IPMU Focus Week

Condensed Matter Physics Meets High Energy Physics

Program & Abstracts

Monday, 8th – Friday, 12th February, 2010
IPMU, University of Tokyo

hosted by the Institute for the Physics and Mathematics of the Universe (IPMU),
in cooperation with the Institute for Solid State Physics (ISSP)

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Preface

Let us welcome you to the IPMU Focus Week “Condensed Matter Physics Meets High Energy Physics”. The interdisciplinary workshop has been organized with the following concept.
Beautiful ideas developed by theorists in one area of physics often have unexpected applications in others. Quantum field theory is an outstanding example. As the basic languageof both condensed matter physics and high energy physics, it has provided fertile ground forinteractions of the two areas of physics, and common techniques using renormalization, symmetry, topology and integrability have been developed. Recently, the AdS/CFT correspondence
has opened a new interface between condensed matter physics and quantum gravity. Hencethe present workshop brings together the two communities to share ideas, identify common
problems and develop new techniques to solve them. We are planning various arrangements
to enhance interactions of condensed matter physicists and high energy physicists, including tutorial lectures and ample time for informal exchanges. Topics will include quantum
criticality, quantum liquid, topological order, integrable systems, graphene, relativistic andnon-relativistic conformal field theories and their holographic descriptions.
The workshop is hosted by the Institute for the Physics and Mathematics of the Universe(IPMU) of the University of Tokyo, in cooperation with the Institute for Solid State Physics(ISSP) of the University of Tokyo. The workshop is the first international conference held at
the new IPMU building on the Kashiwa campus of the University of Tokyo.
This booklet contains the program, the abstracts and the questions that will be raised in
the panel discussion.

Hideo Aoki*, Department of Physics, University of Tokyo,
Hirosi Ooguri*, Caltech & IPMU, University of Tokyo,
Masaki Oshikawa, ISSP, University of Tokyo,
Shinsei Ryu, University of California at Berkeley,Tadashi Takayanagi, IPMU, University of Tokyo.
[Organizers (*: co-chairs)]

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Program
Monday, 8th February ==========================
Registration

8:45—

Opening

9:15–9:30

Welcome Address: Hirosi Ooguri
Opening Remarks: Yasuhiro Iye (Director, ISSP)
Morning Session (chair: Hirosi Ooguri)

Mon-0

Son, Dam

9:30–10:30(Pedagogical Lecture)

10:30–11:00

Coﬀee BreakMon-1

Aoki, Hideo

11:00–12:00

How can condensed-matter problems interact with field theoretic ideas — an overview
Lunch Break 12:00–14:00
Afternoon Session (chair: Sumit Das)

Mon-2

Kachru, Shamit

14:00–15:00

New Horizons in AdS/CFT

15:00–15:30

Coﬀee BreakMon-3

Avishai, Yshai

15:30–16:00

Electron in the Field of Magnetic Monopole: Tight-Binding Solution

Mon-4

Yarom, Amos

16:00–16:30

Large N superfluids

16:30–17:00

Coﬀee Break

Mon-5

Read, Nick

17:00–18:00
3

Tuesday, 9th February ==========================

Morning Session (chair: Mikio Nakahara)
Tue-0
9:00–10:00

Wen, Xiao-Gang
Collective modes and topologcal defects in a topological phase – A unification of gaugeinteraction and Fermi statistics (Pedagogical Lecture)

10:00–10:30

Coﬀee BreakTue-1

Fujimoto, Satoshi

10:30–11:30

Topological Phases of Noncentrosymmetric Superconductors and Superfluids

Tue-2

Nishimura, Jun

11:30–12:00

Precision test of the gauge/gravity duality from first principles
Lunch Break 12:00–14:00
Afternoon Session (chair: Tadashi Takayanagi)

Tue-3

Hartnoll, Sean

14:00–15:00
15:00–15:30

Coﬀee BreakTue-4

Nakamura, Shin

15:30–16:00

Gravity Dual of Spatially Modulated Phase

Tue-5

Hatsugai, Yasuhiro
Correspondence between the bulk quantum states and boundary states in topological

16:00–16:30

phases in condensed matter

16:30–17:00

Coﬀee BreakTue-6

Liu, Hong

17:00–18:00
Banquet 18:00–

4

Wednesday, 10th February ==========================

Morning Session (chair: Hideo Aoki)
Wed-1

Zhang, Shoucheng

9:00–10:00
10:00–10:30

Coﬀee Break

10:30–10:35

Hitoshi fMurayama (Director, IPMU), Welcome address

10:35–10:45

George Smoot, TBA

10:45–11:45

Panel Discussion
Fradkin, Fujimoto, Hartnoll, Kachru, Kitaev, Liu, Minwalla, Zhang
Moderators: Aoki, Ooguri
Lunch Break (11:45–14:00)
Afternoon Session (chair: Akira Furusaki)

Wed-2

Wen, Xiao-Gang

14:00–15:00

Emergence of gravitons from qbit models

15:00–15:30

Coﬀee BreakWed-3

Hashimoto, Koji

15:30–16:00

Holography and Nuclear Physics

Wed-4

Nomura, Kentaro

16:00–16:30

Topological delocalization of two-dimensional massless Dirac fermions

16:30–17:00

Coﬀee BreakWed-5

Son, Dam

17:00–18:00

Quantum anomalies in hydrodynamics

5Thursday, 11th February ==========================

Morning Session (chair: Shinobu Hikami)
Thu-0

Schomerus, Volker

9:00–10:00

Superspace Sigma Models (Pedagogical Lecture)

10:00–10:30

Coﬀee BreakThu-1

Minwalla, Shiraz

10:30–11:30
Thu-2

Kiritsis, Elias

11:30–12:00

On Universality classes in Strongly coupled doped systems
Lunch Break (12:00–14:00)
Afternoon Session (chair: Shinsei Ryu)

Thu-3

Kitaev, Alexei

14:00–15:00

Classification of topological insulators and superconductors

15:00–15:30

Coﬀee BreakThu-4

Sato, Masatoshi

15:30–16:00

Fractionalization and Hidden Symmetry in Topological Orders

Thu-5

Oka, Takashi
Many-body Schwinger-Landau-Zener Mechanism in Nonequilibrium Strongly Corre-

16:00–16:30

16:30–18:30

lated Electron Systems
Poster Session (with Coﬀee)

6Friday, 12th February ==========================

Morning Session (chair: Kenzo Ishikawa)
Fri-0

Read, Nick

9:00–10:00(Pedagogical Lecture)

10:00–10:30

Coﬀee BreakFri-1

Schomerus, Volker

10:30–11:30

The SupersphereFri-2

Natsuume, Makoto

11:30–12:00

Critical phenomena in AdS/CFT duality
Lunch Break (12:00–14:00)
Afternoon Session (chair: Masaki Oshikawa)Fri-3

Takayanagi, Tadashi

14:00–15:00

Entanglement Entropy and Topological Insulators from String Theory

15:00–15:30

Coﬀee BreakFri-4

Tanaka, Akihiro

15:30–16:00

Gauge and gravitational anomalies in graphene-related systems

Fri-5

Nakayama, Yu

16:00–16:30

Universal time-dependent deformations of Schrodinger geometry

16:30–17:00

Coﬀee BreakFri-5

Fradkin, Eduardo

17:00–18:00

Quantum Entanglement and Quantum Criticality

18:00–

Closing7

Poster Presentations
P01

Ahmad, Mohammad Ayaz
Study of short-range correlations in relativistic heavy ion collisions

P02

Ahn, Hyo Chul
The quark mass dependence of the nucleon mass in AdS/QCD

P03

Araki, Yasufumi
Dynamical Theory of Graphene from Strong Coupling Expansion of U(1) Lattice
Gauge Theory with Staggered Fermions

