . . . . . PP-2.1 WED (p120),
CF-10.6 THU (p149), CC-3.1 THU (p163),
CC-7.4 FRI (p214), CF-12.2 FRI (p211),
CC-P.1 FRI (p218), CC-P.3 FRI (p218),
CC-P.7 FRI (p218)
Saravi, Sina . . . . . . . . . . . . . . . EG-5.3 TUE (p94),
CK-10.2 THU (p158), EA-5.4 THU (p166),
EA-5.6 THU (p168)
Sarazin, Xavier . . . . . . . . . . PD-2.3 THU (p171)
Sarkadi, Balázs R. . . . . . . . . CC-P.15 FRI (p218)
Sarracini, Antoine . . . . . . JSI-1.2 WED (p110),
JSI-3.2 WED (p124)
Sasaki, Kakeru . . . . . . . . . . . . CM-5.2 TUE (p90)
Sasaki, Toshitaka . . . . . . . . . CJ-P.10 FRI (p220)
Saseendran, Sandeep . . . . CE-P.16 THU (p172)
Sasikumar, Sharath . . . . . . JSI-P.2 WED (p141)

Sathian, Juna . . . . . . . . . . . . . ∙CI-8.5 FRI (p214),
CI-P.2 FRI (p219), CL-P.12 FRI (p222)
Sato, Shunsuke A. . . . . . . . PP-2.4 WED (p120),
CG-5.3 THU (p159), CG-P.1 THU (p173)
Sattari, Hamed . . . . . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
Sättele, Robin . . . . . . . ∙CM-LIM.4 WED (p119)
Sauder, Grégory . . . . . . . . . . EB-2.5 MON (p63),
EB-9.6 WED (p135), EB-P.2 THU (p176)
Sauer, Gregor . . . . . . . . . . ∙EB-11.6 THU (p155),
EB-P.20 THU (p177)
Sauppe, Mario . . . . . . . . . . . JSI-3.1 WED (p122)
Savchenko, Grigorii . . . . . . CB-9.5 THU (p152)
Savitski, Vasili . . . . . . . . . . . CA-1.3 MON (p54),
CA-5.4 TUE (p96)
Savitsky, Ilya . . . . . . . . . . . . . . ∙CF-5.5 TUE (p99)
Savo, Romolo . . . . . . . . . . . . JSIII-4.3 FRI (p195)
Saxena, Dhruv . . . . . . . . . . CK-8.4 THU (p144),
EF-8.4 FRI (p197), CK-14.2 FRI (p202),
CK-14.3 FRI (p204)
Sayers, Ben D. J. . . . . . . . . CD-P.34 TUE (p102)
Sayrin, Clément . . . . . . . . . . . EB-4.5 TUE (p89)
Scalari, Giacomo . . . . . . . . . EG-3.1 MON (p66),
CB-8.5 THU (p146), CB-8.6 THU (p148),
CC-4.1 FRI (p180), CC-4.3 FRI (p182),
CC-4.5 FRI (p186), ∙CH-13.2 FRI (p183),
EC-3.1 FRI (p201)
Scalora, Michael . . . . . . . ∙CD-P.31 TUE (p102),
CD-7.5 WED (p112), EH-3.5 THU (p152),
EH-P.19 THU (p179)
Scarani, Valerio . . . . . . . . . . . . EB-5.1 TUE (p93)
Scazza, Francesco . . . . . . . . . EB-5.4 TUE (p97)
Schacher, Felix H. . . . . . . CK-10.1 THU (p156)
Schaeffer, Christian . . . . . ∙EB-P.6 THU (p176)
Schafer, Kenneth J. . . . . . . JSI-2.5 WED (p118)
Schäffer, Stefan Alaric . . . EA-P.2 THU (p174)
Schanne-Klein, Marie-Claire
CH-4.3 TUE (p96)
Schaper, Lucas . . . . . . . . . . . CA-P.2 MON (p74),∙JSI-2.6 WED (p120)
Scharmer, Selim . . . . . . . . EB-13.2 THU (p165)
Scheel, Stefan . . . . . . . . . . . . . EB-4.2 TUE (p85),
EA-8.4 FRI (p206)
Scheffter, Kilian . . . . . . . . ∙CF-9.3 WED (p131)
Scheiba, Fabian . . . . . . . . . . CF-3.4 MON (p71),
CG-4.3 THU (p151)
Schemmer, Max . . . . . . . . . . . EA-1.2 TUE (p83),
EA-7.2 FRI (p190)
Schepers, Florian . . . . . . . . CF-8.4 WED (p127)
Scheuer, Jacob . . . . . . . . . . CH-7.5 WED (p127)
Scheuer, Sarah . . . . . . . . . . ∙CA-6.2 WED (p108)
Schiellein, Julien . . . . . . . . . CE-5.2 THU (p151)
Schiemangk, Max . . . . . . CB-10.4 THU (p160),
CE-P.9 THU (p172)
Schilder, Nick J. . . . . . . . . . EH-2.3 THU (p144)
Schilt, Stéphane . . . . . . . . . CF-8.3 WED (p125)
Schimmel, Guillaume . . . CD-8.1 WED (p114)
Schleier-Smith, Monika . . ∙EA-7.3 FRI (p192)
Schlich, Hugo . . . . . . . . . . . . CF-P.4 TUE (p102)
Schliwa, Andrei . . . . . . . . . EB-P.12 THU (p177)
Schlosser, Peter . . . . . . . . . . ∙CA-1.3 MON (p54)
Schlottbom, Matthias . . . CK-P.25 TUE (p105),
CK-P.30 TUE (p105), CK-P.38 TUE (p106),
CK-11.2 THU (p164)
Schmauss, Bernhard . . . . . . CC-6.5 FRI (p208)
Schmeltz, Margaux . . . . . . . . CH-4.3 TUE (p96)

Authors' Index

Schmid, Christoph P. . . . . CG-5.1 THU (p157)
Schmid, Fabian . . . . . . . . . . ED-1.3 MON (p55),
PD-2.1 THU (p170)
Schmid, Heinz . . . . . . . . . . . . EF-8.4 FRI (p197),
CK-14.2 FRI (p202)
Schmid, Martina . . . . . . . JSIV-P.3 WED (p141)
Schmid, William . . . . . . . JSIV-1.5 WED (p120)
Schmidt, Marcel . . . . . . . . . EA-5.1 THU (p162)
Schmidt, Markus . . . . . . . . CD-2.3 MON (p60),
CI-4.6 WED (p135)
Schmidt, Markus A. . . . . . EB-P.32 THU (p178)
Schmidt, Michael . . . . . . . . CM-P.6 MON (p77),
CD-13.5 FRI (p207)
Schmidt, Piet O. . . . . . . . . . PP-1.4 MON (p64),
CB-P.2 MON (p75)
Schmidt, Robert . . . . . . . . . . . EI-2.5 FRI (p196)
Schmidt, Tobias . . . . . . . . . . JSII-2.4 MON (p63)
Schmitt, Julian . . . . . . . . . . . PD-1.8 THU (p170)
Schmittner, Christian . . . . . . CJ-1.4 TUE (p97)
Schmoll, Marvin . . . . . . . . . JSI-2.5 WED (p118)
Schmuck, Johannes . . . . . . EF-6.1 THU (p162),
EF-6.2 THU (p164)
Schnabel, Roman . . . . . . . . EA-P.4 THU (p174)
Schneeweiss, Philipp . . . . . . EA-7.2 FRI (p190)
Schneewind, Merle . . . . . ∙CA-P.15 MON (p74)
Schneider, Barbara . . . . . . ∙CB-8.3 THU (p144)
Schneider, Christian . . . EB-11.2 THU (p151),
EA-5.3 THU (p166), EA-P.20 THU (p175),
EB-P.24 THU (p177), EB-P.32 THU (p178),
EI-2.6 FRI (p196), EF-9.4 FRI (p205)
Schneider, Julian . . . . . . . . . CJ-10.5 FRI (p214)
Schneider, Stefan . . . . . . . . CM-2.1 MON (p58)
Schneider, Thomas . . . . CK-P.15 TUE (p104),
CK-7.5 WED (p134), CI-6.5 FRI (p196)
Schneller, Matthias . . . . . . . CF-11.6 FRI (p209)
Schnorr, Kirsten . . . . . . . . JSI-1.2 WED (p110),
JSI-1.4 WED (p112), JSI-3.2 WED (p124),
JSI-4.1 WED (p128)
Schnürer, Matthias . . . . . . CG-3.4 THU (p145)
Schofield, Ross C. . . . . . . . ∙PD-1.9 THU (p170)
Schofield, Zakary . . . . . . EB-10.4 THU (p145),∙EB-P.27 THU (p177)
Schollmeier, Marius . . . . CG-P.13 THU (p174)
Scholz, Markus . . . . . . . . . ∙JSI-3.4 WED (p126)
Schomerus, Henning . . . . . ∙EC-1.4 FRI (p187),∙EC-P.4 FRI (p223)
Schönbeck, Axel . . . . . . . . ∙EA-P.4 THU (p174)
Schönfeld, Christoph . . . . . ∙EE-5.1 FRI (p211)
Schötz, Johannes . . . . . . . . CF-P.16 TUE (p103)
Schreck, Florian . . . . . . . . EA-P.2 THU (p174),
EA-P.9 THU (p175)
Schreiber, Ondřej . . . . . . . . CJ-10.6 FRI (p216)
Schreiber, Siegfried . . . . . . JSI-2.6 WED (p120)
Schreiber, Thomas . . . . . . . . CJ-1.3 TUE (p97),
CJ-1.4 TUE (p97), CJ-2.4 WED (p113),
CJ-6.3 THU (p145), CJ-8.2 FRI (p192)
Schrinner, Philip . . . . . . . . . . CB-5.1 TUE (p92)
Schrödel, Yannick . . . . . . . ∙PD-1.1 THU (p170)
Schröder, Jochen . . . . . . . . CK-1.4 MON (p68),
EF-3.5 THU (p146)
Schröder, Tim . . . . . . . . . . CK-P.21 TUE (p105),
CK-7.2 WED (p130), EB-12.3 THU (p159),
EB-P.17 THU (p177)
Schroeder, Frederik . . . . . CK-15.6 FRI (p216)
Schroeder, Malte C. . . . . . CD-8.1 WED (p114)
Schuchter, Maximilian . . . . CB-2.1 MON (p66)

Schuck, Carsten . . . . . . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118)
Schuck, P. J. . . . . . . . . . . . . . . . . EI-2.1 FRI (p188)
Schuler, Bruno . . . . . . . . . . . EG-3.5 MON (p70)
Schulte, Jan . . . . . . . . . . . . . CF-10.4 THU (p145)
Schultze, Martin . . . . . . . . CK-11.6 THU (p168)
Schulz, Andreas, S. . . . . . . CK-P.33 TUE (p106)
Schulz, Christof . . . . . . . . . . CA-1.2 MON (p52)
Schulz, Sebastian . . . . . . . . . JSI-5.3 THU (p145)
Schulz, Sebastian A. . . . . . EH-4.2 THU (p158)
Schulz, Sebastian Andreas . CH-3.2 TUE (p84)
Schulz, Wolfgang . . . . . . . CM-P.24 MON (p78)
Schumer, Alexander . . . . . . . EC-1.5 FRI (p187)
Schunemann, Peter . . . . . . . . CD-6.3 TUE (p94)
Schunemann, Peter G. . . CD-P.19 TUE (p101)
Schürstedt, Jasmin . . . . . CH-P.28 WED (p137)
Schürstedt, Jasmin C. . . . . . CL-P.16 FRI (p222)
Schuster, Vittoria . . . . . . . CH-6.2 WED (p116)
Schütte, Bernd . . . . . . . . . . JSI-3.1 WED (p122),
CG-4.5 THU (p153), ∙CG-6.4 THU (p169)
Schüttpelz, Mark . . . . . . . . . CL-P.16 FRI (p222)
Schütz, Markus . . . . . . . . . . CB-P.11 MON (p76)
Schwartz, Tal . . . . . . . . . . . . CK-12.5 FRI (p186)
Schwarz, Ariel . . . . . . . . . . . ∙CL-P.14 FRI (p222)
Schwarz, Benedikt . . . . . . . CB-P.4 MON (p75),
CH-3.3 TUE (p86), CD-6.5 TUE (p96),
EF-2.4 WED (p133), ∙CB-8.1 THU (p142),
CB-8.2 THU (p142), CI-5.1 FRI (p180)
Schwarz, Kevin . . . . . . . . ∙CD-P.30 TUE (p101)
Schwarze, Christopher . EB-13.3 THU (p167)
Schwarzenberg, Markus . . CB-9.6 THU (p154)
Schwefel, Harald G. L. . CD-10.3 WED (p130),
CD-10.4 WED (p132)
Schweickert, Lucas . . . . . . . CK-1.2 MON (p66)
Schweikert, Christian . . . CK-11.5 THU (p168)
Schweinberger, Wolfgang
CD-7.2 WED (p108), CF-9.6 WED (p135),
PD-1.4 THU (p170), CH-13.1 FRI (p181)
Schwenke, Tasja . . . . . . . . CE-P.24 THU (p173)
Schwonnek, Rene . . . . . . . . . . EB-5.1 TUE (p93)
Schwuchow, Anka . . . . . . . . CE-1.3 MON (p55),
CE-1.4 MON (p55)
Sciamanna, Marc . . . . . . . CB-7.2 WED (p130),
JSIII-P.10 FRI (p225)
Sciancalepore, Corrado . . CK-5.6 WED (p120)
Sciarrino, Fabio . . . . . . . . . . . EB-5.3 TUE (p95),
EB-6.1 WED (p109), EA-8.1 FRI (p200)
Scirè, Daniele . . . . . . . . . . . . JSVI-2.5 TUE (p99)
SCOL, Florent . . . . . . . . . . . CA-7.3 WED (p126)
Scotognella, Francesco . . . CF-P.9 TUE (p103),
EI-4.4 FRI (p214)
Scott, Nic J. . . . . . . . . . . . . . . JSII-3.4 MON (p71)
Scotti, Filippo . . . . . . . . . . . . . CI-7.1 FRI (p200)
Scully, Marlan . . . . . . . . . . . . . CL-7.6 FRI (p209)
Scutelnic, Valeriu . . . . . . . CG-P.13 THU (p174)
Sdobnov, Anton . . . . . . . . . CL-1.5 MON (p73),∙CL-4.3 THU (p167), EJ-4.2 FRI (p191)
Sebastião, Hugo . . . . . . . . . CD-P.18 TUE (p101)
Sebek, Matej . . . . . . . . . . . . . CC-1.3 THU (p153)
Secareanu, Radu-Costin . . . EE-4.3 FRI (p205)
Secondo, Ray . . . . . . . . . . . . CE-7.1 THU (p163)
Sedaghat, Setareh . . . . . ∙JSIV-P.3 WED (p141)
Sedaghat, Zohreh . . . . . . . . . CL-P.15 FRI (p222)
Sedao, Xxx . . . . . . . . . . . . ∙CM-P.15 MON (p77),
CH-P.18 WED (p137)
Sedov, Egor . . . . . . . . . . . . . . . ∙CI-P.7 FRI (p219)

See, Tian Long . . . . . . . . . . . . CM-8.5 FRI (p186)
Seegert, Kristian . . . . . . . . . EG-1.1 MON (p52),∙CB-1.3 MON (p54)
Seer, Ali . . . . . . . . . . . . . . . . . ED-3.4 MON (p71),
ED-P.6 MON (p79)
Sefidmooye Azar, Nima . ∙EH-3.6 THU (p154)
Segarra-Martì, Javier . . . . . . EE-3.4 FRI (p197)
Segev, Mordechai . . . . . . . . EC-2.1 FRI (p189),
EC-P.3 FRI (p223)
Seguin, Johanne . . . . . . . . . . CL-2.3 THU (p151)
Segundo, V.W. . . . . . . . . . . . . CF-1.3 MON (p57)
Segura, Martha . . . . . . . . ∙CA-P.20 MON (p75),
CJ-6.2 THU (p143)
Seidel, Marcus . . . . . . . . . . JSI-P.3 WED (p141),
JSI-P.4 WED (p141), CJ-P.19 FRI (p221)
Seidel, Thomas . . . . . . . . . . ∙EJ-1.3 MON (p56),∙CB-P.7 MON (p76), ∙EF-5.2 THU (p158),
EF-6.5 THU (p168)
Seidel, Thomas G. . . . . . . . . EJ-P.2 MON (p79),
EJ-P.8 MON (p80)
Seidl, Angelika . . . . . . . . . . . EE-P.3 WED (p138)
Seidler, Paul . . . . . . . . . . . . . EF-2.3 WED (p133),
CE-9.1 FRI (p188), CK-14.5 FRI (p206)
Seifert, Birger . . . . . . . . . . . . ∙CF-4.5 TUE (p89),
CE-P.18 THU (p172)
Seifert, Paul . . . . . . . . . . . . . . . EI-3.2 FRI (p204),
EI-3.3 FRI (p204)
Seitz, Marc . . . . . . . . . . . . . . ∙PP-1.5 MON (p64),∙CD-P.2 TUE (p100)
Şeker, Enes . . . . . . . . . . . . . . . . CB-3.3 TUE (p86)
Selig, Malte . . . . . . . . . . . . . . . . EI-4.4 FRI (p214)
Sellars, Matthew J. . . . . . . . CE-10.2 FRI (p204)
Selvaraja, Shankar Kumar CH-3.5 TUE (p88),
CK-P.14 TUE (p104), CE-P.23 THU (p173),
CE-P.25 THU (p173), CE-8.3 FRI (p182)
Semenova, Elizaveta . . . . . EG-1.1 MON (p52),
CK-15.6 FRI (p216)
Semmen, Kara . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)Sen, Arnab . . . . . . . . . . . . . . . . EE-3.2 FRI (p193)
Sen, Dipankar . . . . . . . . . . . . . CL-7.6 FRI (p209)
Sen, Raja . . . . . . . . . . . . . . . . . JSVI-2.3 TUE (p97)Şenel, Çağrı . . . . . . . . . . . . . CF-P.10 TUE (p103)
Senellart, Jean . . . . . . . . . . . EB-6.1 WED (p109)
Senellart, Pascale . . . . . . . EB-6.1 WED (p109),
EB-11.4 THU (p153), EA-8.1 FRI (p200)
Senfftleben, Bjoern . . . . . . JSI-P.2 WED (p141)
Senfftleben, Björn . . . . . . . JSI-3.1 WED (p122)
Şengül, Serdar . . . . . . . . . . . . . CB-3.3 TUE (p86)
Senica, Urban . . . . . . . . . . . . CC-4.1 FRI (p180),
CC-4.3 FRI (p182), ∙CC-4.5 FRI (p186),
EC-3.1 FRI (p201)
Seo, Hong-Seok . . . . . . . . CA-11.4 THU (p152)
Seo, Meoung Ho . . . . . . . . . . ED-P.1 MON (p79)
Seo, Sangwon . . . . . . . . . . . . . ED-P.1 MON (p79)
Seo, Young-Seok . . . . . . . . . CL-P.17 FRI (p222)
Sercel, Greg . . . . . . . . . . . . . . JSII-1.4 MON (p57)
Seres, Imre . . . . . . . . . . . . . . . CF-P.6 TUE (p102),∙CF-P.21 TUE (p103), CA-8.5 WED (p120),∙CG-4.1 THU (p149)
Serge-Correales, York E. CE-P.28 THU (p173)
Sergeev, Aleksandr A. . . . . EG-P.8 TUE (p107)
Sergeeva, Kseniia A. . . . . . EG-P.8 TUE (p107)
Sergeyev, Sergey . . . . . . . . . ED-P.9 MON (p79),
EF-P.18 WED (p140)
Sergienko, Alexander . . ∙EB-13.3 THU (p167)

