国際会議出席発表（★：招待講演、☆：⼝頭発表、△：short oral+poster、□：poster）
Year1993 (H5)

海外で開催された国際会議及び、講演★MT-13(Victoria, Canada) (9.21-27)“Low Thermal Conductive Bi-2223 Tapes
Sheathed with Ag-Au Alloys”

1994 (H6)□15th ICEC (Genova, Italy) (6.7-10)“Possibility of Ag2O+YBa2Cu3O7-X ceramics for
low temperature thermoelectric refrigeration”

国内で開催された国際会議△ICT12 (Yokohama) (11.9-11)“Use of Bi2223 Superconducting
Tapes Sheathed with Ag-Au Alloys fora Passive Thermoelement”☆Jpn.-US workshop (Kyoto)□M2S (Grenoble, France) (7.7-11)“Thermal Conductivity of Bi-2212 Single
Crystals Prepared by TSFZ Method”“Phonon Thermal Diffusivity and Conductivityof Oxygen Deficient YBa2Cu3O7”
1995 (H7)1996 (H8)□Phonons'95 (Sapporo)“Thermal Conductivity and Diffusivityof Nd2-XCeXCuO4”☆WTC'96 (Budapest, Hungary) (7.7-10)“Model analyses of thermal conductivity andpurity of doped Ag in Ag+YBa2Cu3O7”□MOS'96 (Karlsruhe, Germany) (8.1-7)“Thermal conductivity and phonon scattering
mechanisms in La1-xMxCuO4”

1997 (H9)1998 (H10)1999 (H11)□LT21 (Prague, Czech) (8.8-14)“Effect of Y-site and Ba-site Substitution on
Thermal Properties of YBa2Cu3O7-d”“Proposal of Three Terminal Method for Low
Temperature Thermal Diffusivity Measurement”□ICM'97 (Cairns, Australia) (7.27-8.1)“Thermal conductivity and phonon scattering of
La1-XSrXMnO3”□CIMTEC'98 (Florence, Italy) (6.18-28)“THERMAL CONDUCTIVITY OF T*-PHASE(Nd1-x-yCexSry)2CuO4 OXIDESUPERCONDUCTORS”“ULTRASONIC AND PHONON THERMAL
TRANSPORT STUDIES ON YBa2Cu3O7-d
OXIDE SUPERCONDUCTORS”☆Phonons'98 (Lancaster, England) (7.26-31)“Two-level-like anomalous phonon scattering in
La1-XSrXMnO3 and La2-XSrXCuO4”□MOS'99 (Stockholm, Sweden) (7.28-8.2)□SCES'99 (Nagano) (8.24-27)“Enhanced Phonon Scattering below Tc Caused First-order-like ferromagnetictransition in (La1-yPry)1-x(Ca1by Zn and Ni Substitution in La1.85Sr0.15CuO4”
zSrz)xMnO3 (X~0.25)”□LT22 (Helsinki, Finland) (8.4-11)
Sound Velocity Anomaly Related to Charge
Ordering in La1-xCaxMnO3”

☆JARCAT Workshop (Kyoto) (5.31)“Sound Velocity Anomalies Related toCharge Ordered Transition in La1xCaxMnO3 (0<x<1)”

2000 (H12)△LLD2k (Tsukuba) (7.23-26)“Heat Transport Anomalies aroundFerromagneticandCharge-order
Transitions in La1-xCaxMnO3”

2001 (H13)2002 (H14)2003 (H15)2004 (H16)□Phonons2001 (Dartmouth, USA) (8.12-17)“Thermal diffusivity of La1-XCaXMnO3 up to
1200 K”□ISS2000 (Tokyo) (10.14)“Thermal contact resistance between
high-Tc superconductor and copper”☆IMR workshop (Sendai) (5.22)“Charge/Orbital Order Fluctuation andLattice Softening in La1-xCaxMnO3”□MT-17 (Genova, Swiss) (9.24-27)“Thermal Conductivity, Thermal Diffusivity and
Thermoelectric Power of Sm-Based Bulk
Superconductors”□SCES'02 (Kraków, Poland) (7.8-15)“THERMAL TRANSPORT IN
FERROMAGNETIC La1-XAEXMnO3 WITHLARGE DIVALENT IONS”△Orbital2001 (Sendai) (9.11-13)“Heat Transport Enhancement in
Ferromagnetic Metallic Phase of La1XBaXMnO3”□LT23 (Hiroshima) (August)“Co Site Substitution Effect on
Thermoelectric Properties in Na(Co1XMX)2O4 (M=Ni, Fe, Mn, Cu)”