P04

Bytsko, Andrei
Non-Hermitian spin chains with real spectra

P05

Chen, Chiang-Mei
The RN/CFT correspondence

P06

Chen, Jiunn-Wei
Peak-Dip-Hump from Holographic Superconductivity

P07

Fialkovsky, Ignat
Quantum field theory as applied to graphene

P08

Fukui, Takahiro
Topological stability of Majorana zero-modes in superconductor-topological insulator
systems

P09

Garcia Garcia, Antonio M
Holographic approach of phase transitions

P10

Goryo, Jun
Electromagnetic response in a quantum spin Hall system with electron correlation

P11

Hasebe, Kazuki
Supersymmetric Quantum Hall Eﬀect and Quantum Spin Model

P12

Hayashi, Mitsuo
Matter production after Inflation in Modular Invariant Supergravity

P13

Hikami, Shinobu
8On an Airy matrix model with a logarithmic potential
P14

Hikida, Yasuaki
The OSP(1|2) WZNW model with and without boundary

P15

Hong, Deog-Ki
Critical Phenomena of Holographic Planar Superconductor

P16

Hotta, Kenji
Creation of D9-brane–anti-D9-brane Pairs from Hagedorn Transition of Closed Strings

P17

Ishikawa, Kenzo
Macroscopic Interferences of Neutrino Waves

P18

Ichinose, Shoichi
Casimir Energy of the Universe and the 5D Warped Model

P19

Kao, Hsien-chung
Ballistic transport, chiral anomaly and emergence of the electron - hole plasma ingraphene

P20

Keeler, Cynthia
Deformations of Lifshitz holography

P21

Kim, Seok
Supersymmetric vacua of mass-deformed N=6 Chern-Simons theory

P22

Koroteev, Peter
Holography and Lorentz Invatiance Violation

P23

Nakata, Kouki
Extended Quantum Dimer Model -Mapping by the S = 1 algebra

P24

Lin, Feng-Li
Holographic Anyons in the ABJM Theory

P25

Maeda, Kengo
Vortex lattice for a holographic superconductor

P26

Maeda, Kenji
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Simulating dense QCD matter with ultracold atomic boson-fermion mixtures
P27

Matsui, Chihiro
Correlation functions for higher spin integrable systems

P28

Meyer, Rene
Adding Flavor to AdS(4)/CFT(3).

P29

Morimoto, Takahiro
Optical Hall conductivity in the graphene quantum Hall system — what happens to
a topological number in ac response

P30

Nishiyama, Seiya
Supersymmetric sigma-Model Based on the SO(2N+1) Lie Algebra of the Fermion
Operators - A way to proper solution -P31

Nitta, MunetoD-brane in Bose-Einstein Condensates

P32

Panthi, Rajesh
Interstellar Bubbles Candidates in the Far Infra-Red Sky

P33

Reﬀert, Susanne
The super Quantum Lifshitz Model from the Nicolai Map

P34

Satoh, Yuji
Entanglement through conformal interfaces

P35

Schmidt-Colinet, Cornelius
Bulk-boundary flows in the Virasoro minimal models

P36

Suzuki, Junji
Density matrix elements at finite temperatures

P37

Wapler, Matthias
2-Dimensional Holographic Quantum Liquids

P38

Yasui, Shigehiro
Fermion structure of non-Abelian vortex in color superconductivity

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P39

Yavartanoo, Hossein
Schrodinger invariant solutions of M-theory with Enhanced Supersymmetry

P40

Li, Wei
On String Embedding of Lifshitz Fixed Point

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Abstracts
Mon-0(Pedagogical Lecture)
Son, Dam
University of Washington

Mon-1
How can condensed-matter problems interact withfield theoretic ideas — an overview
Aoki, Hideo
Department of Physics, University of Tokyo
Various problems and phenomena in condensed-matter physics can accommodate diverse
eﬀective field theories on energy scales orders of magnitude smaller than those encountered inhigh-energy physics. Here I shall give an overview on the following.
(i) Phenomena: superconductivity, magnetism and quantum Hall eﬀect, all of which realize some gauge symmetry breaking. Specifically, unconventional superconductivity (SC)in correlated electron systems accommodate electron mechanisms of SC. Even more exotic
superconductors are now being discovered and discussed, among which are T-reversal broken SC, FFLO states, ferromagnetic SC, noncentrosymmetric SC, and multi-band (i.e., multi
fermion species) SC (as in the most recent iron-based SC). Fractional quantum Hall system
is described in terms of Chern-Simons gauge field in (2+1)D, which accommodates anyons,nonablelions, and also excited states. More generally, topological phases / insulators are an
important avenue, with spin-oﬀ into, e.g., spin Hall eﬀect.
(ii) Spatial dimensionality: realisable in condensed matter are 0D (quantum dots), 1D(quantum wires, nanotubes), 2D (QHE systems, layered cuprates, and recently atomically
2D graphene). These accommodate, respectively, Tomonaga-Luttinger physics, high-Tc SC,
massless Dirac particles, etc.
(iii) Boundary states: bulk and edge states are intimately related (in fact the latter’s existence “topologically protected” for topological states), and topological properties become
visible through boundary states as in QHE edge states, which become peculiar in graphene.
(iv) Non-equilibrium phenomena accommodate wealth of physics, e.g., dielectric breakdown
of a Mott insulator which turn out to be analogous to Schwinger’s QED vacuum decay, or
responses against T-broken perturbations in graphene.

12Mon-2
New Horizons in AdS/CFT
Kachru, Shamit
KITP, University of California, Santa Barbara
The possible symmetry-breaking patterns of ground states in condensed matter systems arereflected in a rich and expanding array of new near-horizon geometries for black branes in
AdS space-times. We discuss the physics that some of these horizons reflect in the dual field
theory, and tie the genericity of their emergence to the attractor mechanism for black holes instring theory. As a concrete example we will mostly focus on branes with near-horizon Lifshitz
symmetry (anisotropic scale invariance), but other examples will be briefly discussed.

Mon-3
Electron in the Field of Magnetic Monopole: Tight-Binding Solution
Avishai, Yshai
Ben Gurion University and University of Tokyo
The Dirac monopole is a central building block in high-energy physics. At the same time,
it appears as an important conceptual tool in condensed matter physics (e.g in the studyof the fractional quantum Hall eﬀect, or spin ice). In the present work, the problem of anelectron on a sphere subject to a central magnetic (monopole) field of strength g = n(~c)/(2e)(n = 0, 1, 2 . . .) is solved within a tight binding model. For highly symmetric lattices, theenergy spectrum (Landau levels) is calculated analytically as function of n and displays abeautiful pattern, distinct from the Hofstadter butterfly. The systematics of level degeneracy
requires the inclusion of magnetic rotations within the theory of point symmetry groups. A
remarkable relation between this problem and that of an electron subject to a central electricfield with spin-orbit interaction is exposed. As a result, it is principally possible to study thephysics of an experimentally inaccessible system (electron in the field of magnetic monopole)in terms of an experimentally accessible one (electron subject to spin-orbit force induced bycentral electric field).

Mon-4
Large N superfluids

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Yarom, Amos
Princeton University
After reviewing the construction of a superfluid phase of gauge theories with a gravity dual,
I will discuss some of its features: its speed of sound and its interaction with a heavy quark.
I will argue that, as opposed to superfluid helium, these features indicate that the low lying
excitations of the theory behave like massless quasi-particles.

Mon-5

Read, Nick
Yale University

Tue-0
Collective modes and topologcal defects in a topological phase– A unification of gauge interaction and Fermi statistics(Pedagogical Lecture)Wen, Xiao-GangMIT
A topological phase is a phase with long range entanglement. We show that the collectivemodes in a topological phase can be a U(1) gauge modes. The ends of strings can fermions.
The new topological order with long range entanglement can unify gauge interaction and Fermi
statistics.