249

Serna, Samuel . . . . . . . . . . . . CD-3.5 MON (p72)
Serra, João . . . . . . . . . . . . . . EH-1.1 WED (p128)
Serrano, Diana . . . . . . . . . . . . EG-5.1 TUE (p92)
Serrano, Esteban . . . . . . . . . . ∙CJ-7.3 FRI (p184)
Serrano, Javier . . . . . . . . . . . CF-1.3 MON (p57),
EE-P.8 WED (p138), EJ-3.1 FRI (p181),
EI-2.3 FRI (p192), EE-3.5 FRI (p197)
Set, Sze Yun . . . . . . . . . . . . . . . CL-6.5 FRI (p197)
Settembrini, Francesca Fabiana
CD-3.3 MON (p68)
Setzpfandt, Frank . . . . . . . . . EG-5.3 TUE (p94),
CK-P.24 TUE (p105), EB-8.4 WED (p125),
CK-10.2 THU (p158), EA-5.4 THU (p166),
EA-5.6 THU (p168), EB-P.34 THU (p178),
EA-6.3 FRI (p186)
Severino, Stefano . . . . . . . CF-9.4 WED (p133),
CG-3.5 THU (p147)
Sevillano, Pascual . . . . . . . . . . CI-6.6 FRI (p196)
Shadrivov, Ilya . . . . . . . . . EH-4.4 THU (p160),
EH-P.3 THU (p178)
Shadymov, Vladimir . . . . . . . CB-5.4 TUE (p96)
Shafarevich, Yulia . . . . . . . . . EJ-P.9 MON (p80)
Shah, Ronak . . . . . . . . . . . . . JSI-2.5 WED (p118)
Shahriar, Selim . . . . . . . . . . CH-7.5 WED (p127)
Shalaby, Mostafa . . . . . . . . . . CC-P.3 FRI (p218)
Shalloo, Rob . . . . . . . . . . . . CF-10.1 THU (p143)
Shamailov, Sophie . . . . . . . CD-9.3 WED (p124)
Shamohammadi, Mehran CH-13.2 FRI (p183)
Shams-Ansari, Amirhassan
CD-3.3 MON (p68), CC-5.1 FRI (p188)
Shan, Hangyong . . . . . . . . . . . EI-2.6 FRI (p196)
Shao, Y. . . . . . . . . . . . . . . . . . . . . EI-2.1 FRI (p188)
Shardlow, Peter C. . . . . . . . CA-7.2 WED (p126)
Sharma, Ashutosh . . . . . . . CC-1.5 THU (p155),
CC-P.2 FRI (p218)
Sharma, Nityanand . . . . . . CH-7.2 WED (p123)
Sharma, Sakshi . . . . . . . . . . . EB-2.4 MON (p63),
EB-12.6 THU (p163), EB-P.10 THU (p176),
EB-P.19 THU (p177)
Sharma, Sangeeta . . . . . . . . ∙CG-1.1 TUE (p83),
CG-3.5 THU (p147)
Sharma, Shubhanshi . . . . EH-P.15 THU (p179)
Sharma, Sudhir . . . . . . . . . . . EC-P.12 FRI (p223)
Sharma, Tarun K. . . . . . . . . JSII-3.4 MON (p71)
Sharp, Christina . . . . . . . ∙EG-6.6 WED (p114),∙CL-3.3 THU (p159)
Shastri, Bhavin . . . . . . . . . . JSIII-5.4 FRI (p207)
Shayeganrad, Gholamreza CM-4.3 TUE (p84)
Shaykin, Andrey . . . . . . . . CG-P.12 THU (p174)
Shcherbakov, Maxim . . . . . CD-11.5 FRI (p187)
Sheil, Brian . . . . . . . . . . . . . . . ED-5.4 FRI (p186)
Shekhawat, Vijay . . . . . . . . . CD-2.6 MON (p62)
Shelwade, Sneha . . . . . . . . CK-P.14 TUE (p104)
Shemer, Amir . . . . . . . . . . . . CL-P.14 FRI (p222)
Shen, Fengjiao . . . . . . . . CH-P.36 WED (p138)
Shen, Li . . . . . . . . . . . . . . . . . . CD-6.2 TUE (p92),
CD-7.6 WED (p114)
Shen, Lijiong . . . . . . . . . . . ∙EB-P.4 THU (p176),
EB-P.11 THU (p176)
Shen, Yijie . . . . . . . . . . . . . CH-12.6 THU (p169),
EC-P.9 FRI (p223)
Shen, Zexiang . . . . . . . . . . . . PP-1.7 MON (p64),
CH-P.8 WED (p136)
Shestaev, Evgeny . . . . . . . . CF-P.21 TUE (p103),
CL-8.5 FRI (p215)
Shi, BoCE-5.3 THU (p151), CI-8.1 FRI (p210)

Shi, Haolian . . . . . . . . . . . . ∙CC-P.10 FRI (p218)
Shi, Jiawei . . . . . . . . . . . . . . . . EF-5.4 THU (p160)
Shi, Lei . . . . . . . . . . . . . . . . . . . CL-1.4 MON (p71)
Shi, Minji . . . . . . . . . . . . . ∙CD-P.15 TUE (p100),∙CD-P.20 TUE (p101), CI-1.1 WED (p109)
Shi, Yihuan . . . . . . . . . . . . . ∙CJ-3.2 WED (p117)
Shi, Yiwen . . . . . . . . . . . . . . . . ∙CJ-P.8 FRI (p220)
Shidlovski, Vladimir . . . . . . CL-8.1 FRI (p211)
Shields, Andrew . . . . . . . . . . . CI-5.3 FRI (p182)
Shih, Wei-Chuan . . . . . . ∙CH-12.5 THU (p169)
Shiloh, Roy . . . . . . . . . . . . . . EA-4.2 THU (p158),∙PD-1.7 THU (p170)
Shim, Je-Ho . . . . . . . . . . . . . CF-9.5 WED (p133)
Shimomura, Suguru . . . ∙JSIII-2.5 THU (p168)
Shin, Dong-Chel . . . . . . . . . . CC-5.3 FRI (p194)
Shin, Jonghwa . . . . . . . . . . . CK-P.10 TUE (p104)
Shin, Seong Sik . . . . . . . . . EE-P.13 WED (p139)
Shinbrough, Kai . . . . . . . . . . ∙EA-1.1 TUE (p83)
Shinde, Saniya . . . . . . . . . . . . . EG-5.3 TUE (p94)
Shinohara, Yasushi . . . . . . . CF-1.2 MON (p55),
CF-2.2 MON (p59), CM-5.2 TUE (p90),∙CG-P.15 THU (p174)
Shiomi, Junichiro . . . . . . . ∙JSVI-2.1 TUE (p93)
Shiposh, Yulija . . . . . . . . . . EF-P.23 WED (p141)
Shiraki, Ryuta . . . . . . . . . . . . . . CI-6.4 FRI (p194)
Shiri, Arash . . . . . . . . . . . . . . EC-P.12 FRI (p223)
Shitov, Vladislav . . . . . . . . . CA-3.3 MON (p68)
Shivayogimath, Abhay . . . CC-1.3 THU (p153)
Shradha, Sai . . . . . . . . . . . . . . . EG-5.3 TUE (p94)
Shribak, Michael . . . . . . . . CH-7.4 WED (p125)
Shumakova, Valentina . . . EG-P.2 TUE (p106),
CF-8.3 WED (p125), CF-9.2 WED (p131)
Shutts, Samuel . . . . . . . . . . . . . CB-4.5 TUE (p91)
Sibilia, Concita . . . . . . . . . . CE-3.5 MON (p71),
JSVI-2.4 TUE (p97), JSVI-2.5 TUE (p99)
Siciliani de Cumis, Mario CH-14.2 FRI (p193)
Siddharth, Anat . . . . . . . . . . . CB-5.4 TUE (p96),∙CB-10.1 THU (p156), CK-14.5 FRI (p206)
Sidiropoulos, Themistoklis
CG-3.5 THU (p147)
Siegel, Jan . . . . . . . . . . . . . . ∙CM-P.1 MON (p77),
CM-4.5 TUE (p86)
Siegrist, Florian . . . . . . . . CD-7.3 WED (p110),
CH-P.19 WED (p137)
Siems, Malte P . . . . . . . . . . . . CM-9.3 FRI (p192)
Siems, Malte Per . . . . . . . . . CD-2.3 MON (p60)
Sierant , Aleksandra . . . . . . . EA-1.6 TUE (p89)
Sieryi, Oleksii . . . . . . . . . . . CL-1.5 MON (p73),
CL-4.4 THU (p167), CL-6.4 FRI (p197)
Sigalotti, Paolo . . . . . . . . . . JSI-P.7 WED (p141)
Sigg, Hans . . . . . . . . . . . . . . CC-1.2 THU (p151)
Sigmund, Ole . . . . . . . . . . . . EG-P.9 TUE (p107),
CK-15.6 FRI (p216)
Silander, Isak . . . . . . . . . . . . ED-2.4 MON (p61),
ED-P.4 MON (p79), ED-4.1 TUE (p83)
Silberhorn, Christine . . . . EB-6.3 WED (p111),
EA-4.5 THU (p160), EA-5.5 THU (p168),
CI-5.5 FRI (p186)
Silies, Martin . . . . . . . . . . . . . . EI-2.6 FRI (p196)
Siliprandi, Jacopo . . . . . . . JSII-3.4 MON (p71)
Sillard, Pierre . . . . . . . . . . . . . CD-4.1 TUE (p82)
Silletti, Laura . . . . . . . . . . . . PP-1.5 MON (p64),
CD-P.2 TUE (p100), ∙EE-4.1 FRI (p201)
Silva, Camila Beli Silva . . . EA-P.2 THU (p174)
Silva, Duarte . . . . . . . . . . . JSIII-P.14 FRI (p225)
Silva, Fernando . . . . . . . . EF-P.17 WED (p140)

Authors' Index

Silva, Nuno . . . . . . . . . . . . ∙JSIII-P.14 FRI (p225)
Silva de Oliveira, ViniciusED-P.4 MON (p79),∙ED-4.1 TUE (p83)
Silva-Toledo, Miguel A. . . CF-3.4 MON (p71),
CG-4.3 THU (p151)
Silveirinha, Mário . . . . . . ∙EH-1.1 WED (p128)
Silverstone, Josh W. . . . . . . EA-3.5 THU (p152)
Silverstone, Joshua W . . . . . EJ-2.4 MON (p62),
CD-P.34 TUE (p102), CK-6.4 WED (p126)
Silvestre, Enrique . . . . . . . CD-P.22 TUE (p101)
Simkhovich, Arie . . . . . . . . CK-12.5 FRI (p186)
Simon, Corentin . . . . . . . ∙CF-P.14 TUE (p103),
EF-2.5 WED (p135)
Simon, Daniel . . . . . . . . . . . . CL-3.2 THU (p159)
Simon, David . . . . . . . . . . . EB-13.3 THU (p167)
Simon, Jeffrey . . . . . . . . . . CE-P.26 THU (p173)
Simoncig, A. . . . . . . . . . . . JSI-3.5 WED (p126),
JSI-4.5 WED (p132)
Simoncig, Alberto . . . . . . . JSI-2.5 WED (p118)
Simonot, Damien . . . . . . . . . ∙EJ-1.4 MON (p56)
Simpson, Emma Rose . . . . JSI-2.5 WED (p118)
Simpson, M. Cather . . . . . PP-2.8 WED (p121),
CL-5.5 FRI (p187), CL-P.2 FRI (p221)
Simsek, Ergun . . . . . . . . . . ∙ED-P.8 MON (p79),∙EJ-4.5 FRI (p197)
Sinclair, Laura C. . . . . . . . . ∙ED-3.1 MON (p67)
Sinelnik, Artem . . . . . . . . . . . . EI-2.2 FRI (p190)
Siñeriz-Niembro, Nuria . . . CE-1.4 MON (p55)Singer, Kilian . . . . . . . . . . EA-P.18 THU (p175),
EA-9.6 FRI (p216)
Singh, Alok . . . . . . . . . . . . EA-P.10 THU (p175)
Singh, Arshdeep . . . . . . . . . . . CI-P.8 FRI (p219)
Singh, Dinesh P. . . . . . . . . CE-P.18 THU (p172)
Singh, Karamdeep . . . . . . . . CI-P.10 FRI (p219)
Singh, Karanveer . . . . . . . CK-P.15 TUE (p104),
CK-7.5 WED (p134), CI-6.5 FRI (p196)
Singh, Neetesh . . . . . . . . . . . CK-P.8 TUE (p104),
CK-4.4 WED (p112), ∙CA-9.6 WED (p134),∙PD-1.6 THU (p170)
Singh, Ravinder . . . . . . . . . . . . CI-5.3 FRI (p182)
Singh, Vikram . . . . . . . . . . . . EG-P.4 TUE (p107)
Singh, Yeshpal . . . . . . . . . . EA-P.10 THU (p175),
EA-P.14 THU (p175)
Singleton, Matthew . . . . . ∙CE-6.2 THU (p159)
Sinkus, Vytautas . . . . . . . . . . CF-11.2 FRI (p203)
Sinobad, Milan . . . . . . . . . ∙CK-P.8 TUE (p104),
CK-4.3 WED (p112), CK-4.4 WED (p112),
CA-9.6 WED (p134), PD-1.6 THU (p170)
Sinquin, Brian . . . . . . . . . . ∙CI-2.3 WED (p121),∙CB-7.5 WED (p132)
Sirbu, Dumitru . . . . . . . . . . . CE-1.1 MON (p53)
Sirotin, Maxim . . . . . . . . . . ∙EA-4.2 THU (p158)
SIRTORI, Carlo . . . . . . . . . JSII-1.5 MON (p57),
CH-4.4 TUE (p96)
Sirutkaitis, Romualdas . . . . CM-6.2 TUE (p92)
Sirutkaitis, Valdas . . . . . . . . CM-6.2 TUE (p92),
CM-8.3 FRI (p182)
Sittig, Robert . . . . . . . . . . CK-11.5 THU (p168),
EA-P.12 THU (p175)
Sivankutty, Siddharth . . ∙CH-P.1 WED (p136),∙CH-10.1 THU (p149)
Sjakste, Jelena . . . . . . . . . . . ∙JSVI-2.3 TUE (p97)
Skalli, Anas . . . . . . . . . . . ∙JSIII-2.4 THU (p166),
JSIII-5.3 FRI (p205), JSIII-6.1 FRI (p211),
JSIII-P.1 FRI (p224), JSIII-P.3 FRI (p224)
Skasyrsky, Yan . . . . . . . . . . . . CA-1.2 MON (p52)Skënderas, Martin . . . . . ∙CB-P.13 MON (p76),∙EF-P.14 WED (p140)
Skenderović, Hrvoje . . . . . . EA-6.2 FRI (p184),∙CL-P.5 FRI (p221)
Skliutas, Edvinas . . . . . . . . . CM-1.1 MON (p52)
Skogen, Erik . . . . . . . . . . . . . . . CB-5.6 TUE (p98)
Skrepetos, Stavros . . . . . . . ∙CM-P.3 MON (p77)
Skubich, Jules . . . . . . . . . . CH-P.22 WED (p137)
Skupin, Stefan . . . . . . . . . . . . ∙EE-2.1 FRI (p181)
Sladek, Juraj . . . . . . . . . . . . . . CM-5.4 TUE (p91),
CM-9.6 FRI (p196)
Slavik, Radan . . . . . . . . . . . . CE-2.4 MON (p61),
CI-8.1 FRI (p210)
Slemp, Michalina . . . . . . . ∙EH-P.6 THU (p178)
Slenders, Eli . . . . . . . . . . . . ∙CH-6.4 WED (p118)
Slimi, Sami . . . . . . . . . . . . . CA-P.19 MON (p75),
CJ-6.2 THU (p143)
Slipchenko, Sergey . . . . . . . CB-9.5 THU (p152)
Slodička, Lukáš . . . . . . . . . . EA-P.7 THU (p175)
Słowikowski, Mateusz . . . CK-P.9 TUE (p104),
CK-P.23 TUE (p105), CH-11.6 THU (p163)
Smajic, Jasmin . . . . . . . . . . . CI-3.1 WED (p123)
Smarzyk, Sebastian . . . . . . JSII-P.1 MON (p80)
Smeets, Stef . . . . . . . . . . . . . CK-P.38 TUE (p106)
Smektala, Frédéric . . . . . . . . . CJ-7.3 FRI (p184)
Smirnov, Lev . . . . . . . . . . . . ∙EC-P.14 FRI (p223)
Smirnova, Daria . . . . . . . . . CD-1.5 MON (p56),∙CD-11.1 FRI (p181), CD-11.5 FRI (p187),
EC-P.14 FRI (p223)
Smirnova, Olga . . . . . . . . . . . CG-1.5 TUE (p89),
EE-P.1 WED (p138), CG-5.4 THU (p161),
EE-4.6 FRI (p209), EC-P.6 FRI (p223)
Smith, Callum R. . . . . . . . . . . . CJ-P.8 FRI (p220)
Smith, Callum Robertson∙CD-P.23 TUE (p101)
Smith, Devin H. . . . . . . . . CE-P.30 THU (p173)
Smith, Graham M. . . . . . . . EH-4.2 THU (p158)
Smith, Jason . . . . . . . . . . . . CH-6.3 WED (p116)
Smith, Jason M. . . . . . . . . . CK-P.22 TUE (p105)
Smith, Joe A. . . . . . . . . . . . . EB-6.5 WED (p113)
Smith, Margaret . . . . . . . . . . . CH-4.5 TUE (p98)
Smith, Peter G. R. . . . . . . CM-7.4 WED (p112),
CM-7.6 WED (p114), CA-6.3 WED (p110),
CJ-5.5 WED (p133), EF-P.11 WED (p140),
CE-P.17 THU (p172), CE-P.30 THU (p173),
CE-9.2 FRI (p190), CE-11.5 FRI (p216),
CD-14.5 FRI (p217)
Smith, Peter Raymond . . . . . CI-5.3 FRI (p182)
Smith, Roland . . . . . . . . . . . PP-2.5 WED (p121),
CG-P.2 THU (p173), CG-P.10 THU (p174)
Smith, Will A.M. . . . . . . CE-P.30 THU (p173),
CD-14.5 FRI (p217)
Smolina, Ekaterina . . . . . . EC-P.14 FRI (p223)
Smorenburg, Peter . . . . . . . CG-4.6 THU (p155)
Smowton, Peter M. . . . . . . . . CB-4.5 TUE (p91)Smrž, Martin . . . . . . . . . . . . CA-P.1 MON (p74),
CA-P.19 MON (p75)
Sneftrup, Peter . . . . . . . . . . . . CM-6.4 TUE (p96)
Sneftrup, Peter S. . . . . . . ∙CM-P.19 MON (p78),
CM-10.2 FRI (p204)
Snigirev, Viacheslav . . . . . . . CB-5.4 TUE (p96),
CE-9.1 FRI (p188), ∙CK-14.5 FRI (p206)
So, Jin-Kyu . . . . . . . . . . . . . . . PP-1.6 MON (p64),
CH-P.4 WED (p136), CH-12.6 THU (p169)
Soares, Ana Carolina Costa
CL-P.10 FRI (p222)

Soavi, Giancarlo . . . . . . . . . . . EI-1.3 FRI (p184),
EI-2.2 FRI (p190)
Sobczak, Grzegorz . . . . . . CB-P.12 MON (p76),
CB-P.21 MON (p76)Soboń, Grzegorz . . . . . . . . . ED-2.4 MON (p61),
ED-2.5 MON (p63), ED-P.4 MON (p79),
ED-4.1 TUE (p83), CD-P.3 TUE (p100),
CJ-P.21 FRI (p221)
Soci, Cesare . . . . . . . . . . . . . EG-3.2 MON (p66),
CK-10.4 THU (p160), CK-14.4 FRI (p204)
Socorro Leránoz, Abián B. CL-1.4 MON (p71)
Sokolov, Alexei . . . . . . . . . . . . CL-7.6 FRI (p209)
Sokolovskii, G. S. . . . . . . . . . . EA-1.4 TUE (p87)
Sokolovskii, Grigorii . . . . ∙CB-9.5 THU (p152)
Sola, Íñigo J. . . . . . . . . . . . . . CF-3.5 MON (p73),
CF-4.4 TUE (p87)
Solano, Pablo . . . . . . . . . . . CK-P.27 TUE (p105),
CK-P.31 TUE (p106)
Solé, Rosa Maria . . . . . . . . CA-P.18 MON (p75),
CE-8.5 FRI (p186)
Soli, Elena . . . . . . . . . . . . . . . CE-2.3 MON (p61)
Soloviev, Alexander . . . . CG-P.12 THU (p174)
Soltanian, Emadreza . . . . CK-13.2 FRI (p190)
Somaschi, Niccolo . . . . . . EB-6.1 WED (p109),
EB-11.4 THU (p153), EA-8.1 FRI (p200)
Sommer, Florian . . . . . . . CF-P.13 TUE (p103),
CL-8.2 FRI (p211)
Somorin, Yinka M. . . . . . CM-P.21 MON (p78)
Son, Byungwoo . . . . . . . . . ∙CC-P.14 FRI (p218)
Son, Seong-Jin . . . . . . . . ∙CH-P.21 WED (p137),
CE-P.4 THU (p171)
Son Tung, Ha . . . . . . . . . . . CK-10.4 THU (p160)
Sondenheimer, René . . . EB-12.6 THU (p163),∙EA-P.8 THU (p175)
Sonderheimer, René . . . . . EB-8.4 WED (p125)
Song, Dong Hoon . . . . . . ∙CA-11.4 THU (p152)
Song, Sirius . . . . . . . . . . . . . . PD-1.5 THU (p170)
Song, Wenqing . . . . . . . . . . CF-7.5 WED (p119)
Sorel, Marc . . . . . . . . . . . . . . CD-14.4 FRI (p215)
Sorelli, Giacomo . . . . . . . . . EB-8.3 WED (p125)
Sorensen, Nicholas J. . . ∙CH-P.27 WED (p137)
Sorger, Volker . . . . . . . . . . ∙JSIII-4.1 FRI (p189)
Sorgi, Alessia . . . . . . . . . . . . ∙CC-4.4 FRI (p184),
CK-13.5 FRI (p196)
Sorianello, Vito . . . . . . . . . ∙CI-3.4 WED (p127)
Soriano, Miguel C. . . . . . JSIII-2.2 THU (p164)
Sorokin, Arseny A. . . . . . . . EB-2.1 MON (p59)
Sorokin, Evgeni . . . . . . . . . . CA-1.1 MON (p52)
Sorokina, Irina T. . . . . . . . . CA-1.1 MON (p52)
Soroush, Masoud . . . . . . . . . ED-P.8 MON (p79)
Sorrentino, Salvatore . . . . CH-2.1 MON (p58),
CL-6.1 FRI (p189), CD-13.2 FRI (p203)
Sortino, Luca . . . . . . . . . . . CH-8.4 WED (p133),∙EI-1.4 FRI (p186), EI-P.3 FRI (p224)Sośnicki, Filip . . . . . . . . . . ∙EB-9.5 WED (p133),
EB-P.21 THU (p177)
Sotillo, Belen . . . . . . . . . . . . . CM-4.2 TUE (p82)
Sotirova, Ana . . . . . . . . . . CM-7.5 WED (p112)
Sotobayashi, Hideyuki . . CH-7.1 WED (p123)
Sotom, Michel . . . . . . . . . . . . . CI-7.5 FRI (p206)
Sotor, Jarosław . . . . . . . . . . . CA-2.3 MON (p60)
Sottocorona, F. . . . . . . . . . . JSI-4.5 WED (p132)
Sottocorona, Filippo . . . . JSI-4.3 WED (p130)
Soukoulis, Costas . . . . . . . . CM-1.4 MON (p54)
Souleiman, Amin . . . . . . . . . ∙CB-5.3 TUE (p94)
Soun, Léna . . . . . . . . . . . . . . JSIII-6.5 FRI (p217)