★チェコ科学アカデミー講演(7.16)□ISS2002 (Yokohama)“Thermal conductivity of YBaCuO
bulk superconductors under appliedfield: effect of content and size ofY211 phase”☆MT-18 (Morioka) (10.21)“Flux Motion Studies by means ofTemperature Measurement in
Magnetizing Processes for HTSCBulks”

文部科学省短期在外研究員（チェコ科学アカデミー）(2003.7.26~9.26)□ICM'03 (Roma, Italy) (7.27-31)“Thermal conductivity and magnetism in (Ca1XSrX)MnO3”☆ICT2003 (La Grande-Motte, France) (8.1721)“Search for p-type Oxide Thermoelectrics –Cobaltites”“Enhanced Thermoelectric Properties at X~0.1
in La1-XSrXCoO3 and La1-XSrX(Co1-YMY)O3(M=Cr, Cu)”
□ICT2004 (Adelaide, Australia) (7.24-31)“Influence of Co-site Substitution on
Thermoelectric Properties in La1-xSrxCoO3”“Size Effect of A-site Cation on n-type
Thermoelectric Properties in CaMnO3-basedSystem”□ASC2004 (Jacksonville, U.S.A) (10.2-11)“Effect of Metal Ring Setting outside HTSC
Bulk Disk on Trapped Field and Temperature
Rise in Pulse Field Magnetizing”☆ISS2003 (Tsukuba) (10.27)“Estimation of generated heat in pulse
field magnetizing for SmBaCuO bulk
superconductor”★ISS2004 (Niigata) (11.16)“Approach from temperature
measurement to trapped fieldenhancement in HTSC bulks by pulse
field magnetizing”“Database for thermal and mechanicalproperties of REBaCuO bulks”

2005 (H17)□SCES’05 (Wien, Austria) (7.28-31)“Anomalous Sound Velocity Behavior of La1XCaXMnO3 (X~0.48) in Applied Field”“Thermal Conductivity Anomaly in
La0.52Ca0.48MnO3 under Applied Field”□EUCAS2005 (Wien, Austria) (9.12-15)“Trapped Field over 4 Tesla on GdBaCuO Bulkby Pulse Field Method and Magnetizing
Mechanis☆PASREG (Tokyo University ofMarine Science and Technology）(10.20)“Thermal Conductivity andThermoelectric Power of DyBaCuO
Bulk Superconductor”☆ISS2005 (Tsukuba) (10.24-26)“Higher trapped field over 5 Tesla on
HTSC bulk by modified pulse fieldmagnetizing”□MT19 (Genova, Italy) (9.19-23)“Low-Thermal-Conductive DyBaCuO Bulk
Superconductor for Current Lead Application”★チェコ科学アカデミー講演(9.11)
2006 (H18)2007 (H19)2008 (H20)2009 (H21)2010 (H22)2011 (H23)☆6th PASREG (Cambridge, England) (9.11-18)“Possible Explanation for Trapped Field
Enhancement on REBaCuO Bulk by Modified
Multi-pulse Technique with Stepwise Cooling(MMPSC)”☆ASC2008 (Chicago, USA) (8.17-23)“Pulsed Field Magnetization for GdBaCuO
Bulk with Stronger Pinning Characteristics”□EUCAS2009 (Dresden, Germany) (9.12-20)“Highly efficient magnetic separation using
five-aligned superconducting bulk magnet”★チェコ科学アカデミー講演 (9.20)“Recent research progresses of Cobaltites andManganites in Iwate”□ASC2010 (Washington DC, USA) (8.1-10)“Analysis of Temperature and Magnetic FieldDistribution in Superconducting Bulk during
Pulsed Field Magnetization”□EUCAS2011 (Den Hague, The Netherland)(9.17-25)“Three-dimensional simulation of magnetic flux
dynamics and temperature rise in HTSC bulk
during pulsed field magnetization”☆ISS2006 (Nagoya) (10.30-11.2)“Importance of initial ‘‘M-shaped’’
trapped field profile in a two-stage
pulse field magnetization (MMPSC)
method”□ISS2007 (Tsukuba) (11.5-7)“Trapped field characteristics on f 65
mm GdBaCuO bulk by modified
multi-pulse technique with stepwise
cooling (MMPSC)”□ISS2008 (Tsukuba) (10.27-29)“Enhancement of total trapped fluxes
on f65 mm GdBaCuO bulk by multipulse techniques”☆ISS2009 (Tsukuba) (11.1-3)“Temperature measurements in smallholes drilled in superconducting bulk
during pulsed field magnetization”□ISS2010 (Tsukuba) (10.31-11.2)“Simulation of flux dynamics in asuperconducting bulk magnetized bymulti-pulse”★チェコ科学アカデミー講演 (9.17)
2012 (H24)☆ASC2012 (Portland, USA) (10.9-13)“Numerical Simulation of Trapped Field andTemperature Rise in MgB2 Bulks Magnetizedby Pulsed Field”★大連理工大講演(6.12-13)□ICEC24-ICMC2012 (Fukuoka)(5.14-18)“Trapped field and temperature rise in
MgB2 bulks magnetized by pulsedfield”