Tue-1
Topological Phases of Noncentrosymmetric Superconductors andSuperfluids
Fujimoto, Satoshi
Kyoto University
In this talk, I review the recent studies on topological phases in noncentrosymmetric superconductors (SCs) and superfluids (SFs). Recently, many classes of SCs with broken inversion
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symmetry in their crystal structures have been experimentally discovered, and are called noncentrosymmetric SCs. In these systems, anti-symmetric spin-orbit interactions due to broken
inversion symmetry give rise to various exotic superconducting properties including the realization of topological order.
In particular, the argument here is focused on the Z2 topological order in the case with
time-reversal symmetry, which is characterized by the existence of topologically protected
gapless surface states, and the non-Abelian topological order in the case without time-reversal
symmetry associated with the level-2 SU(2) Chern-Simons theory, for which the non-Abelian
statistics of vortices described by the Ising conformal field theory is realized. The highlightof this subject is that the non-Abelian topological order is possible even for conventionals-wave superconducting states as long as an applied magnetic field is suﬃciently large. It is
pointed out that the s-wave SC with the anti-symmetric spin-orbit interactions and an appliedmagnetic field has the same topological order as that of a chiral p+ip-wave SC, which is awell-known system realizing the non-Abelian statistics.
Furthermore, I discuss the possibililty of realizing the non-Abelian topological order ins-wave superfluids of ultracold fermionic atoms with laser-generated fictitious ”spin-orbit”
interactions. These works have been done by the collaboration with Masatoshi Sato (ISSP,
Tokyo) and Yoshiro Takahashi (Kyoto).
References[1] M. Sato and S. Fujimoto, Phys. Rev. B79, 094504 (2009).
[2] M. Sato, Y. Takahashi, and S. Fujimoto, Phys. Rev. Lett. 103, 020401 (2009).

Tue-2
Precision test of the gauge/gravity duality from first principles
Nishimura, Jun
KEKAs the main theme of this workshop indicates, the concept of the gauge/gravity duality
seems to be valid at least qualitatively in quite general systems including those relevant tocondensed matter physics. On the other hand, it is poorly understood to what extent theduality actually holds at the quantitative level. I would like to summarize the status of such
issues from the viewpoint of first principle calculations in strongly coupled gauge theories
based by Monte Carlo methods.

Tue-3

15

Hartnoll, Sean
Harvard University

Tue-4
Gravity Dual of Spatially Modulated Phase
Nakamura, Shin
Kyoto University
We analyze the stability of the Reissner-Nordstrom black hole in the 5-dimensional
Einstein+Maxwell+Chern-Simons theory with a negative cosmological constant. We showthat the black hole is unstable if the Chern-Simons (CS) coupling is suﬃciently large. The
unstable mode is circularly polarized and always carries a non-zero momentum, suggesting atransition into a spatially modulated phase. In the possible CFT-dual picture, this suggests
a spontaneous generation of a helical current. We find that the system is barely stable if we
employ the CS coupling obtained from the type IIB supergravity. (Reference: arXiv:0911.0679[hep-th].)

Tue-5
Correspondence between the bulk quantum states and boundary
states in topological phases in condensed matter
Hatsugai, YasuhiroInstitute of Physics, University of Tsukuba
It has been realized that many of important quantum eﬀects are of topological origins incondensed matter physics, especially for quantum ground states with a finite excitation gap.
While such gapped ground states can possess nontrivial geometrical phases as characterized by
the Berry connection, they may look physically featureless as a bulk. However the topologicalfeatures often appear as characteristic phenomena near the boundaries or impurities, which
are caused by edge states. Thus the edge and the bulk are not independent, but intimately
related with each other. We describe this bulk-edge correspondence with several examples that
include quantum Hall systems, spin Hall systems, gapped quantum spin chains (ladders) andphotonic crystals. Graphene as a condensed matter realization of chiral symmetric massless
Dirac fermions in two dimensions are also described by this bulk-edge correspondence.

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Tue-6

Liu, Hong
MIT

Wed-1

Zhang, Shoucheng
Stanford University

Wed-2
Emergence of gravitons from qbit models
Wen, Xiao-GangMIT
We discuss two qbit models, each support a topological phase with long range entanglement.
We show that one phase has collective modes that correspond to gravitons with ommega k3
dispersion. The other phase (with a less reliability) has collective modes that correspond to
gravitons with ommega k dispersion.

Wed-3
Holography and Nuclear Physics
Hashimoto, Koji
RIKEN
QCD describing quarks and gluons is notoriously known as a strongly coupled gauge theory.
AdS/CFT correspondence suggests a way to compute various physical quantities of QCD. I’ll
report on our computations of nuclear force between nucleons (bound states of quarks). This
would be a novel bridge between nuclear physics and particle physics.
17

Wed-4Topological delocalization of two-dimensional massless Diracfermions
Nomura, Kentaro
Tohoku University
It has recently been found that topological insulators exhibit gapless boundary modes which
are described by massless Dirac fermions. We study the problem of Anderson localization in
two dimensional massless Dirac fermion systems, which correspond to surface states of three
dimensional topological insulators. The scaling function of a massless Dirac Hamiltonian
subject to a random scalar potential is computed numerically. Although it belongs to, froma symmetry standpoint, the two-dimensional symplectic class, the scaling function of the
Dirac model monotonically increases with decreasing conductance, in a sharp contrast to theconventional spin-orbit coupled systems. We also provide an argument based on the spectral
flows under twisting boundary conditions, which shows that none of states of the massless
Dirac Hamiltonian can be localized. It is also argued that thehalf-integer quantized Hall phases survive even in the limit of strong disorder or weak magnetic fields.
[1] K. Nomura, M. Koshino, S. Ryu, Phys. Rev. Lett. 99, 146806 (2007)[2] K. Nomura, S. Ryu, M. Koshino, C. Mudry, A. Furusaki, Phys. Rev. Lett.
100, 246806 (2008)

Wed-5
Quantum anomalies in hydrodynamics
Son, Dam
University of Washington
We show that when a volume of quark matter rotates, there is an axial current flowing along
the rotation axis. This eﬀect has been overlooked in all previous treatments of relativistic
fluids until calculations using gauge/gravity duality indicate it existence. The eﬀect is amanifestation of triangle anomalies, and may exhibit itself in heavy ion collisions with nonzero
impact parameter.

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Thu-0Superspace Sigma Models (Pedagogical Lecture)
Schomerus, Volker
DESY
2D Sigma models on target superspaces have many applications ranging from disorderedsystem to the AdS/CFT correspondence. For certain coset superspaces G/H, the associatedsigma model may give rise to a family of conformal field theories with continuously varying
exponents. The solution of such theories is a major challenge that requires developing entirely
new methods. In my first lecture I will review some of the motivation for the study of sigma
models on coset superspaces G/H before revisiting the theory of a compactified free bosonicfield. In this case, the dependence on the compactification radius is well under control. The
model is therefore ideally suited to illustrate some of the techniques and results we shall meetagain when dealing with non-trivial target superspaces.

Thu-1

Minwalla, Shiraz
Tata InstituteThu-2
On universality classes in strongly coupled doped systems
Kiritsis, Elias
University of Crete and APC, Paris

Thu-3
Classification of topological insulators and superconductors
Kitaev, Alexei
California Institute of Technology
Gapped free-fermion Hamiltonians have a topological character, witnessed by the robust19

ness of gapless modes on a boundary between two phases. The hopping matrix of a general
lattice system (possibly with disorder) can be transformed to a Dirac-type operator in thesame universality class, which is characterized using Bott periodicity of Cliﬀord algebras. The
classification depends on the spatial dimension and the presence or absence of charge conservation and time-reversal symmetry. In some cases (e.g., integer quantum Hall systems) the
diﬀerence between phases is stable to interactions, but counterexamples also known.