250

Sowoidnich, Kay . . . . . . . . ∙CH-13.3 FRI (p183)
Sozos, Kostas . . . . . . . . . ∙JSIII-1.1 THU (p156),
JSIII-3.4 FRI (p187)
Špaček, Alexandr . . . . . . . . CA-8.4 WED (p118)
Spaeth, Patrick . . . . . . . . . . CH-14.1 FRI (p189)
Spagnolo, Barbara . . . . . . . CH-15.1 FRI (p201)
Spagnolo, Nicolò . . . . . . . . . . EB-5.3 TUE (p95),
EA-8.1 FRI (p200)
Spampinati, S. . . . . . . . . . . . JSI-3.5 WED (p126)
Spanos, Ioannis . . . . . . . . . . . CC-6.3 FRI (p204)
Speicher, Martin . . . . . . . . CG-P.13 THU (p174)
Speiser, Jochen . . . . . . . . . . CA-P.12 MON (p74)
Spellauge, Maximilian . ∙CM-10.3 FRI (p204),
CM-10.5 FRI (p208)
Spellauge, Tillmann . . . . ∙CH-8.1 WED (p129)
Spezzani, Carlo . . . . . . . . . . JSI-2.5 WED (p118)
Spiekermann, Stefan . . . . CA-P.15 MON (p74)
Spiess, Christopher . . . . . EB-12.6 THU (p163),
EB-P.3 THU (p176), EB-P.10 THU (p176),∙EB-P.18 THU (p177)
Spinks, Michael . . . . . . . . CG-P.13 THU (p174)
Spirito, Davide . . . . . . . . . . . . CE-4.3 TUE (p95)
Spitz, Oliver . . . . . . . . . . . . . . . CI-5.1 FRI (p180)
Spitz, Olivier . . . . . . . . . . . . CB-9.4 THU (p152)
Springate, Emma . . . . . . . . . CG-1.4 TUE (p87),
CF-P.22 TUE (p103), CG-3.1 THU (p143)
Spühler, Gabriel . . . . . . . . . . CF-P.4 TUE (p102)
Squibb, R. . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Squibb, Richard . . . . . . . . . . JSI-5.4 THU (p147)
Squibb, Richard J. . . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130)
Srikanthan, Athithyan . . CH-11.4 THU (p161)
Srinivas, R. . . . . . . . . . . . . . . . . ED-5.1 FRI (p180)
Srinivasa Rao, Allam . . . . . . ∙CI-5.4 FRI (p186)
Srinivasan, Kartik . . . . . . . . ED-P.8 MON (p79),
EF-2.2 WED (p131)
Srocka, Bernd . . . . . . . . . . . . CB-9.6 THU (p154)
St-Jean, Philippe . . . . . . . . . . EC-2.4 FRI (p197)
Stachowiak, Dorota . . . . . . CD-P.3 TUE (p100),∙CJ-P.21 FRI (p221)
Stagira, Salvatore . . . . . . . . . CM-6.3 TUE (p94),
CG-3.2 THU (p143), CE-P.10 THU (p172)
Staliunas, Kestutis . . . . . . . ∙EJ-1.1 MON (p52),
CE-3.3 MON (p69), CA-4.6 TUE (p88),
CK-3.6 TUE (p98)
Stalmashonak, Andrei . . . . CL-1.2 MON (p69),
CL-1.3 MON (p69)
Stark, David . . . . . . . . . . . . ∙CB-9.3 THU (p150)
Stark, Henning . . . . . . . . . . ∙CJ-2.2 WED (p111)
Staude, Isabelle . . . . . . . . . . . EG-5.3 TUE (p94),
CE-4.2 TUE (p93), CK-10.1 THU (p156),
CK-10.6 THU (p162),
CK-11.4 THU (p166), PD-2.9 THU (p171),
EI-2.2 FRI (p190)
Staudte, Andre . . . . . . . . . . . . CF-3.2 MON (p67)
Steed, Craig . . . . . . . . . . . . . . CL-P.11 FRI (p222)
Steeneken, Peter G. . . . . . . . . CK-3.1 TUE (p92)
Stefanov, André . . . . . . . . . . . ∙CL-P.6 FRI (p221)
Stefszky, Michael . . . . . . . . EB-6.3 WED (p111),
EA-4.5 THU (p160), ∙EA-5.5 THU (p168)
Steindl, Petr . . . . . . . . . . . ∙EA-P.13 THU (p175),
EB-P.25 THU (p177)
Steinecke, Morten . . . . . . ∙CD-P.24 TUE (p101)
Steinecker, Sylvia M. . . . . ∙CL-P.16 FRI (p222)
Steinert, Michael . . . . . . . . . CE-4.2 TUE (p93),
CH-6.2 WED (p116)

Steinhauer, Stephan . . . . . . CK-1.2 MON (p66)
Steinke, Sven . . . . . . . . . . . CA-P.22 MON (p75),
CG-P.13 THU (p174)
Steinkopff, Albrecht . . . . . CJ-2.4 WED (p113),
CJ-8.2 FRI (p192)
Steinle, Tobias . . . . . . . . . . CD-7.1 WED (p108)
Steinlechner, Fabian . . . . . . EB-2.4 MON (p63),
EB-8.4 WED (p125), EB-11.6 THU (p155),
EB-12.6 THU (p163), EB-P.3 THU (p176),∙EB-P.10 THU (p176),
EB-P.18 THU (p177), EB-P.19 THU (p177),
EB-P.20 THU (p177), EB-P.31 THU (p178)
Steinleitner, Philipp . . . . . ∙CA-2.3 MON (p60),
CD-7.2 WED (p108), PD-1.4 THU (p170)
Steinmeyer, Günter . . . . . ∙CF-6.2 WED (p109),∙EF-P.6 WED (p139), CF-10.5 THU (p147),∙CG-3.4 THU (p145), ∙CF-12.5 FRI (p215)
Stenger, Nicolas . . . . . . . . . . CK-15.6 FRI (p216)
Stepanenko, Yuriy . . . . . . . CE-7.4 THU (p169),
CD-13.3 FRI (p205)
Stepanov, Evgeny . . . . . . . . . . CF-5.5 TUE (p99)
Stephan, Sven . . . . . . . . . . . . . . EI-2.6 FRI (p196)
Stepien, Ryszard . . . . . . . . . CE-5.1 THU (p149)
Stȩpniewski, Grzegorz . . . CE-7.4 THU (p169),
CJ-9.1 FRI (p200)
Sternfeld, Yael . . . . . . . . . . ∙CH-7.5 WED (p127)
Sterr, Uwe . . . . . . . . . . . . . . . . ED-P.3 MON (p79)
Steshchenko, Tatiana . . . ∙CB-6.4 WED (p126)
Steudel, Max . . . . . . . . . . . . . PD-1.1 THU (p170)
Stiller, Birgit . . . . . . . . . . . . . EB-1.2 MON (p55),
EB-5.6 TUE (p99), ∙EF-1.2 WED (p127),
EA-P.15 THU (p175), EF-7.3 FRI (p183),
CK-13.1 FRI (p188), CD-12.1 FRI (p189),
CD-12.6 FRI (p197), JSIII-P.11 FRI (p225)
Stingel, Ashley Marie . . . . . CF-12.3 FRI (p213)
Stipčević, Mario . . . . . . . . . . . EA-6.2 FRI (p184)
Stivala, Salvatore . . . . . . . . . . ED-6.3 FRI (p192)
Stobbe, Søren . . . . . . . . . . . . EG-P.9 TUE (p107),
EC-2.5 FRI (p197)
Stock, Christian . . . . . . . . ∙CF-P.13 TUE (p103),
CJ-3.4 WED (p119)
Stöcker, Markus . . . . . . . . . PP-2.9 WED (p121),
EB-P.1 THU (p176)
Stockill, Robert . . . . . . . . ∙EB-13.2 THU (p165)
Stoecker, Axel . . . . . . . . . . . ∙CL-3.6 THU (p163)
Stoian, Razvan . . . . . . . . . CH-P.18 WED (p137)
Stoliarov, Dmitrii . . . . . . . ED-P.9 MON (p79),
EF-P.18 WED (p140), ∙CJ-P.9 FRI (p220),
CJ-P.23 FRI (p221)
Stolidi, Adrien . . . . . . . . . . . CL-4.2 THU (p165)
Stoll, Katherine . . . . . . . . . . CD-3.5 MON (p72)
Stoltz, Nick G. . . . . . . . . . . . . . EB-5.5 TUE (p97)
Stone, A. Douglas . . . . . . . . . CJ-1.5 TUE (p99),
CJ-6.6 THU (p149)
Stone, Brandon . . . . . . . . . . EF-2.1 WED (p129)
Stone, James M. . . . . . . . . . . CE-2.2 MON (p59),
CD-4.2 TUE (p82), CH-10.2 THU (p151)
Stonio, Bartłomiej . . . . . . . CK-P.23 TUE (p105)
Stonkus, Konradas . . . . . . CM-11.5 FRI (p216)
Stonytė, Dominyka . . . . . CM-P.27 MON (p78)
Stopiński, Stanisław . . . . . . ∙CB-5.2 TUE (p92),
CK-P.9 TUE (p104), CK-P.23 TUE (p105),∙CH-11.6 THU (p163)
Storp, Jakob . . . . . . . . . . . . JSIII-P.11 FRI (p225)
Strafford, Simon . . . . . . . . . CL-3.5 THU (p161)
Straguzzi, John N. . . . . . . . CK-13.4 FRI (p194)

Authors' Index

Straight, Paul . . . . . . . . . . . . CH-1.5 MON (p57)
Strasser, Gottfried . . . . . . . CB-P.4 MON (p75),
CB-8.2 THU (p142), CC-4.2 FRI (p180)
Stratakis, Emmanuel . . . . . CM-5.3 TUE (p91),
EI-1.2 FRI (p182), CM-9.1 FRI (p188),
CM-9.5 FRI (p196), CD-13.1 FRI (p201),
EI-P.4 FRI (p224)
Strelkov, Vasily . . . . . . . . . . CG-4.6 THU (p155)
Stremplewski, Patrycjusz . . CL-7.2 FRI (p203)
Strickland, Donna . . . . . . . ∙PL-1.1 MON (p72)
Strobel, Tim . . . . . . . . . . . . . EA-5.1 THU (p162)
Strobl, Theodor . . . . . . . . ∙CK-7.3 WED (p132)
Stroganov, Anton . . . . . . ∙EF-P.24 WED (p141),
EC-1.2 FRI (p183)
Stroj, Sandra . . . . . . . . CM-LIM.5 WED (p119)
Strömberg, Axel . . . . . . . . . . . CC-4.6 FRI (p186)
Strotkamp, Michael . . . . . . CA-6.2 WED (p108)
Strunskus, Thomas . . . . . . CK-P.19 TUE (p105)
Stuart, Nicholas . . . . . . . . . CF-P.23 TUE (p103),
CA-8.2 WED (p116)
Stucki, Marco E. . . . . . . . ∙CK-P.21 TUE (p105)
Stuhl, Benjamin K. . . . . . . . ED-3.1 MON (p67)
Stukachev, Sergey . . . . . . CG-P.12 THU (p174)
Stummer, Vinzenz . . . . . . . ∙CF-11.6 FRI (p209)
Stupar, M. . . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Su, Liangbi . . . . . . . . . . . . . . CA-P.9 MON (p74),
CA-P.10 MON (p74)
Suarez, Miguel . . . . . . . . . . . CE-5.2 THU (p151)
Suas-David, Nicolas . . . . . ED-2.3 MON (p61)
Suchita, . . . . . . . . . . . . . . . . . . . ∙CI-P.9 FRI (p219)
Suchowski, Haim . . . . . . . . . EE-5.5 FRI (p215),
EI-P.5 FRI (p224)
Suckow, Stephan . . . . . . . . CA-9.3 WED (p130)
Suda, Satoshi . . . . . . . . . . . . . . CI-6.2 FRI (p190)
Südbeck, Jan . . . . . . . . . . . . EA-P.4 THU (p174)
Suddapalli, Chaitanya Kumar
CD-6.1 TUE (p92), CD-P.19 TUE (p101)
Sudera, Prerna . . . . . . . . CH-P.24 WED (p137),
CH-14.5 FRI (p197)
Sudhop, Stefanie . . . . . . . . . PP-1.9 MON (p64),
CM-P.5 MON (p77)
Südmeyer, Thomas . . . . . . CB-8.4 THU (p144),
CA-11.5 THU (p152), CG-4.4 THU (p153),
ED-6.4 FRI (p194)
Sudo, Teruaki . . . . . . . . . . . EH-P.13 THU (p179)
Suemasa, Aru . . . . . . . . . . . . . CJ-P.10 FRI (p220)
Sugak, Dmytro . . . . . . . . . CE-P.12 THU (p172)
Sugimoto, Yoshimasa . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76), CK-P.17 TUE (p105),
EC-P.11 FRI (p223)
Sugita, Atsushi . . . . . . . . . . ∙EH-P.4 THU (p178)
Sugiura, Muneo . . . . . . . . . CF-10.4 THU (p145)
Sukeert, . . . . . . . . . . . . . . . . . ∙CD-6.1 TUE (p92),∙CD-P.19 TUE (p101)
Sukegawa, Takashi . . . . . . CK-7.3 WED (p132)
Sukhanov, Maxim . . . . . . . . CA-1.2 MON (p52)
Sukhorukov, Andrey . . . . . . EG-5.2 TUE (p92),
EB-P.34 THU (p178)
Sukhorukov, Andrey A. CK-10.2 THU (p158),
PD-2.9 THU (p171)
Šulc, Jan . . . . . . . . . . . . . . . . ∙CA-P.7 MON (p74),
CA-P.8 MON (p74), CA-P.10 MON (p74),
CA-P.11 MON (p74)
Sulmoni, Luca . . . . . . . . . . . . CB-2.3 MON (p68)
Sultanov, Vitaliy . . . . . . . . . PD-2.8 THU (p171)
Sulway, Dominic A . . . . . ∙CK-6.4 WED (p126)

Sulzer, Philipp . . . . . . . . . . . EF-6.1 THU (p162),∙EF-6.2 THU (p164)
Sumetsky, Misha . . . . . . . . . . CK-3.2 TUE (p92)
Sumpf, Bernd . . . . . . . . . . . CB-P.14 MON (p76),
CB-11.4 THU (p166), CH-13.3 FRI (p183)
Sun, Bangshan . . . . . . . . . ∙CM-7.5 WED (p112)
Sun, Dunlu . . . . . . . . . . . . . . CA-P.18 MON (p75)
Sun, Hung-Wei . . . . . . . . . ∙CG-3.5 THU (p147)
Sun, Kai . . . . . . . . . . . . . . . . . . . CB-3.1 TUE (p82)
Sun, Qiushuo . . . . . . . . . . . EA-P.10 THU (p175)
Sun, Shiyu . . . . . . . . . . . . . . . CD-6.2 TUE (p92),
CD-7.6 WED (p114)
Sun, Suwan . . . . . . . . . . . . . EF-P.20 WED (p140)
Sun, Yan-Ting . . . . . . . . . . . . . CC-4.6 FRI (p186)
Sun, Yifan . . . . . . . . . . . . . . ∙EF-4.4 THU (p154),
EF-7.1 FRI (p181), EF-7.4 FRI (p185),
EF-7.5 FRI (p187), ∙EJ-3.3 FRI (p185)
Sun, Yiming . . . . . . . . . . . . . . CB-P.3 MON (p75)
Sun, Yiwei . . . . . . . . . . . . . . . ∙CI-P.11 FRI (p219)
Sun, Zhibin . . . . . . . . . . . . . JSI-1.2 WED (p110),∙JSI-3.2 WED (p124), JSI-4.1 WED (p128)
Sun, Zhipei . . . . . . . . . . . . . CA-9.6 WED (p134),
EI-P.1 FRI (p223)
Sunjerga, Antonio . . . . . . . CD-8.1 WED (p114)
Sünnetçioğlu, Ali Kaan . ∙CB-P.20 MON (p76)
Suntsov, Sergiy . . . . . . . . . . CK-P.3 TUE (p104)
Suppelt, Sven . . . . . . . . . . . . PD-1.1 THU (p170)
Supradeepa, V.R. . . . . . . . . . . . CJ-P.6 FRI (p220)
Şura, Aladin . . . . . . . . . . . . . CF-P.10 TUE (p103)
Suraj, Suraj . . . . . . . . . . . . ∙CE-P.25 THU (p173)
Suret, Pierre . . . . . . . . . . . . . EF-P.2 WED (p139),
EF-7.6 FRI (p187), EF-9.5 FRI (p207),
EF-9.6 FRI (p209)
Susnjar, Peter . . . . . . . . . . . . JSI-P.7 WED (p141)
Suster, Mihai C. . . . . . . . . . ∙CG-P.8 THU (p174)
Suzuki, Daisuke . . . . . . . . . . ∙CM-4.6 TUE (p88)
Suzuki, Hideyuki . . . . . . . JSIII-2.5 THU (p168)
Svejkar, Richard . . . . . . . . . ∙CA-P.8 MON (p74),
CJ-10.6 FRI (p216)
Sverchkov, Sergei . . . . . . . . . CA-1.2 MON (p52)
Svetina, Cristian . . . . . . . ∙JSI-1.1 WED (p108),
JSI-1.4 WED (p112)
Svirplys, Evaldas . . . . . . . . CG-4.5 THU (p153),
CG-6.4 THU (p169)
Swami, Rahul . . . . . . . . . . . . JSVI-1.2 TUE (p85)
Swaminathan, Madhavan . CC-P.10 FRI (p218)
Swann, William C. . . . . . . . ED-3.1 MON (p67)
Swiderski, Angad . . . . . . . . JSI-P.4 WED (p141)
Swift, Gary . . . . . . . . . . . . . . JSI-P.6 WED (p141)
Swift, Simon . . . . . . . . . . . . . CL-P.11 FRI (p222)
Swillo, Marcin . . . . . . . . . . . CE-7.2 THU (p167)
Sydorchuk, Volodymyr . CE-P.12 THU (p172)
Sylvestre, T. . . . . . . . . . . . . ∙EF-P.15 WED (p140)
Sylvestre, Thibaut . . . . . . CF-6.1 WED (p109),
CK-13.1 FRI (p188)
Symonowicz, Joanna . . . ∙CH-8.3 WED (p131)
Synanidis, Adamantios P.
∙EG-6.5 WED (p112)
Syngelakis, Ioannis . . . . . CM-P.12 MON (p77)
Szabó, Gábor . . . . . . . . . . . . CG-P.3 THU (p173)
Szafranska, Karolina . . . CH-P.28 WED (p137)
Szameit, Alexander . . . . . . . EB-2.3 MON (p61),
EB-4.2 TUE (p85), CK-P.31 TUE (p106),
CM-7.3 WED (p110), PP-2.10 WED (p121),
CK-11.3 THU (p166), EA-P.1 THU (p174),
CK-12.2 FRI (p180), EC-1.3 FRI (p185),

EC-2.1 FRI (p189), EA-8.3 FRI (p204),
EA-8.4 FRI (p206), EF-9.1 FRI (p201),
EC-P.1 FRI (p222), EC-P.2 FRI (p223),
EC-P.3 FRI (p223)
Szedlak, Rolf . . . . . . . . . . . . . CH-3.3 TUE (p86),∙CI-5.1 FRI (p180)
Szeghalmi, Adriana . . . . . CK-P.24 TUE (p105),
EE-P.12 WED (p139), EH-2.5 THU (p148),
PD-1.2 THU (p170)
Szkulmowski, Maciej . . . . . . CL-7.2 FRI (p203)
Szuniewicz, Jerzy . . . . . . ∙EB-12.5 THU (p161),
EB-P.21 THU (p177)
Szutor, Bence . . . . . . . . . . . . . ED-6.5 FRI (p196)