2013 (H25)2014 (H26)2015 (H27)□EUCAS2013 (Genova, Italy) (9.15-20)“Trapped magnetic field between double
stacked MgB2 bulks magnetized by pulsedfield”★チェコ科学アカデミー講演(9.22)“Recent research progresses of Cobaltites andManganites in Iwate”☆ASC2014 (Charlotte, USA) (8.9-18)“Recent progress of MgB2 bulk magnets
magnetized by pulsed field”☆ISS2013 (Tokyo) (11.19)“Trapped field and flux dynamics in
MgB2 superconducting bulks
magnetized by pulsed field”☆IU-MRS (Fukuoka) (8.28-31)“Characteristics and trapped field of
REBaCuO and MgB2 superconductingbulks”★サスカチュアン大講演 (12.1-3)☆UK-Japan workshop (Cambridge, England)(4.11-19)“Magnetizing process and trapped field of
REBaCuO and MgB2 superconducting bulks”★PASREG2015 (Liege, Belgium) (9.1-5)“Pulsed field magnetization for (RE)BCO andMgB2 superconducting bulks and theirapplications”

2016 (H28)2017 (H29)2018 (H30)2019 (R1)□MT25 (Seoul, South Korea) (10.18-22)“Trapped field homogeneity in NMR
superconducting bulk magnet by the insertion ofhigh-Jc HTS cylinder with various positions,lengths and shapes”☆ASC2016 (Denver, USA) (9.4-11)“Trapped Field Enhancement of a Thin, High-Jc
MgB2 Bulk without Flux Jumps using Pulsed
Field Magnetization with a Split-type Coil witha Soft Iron Yoke”□MT25 (Amsterdam, The Netherland) (8.269.2)“New proposal of mechanical reinforcement
structures to annular REBaCuO bulk magnet forcompact and cryogen-free NMR spectrometer”★Cambridge 大での招待講演(4.11-13)“Recent research progresses in Iwate”☆ASC2018 (Seattle, USA) (10.28-11.2)“Influence of Inner Diameter and Height ofRing-shaped REBaCuO Bulks on Trapped Field
and Mechanical Stress during Field-cooled
Magnetization”★PASREG2019 (Prague, Czech) (8.27-30)“A new mechanical reinforcement structure for
REBaCuO bulks during field-cooledmagnetization to achieve higher trapped fields
without fracture”★EUCAS2019 (Glasgow, England) (9.1-5)“A Hybrid Trapped Field Magnet Lens
(HTFML): concept and realization”★PASREG2017 (Tokyo) (12.11-12)“Mechanical Reinforcement ofREBaCuO Bulk during Field-Cooled
Magnetization -- Road to Achieve
Trapped Field Higher than 20 Tesla –"★ISS2018 (Tsukuba) (12.12-14)“Mechanical reinforcement ofREBaCuO bulk during field-cooledmagnetization to achieve higher
trapped field without fracture”★ISS2019 (Kyoto) (12.3-5)“A Hybrid Trapped Field Magnet Lens
(HTFML): concept and experimentalrealization”

2020 (R2)2021 (R3)★PASREG (Shanghai, China: WEB) (11.11-13)“A Hybrid Trapped Field Magnet Lens
(HTFML): concept and validation”