Thu-4
Fractionalization and Hidden Symmetry in Topological Orders
Sato, Masatoshi
The Institute for Solid State Physics, University of Tokyo
Fractionalization and hidden symmetry in topological orders are discussed. First, for 2+1
dimensional abelian topological orders, I show that flux insertions (or large gauge transformations) pertinent to the toroidal topology induce automorphisms of the braid group, giving rise
to a unified algebraic structure that characterizes the ground-state subspace and fractionallycharged, anyonic quasiparticles. I also argue topological properties by using this algebra. Then
I generalize this argument to the non-abelian gauge theory in 3+1 dimensions, and discuss
the relation between quark (de)confinement and topological orders.

Thu-5
Many-body Schwinger-Landau-Zener Mechanism in
Nonequilibrium Strongly Correlated Electron Systems
Oka, Takashi
University of Tokyo
The dielectric breakdown may be regarded as a condensed matter realization of the
Schwinger mechanism [1] - creation of electron-positron pairs by electric fields - in which
the threshold for breakdown is considerably reduced due to a quantum leakage of the wave
function. In Mott insulators, a many-body counterpart of this phenomena is shown to takeplace[2], which is here studied with the quantum tunneling formalism due to Dykhne-DavisPechukas as applied to the one-dimensional Hubbard model[3]. We implement this for thequantum tunneling rate with an analytic continuation of the Bethe-ansatz solution for excitedstates to a non-Hermitian case. This enables us to extend the many-body Landau-Zener
picture to the thermodynamic limit, with a remarkable agreement with the time-dependent20

density matrix renormalization group result.
[1] J. Schwinger, Phys. Rev. 82, 664 (1951).
[2] T. Oka and H. Aoki, Phys. Rev. Lett. 95, 137601 (2005); T. Oka and H. Aoki in Lecture
Notes in Physics 762 (Springer, 2009), p.251.
[3] T. Oka and H. Aoki, arXiv:0903.2707 (Phys. Rev. B, to appear).

Fri-0(Pedagogical Lecture)
Read, Nick
Yale University

Fri-1
The Supersphere
Schomerus, Volker
DESY
The second lecture is devoted to the study of sigma models whose target space is an odd
dimensional supersphere. The main goal is to calculate the spectrum of the model as a functionof the sphere’s radius. The supersphere can be approached both through analytical techniquesin the continuum formulation and through numerical studies of a discrete version. I discussboth approaches and show that their results nicely agree. As an application, I shall present
strong evidence for a dual description of the supersphere sigma model. The dual model isa supersymmetric extension of the massless Thirring model. The talk will end with some
speculative comments on possible extensions to strings in Anti-deSitter spaces and the duality
with gauge theory.

Fri-2
Critical phenomena in AdS/CFT duality
Natsuume, Makoto
KEK
We study black holes with second-order phase transition in string theory (R-charged black21

holes and holographic superconductors) and study their static and dynamic critical phenomena. Holographic superconductors have conventional mean-field values for static critical exponents, but R-charged black holes have unconventional ones. For dynamic universality class,holographic superconductors belong to model A and R-charged black holes belong to model B
in the classification of Hohenberg and Halperin. Our analysis suggests that some black holes
do obey the theory of critical phenomena in condensed matter physics.

Fri-3
Entanglement Entropy and Topological Insulatorsfrom String Theory
Takayanagi, Tadashi
IPMU, University of Tokyo
The entanglement entropy has recently been studied by many authors as a useful orderparameter in various condensed matter systems, in addition to its importance in quantum
information theory. In this talk, I will explain how we can calculate the entanglement entropy
in strongly coupled quantum systems obtained by applying the AdS/CFT correspondence.
This enables us to calculate this quantum mechanical quantity in terms of classical diﬀerential
geometry.
In AdS/CFT, such quantum systems are typically obtained from D-branes in string theory.
I will also show how the K-theory classification of D-branes is related to the recent ten-foldclassification of topological insulators. This talk is mainly based on the collaborations with
Shinsei Ryu.

Fri-4
Gauge and gravitational anomalies in graphene-related systems
Tanaka, Akihiro
National Institute for Materials Science
The peculiar chiral structure inherent to the low-energy physics of graphene and the 2+1d
pi-flux state have lead to immense activity and a rich interdisciplinary cross-fertilization over
the years. Here we explore their further implications, focusing on induced fermion numbers,
quantum anomalies, and cross eﬀects inquantum transport. Among our findings are:(1) a nontrivial duality among competing orders, each of which correspond to diﬀerent ways

22

of breaking the chiral symmetry.
(2) emergent gravitational Chern-Simons/gravitational BF theories in several graphenerelated insulators and spin liquids.
The former sheds some new light on the class of quantum critical phemenomena dubbed
the deconfined criticality, while the latter bears direct implications to exotic quantum thermal
Hall transport properties.

Fri-5
Universal time-dependent deformations of Schrodinger geometry
Nakayama, Yu
UC Berkeley
What is the field theory dual for the simplest Schrodinger invariant geometry? In order
to attack the question, I study its exact time-dependent deformations. I present 1) scale
invariant but non-conformal deformation, which sounds peculiar(?), 2) conformal invariant
but non-scale invariant deformation, which sounds impossible(!), 3) both conformal and scale
invariant deformation, which sounds...
All these deformations can be embedded in known supergravity solutions, so they are universal features of the gravity dual of Schrodinger invariant theories. In the course of the
discussion, I also find that any time-dependent chemical potential can be exactly treated in
the gravity dual approach.

Fri-5
Quantum Entanglement and Quantum Criticality
Fradkin, Eduardo
University of Illinois, Urbana-Champaign
The entanglement entropy of a pure quantum state of a bipartite system is defined as the von
Neumann entropy of the reduced density matrix obtained by tracing over one of the two parts.
Critical ground states of local Hamiltonians in one dimension have entanglement that diverges
logarithmically in the subsystem size, with a universal coeﬃcient that is is related to the central
charge of the associated conformal field theory. In this talk I will discuss the extension of theseideas to two dimensional systems, either at a special quantum critical point or in a topologicalphase. We find the entanglement entropy for a standard class of z = 2 quantum critical points
in two spatial dimensions with scale invariant ground state wave functions: in addition to a23

nonuniversal “area law” contribution proportional to the size of the boundary of the region
under observation, there is generically a universal logarithmically divergent correction, and in
its absence a universal finite piece is found. This logarithmic term is completely determinedby the geometry of the partition into subsystems and the central charge of the field theory
that describes the equal-time correlations of the critical wavefunction. On the other hand, ina topological phase there is no such logarithmic term but instead a universal constant term.
We will discuss the connection between this universal entanglement entropy and the natureof the topological phase.

P01
Study of short-range correlations in relativistic heavy ion collisions
Ahmad, Mohammad Ayaz
The Aligarh Muslim University, Aligarh, India
Fluctuations depend on the properties of the system and may carry significant information
about the intervening medium created in the collisions. Underlying dynamics of multiparticle
production in relativistic nuclear collisions can be well understood by studying presence offluctuations in these collisions.
Dynamical fluctuations may arise due to some physical processes taking place in the collisions. As an after eﬀect of the formation of QGP, the multiplicity and pseudorapidity distributions of the secondary particles may show large non-statistical fluctuations in some events.
An event-by-event analysis of fluctuations will surely help in separating dynamical and statistical fluctuations. Experimental and theoretical understandings and information are merging
together to relate the fluctuations with phase transition of the confined hadronic matter to
QGP. The power law behaviour of scaled factorial moments (SFMs) on bin size is known asintermittency, which can predict the existence of dynamical fluctuations. Evidence of powerlaw behaviour in experimental data of e+e- annihilation, hadron-hadron, hadron-nucleus andnucleus-nucleus collisions have been found. Thus, intermittency seems to be a general property
of multiparticle production. No single mechanism has been found to explain the intermittency.

P02
The quark mass dependence of the nucleon mass in AdS/QCD
Ahn, Hyo Chul
Pusan National University24

We study the quark mass dependence of the baryon mass using Bottom- up approach ofholographic QCD. We find that nucleon masses are linear to pion mass square and the slopeof ground state, Roper state and N(1535) are 0.74 GeV, 0.47 GeV and 0.35 GeV respectively.
And We compare our result with Lattice QCD and results of Top-down approach.