T
T. Grochowski, Piotr . . . . CD-7.1 WED (p108)
Tabosa, José W R . . . . . . ∙EA-P.23 THU (p176)
Tachikawa, Saeko . . . . . . . . JSVI-1.2 TUE (p85)
Tachtsidis, Theodoros . . CM-P.31 MON (p78)
Tagliabue, Giulia . . . . . . . . PP-1.13 MON (p65),
JSIV-1.2 WED (p116),
JSIV-P.2 WED (p141)
Taguchi, Yoshitaka . . . . . . EA-3.4 THU (p152),∙JSIII-4.2 FRI (p193)
Tahara, Tahei . . . . . . . . . . . . CH-9.1 THU (p143)
Tai, Le Xuan The . . . . . . . . EF-P.19 WED (p140)
Taira, Takunori . . . . . . . . . . CA-P.24 MON (p75)
Tajalli, Ayhan . . . . . . . . . . . . JSI-P.4 WED (p141)
Takagi, Shigeyuki . . . . . . . . . CB-1.5 MON (p56)
Takahashi, Eiji . . . . . . . . . . ∙CF-8.1 WED (p123)
Takahashi, Eiji J. . . . . . . . . . CG-4.2 THU (p151)
Takahashi, Kenta . . . . . . . . . . . CJ-9.2 FRI (p204)
Takahashi, Shinya . . . . . ∙PP-2.13 WED (p121),∙EI-P.6 FRI (p224)
Takahashi, Yushiro . . . . ∙EE-P.11 WED (p139)
Takanashi, Naoto . . . . . . . . EA-3.6 THU (p154)
Takase, Kan . . . . . . . . . . . . . . EA-2.2 THU (p142)
Takashima, Yoshifumi . . . JSI-2.4 WED (p118)
Takata, Norio . . . . . . . . . . . . PD-2.4 THU (p171)
Takats, Zoltan . . . . . . . . . . . . CL-3.2 THU (p159)
Takeda, Harunobu . . . . . . . . CK-3.3 TUE (p94),∙CK-5.4 WED (p118), CE-6.5 THU (p161)
Takeda, Yoshihiko . . . . . . CK-P.17 TUE (p105),
EC-P.11 FRI (p223)
Takenaka, Mitsuru . . . . . . . CK-8.2 THU (p142)
Takeuchi, Yuichi . . . . . . . . . ∙CJ-P.10 FRI (p220)
Takiguchi, Hiroshi . . . . . . . . CJ-P.10 FRI (p220)
Talandier, Lucas . . . . . . . . JSIII-1.4 THU (p160)
Talbot , Lauris . . . . . . . . . . . CE-3.4 MON (p69),
CM-P.14 MON (p77), CJ-6.5 THU (p147)
Taleb, Hussein . . . . . . . . . . CA-11.3 THU (p150)
Talenti, Francesco R. . . . . . . . EJ-3.3 FRI (p185)
Talone, Benedetta . . . . . . . . . CL-6.5 FRI (p197)
Talts, Ülle-Linda . . . . . . . . CD-1.2 MON (p54),
EH-4.1 THU (p156)
TALUKDER, RIA . . . . . . . ∙JSIII-5.3 FRI (p205)
Tamashevich, Yaraslau . . . . . EG-4.4 TUE (p86)Tamma, Vincenzo . . . . . . . EB-7.4 WED (p119)
Tamošauskas, Gintaras . . CD-P.25 TUE (p101)
Tamotsu, Sohta . . . . . . . . . . EH-P.4 THU (p178)
Tamulienė, Viktorija . . . . . CD-P.8 TUE (p100)
Tamura, Koichi . . . . . . . . . CF-10.4 THU (p145)
Tan, Peng Kian . . . . . . . . . . EB-P.11 THU (p176)
Tan, Ping-Heng . . . . . . . . . . . . CE-4.3 TUE (p95)
Tan, Qi Ying . . . . . . . . . . . . . CK-14.4 FRI (p204)

251

Tan, Qinggui . . . . . . . . . . . . . CI-P.11 FRI (p219)
Tan, Ryan Ron Zee . . . . . . . . CL-P.3 FRI (p221),
CL-P.4 FRI (p221)
Tanabe, Takasumi . . . . . . CD-P.17 TUE (p101),
CK-P.26 TUE (p105), CI-8.3 FRI (p212)
Tanaka, Hiroki . . . . . . . . . . CK-P.3 TUE (p104),
CA-6.1 WED (p108), CA-11.1 THU (p148)
Tanaka, Katsuya . . . . . . . CK-10.1 THU (p156)
Tanaka, Koichiro . . . . . . . . EE-1.2 WED (p109),
PP-2.13 WED (p121), EE-P.9 WED (p139),
EI-P.6 FRI (p224)
tanaka, Shuya . . . . . . . . . . . . . . CI-8.3 FRI (p212)
Tancogne-Dejean, Nicolas ∙CG-1.2 TUE (p85)
Tanemura, Takuo . . . . . . . . JSIII-4.2 FRI (p193)
Tang, Dawei . . . . . . . . . . . . . CH-7.2 WED (p123)
Tang, Hanzhi . . . . . . . . . . . . CK-8.2 THU (p142)
Tang, Mingchu . . . . . . . . . . . . CB-4.5 TUE (p91)
Tang, Stanley . . . . . . . . . . . . . . CJ-7.4 FRI (p186),
CJ-P.12 FRI (p220)
Tang, Yilin . . . . . . . . . . . . . . . . EG-5.3 TUE (p94)
Tangarife Villamizar, Nicolás Eduardo
EB-12.6 THU (p163)
Tanghe, Ivo . . . . . . . . . . . . . . CK-8.4 THU (p144)
Tani, Francesco . . . . . . . . CH-10.5 THU (p153)
Tani, Mizuki . . . . . . . . . . . . CM-P.8 MON (p77),∙CM-5.2 TUE (p90)
Tanida, Jun . . . . . . . . . . . . . JSIII-2.5 THU (p168)
Taniguchi, Takashi . . . . . PP-2.13 WED (p121),
EI-2.6 FRI (p196), EI-3.2 FRI (p204),
EI-4.2 FRI (p212), EI-4.5 FRI (p216),
EI-P.6 FRI (p224)
tanikawa, Koya . . . . . . . . . . . . ∙CI-8.3 FRI (p212)
Tanimura, Hirotaka . . . . . . CB-1.5 MON (p56)
Tanizawa, Ken . . . . . . . . . . . CK-8.2 THU (p142)
Tanner, Michael . . . . . . . . CH-11.2 THU (p159)
Tanomura, Ryota . . . . . . . . JSIII-4.2 FRI (p193)
Tanyag, Rico M. . . . . . . . . . JSI-3.1 WED (p122)
Tanzilli, Sébastien . . . . . . . . EB-2.5 MON (p63),
EB-9.6 WED (p135), EB-11.4 THU (p153),
EB-P.2 THU (p176)
Tapani, Tilaike . . . . . . . . . . . EH-2.4 THU (p146)
Taranta, Austin . . . . . . . . . . . CE-2.4 MON (p61)
Tarasov, Aleksandr . . . . . . ∙CD-P.4 TUE (p100)
Taray, Derya . . . . . . . . . . . . . ED-1.3 MON (p55)
Tarrago Velez, Santiago . . . ∙EA-9.5 FRI (p214)
Tartakovskii, Alexander I. . . EI-4.2 FRI (p212)
Tartari, Enrico . . . . . . . . . ∙CL-3.1 THU (p157),
CL-3.4 THU (p161)
tasaka, Shun . . . . . . . . . . . . . . . CI-8.3 FRI (p212)
Täschler, Philipp . . . . . . . . CK-6.2 WED (p124),
CB-8.3 THU (p144), ∙CB-9.1 THU (p148)
Tasker, Joel F. . . . . . . . . . . . . EB-6.2 WED (p109)
Tasolamprou, Anna C. . . . . CC-6.3 FRI (p204)
Tassin, Philippe . . . . . . . . . CK-8.3 THU (p144),
EA-3.1 THU (p148), CK-15.3 FRI (p212)
Tatar-Mathes, Philipp . . . . CB-2.2 MON (p66)
Tate, James . . . . . . . . . . . . . . CH-13.6 FRI (p187)
Tate, Naoya . . . . . . . . . . . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118), CE-6.5 THU (p161)
Tavakol, Hamed . . . . . . . . . JSI-P.4 WED (p141)
Taverne, Mike . . . . . . . . . . . CK-P.7 TUE (p104),
CE-P.15 THU (p172)
Tawy, Goronwy . . . . . . . . ∙CA-6.3 WED (p110),
CE-9.2 FRI (p190)
Taylor, Jonathan M. . . . . . EG-6.6 WED (p114)
Taylor, Patrick J. . . . . . . . . . CE-6.6 THU (p163)

Teimourpour, Mohammad Hosain
CB-3.3 TUE (p86)
Teisset, Catherine Y. . . . . CF-10.6 THU (p149)
Teller, Markus . . . . . . . . . . . PD-2.6 THU (p171)
Templ, Wolfgang . . . . . . . . . CI-3.4 WED (p127)
ten Brummelaar, Theo A. JSII-3.4 MON (p71)
Tenbrake, Lukas . . . . . . . . . ∙CK-15.5 FRI (p214)
Tenne, Ron . . . . . . . . . . . . . . . ∙EG-5.4 TUE (p96)
Tennyson, Jonathan . . . . . . ED-2.4 MON (p61)
Ter-Avetisyan , Sargis . . . ∙CG-P.6 THU (p174)
Terai, Hirotaka . . . . . . . . . . EA-2.2 THU (p142),
EB-P.9 THU (p176)
Terashi, Yuhei . . . . . . . . . . . . . CI-6.3 FRI (p192)
Tessier, Gilles . . . . . . . . . . . . CJ-4.2 WED (p123),
CL-6.2 FRI (p191)
Thai, Quang Minh . . . . . . ∙CL-2.3 THU (p151),∙CC-P.16 FRI (p218)
Theiner, Dominik . . . . . . . . CC-4.2 FRI (p180),∙CC-7.2 FRI (p210)
Thellier, Elio . . . . . . . . . . ∙CA-11.3 THU (p150)
Theodosi, Anna . . . . . . . . . PP-1.8 MON (p64),
CM-P.4 MON (p77)
Theophilo, Klara . . . . . . . . . EA-2.1 THU (p142)
Thesinga, Jelto . . . . . . . . . . CA-P.23 MON (p75),
CE-6.4 THU (p161)
Theurer, Lara Sophie . . . ∙CB-P.14 MON (p76),
CB-11.4 THU (p166)
Thibault, Franck . . . . . . . . . ED-1.2 MON (p53)
Thibon, Louis . . . . . . . . . . . . CL-P.15 FRI (p222)
Thiele, Frederik . . . . . . . . . . . ∙CI-5.5 FRI (p186)
Thiem, Hendrick . . . . . . . ∙CB-P.11 MON (p76)
Thierstein, Emily . . . . . . . . JSI-4.6 WED (p134)
Thies, Andreas . . . . . . . . . EB-12.3 THU (p159),
CB-11.1 THU (p162)
Thiré, Nicolas . . . . . . . . . . . . CF-12.3 FRI (p213)
Thomale, Ronny . . . . . . . . . . . EC-1.3 FRI (p185)
Thomas, Sarah . . . . . . . . . EB-10.4 THU (p145),
EB-12.5 THU (p161)
Thomas, Sarah E. . . . . . . . . . . EA-8.1 FRI (p200)
Thomas, Tyler . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)Thomm, Robin . . . . . . . . . EB-11.5 THU (p153),
EB-P.35 THU (p178)
Thompson, James O. F. . . CF-P.22 TUE (p103)
Thomson, Mark . . . . . . . . . . . CC-6.1 FRI (p200)
Thomson, Robert R . . . . . JSII-3.4 MON (p71),
CD-4.2 TUE (p82), CH-10.2 THU (p151)
Thoraval, Jérémy . . . . . . . . . . . EI-3.1 FRI (p200)
Thottoli, Ajmal . . . . . . . . . . ∙CK-P.6 TUE (p104)
Thoumany, Pierre . . . . . . . . ED-P.6 MON (p79)
Thourhout, Dries Van . . . CK-8.4 THU (p144)
Thrane, Paul . . . . . . . . . . . . . CL-4.4 THU (p167)
Thumm, Uwe . . . . . . . . . . . . CG-6.1 THU (p163)
Tian, Hao . . . . . . . . . . . . . . . . . CB-5.4 TUE (p96)
Tian, Jingyi . . . . . . . . . . . . CK-10.4 THU (p160),
CD-12.2 FRI (p191), ∙CK-14.4 FRI (p204)
Tian, Wenlong . . . . . . . . . . . PP-1.2 MON (p64),
CA-P.13 MON (p74), CA-P.21 MON (p75),
CA-10.1 THU (p142)
Tian, Xuan . . . . . . . . . . . . . . . PP-1.2 MON (p64),
CA-P.21 MON (p75), ∙CA-10.1 THU (p142)
Tian, Yi . . . . . . . . . . . . . . . . . . CC-3.5 THU (p169)
Tiana-Alsina, Jordi . . . . . . CB-P.8 MON (p76),
CB-P.19 MON (p76), EF-P.21 WED (p140)
Tibai, Zoltán . . . . . . . . . . . . . CC-P.5 FRI (p218),
CC-P.13 FRI (p218), CC-P.15 FRI (p218)

Authors' Index

Tielrooij, Klaas-Jan . . . . . . . . EI-4.5 FRI (p216)
Tien Dat, Pham . . . . . . . . . . . ∙CI-8.2 FRI (p210)
Tikan, Alexey . . . . . . . . . . . ∙EF-3.1 THU (p142),
EF-3.2 THU (p142), EC-1.2 FRI (p183),
EF-9.2 FRI (p203)
Tikhodeeva, Ekaterina . . . JSI-P.3 WED (p141)
Tillman, Benjamin . . . . . . EH-1.3 WED (p132)
Tilmann, Benjamin . . . . . . EG-1.2 MON (p54),
EH-3.2 THU (p150), EI-1.4 FRI (p186)
Timonen, Hilkka . . . . . . . . CH-P.6 WED (p136)
Tirole, Romain . . . . . . . . . ∙EH-1.3 WED (p132)
Tisch, John . . . . . . . . . . . . . . . CG-1.4 TUE (p87),
CG-P.10 THU (p174)
Tisch, John W.G. . . . . . . . . CG-3.1 THU (p143),
EE-4.6 FRI (p209)
Tittil, Andreas . . . . . . . . . . . EH-3.2 THU (p150)
Tittonen, Ilkka . . . . . . . . . . . EG-2.4 MON (p62),
EB-P.29 THU (p178)
Tiwari, Balsant . . . . . . . . . . EA-P.14 THU (p175)
Tiwari, Priyanshu . . . . . . . . EA-5.6 THU (p168)
Tiwari, Sunny . . . . . . . . . . . . EG-1.2 MON (p54)
Tizzard, Graham . . . . . . . . . CE-1.1 MON (p53)
Togawa, Moto . . . . . . . . . . . JSI-P.2 WED (p141)
Togawa, Ryuichi . . . . . . . . . CB-P.16 MON (p76)
Tokizane, Yu . . . . . . . . . . . . . CC-P.11 FRI (p218)
Tokunaga, Eiji . . . . . . . . . . . CE-7.1 THU (p163)
Toma, Andrea . . . . . . . . . . . PD-2.8 THU (p171)
Tomasino, Alessandro . . . CC-3.4 THU (p167),
CC-5.1 FRI (p188)
Tomaszewska-Rolla, Dorota∙ED-2.5 MON (p63)Tomczyk, Monika . . . . . . . . CE-3.5 MON (p71)
Tomescu, Roxana . . . . . . . . . . CK-2.2 TUE (p86)
Tomii, Naoya . . . . . . . . . . . . CA-9.5 WED (p132)
Tomilov, Sergei . . . . . . . . . ∙CA-2.2 MON (p60),
CF-12.2 FRI (p211)
Tomishige, Yoshitaka . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118)
Tomita, Arata . . . . . . . . . . . . . CM-4.6 TUE (p88)
Tomlinson, Stephanie . . . CA-8.2 WED (p116)
Tondusson, Marc . . . . . . . . . CE-10.3 FRI (p206)
Tonello, Alessandro . . . . CD-9.1 WED (p122),
EF-P.10 WED (p140), ∙EF-7.5 FRI (p187),
CD-13.3 FRI (p205)
Tongay, Sefaattin . . . . . . . . . . . EI-2.6 FRI (p196)
Toninelli, Costanza . . . . . . EA-4.1 THU (p156)
Töpfer, Sebastian . . . . . . . . EB-8.1 WED (p123),
EB-8.2 WED (p123), EB-8.4 WED (p125)
Torcheboeuf, Nicolas . . . . ∙CF-P.4 TUE (p102)
Torner, Lluís . . . . . . . . . . . . EF-6.6 THU (p168),
EC-3.3 FRI (p205)
Torosov, Boyan T. . . . . . . . EB-11.5 THU (p153)
Torre, Cyril . . . . . . . . . . . . . ∙CH-9.2 THU (p145)
Torregrosa, Adrián J. . . . ∙CD-P.33 TUE (p102)
Torres, Estrella . . . . . . . . . . . CB-2.3 MON (p68)
Torres, Jan P. . . . . . . . . . . . . EB-8.1 WED (p123)
Torres-Company, Victor . CK-1.4 MON (p68),
CD-P.1 TUE (p100), CF-P.7 TUE (p102),
CK-P.35 TUE (p106), ∙CI-2.1 WED (p115),
CI-2.2 WED (p119), EF-3.5 THU (p146),
CK-9.3 THU (p152), ED-6.2 FRI (p190)
Torrioli, Guido . . . . . . . . . . . CC-4.1 FRI (p180),
CC-4.5 FRI (p186)
Tortarolo, Giorgio . . . . . . . . . CL-6.3 FRI (p195)
Torun, Cem Güney . . . . . ∙EB-12.3 THU (p159)
Torun, Hamdi . . . . . . . . . . . . . CI-8.5 FRI (p214),

CI-P.2 FRI (p219)
Tosa, Valer . . . . . . . . . . . . . . . CM-6.3 TUE (p94),
CG-4.5 THU (p153)
Totero Gongora, Juan S. . . CH-1.1 MON (p53)
Totero Gongora, Juan SebastianCC-3.5 THU (p169), ED-6.3 FRI (p192)
Tóth, György . . . . . . . . . . . . CE-P.6 THU (p171),
CC-P.5 FRI (p218), CC-P.9 FRI (p218),
CC-P.13 FRI (p218)
Tóth, Szabolcs . . . . . . . . . . . CF-P.6 TUE (p102),
CA-8.5 WED (p120), CG-4.1 THU (p149)
Toumi, Johnny . . . . . . . . . . . . ∙CL-P.8 FRI (p222)
Tourlouki, Konstantina CM-P.31 MON (p78)
Tournié, Eric . . . . . . . . . . . . . CB-4.1 TUE (p90),
CB-4.2 TUE (p90)
Touš, Jan . . . . . . . . . . . . . . . CH-P.12 WED (p136)
Tovar, Pedro . . . . . . . . . . . . . . CJ-P.16 FRI (p220)
Townend, Daniel J. . . . . . ∙CH-7.2 WED (p123)
Townsend, Paul D. . . . . . . . CI-3.3 WED (p125)
Trabattoni, Andrea . . . . . . PP-1.5 MON (p64),
CK-1.6 MON (p72), CD-P.2 TUE (p100),
JSI-5.3 THU (p145), CG-3.2 THU (p143),
EE-4.1 FRI (p201)
Trabbatoni, Andrea . . . . . . JSI-5.4 THU (p147)
Trainor, Luke S. . . . . . . . CD-10.3 WED (p130),
CD-10.4 WED (p132)
Tran, Kevin . . . . . . . . . . . . . . CE-5.4 THU (p153)
Tränkle, Günther . . . . . . . . CB-P.5 MON (p75),
CB-P.14 MON (p76), CF-6.5 WED (p113)
Trassinelli, Martino . . . . . . . EJ-1.4 MON (p56)
Traub, Martin . . . . . . . . . . . CA-6.6 WED (p114)
Trautvetter, Johannes . . . . JSVI-1.2 TUE (p85)
Travers, John . . . . . . . . . . . . . CF-3.3 MON (p69)
Travers, John C. . . . . . . . . . . CD-4.2 TUE (p82),
CD-5.4 TUE (p91), CF-6.3 WED (p111),
EE-4.1 FRI (p201), EE-4.4 FRI (p205),
EE-4.5 FRI (p207)
Trawi, Firas . . . . . . . . . . . . . CG-4.4 THU (p153)
Trebaol, Stéphane . . . . . . . . ∙CK-3.5 TUE (p96),∙CB-10.3 THU (p158)
Trefilov, Daniil . . . . . . . . . ∙EB-P.14 THU (p177)
Treglia, Antonella . . . . . . . CE-P.10 THU (p172)
Trendle, Tobias . . . . . . . . . . . . CL-5.2 FRI (p183)
Treps, Nicolas . . . . . . . . . . . EB-8.3 WED (p125),
EA-3.2 THU (p150), EB-12.2 THU (p159),
EB-13.4 THU (p167), EB-13.6 THU (p169)
Tresp, Christoph . . . . . . . . . ED-P.6 MON (p79)
Trichet, Aurelien . . . . . . . . CH-6.3 WED (p116)
Trifonov, Anton . . . . . . . . CA-10.5 THU (p146),
CD-11.2 FRI (p183)
Tripathi, Anshuman . . . . . . . CL-7.5 FRI (p207)
Tripathy, Manoj . . . . . . . . . . . . EI-P.4 FRI (p224)
Tripier-Mondancin, Niels
EB-12.2 THU (p159)
Trippenbach, Marek . . . . EF-P.19 WED (p140)
Triscari, Andrea . . . . . . . . . . EF-3.1 THU (p142)
Trisorio, Alexandre . . . . . CA-11.5 THU (p152)
Trivedi, Manish . . . . . . . . . . CK-14.3 FRI (p204)
Trivedi, Sudhir . . . . . . . . . . . CA-3.1 MON (p66)
Trivino, Noelia Vico . . . . . CK-14.2 FRI (p202)
TROISI, TESS . . . . . . . . . . ∙EB-9.6 WED (p135)
Trost, Florian . . . . . . . . . . . . JSI-5.2 THU (p145)
Trotta, Rinaldo . . . . . . . . . . . . EB-5.3 TUE (p95),
EA-4.4 THU (p160)
Trovatello, C. . . . . . . . . . . . . . ∙EI-2.1 FRI (p188)
Trovatello, Chiara . . . . . . . . . . EI-4.2 FRI (p212)

Trubetskov, Michael . . . . . PD-1.4 THU (p170),
CH-13.1 FRI (p181)
Trull, Jose . . . . . . . . . . . . . CD-P.31 TUE (p102),
CD-7.5 WED (p112), EH-3.5 THU (p152),
EH-P.19 THU (p179)
Truong, Gar-Wing . . . . . . . CE-3.2 MON (p67),
CE-6.1 THU (p157)
Truong, Mihn Duy . . . . . . CK-P.37 TUE (p106)
Truong, Minh Duy . . . . . . CH-1.6 MON (p57),
EG-P.7 TUE (p107), CH-P.29 WED (p137)
Truong, Tran-Chau . . . . . . . CF-3.2 MON (p67)
Tsang, Hon Ki . . . . . . . . . . CK-11.1 THU (p162)
Tsarapkin, Aleksei . . . . . ∙EH-5.6 THU (p168)
Tsarev, Maxim . . . . . . . . . . . . EG-3.5 MON (p70)
Tschernajew, Maxim . . . . . CF-P.21 TUE (p103)
Tschernig, Konrad . . . . . EA-P.16 THU (p175)
Tseng, Chin-Hao . . . . . . . . . . . CI-8.4 FRI (p214)
Tsibidis, George . . . . . . . . ∙CM-5.3 TUE (p91),∙CM-9.1 FRI (p188), ∙CM-9.5 FRI (p196)
Tsigaridas, George . . . . . CH-P.17 WED (p137)
Tsigaridas, Georgios . . . . . CL-2.2 THU (p151)
Tsilikas, Ioannis . . . . . . . CH-P.17 WED (p137),
CL-2.2 THU (p151), JSIII-3.4 FRI (p187)
Tsilipakos, Odysseas . . . . CM-1.4 MON (p54),
PP-1.8 MON (p64), CM-P.4 MON (p77),∙CK-P.41 TUE (p106),∙EH-3.3 THU (p150), CM-9.1 FRI (p188),
CM-11.4 FRI (p214)
Tsirigotis, Aris . . . . . . . . CH-P.17 WED (p137),
CL-2.2 THU (p151), ∙JSIII-3.4 FRI (p187)
Tsitavets, Yana . . . . . . . . . . . . EJ-P.9 MON (p80)
Tsouassis, Simon . . . . . . . . . CB-P.9 MON (p76)
Tsui, Hei Chit Leo . . . . . . . . CE-1.1 MON (p53)
Tsujimoto, Yoshiaki . . . . ∙EB-12.4 THU (p161)
Tsukerman, Igor . . . . . . . . ∙EH-1.5 WED (p134)
Tsusaka, Hiroki . . . . . . . . . EE-P.2 WED (p138),∙EE-5.6 FRI (p217)
Tu, Yiming . . . . . . . . . . . . . . ∙CJ-4.1 WED (p123)
Tuchin, Valery . . . . . . . . . . . . EJ-P.6 MON (p80)
Tuennermann, Andreas . ∙CA-7.1 WED (p122)
Tul Noor, Atia . . . . . . . . . . . JSI-5.3 THU (p145)
Tümmler, Johannes . . . . . . JSI-3.1 WED (p122)
Tung, Jung-Chen . . . . . . . . ∙CE-P.8 THU (p172)
Tuniz, Alessandro . . . . . . . CD-2.3 MON (p60)
Tünnermann, Andreas . . . . . CJ-1.3 TUE (p97),
CJ-8.2 FRI (p192)
Tünnermann, Henrik . . . . JSI-P.4 WED (p141)
Tuorila, Heidi . . . . . . . . . . . . ∙CB-5.5 TUE (p96)
Turchanin, Andrey . . . . . . . CD-2.3 MON (p60)
Turchinovich, Dmitry . . . . CE-7.1 THU (p163)
Turitsyn, Sergei . . . . . . . . . . . CJ-P.17 FRI (p221)
Turley, Freya . . . . . . . . . . . . ∙CL-4.1 THU (p163)
Turnár, Szabolcs . . . . . . . . ∙CC-P.15 FRI (p218)
Turner, James . . . . . . . . . . . . JSI-4.6 WED (p134)
Turnšek, J. . . . . . . . . . . . . . . . JSI-4.5 WED (p132)
Turo, Bryan . . . . . . . . . . . . . . . CF-4.2 TUE (p83)
Turpaud, Victor . . . . . . . . . . ∙CD-5.5 TUE (p91)
Turpin, Elsa . . . . . . . . . . . . . . CJ-2.5 WED (p115)
Tusnin, Aleksandr . . . . . . . EF-3.1 THU (p142),
EF-3.2 THU (p142), ∙EC-1.2 FRI (p183),
EF-9.2 FRI (p203)
Tuthill, Peter . . . . . . . . . . . . JSII-3.3 MON (p69)
Twayana, Krishna . . . . . . . CD-P.1 TUE (p100),∙CF-P.7 TUE (p102)
Tyazhev, Aleksey . . . . . . . . . CA-2.4 MON (p62)
Tyborski, Christoph . . . . . ∙CE-P.9 THU (p172)

252

Tye, Caitlin . . . . . . . . . . . . ∙CH-11.2 THU (p159)
Tykalewicz, Boguslaw . . . CA-8.3 WED (p118)
Tykalewiz, Boguslaw . . . . CA-8.4 WED (p118)
Tyulnev, Igor . . . . . . . . . . . . CD-P.5 TUE (p100),∙CD-7.1 WED (p108), ∙EC-P.6 FRI (p223)
Tzallas, Paraskevas . . . . . ∙CG-5.5 THU (p161)
Tzortzakis, Stelios . . . . . . . CM-3.2 MON (p66),
CM-P.12 MON (p77), EE-2.3 FRI (p187),
CC-6.3 FRI (p204)
Tzortzakis, Stelios Tzortzakis
CM-11.4 FRI (p214)

U
Uchida, Atsushi . . . . . . . . . CD-P.17 TUE (p101)
Uchida, Kento . . . . . . . . . . ∙EE-1.2 WED (p109),
EE-P.9 WED (p139)
Udem, Thomas . . . . . . . . . ∙ED-1.3 MON (p55),
CK-7.3 WED (p132), PD-2.1 THU (p170)
Ueda, Kiyoshi . . . . . . . . . . . JSI-2.5 WED (p118)
Ueno, Keiji . . . . . . . . . . . . . . . . . EI-P.2 FRI (p224)
Uji, Yoshiki . . . . . . . . . . . . . . CI-3.5 WED (p127)
Ul-Hassan, Jawad . . . . . . . EB-11.1 THU (p149)
Ulanov, Alexander . . . . . ∙CK-9.4 THU (p152),
CK-9.5 THU (p154)
Ulčinas, Orestas . . . . . . . . . . CM-4.4 TUE (p86)
Ulibarenna, Andrés . . . . . . EB-9.3 WED (p131)
Ullsperger, Tobias . . . . . . . CG-4.4 THU (p153)
Ulmer, Anatoli . . . . . . . . . . . JSI-3.1 WED (p122)
Umair, Muhammad A. . . . . CC-4.4 FRI (p184)
Umeki, Takeshi . . . . . . . . . . EA-2.2 THU (p142),
EA-2.6 THU (p148), EA-3.6 THU (p154)
Umezawa, Toshimasa . . ∙CI-3.2 WED (p125),
CB-10.5 THU (p160)
Undisz, Andreas . . . . . . . . . CM-2.1 MON (p58)
Unger, Sonja . . . . . . . . . . . . . . CE-1.3 MON (p55)
Unterrainer, Karl . . . . . . . . . CC-4.2 FRI (p180),
CC-7.2 FRI (p210)
Urban, David . . . . . . . . . . . . . ∙EI-3.5 FRI (p208)
urech, alex . . . . . . . . . . . . . . . EA-P.9 THU (p175)
Uren, Robin . . . . . . . . . . . . CM-P.30 MON (p78)
Urvoy, Alban . . . . . . . . . . . . . . EB-5.2 TUE (p93),
EA-2.3 THU (p144), EA-7.4 FRI (p196)
Usenko, Sergey . . . . . . . . . . JSI-P.2 WED (p141)
Ustimchik, Vasilii . . . . . . . . CJ-5.1 WED (p129)
Utéza, Olivier . . . . . . . . . . . CM-3.4 MON (p68),
CL-4.2 THU (p165), CM-10.4 FRI (p206)
Utke, Ivo . . . . . . . . . . . . . . . . EH-5.6 THU (p168)
Uto, Takahiro . . . . . . . . . . . . . . EI-4.1 FRI (p210)
Uusitalo, Topi . . . . . . . . . . . EG-1.4 MON (p56),
PP-2.3 WED (p120), CE-P.3 THU (p171)
Uvarova, Anastasia . . . . . ∙CA-3.5 MON (p72),
CF-P.4 TUE (p102)
Uzan, Ayelet J. . . . . . . . . . . . CG-5.4 THU (p161)

V
Vabek, Jan . . . . . . . . . . . . . . . CG-6.2 THU (p165)
Vagniluca, Ilaria . . . . . . . . EB-P.22 THU (p177)
Vahl, Alexander . . . . . . . . . CK-P.19 TUE (p105)
Vahlbruch, Henning . . . . . EA-5.2 THU (p164)
Vaia, Richard A. . . . . . . . . CD-P.11 TUE (p100),
CD-P.16 TUE (p100)
Vailakis, George . . . . . . . . . . . . EI-1.2 FRI (p182)
Vainio, Markku . . . . . . . . . CH-5.3 WED (p115),
CH-P.6 WED (p136), CH-14.3 FRI (p195)

Vaissiere, Nicolas . . . . . . . . . CB-5.3 TUE (p94)
Valdivia-Berroeta, Gabriel A.
CC-3.2 THU (p165)
Valencia Molina, Laura Daniela∙PD-2.9 THU (p171)
Valente, Denise . . . . . . . . . CD-P.11 TUE (p100)
Valentin, Constance . . . . . CG-4.6 THU (p155),
CG-P.4 THU (p173)
Valentini, Gianluca . . . . . CH-8.4 WED (p133)
Valeri, Mauro . . . . . . . . . . . . . EB-5.3 TUE (p95)
Valiente, Manuel . . . . . . . . . CH-15.1 FRI (p201)
Valiente, Rafael . . . . . . . . . . . CE-1.4 MON (p55)
Valiulis, Gintaras . . . . . . CD-10.6 WED (p134)
Vallan, Alberto . . . . . . . . . . CL-2.5 THU (p153),
CH-11.5 THU (p161)
Valle, Angel . . . . . . . . . . . . . ∙CB-P.8 MON (p76),∙EB-P.8 THU (p176)
Valle-Miñon, Marcos . . . . . EB-P.8 THU (p176)
Vallée, Fabrice . . . . . . . . . . . JSVI-1.4 TUE (p89)
Vallée, Réal . . . . . . . . . . . . . . CE-1.2 MON (p53),
CJ-6.5 THU (p147)
Vallés, Adam . . . . . . . . . . . . . . CM-4.6 TUE (p88)
Vallet, Marc . . . . . . . . . . . . . . CA-4.2 TUE (p82),
CA-4.5 TUE (p86), CI-2.3 WED (p121)
Vallon, Raphaël . . . . . . . . . . CH-16.5 FRI (p217)
Vamos, Lenard . . . . . . . . . ∙CD-P.5 TUE (p100),
EC-P.6 FRI (p223)
van Breugel, Suse J. . . . . . ∙PP-2.8 WED (p121),∙CL-5.5 FRI (p187), ∙CL-P.2 FRI (p221)
van de Groep, Jorik . . . . . EH-4.3 THU (p158),
CK-13.6 FRI (p196)
van den Hove, Daniel . . . . . CL-1.4 MON (p71)
van der Geest, Maarten . . . CF-2.3 MON (p61)
van der Hoeven, Maarten
CK-P.21 TUE (p105)
van der Laan, Fons . . . . . . . . EB-1.3 MON (p55)
van der Meer, Harmen . . EA-P.11 THU (p175)
Van der Sande, Guy . . . ∙JSIII-1.2 THU (p158),
JSIII-P.5 FRI (p224), JSIII-P.8 FRI (p224),
JSIII-P.9 FRI (p225)
van der Slot, Peter . . . . . . . . . CB-5.1 TUE (p92)
van der Vegt, Jaap J.W. . . CK-P.25 TUE (p105),
CK-P.30 TUE (p105), CK-P.38 TUE (p106),
CK-11.2 THU (p164)
Van Erps, Jürgen . . . . . . . . CK-P.20 TUE (p105)
van Gorp, Freek . . . . . . . . ∙EH-4.3 THU (p158)
van Kempen, Kees . . . . . . . CH-16.2 FRI (p213)
Van Laer, Raphaël . . . . . . . . CK-1.4 MON (p68)
van Leent, Tim . . . . . . . . . . . ∙EB-5.1 TUE (p93),
EB-9.2 WED (p131)
van Rees, Albert . . . . . . . . . . . CB-5.1 TUE (p92)
Van Stryland, Eric . . . . . . . CE-7.1 THU (p163)
van Thiel, Thierry . . . . . . EB-13.2 THU (p165)
Van Vaerenbergh, Thomas
CK-P.11 TUE (p104)
Vanackere, Tom . . . . . . . . . . CD-3.2 MON (p68)
Vandekerckhove, Tom . . . ∙CD-3.2 MON (p68)
Vanderhaegen, Aline . . . . . EF-9.3 FRI (p205),∙CF-11.1 FRI (p201)
Vandezande, Wouter . . . . . CH-15.3 FRI (p205)
Vaneecloo, Julien . . . . . . . . . . EA-8.2 FRI (p202)
Vanholsbeeck, Frédérique CL-P.11 FRI (p222)
Vanmol, Koen . . . . . . . . . . . CK-P.20 TUE (p105)
Vanna, Renzo . . . . . . . . . . . . CH-2.1 MON (p58),
CL-6.1 FRI (p189), CL-6.5 FRI (p197),
CD-13.2 FRI (p203)

Authors' Index

VANVINCQ, Olivier . . . . CA-7.3 WED (p126),
CH-P.1 WED (p136), ED-6.6 FRI (p196)
Várallyay, Zoltán . . . . . . . . CF-P.21 TUE (p103)
Varanavičius, Ar ūnas . . CD-10.6 WED (p134)
Vardanyan, Vahagn . . . . . . JSI-P.3 WED (p141)
Varghese, Thejus . . . . . . . . . CE-2.1 MON (p59)
Varjú, Katalin . . . . . . . . . . . CG-4.5 THU (p153),
CG-P.3 THU (p173)
Varming, Poul . . . . . . . . . . CK-P.35 TUE (p106),
CJ-P.22 FRI (p221)
Varshney, Ravendra K. . . ∙EH-P.8 THU (p178)
Varshney, Shailendra K. . . . . CI-P.3 FRI (p219)
Varshney, Shailendra Kumar
EH-P.15 THU (p179)
Vasileiadis, Thomas . . . . . CG-3.5 THU (p147)
Vasko, Kostiantyn . . . . . . . . CE-2.3 MON (p61),
CJ-4.2 WED (p123)
Vast, Nathalie . . . . . . . . . . . . JSVI-2.3 TUE (p97)
Vavassori, Paolo . . . . . . . . . EH-2.4 THU (p146)
Védrine, Christophe . . . . . . CL-P.15 FRI (p222)
Vega, Andrés . . . . . . . . . . . . EB-8.4 WED (p125),
EB-P.34 THU (p178), EA-6.3 FRI (p186)
Veilleux, Sylvain . . . . . . . . ∙JSII-1.1 MON (p53)
Veisz, Laszlo . . . . . . . . . . . . . CG-3.6 THU (p149)
Velasco, Cruz I. . . . . . . . . . ∙EG-P.1 TUE (p106)
Velez, Christian . . . . . . . . CB-11.6 THU (p168)
Velkov, Dimitar . . . . . . . . CA-10.5 THU (p146)
Vella , Angela . . . . . . . . . . . EG-P.5 TUE (p107),∙CH-6.6 WED (p120),∙EE-P.5 WED (p138), CC-2.4 THU (p163),
CC-7.3 FRI (p212), CC-7.6 FRI (p216)
Velmiskin , Vladimir . . . . . CJ-5.3 WED (p131)
Velmuzhov, Alexander . . . . CA-1.2 MON (p52)
Velpula, Praveen K. . . . . . CF-10.1 THU (p143)
Velsink, Matthijs . . . . . . CH-P.24 WED (p137),∙CH-14.5 FRI (p197)
Venet, Caroline . . . . . . . . . . CL-2.3 THU (p151)
Vengelis, Julius . . . . . . . . . . . CD-P.8 TUE (p100)
Vengris, Mikas . . . . . . . . . . . CM-1.1 MON (p52)
Venkat, Prachi . . . . . . . . . . . ∙CM-5.5 TUE (p91)
Venkataraman, Vivek . . . CD-P.32 TUE (p102)
Venkatasubramani, Lakshmi Narayanan
CI-6.1 FRI (p188)
Venkatesan, Sandhya . . . . . . EE-4.3 FRI (p205)
Venkitesh, Deepa . . . . . . . . . . CI-6.1 FRI (p188),
CI-7.3 FRI (p204), CI-P.10 FRI (p219)
Venturi, Linda . . . . . . . . . . CH-6.6 WED (p120)
Verhoef, Aart . . . . . . . . . . . ∙CH-1.5 MON (p57),
CL-7.6 FRI (p209)
Verlot, Pierre . . . . . . . . . . . . . . EA-9.2 FRI (p210)
Verma, Abhinav . . . . . . . . . ∙EA-P.6 THU (p175)
Vermeulen, Nathalie . . . . ∙CE-7.1 THU (p163)
Vernuccio, Federico . . . . . CH-2.1 MON (p58),
CL-6.1 FRI (p189), ∙CD-13.2 FRI (p203)
Veron, Emmanuel . . . . . . . . . CE-4.5 TUE (p99)
Verschaffelt, Guy . . . . . . JSIII-1.2 THU (p158),
JSIII-P.5 FRI (p224), JSIII-P.8 FRI (p224),
JSIII-P.9 FRI (p225)
Versmold, Carlotta . . . . . . . EA-P.1 THU (p174)
Versteeg, Rolf . . . . . . . . . . . EE-1.5 WED (p113)
Veselov, Dmitry . . . . . . . . . . CB-9.5 THU (p152)
Veselský, Karel . . . . . . . . . ∙CA-P.10 MON (p74)
Vestergaard, Lea . . . . . . . . . CK-4.5 WED (p114)
Vewinger, Frank . . . . . . . . CD-7.4 WED (p112),
PD-1.8 THU (p170)
Vexiau, Romain . . . . . . . . . . . EA-7.5 FRI (p196)

Veyrinas, Kevin . . . . . . . . . CG-4.6 THU (p155)
Vezzoli, Stefano . . . . . . . . . EH-1.3 WED (p132)
Vialla, Fabien . . . . . . . . . . . . JSVI-1.4 TUE (p89)
Viana, Bruno . . . . . . . . . . . . CA-3.2 MON (p68),
CE-4.4 TUE (p97), ∙CE-4.5 TUE (p99),
CE-10.4 FRI (p206)
Vicencio, Rodrigo . . . . . . ∙CK-P.31 TUE (p106)
Vicencio, Rodrigo A. . . . CK-P.16 TUE (p105),
CK-P.27 TUE (p105), CK-12.3 FRI (p182)
Vicencio, Rodrigo Andres CK-P.1 TUE (p104)
Vicidomini, Giuseppe . . CH-6.4 WED (p118),
CL-6.3 FRI (p195)
Vidal, Cynthia . . . . . . . . . . . ∙EG-1.2 MON (p54)
Vidal, Xavier . . . . . . . . . . . . . . CA-5.3 TUE (p96)
Viedma, David . . . . . . . . . . . ∙EC-P.5 FRI (p223)
Viejo Rodríguez, Alba . . . . CE-P.1 THU (p171)
Viellerobe, Bertrand . . . . . CL-2.4 THU (p153)
Vievard, Sebastien . . . . . . . JSII-1.3 MON (p55)Vigne, Nathan . . . . . . . . . . CD-8.4 WED (p118),
EF-4.2 THU (p152), ∙EF-4.3 THU (p152),
EF-5.2 THU (p158)
Vignjevic, Luka . . . . . . . . . . . ∙EC-P.9 FRI (p223)
Viheriälä, Jukka . . . . . . . . . . . CB-5.5 TUE (p96),
PP-2.3 WED (p120), CE-P.3 THU (p171)
Vijayan, Ponraj . . . . . . . . CK-11.5 THU (p168),
EA-P.12 THU (p175)
Viktorov, Evgeny . . . . . . . . CB-7.3 WED (p130),
EF-P.24 WED (p141)
Vila-Comamala, Joan . . . . JSI-1.4 WED (p112)
Vilaseca, Ramon . . . . . . . CD-P.31 TUE (p102),
CD-7.5 WED (p112)
Vildoso, Paloma . . . . . . . . ∙CK-P.1 TUE (p104),∙CK-12.3 FRI (p182)
Villa, Andrea . . . . . . . . . . . . ∙CF-P.9 TUE (p103),
EI-4.4 FRI (p214)
Villa, Nicolas . . . . . . . . . . . . CL-3.1 THU (p157),
CL-3.4 THU (p161)
Villafane, Viviana . . . . . . . EB-12.3 THU (p159)
Villanueva, Luis Guillermo
JSII-2.4 MON (p63), CD-5.2 TUE (p90)
Villas-Boas, Celso J. . . . . EB-11.2 THU (p151),
EB-11.5 THU (p153)
Villatoro, Joel . . . . . . . . . . . CH-8.6 WED (p135)
Vilson, Alex . . . . . . . . . . . . . . . CI-6.5 FRI (p196)
Vincenti, Maria A. . . . . . CD-P.31 TUE (p102)
Vincenti, Maria Antonieta
CD-7.5 WED (p112)
Vincenti, Maria Antonietta
EH-3.5 THU (p152)
Vincetti, Luca . . . . . . . . . . . . CE-2.3 MON (p61)
VINCI, Tommaso . . . . . . CG-P.14 THU (p174)
Vinel, Vincent . . . . . . . . . . . . EG-2.1 MON (p58)
Viotti, Anne-Lise . . . . . . . PD-1.3 THU (p170)
Virgili, Tersilla . . . . . . . . . . CH-8.4 WED (p133)
Virkkula, Aki . . . . . . . . . . . CH-P.6 WED (p136)
Virtanen, Heikki . . . . . . . . PP-2.3 WED (p120),
CE-P.3 THU (p171)
Virte, Martin . . . . . . . . . . . . PP-1.10 MON (p64),
CB-P.13 MON (p76), CB-P.18 MON (p76),
CB-P.22 MON (p76), CK-P.20 TUE (p105),
CB-6.3 WED (p126), CI-4.5 WED (p133),
EF-P.4 WED (p139), EF-P.14 WED (p140)
Vismarra, Federico . . . . . . ∙CF-1.3 MON (p57),
CF-3.3 MON (p69), CG-5.3 THU (p159),∙EE-3.1 FRI (p189), EE-3.4 FRI (p197)
Visser, Tess . . . . . . . . . . . . . . . CH-4.5 TUE (p98)