P03
Dynamical Theory of Graphene from Strong Coupling Expansion ofU(1) Lattice Gauge Theory with Staggered Fermions
Araki, Yasufumi
Dept. of Physics, Univ. of Tokyo
The low-energy eﬀective theory of graphene can be described by the (2+1)-dimensional
massless Dirac particles with the fine structure constant enhanced by 300 times due to the small
fermi velocity of electrons. We regularize this eﬀective theory in terms of the strong couplingU(1) lattice gauge theory with staggerd fermions which have global chiral symmetry. We carryout analytic calculations of the theory by using the techinique of strong coupling expansion:
We found that the mono-layer graphene at strong coupling shows exciton condensation due
to similar mechanism as the dynamical breaking of chiral symmetry in gauge theories.
We derive the magnitude of the condensation together with the mass-gap of fermions andcollective excitons up to the next-to-leading order of the strong coupling expansion. A newformula for the mass of pseudo Nambu-Goldstone exiton is derived, which is analogous to theGell-Mann-Oakes-Renner relation in quantum choromodynamics (QCD).

P04
Non-Hermitian spin chains with real spectra
Bytsko, Andrei
Steklov Mathematics Institute, St.Petersburg
An open spin chain with quantum group symmetry is an example of a quantum mechanicalsystem that has a non-Hermitian Hamiltonian but yet its spectrum can be real. A class of suchmodels will be discussed from the point of view of the theory of quasi-Hermitian operators.

P05

25

The RN/CFT correspondence
Chen, Chiang-Mei
Department of Physics, National Central University, Taiwan
We considered the quantum gravity description of the near extremal extremal ReissnerNordstrom (RN) black hole in the viewpoint of the AdS/CFT correspondence. We show thatthe absorption rate of a scalar filed in RN background matches the two-point function of CFT
which supports the RN/CFT correspondence.

P06
Peak-Dip-Hump from Holographic Superconductivity
Chen, Jiunn-Wei
National Taiwan University
We study the fermionic spectral function in a holographic superconductor model. At zerotemperature, the black hole has zero horizon and hence the entropy of the system is zeroafter the back reaction of the condensate is taken into account. We find the system exhibits
the famous peak-dip-hump lineshape with a sharp low-energy peak followed by a dip then ahump at higher energies. This feature is widely observed in the spectrum of several high-Tc
superconductors. We also find a linear relation between the gap in the fermionic spectrum
and the condensate, indicating the condensate is formed by fermion pairing.

P07
Quantum field theory as applied to graphene
Fialkovsky, Ignat
High Energy and Particle Physics Department, St Petersburg State University
and Instituto de Fisica da Universidade de Sao Paulo
The low-energy quasi-particles in graphene are known to be described as Dirac fermionsin 2+1 dimensions. This model possesses a rigorous quantum field theoretical treatment,
and adopting this approach we investigate the interaction of quasi-particles in graphene withquantum and classical electromagnetic field.
We show that the presence of parity-odd terms in the polarization tensor of Dirac quasiparticles (i.e. in the conductivity tensor) leads to rotation of polarization of the electromagnetic waves passing through suspended graphene films. Parity-odd Chern-Simons type con-26

tributions appear in external magnetic field, giving rise to a quantum Faraday eﬀect, thoughother sources of parity-odd eﬀects may also be discussed. The estimated order of the eﬀect iswell above the sensitivity limits of modern optical instruments. The possible quantization of
the eﬀect is discussed.
We also present a calculation of the Casimir energy between a suspended graphene film
and a parallel plane perfect conductor, using two diﬀerent approaches. First, we use the
QFT approach and evaluate the leading order diagram in a theory with 2+1 dimensional
fermions interacting with 3+1 dimensional photons. Next, we consider an eﬀective theory
for the electromagnetic field with matching conditions induced by quantum quasi-particles ingraphene. The two approaches turn out to be the complementary. The Casimir interaction
itself appears to be rather weak but potentially measurable. It exhibits strong dependence on
the mass of the graphene quasi-particles.

P08
Topological stability of Majorana zero-modes insuperconductor-topological insulator systems
Fukui, Takahiro
Ibaraki University
We derive an index theorem for zero-energy Majorana fermion modes in a superconductortopological insulator system in both two and three dimensions, which is valid for models withchiral symmetry as well as particle-hole symmetry. For more generic models without chiralsymmetry, we suggest that Majorana zero-modes are classified by Z2 .

P09
Holographic approach of phase transitions
Garcia Garcia, Antonio M
University of Lisboa, Portugal
We provide a description of phase transitions at finite temperature in strongly coupled field
theories using holography. For this purpose, we introduce a general class of gravity duals
to superconducting theories that exhibit various types of phase transitions (first or second
order with both mean and non-mean field behavior) as parameters in their Lagrangian arechanged. Moreover the size and strength of the conductivity coherence peak can also becontrolled. Our results suggest that certain parameters in the gravitational dual control the27interactions responsible for binding the condensate and the magnitude of its fluctuations close
to the transition.
In collaboration with: Sebastian Franco (Santa Barbara), Diego Rodriguez-Gomez (Queen
Mary, London)
Reference: arXiv:0911.1354

P10Electromagnetic response in a quantum spin Hall system withelectron correlation
Goryo, Jun
Institute for Industrial Science, the University of Tokyo
Kane-Mele model for Graphene shows the quantum spin Hall eﬀect. We investigate thismodel with the electron correlation, i.e., on-site Coulomb coupling. This interaction can be
expressed to introduce an auxiliary field coupled to the electron spin (sx , sy , sz ). Electromagnetic response of the system can be derived to integrate out Fermions and the auxiliary
field.
We find that, in the strong coupling limit, the system becomes superconducting when sz
is conserved, and becomes insulating when sz -conservation is broken by the Rashba term. In
our discussions, BF-term plays an important role.

P11
Supersymmetric Quantum Hall Eﬀect and Quantum Spin Model
Hasebe, Kazuki
Kagawa National College of Technology
We present a supersymmetric model of the quantum Hall eﬀect and quantum spin model(AKLT model). We derive a supersymmetric Laughlin wavefunction and a supersymmetricvalence bond state. The supersymmetric wavefunction realizes known quantum Hall statessuch as Laughlin, Moore-Read states in extremal limits. We discuss several properties peculiar
to the supersymmetric states.
This work was in collaboration with Y. Kimura, D.P. Arovas, XL Qi, SC Zhang, and K.
Totsuka.

28

P12
Matter production after Inflation in Modular Invariant Supergravity
Hayashi, Mitsuo
Dept. of Physics, Tokai University

P13
On an Airy matrix model with a logarithmic potential
Hikami, Shinobu
Dept. of Basic Sciences, University of Tokyo
The Airy matrix model with a logarithmic potential, the so called Kontsevich-Penner model,
is derived from a Gaussian two-matrix model though a duality. Using the Virasoro constraints,
we find that in addition to the parameter tn , which appears in the KdV hierarchies, one needs
to introduce half-integer indices tn/2 to characterize the model.The free energy as a function of
those parameters may be obtained from the Virasoro constraints. One finds the large N limit
by solving an integral equation. The Kontsevich-Penner model, in its dual version, can behandled explicitly through the Fourier transform of n-point correlation function, from which
one deduces values for topological invariants.
(In collaboration with E. Brezin, LPT, Ecole Normale Superieure.)

P14
The OSP(1|2) WZNW model with and without boundary
Hikida, Yasuaki
Keio University
We study the WZNW model associated with a supergroup OSP(1|2). Correlation functions
can be obtained by making use of a relation to N = 1 super Liouville field theory. Moreover,branes in the OSP(1|2) model are constructed by solving constraints coming from world-sheet
duality.