Vissers, Ewoud . . . . . . . . . . . CD-3.2 MON (p68)
Vitali, Valerio . . . . . . . . . . . ∙CK-P.2 TUE (p104),
CK-5.2 WED (p116), CK-6.3 WED (p124),
CE-8.6 FRI (p186)
Vitanov, Nikolay V. . . . . . EB-11.5 THU (p153)
Viti, Leonardo . . . . . . . . . . . . CC-4.4 FRI (p184)
Vitiello, Miriam . . . . . . . . . . CC-4.4 FRI (p184),
CK-13.5 FRI (p196)
Vittadello, Laura . . . . . . ∙CH-P.5 WED (p136),
CE-P.12 THU (p172)
Vivien, Laurent . . . . . . . . . . CD-3.5 MON (p72),
EB-3.1 MON (p67), CD-5.5 TUE (p91)
Vladimirova, Anastasiia . . . EC-2.5 FRI (p197)
Vlasov, Aleksandr . . . . . ∙PP-2.3 WED (p120),∙CE-P.3 THU (p171)
Vlieg, Elger . . . . . . . . . . . . . . JSIII-3.1 FRI (p181)
Vlieg, Elger A. . . . . . . . . . JSIII-2.2 THU (p164),∙JSIII-4.4 FRI (p197)
Vlk, Marek . . . . . . . . . . . . . . . . CH-3.1 TUE (p82)
Vo Van Qui, Henri . . . . . . . CD-1.3 MON (p54)
Vocanson, Francis . . . . . . . EH-4.5 THU (p160)
Vodopyanov, Konstantin . . CF-3.1 MON (p67)
Vogel, Sönke . . . . . . . . . . . . CM-P.24 MON (p78)
Vogel, Tim . . . . . . . . . . . . . . CC-2.1 THU (p157),
CC-3.1 THU (p163), ∙CC-7.4 FRI (p214),
CC-P.3 FRI (p218), CC-P.7 FRI (p218)
Vogeley, Nick . . . . . . . . . . . CH-P.2 WED (p136)
Vogler-Neuling, Viola V. . EH-4.1 THU (p156)
Vogler-Neuling, Viola Valentina∙CD-1.2 MON (p54)
Vogt, Dominik . . . . . . . . . . . . CC-6.5 FRI (p208)
Vogwell, Josh . . . . . . . . . . . . EE-P.1 WED (p138)
Voicu, Flavius-Marian . . . . CA-P.4 MON (p74)Vojtěch, Josef . . . . . . . . . . . . . . CI-8.1 FRI (p210)
Vollmer, Sergej . . . . . . . . . . EA-4.6 THU (p162)
Voloshin, Andrey . . . . . . . . ∙CB-5.4 TUE (p96),
CK-9.2 THU (p150), CK-14.1 FRI (p200)
Volpe, Giorgio . . . . . . . . . . . CK-14.3 FRI (p204)
Volpert, Marion . . . . . . . . CH-P.22 WED (p137)
Volpp, Joerg . . . . . . . . ∙CM-LIM.2 WED (p117)
Volz, Jürgen . . . . . . . . . . . . . . ∙EA-1.2 TUE (p83),
EA-7.2 FRI (p190)
Volz, Sebastian . . . . . . . . . JSVI-1.3 TUE (p87),
JSVI-2.2 TUE (p95)
vom Bruch, Felix . . . . . . . . . EA-5.5 THU (p168)
vom Hövel, Thilo . . . . . . . CD-7.4 WED (p112)
von der Weid, Jean Pierre CJ-P.16 FRI (p220)
Vorobev , Artem S . . . . . . . CK-P.6 TUE (p104),
CK-P.32 TUE (p106),∙CH-P.14 WED (p136)
Voronin, Aleksandr . . . . . . . . CF-5.5 TUE (p99)
Vos, Willem L . . . . . . . . . . . CH-1.6 MON (p57),
CK-P.25 TUE (p105), CK-P.30 TUE (p105),∙CK-P.33 TUE (p106),∙CK-P.37 TUE (p106),∙CK-P.38 TUE (p106), EG-P.7 TUE (p107),
PP-2.6 WED (p121),∙CH-P.29 WED (p137),
CK-11.2 THU (p164), CI-P.13 FRI (p219)
Vosoughi Lahijani, Babak . EC-2.5 FRI (p197)
Voumard, Thibault . . . . . . JSII-2.4 MON (p63),
CK-9.5 THU (p154)
Vovla, Stavroula . . . . . . . . . . CM-6.3 TUE (p94)
Vozzi, Caterina . . . . . . . . . . CF-2.5 MON (p63),
CM-6.3 TUE (p94), JSI-5.5 THU (p149),
CG-3.2 THU (p143), CE-P.10 THU (p172)

253

Vrakking, Marc . . . . . . . . . . . CM-6.4 TUE (p96)
Vrakking, Marc J.J. . . . . . . JSI-3.1 WED (p122),
CG-4.5 THU (p153), CG-6.4 THU (p169),
EE-3.2 FRI (p193)
Vrehen, Joris . . . . . . . . . . . . PP-2.6 WED (p121),
CI-P.13 FRI (p219)
Vreman, Timon J. . . . . . . . CK-P.33 TUE (p106)
Vučković, Jelena . . . . . . . . . . CD-5.1 TUE (p90),
EA-2.4 THU (p144), EB-11.1 THU (p149)
Vukovic, Natasha . . . . . . ∙CH-11.4 THU (p161)
Vurpillot, François . . . . . . CH-6.6 WED (p120)
Vyhlidal, David . . . . . . . . . . . CA-P.8 MON (p74)

W
W. Larsen, Esben . . . . CM-LIM.3 WED (p117)
Wabnitz, Stefan . . . . . . . . . ∙EF-1.1 WED (p123),
EF-4.4 THU (p154), ED-5.5 FRI (p186),
EF-7.1 FRI (p181), EF-7.4 FRI (p185),
EF-7.5 FRI (p187), EJ-3.3 FRI (p185)
Wackerow, Stefan . . . . . . CM-P.30 MON (p78),
CK-P.13 TUE (p104)
wada, Koshiro . . . . . . . . . . . . . CI-8.3 FRI (p212)
Wada, Shin-ichi . . . . . . . . . JSI-2.4 WED (p118)
Wadsworth, William J. . . . . CD-4.2 TUE (p82)
Wagner, Jonas . . . . . . . CM-LIM.4 WED (p119)
Wagner, Lukas . . . . . . . . . . . EA-5.1 THU (p162)
Wagnon, Benoit . . . . . . . . . . CK-12.6 FRI (p186)
Wahid, Ammar bin . . . . . . . . EE-4.1 FRI (p201)
Wahn, Hannes . . . . . . . . . . . . CL-1.2 MON (p69)
Wai, P. K. A. . . . . . . . . . . . . CD-P.27 TUE (p101),
CF-P.1 TUE (p102), CJ-3.2 WED (p117)
Wakui, Kentaro . . . . . . . . . EB-12.4 THU (p161)
Walbaum, Till . . . . . . . . . . . . . . CJ-1.4 TUE (p97)
Walch, Pierre . . . . . . . . . . . . CD-P.7 TUE (p100),
CD-8.1 WED (p114)
Walden, Sarah L. . . . . . . ∙CK-10.1 THU (p156)
Wale, Michael . . . . . . . . . . . . CK-15.2 FRI (p210)
Walke, Daniel . . . . . . . . . . CG-P.16 THU (p174)
Wallace, James Kent . . . . . JSII-1.4 MON (p57)
Wallace, Michael . . . . . . . CK-P.34 TUE (p106)
Wallace, Patrick . . . . . . . . . JSI-P.6 WED (p141)
Wallin, Anders . . . . . . . . . . . ED-P.3 MON (p79)
Wallmeier, Kristin . . . . . . ∙CH-13.5 FRI (p187)
Walmsley, Ian . . . . . . . . . . EB-10.4 THU (p145),
EB-12.5 THU (p161)
Walmsley, Ian A. . . . . . . . . CM-7.5 WED (p112)
Walschaers, Mattia . . . . . . EB-8.3 WED (p125),
EB-12.2 THU (p159)
Walsh, Mathieu . . . . . . . . . . ED-2.6 MON (p63)Walther, Nico . . . . . . . . . . . CF-P.21 TUE (p103)
Wan, Qiuming . . . . . . . . . . . EE-P.2 WED (p138)
Wan, Yating . . . . . . . . . . . . . . . CB-5.6 TUE (p98)
Wang, Andong . . . . . . . . . . ∙CM-2.2 MON (p58)
Wang, Benquan . . . . . . . . . . PP-1.6 MON (p64),∙PP-1.7 MON (p64), CH-P.4 WED (p136),∙CH-P.8 WED (p136)
Wang, Bin . . . . . . . . . . . . . . . . CF-2.1 MON (p59)
Wang, Chengli . . . . . . . . . . . . CE-8.1 FRI (p180)
Wang, Chun-Ta . . . . . . . . CH-P.30 WED (p138)
Wang, Daqing . . . . . . . . . . CH-P.2 WED (p136),
EA-9.6 FRI (p216)
Wang, Di . . . . . . . . . . . . . . . . . CI-P.11 FRI (p219)
Wang, Dongze . . . . . . . . . . CK-11.5 THU (p168)
Wang, Geyang . . . . . . . . . . . . PP-1.2 MON (p64),∙CA-P.13 MON (p74), CA-P.21 MON (p75),

CA-10.1 THU (p142)
Wang, Hao . . . . . . . . . . . . . . ∙JSIII-P.4 FRI (p224)
Wang, Haochuan . . . . . . . . CF-10.6 THU (p149)
Wang, Hsuan-Sen . . . . . . . . ∙CE-3.1 MON (p67)
Wang, Hui . . . . . . . . . . . . . . ∙EB-P.7 THU (p176)
Wang, Huijun . . . . . . . . . . . . ∙CM-4.3 TUE (p84)
Wang, Hushan . . . . . . . . . . . CF-P.11 TUE (p103)
Wang, Jingjing . . . . . . . . . CH-P.36 WED (p138)
Wang, Kai . . . . . . . . . . . . . . CK-4.4 WED (p112),
CA-9.6 WED (p134), PD-1.6 THU (p170)
Wang, Lan . . . . . . . . . . . . . . . . EG-3.2 MON (p66)
Wang, Li . . . . . . . . . . . . . . . . . CA-2.1 MON (p58),
CA-10.3 THU (p144), CA-10.6 THU (p148)
Wang, Lingxiao . . . . . . . . . . . CC-6.1 FRI (p200)
Wang, Luyao . . . . . . . . . . . ∙EH-4.4 THU (p160)
Wang, Qi Jie . . . . . . . . . . . . . . EG-3.2 MON (p66)
Wang, Qing . . . . . . . . . . . ∙EF-P.18 WED (p140),
CL-P.7 FRI (p222)
Wang, Qizhou . . . . . . . . . . . CH-2.2 MON (p58),
JSIII-P.6 FRI (p224), JSIII-P.12 FRI (p225)
Wang, Ru-Pan . . . . . . . . . . . JSI-4.6 WED (p134)
Wang, Rui . . . . . . . . . . . . . . . . . CK-3.4 TUE (p96)
Wang, Rui Ning . . . . . . . . . . . CB-5.4 TUE (p96),
CK-4.2 WED (p110), PP-2.2 WED (p120),
CE-P.2 THU (p171), CE-8.1 FRI (p180),
CE-8.2 FRI (p180), CE-9.1 FRI (p188),
CK-14.1 FRI (p200), EF-9.2 FRI (p203)
Wang, Ruijun . . . . . . . . . . . CK-6.2 WED (p124),
CB-9.3 THU (p150)
Wang, Shu Min . . . . . . . . . . EA-3.1 THU (p148)
Wang, Sitong . . . . . . . . . . . . . CI-P.11 FRI (p219)
Wang, Siyang . . . . . . . . . . . . PD-1.5 THU (p170)
Wang, Wenlong . . . . . . . . . CD-9.3 WED (p124)
Wang, Xianglin . . . . . . . . . . CF-P.11 TUE (p103)
Wang, Xiaocong . . . . . . . . . . ∙CD-4.6 TUE (p88)
Wang, Xinyue . . . . . . . . . . . CE-P.22 THU (p173)
Wang, Xiyue Sissi . . . . . . . ∙JSIII-4.3 FRI (p195)
Wang, Yangxiao . . . . . . . . . CA-P.10 MON (p74)
Wang, Yicheng . . . . . . . . . . . CA-2.2 MON (p60),∙CC-3.1 THU (p163), CF-12.2 FRI (p211)
Wang, Yishan . . . . . . . . . . . CF-P.11 TUE (p103)
Wang, Yu . . . . . . . . . . . . . . . . ∙PP-1.6 MON (p64),∙CH-P.4 WED (p136)
Wang, Yulei . . . . . . . . . . . . . . . CA-5.2 TUE (p94),
CA-5.5 TUE (p98)
Wang, Yunzhuo . . . . . . . . . . JSIII-4.2 FRI (p193)
Wang, Yutao . . . . . . . . . . ∙CK-10.4 THU (p160),
CK-14.4 FRI (p204)
Wang, Zhaohui . . . . . . . . . . CM-3.1 MON (p66)
Wang, Zhen . . . . . . . . . . . . . CH-14.2 FRI (p193)
Wang, Zhixin . . . . . . . . . . . CK-6.2 WED (p124),
CB-9.3 THU (p150)
Wang, Zilong . . . . . . . . . . . . CK-1.6 MON (p72),
PD-1.2 THU (p170)
Wang, Ziyao . . . . . . . . . . . CF-10.4 THU (p145),
EE-4.2 FRI (p203), ∙CJ-10.1 FRI (p210),
CJ-10.2 FRI (p210), CJ-10.3 FRI (p212)
Wanie, Vincent . . . . . . . . . . . PP-1.5 MON (p64),
CK-1.6 MON (p72), CD-P.2 TUE (p100),CG-3.2 THU (p143), EE-4.1 FRI (p201)
Ward, Matthew . . . . . . . . . . CH-P.6 WED (p136)
Ware, Matthew . . . . . . . . . . . JSI-5.4 THU (p147)
Warner, Craig . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)
Warner, Hana K. . . . . . . . . . CD-3.3 MON (p68)
Warren-Smith, Stephen . . . CJ-6.6 THU (p149)

Authors' Index

Wasiak, Michał . . . . . . . . . . . . CB-3.2 TUE (p84)
Wasige , Edward . . . . . . . . JSIII-5.5 FRI (p209),
JSIII-P.16 FRI (p225)
Wasilewski, Wojciech . . EB-10.6 THU (p149),
EA-P.21 THU (p175)
Watanabe, Eiichiro . . . . . . CK-P.17 TUE (p105)
Watanabe, Kei . . . . . . . . . . . EA-2.2 THU (p142),
EA-3.6 THU (p154)
Watanabe, Kenji . . . . . . . . PP-2.13 WED (p121),
EI-2.6 FRI (p196), EI-3.2 FRI (p204),
EI-4.2 FRI (p212), EI-4.5 FRI (p216),
EI-P.6 FRI (p224)
Wätzel, J. . . . . . . . . . . . . . . . . JSI-3.5 WED (p126)
Wayland, Jordan . . . . . . . EA-P.10 THU (p175)
Wcisło, Piotr . . . . . . . . . . . . . ED-1.2 MON (p53)
Weaver, Bruce . . . . . . . . . . . . ∙CK-3.4 TUE (p96)
Weaver, Matthew . . . . . . . EB-13.2 THU (p165)
Webb, Jonathan . . . . . . . . . ∙EB-9.3 WED (p131)
Weber, Jonas H. . . . . . . . . . . EA-5.1 THU (p162)
Weeks, Reagan . . . . . . . . . . . ED-2.1 MON (p59)
Wegener, Philipp . . . . . . . . . CA-3.5 MON (p72)
Wegner, Ulrike . . . . . . . . . . . . EE-4.3 FRI (p205)
Wei, Tingting . . . . . . . . . . CH-P.36 WED (p138)
Wei, Xiaoming . . . . . . . . . . CD-9.3 WED (p124)
Wei, Yi-An . . . . . . . . . . . . . . ∙CL-P.13 FRI (p222)
Wei, Zheng . . . . . . . . . . . . . . ∙CF-P.2 TUE (p102),
PD-1.4 THU (p170)
Wei, Zhiyi . . . . . . . . . . . . . . . . PP-1.2 MON (p64),
CA-P.13 MON (p74), CA-P.21 MON (p75),
CA-10.1 THU (p142)
Weidemann, Sebastian . PP-2.10 WED (p121),
EC-P.1 FRI (p222)
Weigand, Helena . . . . . . . . CD-1.2 MON (p54),∙EH-4.1 THU (p156)
Weigel, Alexander . . . . . . . CA-2.3 MON (p60),
CF-9.6 WED (p135), CL-2.1 THU (p149),
PD-1.4 THU (p170)
Weih, Robert . . . . . . . . . . . . CB-8.1 THU (p142),
CI-5.1 FRI (p180)
Weihs, Gregor . . . . . . . . . . . . EB-3.2 MON (p67)
Weikum , Eric Maximilian∙EG-P.5 TUE (p107)
Weil, Michael T. . . . . . . . . CH-P.27 WED (p137)
Weinfurter, Harald . . . . . . . . EB-5.1 TUE (p93),
PP-2.9 WED (p121), EB-9.2 WED (p131),
EA-P.1 THU (p174), EB-P.1 THU (p176)
Weise, Dennis . . . . . . . . . . . CF-7.3 WED (p117)
Weissbach, Margret . . . . . . . CM-9.4 FRI (p194)
Weissflog, Maximilian . . CK-10.6 THU (p162)
Weissflog, Maximilian A. . EG-5.3 TUE (p94),∙CK-10.2 THU (p158)
Weitenberg, Johannes . . . . ED-1.3 MON (p55),
PD-2.1 THU (p170)
Weitz, Martin . . . . . . . . . . CD-7.4 WED (p112),
PD-1.8 THU (p170)
Welch, Matthew . . . . . . . . . . . CI-7.5 FRI (p206)
Wen, Xiaoxiao . . . . . . . . . . ∙CF-P.8 TUE (p102),
CF-P.12 TUE (p103), CD-9.3 WED (p124)
Weng, Hao-Cheng . . . . . . ∙EB-6.5 WED (p113)
Wenger, Jérôme . . . . . . . . . . EG-1.2 MON (p54),
EG-5.5 TUE (p96), PP-2.12 WED (p121),
EH-P.16 THU (p179)
Wengerowsky, Sören . . . . . EB-9.4 WED (p133)
Wenthaus, Lukas . . . . . . . . . JSI-3.4 WED (p126)
Wenzel, Hans . . . . . . . . . . . . CB-P.5 MON (p75),
CB-4.4 TUE (p91), CF-6.5 WED (p113),