P15
Critical Phenomena of Holographic Planar Superconductor
29

Hong, Deog-Ki
Pusan National University
We have studied the critical behavior of strongly interacting planar superconductors in theframework of gauge/string duality. We found the interesting relations among the criticalexponents of soft modes of strongly interacting planar superconductors.

P16
Creation of D9-brane–anti-D9-brane Pairs from Hagedorn Transitionof Closed Strings
Hotta, Kenji
Hokkaido University
It is well known that one-loop free energy of closed strings diverges above the Hagedorn
temperature. One explanation for this divergence is that a ‘winding mode’ in the Euclidean
time direction becomes tachyonic above the Hagedorn temperature. The Hagedorn transitionof closed strings has been proposed as a phase transition via condensation of this winding
tachyon. But we have not known the stable minimum of the potential of this winding tachyonso far. On the other hand, we have previously calculated the finite temperature eﬀective
potential of open strings on D-brane–anti-D-brane pairs, and shown that a phase transition
occurs near the Hagedorn temperature and D9-brane–anti-D9-brane pairs become stable. In
this paper, we present a conjecture that D9-brane–anti-D9-brane pairs are created by the
Hagedorn transition of closed strings, and describe some circumstantial evidences.
We show that two types of the amplitude of open strings in the closed string vacuum limit at
the Hagedorn temperature approaches to those of closed strings with winding tachyon insertion
near the Hagedorn temperature. We also show that the potential energy at the open string
vacuum decreases limitlessly as the temperature approaches to the Hagedorn temperature.
It is natural to think that the open string vacuum becomes the global minimum near the
Hagedorn temperature.

P17
Macroscopic Interferences of Neutrino Waves
Ishikawa, Kenzo
Hokkaido University
I report our work on neutrino coherence and new macroscopic interferences of neutrino
30

waves. It is shown that interferences depend on the masses and coherence lengths of theneutrino. Implications for high energy baseline experiments and low energy flavour oscillation
using reactor neutrino are considered.

P18
Casimir Energy of the Universe and the 5D Warped Model
Ichinose, Shoichi
University of Shizuoka
Casimir energy is obtained in the 5D warped model. The warp parameter is properly
renormalized. Regarding Casimir energy as the main contribution of the cosmological constant,
we show its renormalization behavior. This is a solution to the cosmological problem.
Related reference: ArXiv:1001.0222 [hep-th]

P19
Ballistic transport, chiral anomaly and emergence of the electron hole plasma in graphene
Kao, Hsien-chung
National Taiwan Normal University
The process of coherent creation of particle - hole excitations by an electric field in graphene
is quantitatively described using a dynamic ”first quantized” approach. We calculate theevolution of current density, number of pairs and energy in ballistic regime using the tightbinding model. The series in electric field strength E up to third order in both DC and AC
are calculated. We show how the physics far from the two Dirac points enters various physicalquantities in linear response and how it is related to the chiral anomaly. The third harmonic
generation and the imaginary part of conductivity are obtained. It is shown that at certain
time scale tnl E −1/2 the physical behaviour dramatically changes and the perturbation theory
breaks down. Beyond the linear response physics is explored using an exact solution of thefirst quantized equations. While for small electric fields the I-V curve is linear characterized
by the universal minimal resistivity, at t > tnl the conductivity grows fast. The copious paircreation (with rate E 3/2 ), analogous to Schwinger’s electron - positron pair creation fromvacuum in QED, leads to creation of the electron - hole plasma at ballistic times of order tnl .
This process is terminated by a relaxational recombination.

31

P20
Deformations of Lifshitz holography
Keeler, Cynthia
Harvard University
The simplest gravity duals for quantum critical theories with z = 2 ‘Lifshitz’ scale invarianceadmit a marginally relevant deformation. Generic black holes in the bulk describe the field
theory with a dynamically generated momentum scale Λ as well as finite temperature T .
We describe the thermodynamics of these black holes in the quantum critical regime whereT  Λ2 . The deformation changes the asymptotics of the spacetime mildly and leads tointricate UV sensitivities of the theory which we control perturbatively in Λ2 /T .

P21
Supersymmetric vacua of mass-deformed N=6 Chern-Simons theory
Kim, Seok
Seoul National University

P22
Holography and Lorentz Invatiance Violation
Koroteev, Peter
University of Minnesota
Recently a family of solutions of Einstein equations in backgrounds with broken Lorentz
invariance was found ArXiv:0712.1136. We show that the gravitational solution recently obtained by Kachru, Liu and Mulligan in ArXiv:0808.1725 is a part of the former solution
which was derived earlier in the framework of extra dimensional theories. We show how theenergy-momentum and Einstein tensors are related and establish a correspondence between
parameters which govern Lorentz invariance violation. Then we demonstrate that scaling behavior of two point correlation functions of local operators in scalar field theory is reproduced
correctly for two cases with critical values of scaling parameters. Therefore, we complete thedictionary of “tree-level” duality for all known solutions of the bulk theory. In the end we
speculate on relations between RG flow of a boundary theory and asymptotic behavior ofgravitational solutions in the bulk.
32

P23
Extended Quantum Dimer Model -Mapping by the S = 1 algebra
Nakata, Kouki
Kyoto University YITP(Yukawa Institute for Theoretical Physics)
Since P.W.Anderson’s 1973 paper[1], the search for a resonating valence bond(RVB) stateshas been one of the recurrent theme in research on frustrated antiferromagnets. Quantum
Dimer Model(QDM) proposed by Rokhsar and Kivelson in 1988 [2] exhibits crystalline orderand confined spinons on the square lattice,except at RK-point. On the point,a short-ranged
RVB state is realized.
Recently Moessner and Sondhi have revealed that there is a truly short-ranged RVB phase
for a finite range of parameters on the triangular lattice[3]. What is more, they have noticed
that Ising gauge physics is exactly the physics of the short-ranged RVB and have mapped the
QDM to an Ising gauge theory[4].
Refering to these research,we propose Extended QDM(EQDM).This model is defined by
the S=1 algebra and we have succeeded in deriving a S=1 spin Hamiltonian which is completely consistent with EQDM.Furthermore,this model exhibits the phase transitions(e.g.fromcolumnar to herringbone) pointed out by Papanikolaou et al. [5] as well as the usual QDM
transitions.
We now detecting a spin liquid region of EQDM.
[1]P.W.Anderson,Mater.Res.Bull.8,153(1973); Science235,1196(1987)[2]D.S.Rokhsar and S.A.Kivelson,Phys.Rev.Lett.61,2376(1988)[3]R.Moessner and S.L.Sondhi,Phys.Rev.Lett.86,1881(2001)[4]R.Moessner and S.L.Sondhi,Phys.Rev.B.65,024504(2001)[5]S.Papanikolaou,K.S.Raman,and E.Fradkin,Phys.Rev.B.75,094406(2007)

P24
Holographic Anyons in the ABJM Theory
Lin, Feng-Li
Dept. of Physics, National Taiwan Normal University
We consider the holographic anyons in the ABJM theory from three diﬀerent aspects of
AdS/CFT correspondence. First, we identify the holographic anyons by using the field equations of supergravity, including the Chern-Simons terms coupled to the probe branes. We findthat the composite of Dp-branes wrapped over CP3 with the worldvolume magnetic fields can
33

be the anyons. Next, we discuss the possible candidates of the dual anyonic operators on the
CFT side, and find the agreement of their anyonic phases with the supergravity analysis. Finally, we try to construct the brane profile for the holographic anyons by solving the equationsof motion and Killing spinor equations for the embedding profile of the wrapped branes. As
a by product, we find a BPS spiky brane for the dual baryons in the ABJM theory.

P25
Vortex lattice for a holographic superconductor
Maeda, Kengo
Shibaura Institute of Technology
We investigate the vortex lattice solution in a (2+1)-dimensional holographic model of superconductors constructed from a charged scalar condensate. The solution is obtained perturbatively near the second-order phase transition and is a holographic realization of the
Abrikosov lattice. Below a critical value of magnetic field, the solution has a lower free energy
than the normal state. Both the free energy density and the superconducting current are
expressed by nonlocal functions, but they reduce to the expressions in the Ginzburg-Landau(GL) theory at long wavelength. As a result, a triangular lattice becomes the most favorable
solution thermodynamically as in the GL theory of type II superconductors.