CB-10.4 THU (p160),
CB-11.2 THU (p164),
CB-11.4 THU (p166), CB-11.5 THU (p168)
Wernet, Philippe . . . . . . . . . . EE-3.3 FRI (p195)
Wernicke, Tim . . . . . . . . . . . CB-2.3 MON (p68)
Weßels, Peter . . . . . . . . . . . . CA-P.15 MON (p74)
Westerveld, Wouter J. . . . . . CK-3.1 TUE (p92)
Weston, Nick J. . . . . . . . . . . . . CH-4.2 TUE (p94)
Wetzel, B. . . . . . . . . . . . . . . EF-P.15 WED (p140)
Wetzel, Benjamin . . . . . . CD-9.1 WED (p122),
EF-P.10 WED (p140), EF-7.5 FRI (p187),∙CD-13.4 FRI (p205), EF-10.4 FRI (p215),
EE-5.3 FRI (p213)
Weyers, Markus . . . . . . . . . CK-7.2 WED (p130)
Wheatley, Robert . . . . . . . CE-P.18 THU (p172)
Wheatley, Robert Alastair . . CF-4.5 TUE (p89)
Wheeler, Natalie . . . . . . . . . CE-2.1 MON (p59),
CH-10.3 THU (p151)
Wheeler, Natalie V. . . . . . . CE-2.4 MON (p61),
CE-2.5 MON (p63), CH-10.4 THU (p153),
CJ-9.3 FRI (p204)
Whitaker, Mathew . . . . . . . CE-5.3 THU (p151)
Wicht, Andreas . . . . . . . . . . CB-P.5 MON (p75),
CB-10.4 THU (p160), CE-P.9 THU (p172)
Widengren, Jerker . . . . . . . . . CL-5.4 FRI (p187)
Wiebusch, Gerd . . . . . . . CH-P.28 WED (p137),
CL-P.16 FRI (p222)
Wiechert, Volker . . . . . . . . . . EG-5.4 TUE (p96)
Wieck, Andreas D. . . . . . . EA-5.1 THU (p162)
Wieczorek, Witlef . . . . . . . EA-3.1 THU (p148),
CK-15.3 FRI (p212)
Wiedemann, Philipp . . . . . . . EF-7.3 FRI (p183)
Wienke, Andreas . . . . . . . CD-P.24 TUE (p101),
CE-P.24 THU (p173)
Wieser, Wolfgang . . . . . . . . . . CL-8.1 FRI (p211)
Wigger, Daniel . . . . . . . . . . . . ∙EI-2.5 FRI (p196)
Wiggert, Moritz . . . . . . . . . . CJ-3.4 WED (p119)
Wijaya, Stefanus . . . . . . . . . . . EE-5.2 FRI (p211)
Wikmark, Hampus . . . . . . CG-4.6 THU (p155)
Wildi, Thibault . . . . . . . . . . JSII-2.4 MON (p63),
CK-4.4 WED (p112), CK-9.4 THU (p152),∙CK-9.5 THU (p154)
Wilk, Rafal . . . . . . . . . . . . . . ED-3.4 MON (p71),
ED-P.6 MON (p79), CH-P.35 WED (p138),
CC-6.5 FRI (p208)
Wilkinson, Iain . . . . . . . . . CG-P.16 THU (p174)
Will, Ingo . . . . . . . . . . . . . . . JSI-3.1 WED (p122)
Will, Jonathan . . . . . . . . . . . CF-9.3 WED (p131)
Willburger, Theresa . ∙CM-LIM.6 WED (p121)
Willenberg, Benjamin . . . CF-7.1 WED (p115),
CF-9.1 WED (p129), ∙CC-2.2 THU (p161)
Williams, Gregory . . . . . . . . . CJ-1.1 TUE (p93)
Williams, Kevin . . . . . . . . . . JSIII-P.7 FRI (p224)
Williamson, James . . . . . . CH-7.2 WED (p123),
CH-10.6 THU (p155)
Willke, Benno . . . . . . . . . . . EA-5.2 THU (p164)
Willms, Stephanie . . . . . . CD-9.4 WED (p124),
EF-P.1 WED (p139), EF-5.3 THU (p158)
Wilmart, Quentin . . . . . . . . . CD-6.4 TUE (p96)Wind, Nils . . . . . . . . . . . . . . . JSI-3.4 WED (p126)
Windeler, Robert . . . . . . . . . . CJ-1.1 TUE (p93)
Winge, David . . . . . . . . . . . . JSIII-5.2 FRI (p205)
Winghart, Marc-Oliver . . . EE-3.2 FRI (p193),∙EE-3.3 FRI (p195)
Winiger, Joel . . . . . . . . . . . . CD-1.2 MON (p54),
EH-4.1 THU (p156)

Winkelmann, Lutz . . . . . . . . EE-4.1 FRI (p201)
Winkler, Georg . . . . . . . . . . CE-6.1 THU (p157)
Winkler, Lisa . . . . . . . . . . . . . ∙CB-5.1 TUE (p92)
Winnerl, Stephan . . . . . . . ∙EE-P.3 WED (p138),
CC-P.7 FRI (p218)
Winter, Jan . . . . . . . . . . . . . . CM-P.6 MON (p77),
CM-10.5 FRI (p208)
Wirthl, Vitaly . . . . . . . . . . . . ED-1.3 MON (p55)Wirz, Witalij . . . . . . . . . . . . CA-6.6 WED (p114)
Wisal, Kabish . . . . . . . . . . . . . . CJ-1.5 TUE (p99),
CJ-6.6 THU (p149)
Wiśniewski, Piotr . . . . . . . . CK-P.9 TUE (p104)
Withford, Michael . . . . . . JSII-3.2 MON (p69),
CJ-4.6 WED (p127)
Withford, Michael J. . . . . . JSII-3.3 MON (p69),
CM-7.1 WED (p108)
Witlox, Martijn . . . . . . . . EA-P.11 THU (p175)
Witte, Stefan . . . . . . . . . . . . CF-P.15 TUE (p103),
CH-6.1 WED (p114),
CH-P.24 WED (p137), CG-P.7 THU (p174),
CH-14.5 FRI (p197)
Wittenbecher, Lucas . . . . . CH-13.3 FRI (p183)
Wittwer, Valentin J. . . . . . CG-4.4 THU (p153),
ED-6.4 FRI (p194)
Witz, Norbert . . . . . . . . . . CK-11.5 THU (p168)
Wohlfeil, Shulin . . . . . . . . ∙CF-6.5 WED (p113)
Wójtewicz, Szymon . . . . . . . ED-1.2 MON (p53)
Wojtusiak, Agnieska . . . . . CA-8.2 WED (p116)
Woldegeorgis, Abel H. . . CF-10.6 THU (p149)
Wolf, Alexey A. . . . . . . . . . . . CJ-P.20 FRI (p221)
Wolf, Jean-Pierre . . . . . . . . CD-8.1 WED (p114)
Wolf, Martin . . . . . . . . . . . . CG-3.5 THU (p147)
Wolf, Niels . . . . . . . . . . . . . . PD-1.8 THU (p170)
Wolf, Sebastian . . . . . . . . . EB-8.6 WED (p127),∙CL-5.2 FRI (p183)
Wolf, Thomas . . . . . . . . . . . . JSI-5.4 THU (p147)
Wolfersberger, Delphine . CB-7.2 WED (p130)
Wolff, Christian . . . . . . . . . . EB-1.2 MON (p55),
CK-13.1 FRI (p188)
Wolff, Joanna . . . . . . . . . . . . . ∙EI-3.1 FRI (p200)
Wöllenstein, Jürgen . . . . . . . CL-5.2 FRI (p183)
Wolley, Osian . . . . . . . . . . . . . EA-6.1 FRI (p180)
Wolterink, Tom . . . . . . . . . . . EB-2.3 MON (p61)
Wolterink, Tom A. W. . . ∙CK-12.2 FRI (p180),∙EA-8.4 FRI (p206)
Wolters, Janik . . . . . . . . . . EB-10.3 THU (p145),
JSIII-P.1 FRI (p224)
Won, Seungjai . . . . . . . . . ∙CD-P.13 TUE (p100)
Wondraczek, Katrin . . . . . . CE-1.4 MON (p55),
CJ-5.1 WED (p129)
Wong, Kai-Fu . . . . . . . . . . . ∙CK-1.6 MON (p72)
Wong, Kam Sing . . . . . . . . . EG-P.8 TUE (p107)
Wong, Kenneth . . . . . . . . . . EF-3.3 THU (p144)
Wong, Kenneth K. Y. . . . JSIII-1.5 THU (p160),
CH-15.2 FRI (p205)
Wong, Kenneth Kin-Yip . . CF-P.8 TUE (p102),
CF-P.12 TUE (p103), EJ-3.5 FRI (p187)
Woo, Taeho . . . . . . . . . . . . . CF-P.20 TUE (p103)
Wood, Thomas . . . . . . . . . . CK-5.6 WED (p120)
Wood , Vanessa . . . . . . . . . CD-1.2 MON (p54),
EH-4.1 THU (p156)
Wörner, Hans Jakob . . . . . . CF-1.3 MON (p57)
Wössner, Valentin . . . . . . . CG-6.5 THU (p169)
Wrachtrup, Joerg . . . . . . . . EB-7.2 WED (p117)
Wright, David . . . . . . . . . . . JSII-1.2 MON (p55),
PP-1.12 MON (p65), JSII-P.2 MON (p80)254

Wright, Hollie . . . . . . . . . . . . ∙CH-4.2 TUE (p94)
Wright, Lewis D. . . . . . . . . CA-6.3 WED (p110),
CE-9.2 FRI (p190)
Wright, Thomas . . . . . . . . . JSII-2.1 MON (p59)
Wright, Thomas A. . . . . . CH-10.2 THU (p151)
Wu, Cheng-Yu . . . . . . . . . . CK-P.40 TUE (p106)
Wu, Dakun . . . . . . . . . . . . . . . ED-2.5 MON (p63)
Wu, Dong . . . . . . . . . . . . . . . ∙CD-6.2 TUE (p92),
CD-7.6 WED (p114)
Wu, Guiling . . . . . . . . . . . . . . CI-P.11 FRI (p219)
Wu, Guorong . . . . . . . . . . . ∙JSI-P.5 WED (p141)
Wu, Jinhua . . . . . . . . . . . . . . . CL-3.5 THU (p161)
Wu, Kan . . . . . . . . . . . . . . . . . . CJ-P.11 FRI (p220)
Wu, Ming-Hsiung . . . . . . . . CA-P.3 MON (p74),∙CC-P.12 FRI (p218)
Wu, Qianchao . . . . . . . . . . CE-P.14 THU (p172)
Wu, Qiang . . . . . . . . . . . . . . . . ED-5.5 FRI (p186)
Wu, Ying K. . . . . . . . . . . . . . JSI-P.6 WED (p141)
Wu, Yingxuan . . . . . . . . . . . . CF-1.3 MON (p57),
CG-5.3 THU (p159), EE-3.1 FRI (p189),
EE-3.4 FRI (p197)
Wu, Yudi . . . . . . . . . . . . . . . . . ∙CD-6.6 TUE (p98)
Wu, Zhihan . . . . . . . . . . . . . . PD-1.5 THU (p170)
Wührer, Christian . . . . . . . CA-6.6 WED (p114)
Würthwein, Thomas . . . . . CH-13.5 FRI (p187)
Wyatt, Adam . . . . . . . . . . . . . . CG-1.4 TUE (p87)
Wyatt, Adam S. . . . . . . . . . CF-P.22 TUE (p103),CG-3.1 THU (p143)
Wynne, Laura . . . . . . . . . . . . . CH-3.2 TUE (p84)

X
Xia, Yi . . . . . . . . . . . . . . . . . . . . EA-9.1 FRI (p210)
Xiang, Chushuang . . . . . . . JSVI-1.1 TUE (p83)
Xiang, Fei . . . . . . . . . . . . ∙JSIV-1.4 WED (p118),
JSIII-P.12 FRI (p225)
Xiang, Mingjun . . . . . . . . . . . CC-6.1 FRI (p200)
Xiang, Yuchen . . . . . . . . . . . CL-3.2 THU (p159)
Xiao, Huaifeng . . . . . . . . . . ∙PP-1.1 MON (p64),∙CA-P.6 MON (p74)
Xiao, Jianling . . . . . . . . . . PP-2.11 WED (p121),∙EH-4.2 THU (p158), ∙EH-4.6 THU (p162),
CL-4.6 THU (p169), EH-P.1 THU (p178)
Xie, Jiwei . . . . . . . . . . . . . . . . . CL-1.4 MON (p71)
Xie, Shouyi . . . . . . . . . . . . . . . CE-10.2 FRI (p204)
Xie, Xhinua . . . . . . . . . . . . . . JSI-1.2 WED (p110)
Xie, Xinhua . . . . . . . . . . . . . . JSI-3.2 WED (p124)
Ximendes, Erving C. . . . . . CL-P.10 FRI (p222)
Xin, Feifei . . . . . . . . . . . . . . . . EF-10.5 FRI (p215)
Xiong, Meng . . . . . . . . . . . . . EG-1.1 MON (p52),∙CK-15.6 FRI (p216)
Xomalis, Angelo . . . . . . . . . EG-6.4 WED (p112)
Xu, Bin-Bin . . . . . . . . . . . . . . CE-10.2 FRI (p204)
Xu, Bingxin . . . . . . . . . . . . . ∙ED-2.2 MON (p59)
Xu, Gang . . . . . . . . . . . . . . CD-8.5 WED (p120),PD-2.7 THU (p171)
Xu, Lei . . . . . . . . . . . . . . . . . . CD-1.5 MON (p56),
CK-10.5 THU (p160), CD-11.2 FRI (p183),
JSIII-5.4 FRI (p207)
Xu, Lin . . . . . . . . . . . . . . . . . . . CD-6.6 TUE (p98),
CD-7.6 WED (p114), CJ-9.3 FRI (p204)
Xu, Lu . . . . . . . . . . . . . . . . . . ∙CG-4.2 THU (p151)
Xu, X. . . . . . . . . . . . . . . . . . . . . . . EI-2.1 FRI (p188)
Xu, Xiaodong . . . . . . . . . . . . PP-1.2 MON (p64),
CA-P.13 MON (p74), CA-P.21 MON (p75),
CA-10.1 THU (p142),

CA-10.4 THU (p144), CA-10.5 THU (p146)
Xu, Yiqing . . . . . . . . . . . . . . CD-8.5 WED (p120),
CD-9.3 WED (p124), ∙EF-3.4 THU (p144),
EF-3.6 THU (p148)
Xu, Zicong . . . . . . . . . . . . . . ∙EA-3.4 THU (p152)
Xuan, Zhenghe . . . . . . . . . . CK-8.4 THU (p144)
Xue, Jia . . . . . . . . . . . . . . . . CH-P.33 WED (p138)
Xue, Tianyuan . . . . . . . . . . . ∙CL-1.3 MON (p69)
Xue, Wen-Ze . . . . . . . . . . . CA-10.3 THU (p144),
CA-10.6 THU (p148)

Y
Yabana, Kazuhiro . . . . . . . EE-P.6 WED (p138),
EJ-3.2 FRI (p183)
Yabuno, Masahiro . . . . . . . . EA-2.2 THU (p142)
Yacomotti, Alejandro M. . . . EF-8.2 FRI (p193)
Yacomotti, Alejandro Martin∙EF-8.1 FRI (p189)
Yadav, Amit . . . . . . . . . . . CM-P.31 MON (p78),
CJ-P.3 FRI (p220)
Yadav, Deepanshu . . . . . . . CD-P.32 TUE (p102)
Yaffe, Noa . . . . . . . . . . . . . . EE-P.14 WED (p139)
Yakar, Ozan . . . . . . . . . . . . . . ∙CD-6.4 TUE (p96)
Yakhnevych, Uliana . . . . CE-P.12 THU (p172)
Yakovlev, Ivan . . . . . . . . . . CG-P.12 THU (p174)
Yakovlev, Vladislav . . . . . CG-P.11 THU (p174)
Yakovlev, Vladislav S. . . . . CF-P.16 TUE (p103)
Yaliraki, Sophia . . . . . . . . . . CK-14.2 FRI (p202)
Yallew, Henock D. . . . . . . . . CH-3.1 TUE (p82)
Yalunin, Sergey V. . . . . . . . . EG-3.3 MON (p68)
Yam, Vy . . . . . . . . . . . . . . . . . CK-P.5 TUE (p104),
CK-10.3 THU (p158)
Yamada, Atsushi . . . . . . . . . . . EJ-3.2 FRI (p183)
Yamada, Hirohito . . . . . . . . CK-8.2 THU (p142)
Yamada, Shunsuke . . . . . . ∙EE-P.6 WED (p138),∙EJ-3.2 FRI (p183)
Yamada, Takahiro . . . . . . . . CJ-P.10 FRI (p220)
Yamaizumi, Koki . . . . . . . . . . . CJ-8.3 FRI (p194)
Yamamoto, Naokatsu . . . . . CI-3.2 WED (p125)
Yamamoto, Takashi . . . . . EB-11.3 THU (p151),
EB-P.9 THU (p176)
Yamashima, Taichi . . . . . . EA-2.6 THU (p148),
EA-3.6 THU (p154)
Yamashita, Hiroshi . . . . . JSIII-2.5 THU (p168)
Yamazaki, Masaaki . . . . . . . . . CJ-9.2 FRI (p204)
Yamazaki, Tomohiro . . . . . EB-P.9 THU (p176)
Yamilov, Alexey . . . . . . . . . . CH-1.2 MON (p53)
Yan, Haochen . . . . . . . . . CD-10.5 WED (p132)
Yan, Jieyu . . . . . . . . . . . . . . . . PD-1.5 THU (p170)
Yan, Jingshi . . . . . . . . . . . . . . CE-7.1 THU (p163)
Yan, Jun . . . . . . . . . . . . . . . . . JSI-P.6 WED (p141)
Yan, Libin . . . . . . . . . . . . . . . EH-4.6 THU (p162)
Yan, Siqi . . . . . . . . . . . . . . . . . . CC-5.5 FRI (p196)
Yanagi, Kazuhiro . . . . . . . PP-2.13 WED (p121),
EI-P.6 FRI (p224)
Yanagisawa, Takauyuki . . CA-9.5 WED (p132)
Yanagishima, Taiki . . . . . . EG-6.3 WED (p110)
Yanase, Satoshi . . . . . . . . . . CH-7.1 WED (p123)
Yang, Chan-Shan . . . . . . . . . CL-P.13 FRI (p222)
Yang, Dongwook . . . . . . . . ∙CM-8.2 FRI (p180)
Yang, Joshua . . . . . . . . . . . . . . CD-5.1 TUE (p90),
EB-11.1 THU (p149)
Yang, Ki Youl . . . . . . . . . . . . . CD-5.1 TUE (p90),
EA-2.4 THU (p144), CK-8.6 THU (p148)
Yang, Muyi . . . . . . . . . . . . ∙CK-10.6 THU (p162)

Authors' Index

Yang, Ningchen . . . . . . . . . JSI-1.2 WED (p110),
JSI-3.2 WED (p124)
Yang, Sen . . . . . . . . . . . . . . . EB-7.2 WED (p117)
Yang, Xueming . . . . . . . . . . JSI-P.5 WED (p141)
Yang, Yihao . . . . . . . . . . . . . . CK-14.4 FRI (p204)
Yang, Yijun . . . . . . . . . . . . . . . CD-5.5 TUE (p91)
Yang, Yujia . . . . . . . . . . . . . . . CK-3.4 TUE (p96),
EG-6.2 WED (p108), EF-9.2 FRI (p203)
Yang, Zhaoju . . . . . . . . . . . . . EC-2.1 FRI (p189),
EC-P.3 FRI (p223)
Yang, Zhongmin . . . . . . . . CD-9.3 WED (p124)
Yang, Zhuohui . . . . . . . . . . . . CB-1.2 MON (p54)
Yang, Ziwei . . . . . . . . . . . . . ∙CD-11.5 FRI (p187)
Yannopoulos, Spyros . . . . CH-16.3 FRI (p215)
Yao, Alison M . . . . . . . . . . . . EA-2.5 THU (p146)
Yao, K. . . . . . . . . . . . . . . . . . . . . . EI-2.1 FRI (p188)
Yao, Weichao . . . . . . . . . . . . CA-2.2 MON (p60),∙CF-12.2 FRI (p211)
Yao, Weiming . . . . . . . . . . . . JSIII-P.7 FRI (p224)
Yao, Yuanzhao . . . . . . . . . . . CB-1.5 MON (p56),
CB-P.16 MON (p76), CK-P.17 TUE (p105),
EC-P.11 FRI (p223)
Yarotskaya, Irina . . . . . . . . . CB-9.5 THU (p152)
Yashima, Hiroyuki . . . . . . ∙CI-3.5 WED (p127)
Yashkov, Mikhail V. . . . . . CJ-3.1 WED (p115)
Yasui, Takeshi . . . . . . . . . . . ∙CC-P.11 FRI (p218)
Ye, Zhichao . . . . . . . . . . . . . . CD-P.1 TUE (p100),EF-3.5 THU (p146)
Yehouessi, Jean-Paul . . . . . CJ-3.6 WED (p121)
Yelo-Sarrión, Jesús . . . . . . ∙EF-6.4 THU (p166)
Yeo, Xi Jie . . . . . . . . . . . . . . EB-P.11 THU (p176)
Yerolatsitis, Stephanos . . JSII-1.2 MON (p55),
JSII-2.1 MON (p59), PP-1.12 MON (p65),
JSII-P.2 MON (p80), CD-4.2 TUE (p82)
Yesharim, Ofir . . . . . . . . . ∙CD-9.5 WED (p126)
Yessenov, Murat . . . . . . . . . ∙CF-P.5 TUE (p102),∙CH-7.6 WED (p127)
Yeung, Matthew . . . . . . . . . . . CF-5.1 TUE (p93)
Yildirim, Mustafa . . . . . . JSIII-1.5 THU (p160),∙JSIII-1.6 THU (p162)
Yildiz, Benjamin . . . . . . . . . . . CJ-1.4 TUE (p97),∙CJ-6.3 THU (p145)
Yilmaz, Hasan . . . . . . . . . . . CH-1.2 MON (p53)
Yin, Chunming . . . . . . . . . . CE-10.2 FRI (p204)
Yin, Ruochen . . . . . . . . . . . . . CD-4.4 TUE (p86)
Yin, Yumeng . . . . . . . . . . . ∙CH-6.3 WED (p116)
Ying, Cuifeng . . . . . . . . . . . . CD-1.5 MON (p56)
Yokota, Masayo . . . . . . . . . EB-11.3 THU (p151)
Yoneda, Yuto . . . . . . . . . . . . . ∙CA-4.4 TUE (p86)
Yonezu, Yuya . . . . . . . . . . . . CK-6.4 WED (p126)
Yoo, Jason J. . . . . . . . . . . . . EE-P.13 WED (p139)
Yoon, Hoon Hahn . . . . . . . . . . EI-P.1 FRI (p223)
Yoshikawa, Jun-ichi . . . . . . EA-2.2 THU (p142)
Yoshiki, Wataru . . . . . . . . . CA-9.5 WED (p132)
Yoshioka, Hiroaki . . . . . . . . CK-3.3 TUE (p94),
CK-5.4 WED (p118)
Young, Andrew B . . . . . . . EA-P.20 THU (p175)
Young, Christina . . . . . . . . . . CH-4.5 TUE (p98)
Yousefi, Arman . . . . . . . . . . CD-1.5 MON (p56)
Yu, Changyuan . . . . . . . . . . . . CL-P.7 FRI (p222)
Yu, Fei . . . . . . . . . . . . . . . . . . . ED-2.5 MON (p63)
Yu, Haohai . . . . . . . . . . . . . CA-P.19 MON (p75)
Yu, In Cheol . . . . . . . . . . . . ∙CF-9.5 WED (p133)
Yu, Jialiang . . . . . . . . . . . . . . . ED-P.3 MON (p79)
Yu, Kyoungsik . . . . . . . . . . . CK-7.4 WED (p132)

Yu, Nan Ei . . . . . . . . . . . . . CH-P.21 WED (p137),
CE-P.4 THU (p171), CC-P.14 FRI (p218)
Yu, Siyuan . . . . . . . . . . . . . . . . CB-1.2 MON (p54)
Yu, Yang . . . . . . . . . . . . . . . . . PP-1.2 MON (p64),
CA-P.13 MON (p74), CA-P.21 MON (p75),
CA-10.1 THU (p142)
Yu, Yi . . . . . . . . . . . . . . . . . . . EG-1.1 MON (p52),
CB-1.3 MON (p54), CB-1.4 MON (p56),
CB-10.2 THU (p158), CK-15.6 FRI (p216)
Yu, Ying . . . . . . . . . . . . . . . . . ∙CB-1.2 MON (p54)
Yu, Yuan . . . . . . . . . . . . . . . . CK-5.3 WED (p116)
Yuan, Bocheng . . . . . . . . . . ∙PP-1.3 MON (p64),∙CB-P.1 MON (p75), CB-P.3 MON (p75)
Yuan, Guanghui . . . . . . . . . . CK-14.4 FRI (p204)
Yuan, Hao . . . . . . . . . . . . . . . CF-P.11 TUE (p103)
Yuan, Hui . . . . . . . . . . . . . . . . . CC-6.1 FRI (p200)
Yumnam, Daniel . . . . . . . . CE-P.25 THU (p173)
Yurchenko, Sergey . . . . . . . . ED-2.4 MON (p61)
Yvind, Kresten . . . . . . . . . . . EG-1.1 MON (p52),
CK-P.35 TUE (p106), EG-P.9 TUE (p107),
CE-7.1 THU (p163), CK-15.6 FRI (p216)

Z
Zablah, Andrea . . . . . . . . . CD-P.12 TUE (p100)
Zaccardi, Zachary . . . . . . . CC-3.2 THU (p165)
Zadeh, Iman Esmaeil . . . . . EB-P.7 THU (p176)
Zadravec, Dusan . . . . . . . . . . CF-P.4 TUE (p102)
Zahariev, Peter . . . . . . . . . EA-P.18 THU (p175)
Zahertar, Shahrzad . . . . . . CE-5.3 THU (p151)
Zair, Amelle . . . . . . . . . . . . . CG-4.6 THU (p155)
Zajnulina, Marina . . . . . JSIII-1.3 THU (p158),
JSIII-P.17 FRI (p225)
Zakoldaev, Roman . . . . . . . . CH-3.1 TUE (p82)
Zalden, Peter . . . . . . . . . . . ∙CM-10.1 FRI (p200)
Zalesskaia, Iuliia . . . . . . . . ∙CJ-5.1 WED (p129)
Zambito, Giorgio . . . . . . . . CK-15.1 FRI (p210)
Zaminga, Sara . . . . . . . . . . . CB-9.4 THU (p152)
Zander, Jascha . . . . . . . . . . . EA-P.4 THU (p174)
Zang, Xiaorun . . . . . . . . . . . . . EG-4.4 TUE (p86)
Zangeneh Kamali, Khosro
CD-1.5 MON (p56), ∙CK-10.5 THU (p160),
CD-11.2 FRI (p183)
Zangrando, M. . . . . . . . . . . JSI-3.5 WED (p126)
Zangrando, Marco . . . . . . JSI-2.5 WED (p118),
JSI-4.3 WED (p130)
Zanin, Guilherme L. . . . . EB-13.4 THU (p167)
Zaouter, Yoann . . . . . . . . . . . CF-1.4 MON (p57),
CF-P.3 TUE (p102)
Zapata, Felipe . . . . . . . . . . . JSI-4.3 WED (p130)
Zaquine, Isabelle . . . . . . . . . EB-3.1 MON (p67)
Zardo, Ilaria . . . . . . . . . . . . ∙JSVI-1.2 TUE (p85)
Zarebidaki, Homa . . . . . . . . CE-9.3 FRI (p192),
CE-9.6 FRI (p196)
zarei, mehrdad . . . . . . . . . . ∙EA-P.9 THU (p175)
Zargar-Shoshtari, KamranPP-2.8 WED (p121), CL-5.5 FRI (p187),
CL-P.2 FRI (p221)
Zatorska, Magdalena . . ∙CH-P.31 WED (p138)
Zaumseil, Jana . . . . . . . . . . EH-P.14 THU (p179)
Zaushitsyna, Tatyana . . . . . CJ-5.3 WED (p131)
Zavatta, Alessandro . . . . . . . EB-5.4 TUE (p97),
EF-P.16 WED (p140), EB-P.22 THU (p177)
zawada, michał . . . . . . . . . . EA-P.9 THU (p175)
Zawilski, Kevin . . . . . . . . . . . CD-6.3 TUE (p94)

Zayats, Anatoly . . . . . . . . . . EG-2.5 MON (p62),∙CK-2.1 TUE (p82)Żbik, Mateusz . . . . . . . . . . . . CK-P.9 TUE (p104)
Zedane, Serhane . . . . . . . . . JSI-1.2 WED (p110)
Zeitner, Uwe D. . . . . . . . . . EH-2.5 THU (p148),
CD-11.3 FRI (p185), CD-11.4 FRI (p187)
Zelan, Martin . . . . . . . . . . . CI-2.2 WED (p119),
ED-6.2 FRI (p190)
Zeller, Viola . . . . . . . . . . . . . . . EG-4.3 TUE (p86)
Zelsmann, Marc . . . . . . . . CL-3.1 THU (p157),
CL-3.4 THU (p161)
Zeludev, Nikolay . . . . . . . . . EH-5.4 THU (p166)
Zeng, Huang-Jun . . . . . . CA-10.3 THU (p144),
CA-10.6 THU (p148)
Zeng, Shuwen . . . . . . . . . . . ∙CL-P.3 FRI (p221),∙CL-P.4 FRI (p221)
Zeng, Xinglin . . . . . . . . . . . ∙CD-12.1 FRI (p189)
Zeninari, Virginie . . . . . . . CH-16.5 FRI (p217)
Zentgraf, Thomas . . . . . . CK-P.39 TUE (p106)
Zerbib, Maxime . . . . . . . . EF-P.15 WED (p140),∙CK-13.1 FRI (p188)
Zerebecki, Swen . . . . . CM-LIM.1 WED (p115)
ZERGIOTI, IOANNA . . ∙CM-11.1 FRI (p210),
CL-P.18 FRI (p222)
Zervas, Michalis . . . . . . . CH-11.4 THU (p161)
Zeuner, Katharina D. . . . . . CK-1.2 MON (p66)
Zha, Zimin . . . . . . . . . . . . . EF-P.20 WED (p140)
Zhai, Min . . . . . . . . . . . . . . . . CC-P.10 FRI (p218)
Zhai, Ziwei . . . . . . . . . . . . . . . ∙CJ-9.4 FRI (p206)
Zhan, Minjie . . . . . . . . . . . . CA-P.22 MON (p75)
Zhan, Ziyu . . . . . . . . . . . . . . . JSIII-P.4 FRI (p224)
Zhang, A. Ping . . . . . . . . . . CH-14.4 FRI (p197)
Zhang, Baichao . . . . . . . . . . JSI-P.5 WED (p141)
Zhang, Chi . . . . . . . . . . . . . . EB-P.35 THU (p178)
Zhang, Fengling . . . . . . . ∙CF-P.15 TUE (p103),
CH-6.1 WED (p114)
Zhang, Ge . . . . . . . . . . . . . CA-10.3 THU (p144),
CA-10.6 THU (p148)
Zhang, Hankai . . . . . . . . . . JSI-1.2 WED (p110),
JSI-3.2 WED (p124)
Zhang, Hongyi . . . . . . . . . ∙CK-5.5 WED (p118)
Zhang, Huaijin . . . . . . . . . CA-P.19 MON (p75)
Zhang, Jihua . . . . . . . . . . . . CD-3.4 MON (p70),
EG-5.2 TUE (p92), CK-10.2 THU (p158),
PD-2.9 THU (p171)
Zhang, Jing . . . . . . . . . . . . . . CK-13.2 FRI (p190)
Zhang, Jun . . . . . . . . . . . . . . . PP-1.9 MON (p64),
CM-P.5 MON (p77)
Zhang, Junyin . . . . . . . . . . . . EB-1.2 MON (p55)Zhang, Kevin . . . . . . . . . . . . . . CB-4.3 TUE (p91)
Zhang, Lu . . . . . . . . . . . . . . . . EG-P.8 TUE (p107)
Zhang, Luosha . . . . . . . . . . EB-P.34 THU (p178)
Zhang, Peixiong . . . . . . . . . CA-P.18 MON (p75)
Zhang, Qi . . . . . . . . . . . . . . . . . EF-8.2 FRI (p193)
Zhang, Qianyi . . . . . . . . . . ∙CM-11.2 FRI (p212)
Zhang, S. . . . . . . . . . . . . . . . . . . . EI-2.1 FRI (p188)
Zhang, Shengnan . . . . . . . EA-P.14 THU (p175)
Zhang, Shuangyou . . . . . ∙CK-5.1 WED (p114),
CD-10.5 WED (p132), CK-8.1 THU (p142),
CK-8.6 THU (p148), ED-6.1 FRI (p188)
Zhang, Shuyan . . . . . . . . . . . . CL-P.3 FRI (p221),
CL-P.4 FRI (p221)
Zhang, Wei . . . . . . . . . . . . . . . . EB-5.1 TUE (p93)
Zhang, Weikang . . . . . . . . ∙JSIII-5.5 FRI (p209)
Zhang, Weiqing . . . . . . . . . . JSI-P.5 WED (p141)

255

Zhang, Xinliang . . . . . . . . . CK-5.3 WED (p116)
Zhang, Xintong . . . . . . . . . . . CD-4.6 TUE (p88)
Zhang, Xinzhi . . . . . . . . . . . . CI-3.1 WED (p123)
Zhang, Xiupu . . . . . . . . . . . CB-P.17 MON (p76)Zhang, Xuejun . . . . . . . . . . . . CL-1.4 MON (p71)
Zhang, Yani . . . . . . . . . . . ∙CH-P.33 WED (p138)
Zhang, Yaojing . . . . . . . . . CK-5.1 WED (p114),∙CD-10.5 WED (p132)
Zhang, Yong . . . . . . . . . . . . . ∙CD-1.1 MON (p52)
Zhang, Yu . . . . . . . . . . . . . . . ED-2.1 MON (p59),
CF-P.22 TUE (p103), ∙CK-13.2 FRI (p190)
Zhang, Yunshan . . . . . . . . . . PP-1.3 MON (p64),
CB-P.1 MON (p75), CB-P.3 MON (p75)
Zhang, Zhe . . . . . . . . . . . . . . . ∙EC-2.2 FRI (p193)
Zhang, Zhelin . . . . . . . . . . . CC-3.3 THU (p167)
Zhang, Zhonghan . . . . . . . CA-P.10 MON (p74)
Zhang, Zhuang-Yan . . . . . . ∙EE-3.2 FRI (p193),
EE-3.3 FRI (p195)
Zhao, Kaixiang . . . . . . . . . . JSI-4.6 WED (p134)
Zhao, Li . . . . . . . . . . . . . . . . CE-P.24 THU (p173)
Zhao, Peng Cheng . . . . . . . CH-14.4 FRI (p197)
ZHAO, PING . . . . . . . . . . . ∙CD-2.6 MON (p62),
CD-P.1 TUE (p100)
Zhao, Wei . . . . . . . . . . . . . . . CF-P.11 TUE (p103)
Zhao, Yongguang . . . . . . . . . CA-2.1 MON (p58)
Zhao, Yue . . . . . . . . . . . . . . . . CF-12.1 FRI (p211)
Zharkova, Ekaterina . . . . CM-P.20 MON (p78)
Zheludev, Nikolay . . . . . . . EG-2.2 MON (p58),
PP-1.6 MON (p64), EG-3.2 MON (p66),
CH-6.5 WED (p118), EH-1.2 WED (p130),
CH-P.4 WED (p136), EC-P.9 FRI (p223)
Zheludev, Nikolay I. . . . . . . PP-1.7 MON (p64),
CH-P.8 WED (p136), CH-12.1 THU (p163),
CH-12.6 THU (p169), ED-5.3 FRI (p184),
EJ-4.1 FRI (p189), EC-3.5 FRI (p207)
Zheng, Di . . . . . . . . . . . . . . . CH-15.1 FRI (p201)
Zheng, Jiaan . . . . . . . . . . . . . CA-P.2 MON (p74),
JSI-P.4 WED (p141), PD-1.1 THU (p170)
Zheng, Jian . . . . . . . . . . . . . EF-P.22 WED (p140)
Zheng, Lei . . . . . . . . . . . . . . . . ∙CE-8.4 FRI (p184)
Zheng, Li . . . . . . . . . . . . . . . . . PP-1.2 MON (p64),
CA-P.21 MON (p75), CA-10.1 THU (p142)
Zheng, Lihe . . . . . . . . . . . . CA-10.6 THU (p148)
Zheng, Yu . . . . . . . . . . . . . . . . . CD-4.4 TUE (p86)
Zheng, Ze . . . . . . . . . . . . . . . ∙CD-1.5 MON (p56)
Zherebtsov, Evgenii . . . . . . ∙CL-1.5 MON (p73)
Zhigilei, Leonid . . . . . . . . . . ∙CM-5.1 TUE (p90)
Zhiyuan, Xie . . . . . . . . . . . . . EG-3.4 MON (p68)Zhluktova, Irina . . . . . . . . EB-P.14 THU (p177)
Zhong, Hancheng . . . . . . . . CB-1.2 MON (p54)
Zhong, Qi . . . . . . . . . . . . . . . . . EC-1.5 FRI (p187)
Zhong, Shiyang . . . . . . . . . JSI-4.3 WED (p130)
Zhong, Xiaoyan . . . . . . . . . . EG-P.8 TUE (p107)
Zhonghan, Zhang . . . . . . . . CA-P.9 MON (p74)
Zhou, Binbin . . . . . . . . . . . . . CC-5.5 FRI (p196),∙CC-6.2 FRI (p204)
Zhou, Kai . . . . . . . . . . . . . . . . . CC-6.1 FRI (p200)
Zhou, Linjie . . . . . . . . . . . . . CK-5.5 WED (p118)
Zhou, Meng . . . . . . . . . . . . . . CF-P.8 TUE (p102),
CF-P.12 TUE (p103)
Zhou, Sheng . . . . . . . . . . . . . EA-P.2 THU (p174)
Zhou, Siyan . . . . . . . . . . . . . . . CC-6.2 FRI (p204)
Zhou, Xuetong . . . . . . . . ∙CK-11.1 THU (p162)
Zhou, Yi . . . . . . . . . . . . . . . . . CF-P.8 TUE (p102),
JSIII-1.5 THU (p160), ∙EF-5.4 THU (p160),

EJ-3.5 FRI (p187), CH-15.2 FRI (p205)
Zhou, Yiru . . . . . . . . . . . . . . . . EB-5.1 TUE (p93),
EB-9.2 WED (p131)
Zhou, Zifan . . . . . . . . . . . . . CH-7.5 WED (p127)
Zhu, Changlong . . . . . . . . . ∙EB-1.2 MON (p55),∙EA-P.15 THU (p175), EF-7.3 FRI (p183)
Zhu, Di . . . . . . . . . . . . . . . . . . . CJ-P.11 FRI (p220)
Zhu, Jiangfeng . . . . . . . . . . . PP-1.2 MON (p64),
CA-P.13 MON (p74), CA-P.21 MON (p75),
CA-10.1 THU (p142)
Zhu, Simeng . . . . . . . . . . . . . PP-1.3 MON (p64),
CB-P.1 MON (p75)
Zhu, Siyuan . . . . . . . . . . . PP-2.12 WED (p121),
EH-P.16 THU (p179)
Zhu, Tao . . . . . . . . . . . . . . . . . . ED-5.5 FRI (p186)
Zhu, Wei . . . . . . . . . . . . . . . ∙CE-P.14 THU (p172)
Zhu, Xiaoyang . . . . . . . . . . . . . EI-4.4 FRI (p214)
Zhu, Zexiu . . . . . . . . . . . . . . . JSI-P.5 WED (p141)
Zhukov, Vladimir . . . . . . . CM-3.3 MON (p68),
CM-P.7 MON (p77)
Zhuravlov, Artem . . . . . . ∙CM-P.28 MON (p78)
Ziani, Zoheir . . . . . . . . . . . . . EF-3.3 THU (p144)
Zichi, Julien . . . . . . . . . . . . . . CK-1.2 MON (p66)
Zicoschi, Alessio . . . . . . . . . . EA-9.1 FRI (p210)Žídek, Karel . . . . . . . . . . . . CD-P.28 TUE (p101),
CH-8.5 WED (p133), CH-P.12 WED (p136)
Ziefuß, Anna . . . . . . . . CM-LIM.1 WED (p115)
Ziefuss, Anna Rosa . . . . . . CM-10.3 FRI (p204)
Zielinska, Joanna . . . . . . . . . EB-1.3 MON (p55)
Zigman, Mihaela . . . . . . . . CL-2.1 THU (p149),
CH-13.1 FRI (p181)
Zilli, Attilio . . . . . . . . . . . . . . EG-2.1 MON (p58),
PD-2.8 THU (p171)
Zimmermann, Conrad . . . . EB-1.4 MON (p57)
Zimmermann, Julian . . . . JSI-3.1 WED (p122)
Zin Elabedine, Ghassen . CA-P.18 MON (p75),
CA-P.19 MON (p75)
Zink, Christof . . . . . . . . . . CB-11.1 THU (p162)
Zinner, Nikolaj Thomas . . EB-P.5 THU (p176)
Zitelli, Mario . . . . . . . . . . . . EF-4.4 THU (p154),
EF-7.1 FRI (p181), ∙EF-7.4 FRI (p185),
EF-7.5 FRI (p187), EJ-3.3 FRI (p185)
Žitnik, M. . . . . . . . . . . . . . . JSI-3.5 WED (p126),∙JSI-4.5 WED (p132)
Zografopoulos, Dimitrios CM-1.4 MON (p54)
Zolotovskaya, Svetlana A.
CK-P.13 TUE (p104)
Zou, Chengjun . . . . . . . . . CK-10.1 THU (p156)
Zu, Lijiao . . . . . . . . . . . . . . . . . CL-1.4 MON (p71)
Zuber, David . . . . . . . . . . . . . CF-11.3 FRI (p205)
Zukauskas, Andrius . . . . . . CD-2.4 MON (p60)
Zukerstein, Martin . . . . . ∙CM-3.3 MON (p68),
CM-P.7 MON (p77)
Zunino, Alessandro . . . . . . . ∙CL-6.3 FRI (p195)
Zurak, Luka . . . . . . . . . . . . . . . CK-2.3 TUE (p86)
Zurakowski, Ryan . . . . . . . CE-P.21 THU (p172)
Zurita-Miranda, Olivia . . . CJ-P.15 FRI (p220)
Zurrón-Cifuentes, Óscar . . . EI-2.3 FRI (p192)
Žvirblis, Rokas . . . . . . . . . . . CE-11.2 FRI (p212)
Zwilich, Michael . . . . . . . ∙CF-8.4 WED (p127)
Zwiller, Val . . . . . . . . . . . . . . . CK-1.2 MON (p66)
Zyla, Gordon . . . . . . . . . . . ∙CM-1.4 MON (p54),∙CH-12.4 THU (p167)

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