P26
Simulating dense QCD matter with ultracold atomic boson-fermion
mixtures
Maeda, Kenji
University of Tokyo
We delineate, as an analog of two-flavor dense quark matter, the phase structure of a manybody mixture of atomic bosons and fermions in two internal states with a tunable bosonfermion attraction. The bosons b correspond to diquarks, and the fermions f to unpaired
quarks. For weak b-f attraction, the system is a mixture of a Bose-Einstein condensate anddegenerate fermions, while for strong attraction composite b-f fermions N, analogs of thenucleon, are formed, which are superfluid due to the N-N attraction in the spin-singlet channel.
We determine the symmetry breaking patterns at finite temperature as a function of the b-f
coupling strength, and relate the phase diagram to that of dense QCD.

34

P27
Correlation functions for higher spin integrable systems
Matsui, Chihiro
Department of Physics, The University of Tokyo
Various integrable systems, which belong to Uq(sl2)-symmetry, such as the sine (sinh)Gordon model and the XXZ model, have been studied. Calculation of correlation functions ofthem is one of the most interesting topics in study of integrable systems.
The biggest problem in computation of correlation functions via the Bethe ansatz is how
to deal with sums which arise as a result of commutation relations among the monodromy
matrix elements. The induction method in respect to the total spin of a system and changeof basis are well-known methods to resolve this problem.
We derived multi-integral expressions of correlation functions for higher spin integrable
systems. Furthermore, it was showed that the number of terms in sums appeared in correlation
functions of higher spin integrable systems are reduced to that of spin 1/2 integrable systems byconsidering actions of the Uq(sl2) algebra on irreducible subspaces in multiple tensor products.

P28
Adding Flavor to AdS(4)/CFT(3)Meyer, Rene
University of Crete, Heraklion, Crete, Greece
In this talk I present results of a recent attempt to introduce quenced fundamental (quarklike) degrees of freedom into the N=6 supersymmetric Chern-Simons-Matter theory put forward by Aharony, Bergman, Jaﬀeris and Maldacena (ABJM). The additional fields are introduced by means of probe branes embedded in the dual AdS4xCP3 geometry. I discuss several
intersections, space-filling and defect-like, which might also be of interest for holograpic descriptions of condensed matter systems.

P29
Optical Hall conductivity in the graphene quantum Hall system —what happens to a topological number in ac response
Morimoto, Takahiro

35

University of Tokyo
The quantum Hall eﬀect represents a topological number, which is because the (dc) Hall
conductivity, expressed as a current-current correlation function, coincides with a Berry’s
curvature so that the Hall conductivity becomes the Chern number of a U(1) bundle overthe Brillouin zone spanned as a 2-dimensional torus.We can then pose an intriguing question:
what will happen to the topological number if we go over to ac response, i.e., the optical Hall
conductivity, σxy (ω).
Although one might at first expect the quantum Hall behavior be washed out in ac, wehave revealed that the series of steps (plateaus) in the Hall conductivity against the Fermi
energy is unexpectedly retained in the optical Hall conductivity even in the THz regime, forboth the ordinary two-dimensional electron gas and the massless Dirac model of graphene instrong magnetic fields. While the plateau height in ac deviates from the quantized values,
the eﬀect is indeed robust against significant strengths of disorder, which we attribute toan eﬀect of Anderson localization. Specifically, an important source of disorder in actual
graphene (single atomic layer of carbon atoms in the form of a honeycomb lattice) is known
to be ripples (corrugation of the atomic plane), which eﬀectively acts as a random gauge field.
Owing to Atiyah-Singer’s theorem which ensures protected chiral zero modes, the Landaulevel that resides at the Dirac point (electron-hole symmetric point) remains delta-function
like, because a random gauge field respects the chiral symmetry. We have shown that theprotection is inherited by the ac response as an anomalously sharp step structure in the
optical Hall conductivity.

P30
Supersymmetric sigma-Model Based on the SO(2N+1) Lie Algebraof the Fermion Operators - A way to proper solution Nishiyama, Seiya
Centro de Fisica Computacional, Departamento de Fisica, Universidade de Coimbra
The extended supersymmetric sigma-model is proposed on the bases of SO(2N+1) Lie algebra spanned by fermion annihilation-creation operators and pair operators. The canonicaltransformation, extension of an SO(2N) Bogoliubov transformation to an SO(2N+1) group, isintroduced. To construct consistent anomaly-free supersymmetric coset models, we must embed an SO(2N+1) group into an SO(2N+2) group and use SO(2N+2)/U(N+1) coset variableson the Kaehler manifold. We adopt a coset coordinate in an anomaly-free spinor representationof SO(2N+2) group and give a corresponding Kaehler potential and a Killing potential for an
anomaly-free SO(2N+2)/U(N+1) model based on each positive chiral spinor representation.
Then we have a f-deformed reduced scalar potential. It is minimized with respect to the VEV36

of anomaly-free supersymmetric sigma-model fields. Thus we find an interesting f-deformed
proper solution for an anomaly-free SO(12)/SU(6)XU(1) supersymmetric sigma-model.

P31
D-brane in Bose-Einstein Condensates
Nitta, Muneto
Keio University
We show that wall-vortex composite solitons, analogues of D-brane in string theory, canbe realized in rotating phase-separated two-component Bose-Einstein condensates and they
are experimentally observable. The structure is analyzed by the generalized nonlinear sigma
model for the pseudospin of this system. The wall-vortex junction has a characteristic spin
texture and a negative monopole charge density, which can be identified as a point defect atinterface, called boojum.

P32
Interstellar Bubbles Candidates in the Far Infra-Red Sky
Panthi, Rajesh
Tribhuvan University
I present the results of numerical simulations for the first 104 years of the developmentof spherically symmetric interstellar bubble formed by the Asymptotic Giant Branch (AGB)
wind. Assuming three phase interstellar medium (ISM) model we estimate the size of the interstellar bubbles. Our result will be based on 106 virtual stellar wind particles and discussed
in the context of early and late AGB star. In addition to the numerical simulations, we systematically searched the bubble like structure in the IRASS (Infrared Astronomical Satellite
Survey) and measured their sizes. A comparison between the results of the numerical simulations and the observations is discussed. It is found that the size of the interstellar bubble lie
in the range 1.48 pc to 39.20 pc if the stellar wind speed is 15 km/s (early AGB wind). The
size of the bubble ranges 2.82 pc to 74.64 pc if the stellar wind speed goes to 75 km/s (i.e.,late AGB phase).
The cold ISM forms small-sized bubble whereas the hot ISM produces large-sized bubble.
However the stability of cold interstellar bubble is higher than that of the hot interstellar
medium. As a preliminarily investigation we propose 8 interstellar bubble candidates, probably
shaped by the White Dwarf and the Pulsar. The first four candidates are relatively small-sized37

(major diameter ¡ 0.88 pc) because of the low speed stellar wind emitted during the evolutionof White Dwarfs. The last four bubble candidates are intermediate sized, probably shaped by
the relativistic wind of the Pulsar. The emission feature of the outer shocked region should
be studied in the future in order to justify the nature of the interstellar bubble.

P33
The super Quantum Lifshitz Model from the Nicolai Map
Reﬀert, Susanne
IPMU
In this talk, I will describe a method based on the Nicolai map of stochastic quantization to
generate non-Lorentz invariant quantum field theories. This method gives rise to non-Lorentz
invariant field theories such as the quantum Lifshitz model and Horava-Lifshitz gravity. This
formalism is easy to use in concrete calculations. I will illustrate this by deriving the Feynman
rules for an interacting version super quantum Lifshitz model.

P34
Entanglement through conformal interfaces
Satoh, Yuji
University of Tsukuba
We consider entanglement through permeable interfaces in the c=1 (1+1)-dimensional conformal field theory. We compute the partition functions with the interfaces inserted. By the
replica trick, the entanglement entropy is obtained analytically. The entropy scales logarithmically with respect to the size of the system, similarly to the universal scaling of the ordinary
entanglement entropy in (1+1)-dimensional conformal field theory. Its coeﬃcient, however,is not constant but controlled by the permeability, the dependence on which is expressed
through the dilogarithm function. The sub-leading term of the entropy counts the winding
numbers, showing an analogy to the topological entanglement entropy which characterizes the
topological order in (2+1)-dimensional systems.

P35
Bulk-boundary flows in the Virasoro minimal models

38Schmidt-Colinet, Cornelius
IPMU
We consider the behaviour of boundary conditions under the least-relevant bulk perturbation for the Virasoro minimal models. Combining perturbative RG techniques, insightsfrom defects, and results from non-perturbative boundary flows, we determine the boundary
condition at the infrared fixed point.

P36
Density matrix elements at finite temperatures
Suzuki, Junji
Shizuoka University
Exact evaluation of density matrix elements of spin chains at finite temperature will be
discussed in view of the quantum information.

P37
2-Dimensional Holographic Quantum Liquids
Wapler, Matthias
CQUeST, Sogang University
We study the low-temperature limit of holographic fundamental matter in a 2+1 dimensional defect setup at fixed mass and finite baryon number density. This defect case is special,
as we find novel non-trivial temperature independent scaling solutions for the probe-brane
embeddings as opposed to e.g. the usual “narrow funnel” low-temperature limit. By studying the thermodynamics, we observe a quantum liquid with density-dependent ground-statedegeneracy and energy, and suppressed heat capacity.

P38
Fermion structure of non-Abelian vortex in color superconductivity
Yasui, Shigehiro
KEK
We study the internal fermionic structure of a non-Abelian vortex in color superconductivity39

by using the Bogoliubov-de Gennes (B-dG) equation. The non-Abelian vortices appear in the
Color-Flavor-Locked phase associated with the symmetry breaking pattern SU(3)c+L+R →SU(2)c+L+R × U(1)c+L+R . We analyze quark spectrum in the B-dG equation by treating thediquark gap having the vortex configuration as a background field. We find that there arezero energy states (zero modes) inside the vortex, and that triplet and singlet zero modes
form a multiplet of the unbroken symmetry. We also discuss the low energy eﬀective theoryof fermion zero modes in 1+1 dimensions.

P39
Schrodinger invariant solutions of M-theory with Enhanced
Supersymmetry
Yavartanoo, Hossein
Korea institute for advanced study
We find the most general solution of 11-dimensional supergravity compatible with N = 2
super-Schrodinger symmetry with six supercharges and SU(2) × SU(2) × U(1) × Z2 global
symmetry. It can be viewed as a one-parameter extension of a recently constructed solution by
Ooguri and Park. Our original motivation was to find the gravity dual of the non-relativistic
ABJM theory. But, our analysis shows that no such solution exists within the reach of ourassumptions. We discuss possible reasons for the non-existence of the desired solution. We
also uplift a super-Schrodinger solution in IIB supergravity of Donos and Gauntlett to 11dimension and comment on its properties.

P40
On String Embedding of Lifshitz Fixed Point
Li, Wei
IPMU, Tokyo University
The aim of this work is to find the string theory dual of the Lifshitz fixed point.
We construct a 5D gravitational Lifshitz solution, albeit with non-constant dilaton, in a
D3-D7 system. To cure the problem of a diverging dilaton at the boundary, we further finda solution interpolating between the Lifshitz geometry in IR and AdS5 in UV. On the field
theory side, this interpolating solution corresponds to an anisotropic RG flow between the N=4
SYM and the Lifshitz theory. We also present some no-go theorems against the embedding of
4D (constant-dilaton) Lifshitz solution in various string compactifications.

40

[1] arXiv: 0905.0688 (with T. Azeyanagi and T. Takayanagi).
[2] arXiv: 0908.0363 (with T. Nishioka and T. Takayanagi).

41Panel discussion■Panelists:

E. Fradkin, S. Fujimoto, S. Hartnoll, S. Kachru, A. Kitaev, H. Liu, S. Minwalla,

and S. C. Zhang■Moderators: H. Aoki and H. Ooguri■Proposed questions:

1. Can we perform a test of the AdS/CFT correspondence in condensed matter or atomic
physics laboratories?
2. Can string theory give new insights on integrable lattice models or field theories, or can
it give something beyond the Bethe ansatz solvability?
3. What is a (conformal) field theory describing the plateau transition of the 2d quantum
Hall eﬀect?
4. What are ground states of strongly correlated lattice models, such as the 2d Hubbard
model, the S = 1/2 Heisenberg model on the Kagome lattice?
5. Is there a metal-insulator transition in (2+1)-dimensional electron systems in the presence of both interactions and disorder?
6. Can we describe strongly correlated systems out of equilibrium?
7. Can we solve the critical theory of the 3d Ising model?
8. Can we classify fixed point Hamiltonians including topological phases?
9. Can we find new classes of non-perturbative phenomena/treatments?
10. Will non-abelian statistics arise in condensed-matter physics beyond the fractional quantum Hall systems?
11. How can we expand the NG approach in systems with more than one gauge symmetries
are spontaneously broken, where condensed matter examples are multiband superconductors/cold atoms, ferromagnetic superconductors, etc.
12. Are there the strong-coupling theories/treatments developed in the condensed-matterphysics applicable to HEP?
13. Can you provide a useful definition of a “Mott insulator” in terms of continuum field
theoretic calculables, as opposed to in terms of dynamics of an underlying lattice model(c.f. the Hubbard model with strong repulsive interactions at half-filling)? In particular,
how would theorists working with gravity duals or with an abstract formalism that
calculates correlation functions in a quantum field theory, be able to characterize a
Mott insulator as opposed to a band-theoretic insulator? (Kachru)
14. What is a useful definition of a glass phase? Are there aspects of the glass transition(e.g. divergence in viscosity) that might be amenable to a gravity treatment, or that inany case remain mysterious from existing theoretical models? (Kachru)
15. Are there simple examples of quantum critical points where the scaling dimensions ofa significant number of scaling operators are known from experiment? If so, which
examples? (Kachru)
4216. Are there places in condensed matter or atomic/molecular/optical physics where
adjoint-like large N gauge theories may be reasonable models of underlying phenomena? If not, is there a serious possibility of (and interest in) engineering such systems
using optical lattices? (Kachru)
17. What is known, within controlled computations, about disordered strongly interacting
systems in 2+1 dimensions? Are there ‘localisation’ transitions? Can AdS/CFT help
here? (Hartnoll)
18. To what extent is the ‘strange metal’ region of the heavy fermion compounds theoretically understood? Various non-controlled computations (Hertz-Millis etc.) seemto reproduce some scalings, but I have received conflicting statements from the condmat community about the extent to which comparing these computations with data ismeaningful. Can AdS/CFT help here? (Hartnoll)
19. To what extent does the ‘strange metal’ region of the cuprates or of the heavy fermions
have well-define quasiparticles excitations? (Hartnoll)
20. Some intersecting D-brane systems at finite density have a Fermi surface at weak coupling. Is there any trace of these Fermi surfaces in the strongly coupled gravitational
dual? (Hartnoll)
21. Is the Zk parafermion CFT (or Wess-Zumino-Witten CFT) a unique field theory which
describes non-Abelian anyons? (Fujimoto)22. Is there a deep theoretical structure associated with the minus sign problem with quantum Monte Carlo simulation? (Zhang)
23. Can we learn about axions, theta vacuum and strong CP problem from topologicalinsulators? (Zhang)
24. What are the promising probes of Majorana fermions in cond mat and high energy?
(Zhang)43