{"id":138,"date":"2021-08-15T05:26:59","date_gmt":"2021-08-14T20:26:59","guid":{"rendered":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/?page_id=138"},"modified":"2026-03-27T12:19:44","modified_gmt":"2026-03-27T03:19:44","slug":"publications","status":"publish","type":"page","link":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/publications\/","title":{"rendered":"\u7814\u7a76\u6210\u679c"},"content":{"rendered":"\n
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\u6700\u8fd1\u306e\u51fa\u7248\u8ad6\u6587\u7b49<\/h2>\n\n\n\n
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  1. Giacomo Marmorini<\/em><\/strong>, Takeshi Fukuhara, Daisuke Yamamoto<\/em><\/strong>
    Measuring Entanglement Without Local Addressing in Quantum Many-Body Simulators via Spiral Quantum State Tomography
    <\/a>PRX Quantum 7<\/strong>, 010355 (2026)
    Published 18 March, 2026
    DOI: https:\/\/doi.org\/10.1103\/1xzz-njyy

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  2. Shunichiro Kinoshita, Keiju Murata, Daisuke Yamamoto<\/em><\/strong>, Ryosuke Yoshii
    Simulating Quantum Field Theories with Boundaries in Curved Spacetimes Using Open Spin Systems<\/a>
    DOI:10.48550\/arXiv.2602.17935

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  3. K. Nihongi, T. Kida, Y. Narumi, Y. Etoh<\/em><\/strong>, D. Yamamoto<\/strong><\/em>, M. Matsumoto, N. Kurita, H. Tanaka, K. Yu. Povarov, S. A. Zvyagin, J. Wosnitza, K. Kindo, Y. Uwatoko, M. Hagiwara
    Pressure-Tuned Metamagnetism and Emergent Three-Body Interactions in CsFeCl3<\/a>
    DOI:10.48550\/arXiv.2512.21682

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  4. Daichi Imagawa<\/em><\/strong>, Keiju Murata, Daisuke Yamamoto<\/em><\/strong>
    Operator dependence and robustness of spacetime-localized response in a quantum critical spin chain<\/a>
    Physical Review B 113<\/strong>, 014311 (2026)
    Published 20 January, 2026
    DOI: https:\/\/doi.org\/10.1103\/nqs6-7t2p

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  5. Yuki Miyazaki, Shiori Tanigawa<\/em><\/strong>, Giacomo<\/em><\/strong> Marmorini<\/em><\/strong>, Nobuo Furukawa, Daisuke Yamamoto<\/em><\/strong>
    A sine-square deformation approach to quantum critical points in one-dimensional systems<\/a>
    DOI:10.48550\/arXiv.2512.14149

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  6. Yoshiyuki Kakihara<\/em><\/strong>, Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini<\/em><\/strong>
    Compressed sensing quantum state tomography for qudits: A comparison of Gell-Mann and Heisenberg-Weyl observable bases<\/a>
    DOI:10.48550\/arXiv.2505.10462

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  7. Kazuma Nagao, Daisuke Yamamoto<\/em><\/strong>, Seiji Yunoki, Ippei Danshita
    Melting of a Bosonic Mott Insulator in Kagome Optical Lattices with Sign-Inverted Hopping<\/a>
    DOI:10.48550\/arXiv.2504.19407

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  8. Shunichiro Kinoshita, Keiju Murata, Daisuke Yamamoto<\/em><\/strong>, Ryosuke Yoshii
    Spin systems as quantum field theories in inflationary universe: A study with Unruh-DeWitt detectors<\/a>
    Physical Review Research 7<\/strong>, 043135 (2025).
    Published 5 November 2025
    DOI:10.1103\/s3qb-n94w

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  9. Shunichiro Kinoshita, Keiju Murata, Daisuke Yamamoto<\/em><\/strong>, Ryosuke Yoshii
    Spin systems as quantum simulators of quantum field theories in curved spacetime<\/a>
    Physical Review Research 7<\/strong>, 023197 (2025).
    Published 29 May 2025
    DOI: 10.1103\/PhysRevResearch.7.023197

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  10. Yuki Miyazaki<\/em><\/strong>, Giacomo Marmorini<\/em><\/strong>, Nobuo Furukawa, and Daisuke Yamamoto<\/em><\/strong>
    R\u00e9nyi entropy of the permutationally invariant part of the ground state across a quantum phase transition<\/a>
    Physical Review A 110<\/strong>, 052422 (2024)
    Published 18 November 2024
    DOI: 10.1103\/PhysRevA.110.052422

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  11. Katsuki Nihongi, Takanori Kida, Daisuke Yamamoto<\/em><\/strong>, Yasuo Narumi, Julien Zaccaro, Yusuke Kousaka, Katsuya Inoue, Yoshiya Uwatoko, Koichi Kindo, and Masayuki Hagiwara
    Field-Induced Quantum Phase Transitions in the Pressure-Tuned Triangular-Lattice Antiferromagnet CsCuCl3<\/sub><\/a>
    Journal of the Physical Society of Japan 93<\/strong>, 084704 (2024).
    Published 26 July 2024
    DOI: 10.7566\/JPSJ.93.084704

    JPS Hot Topics\u306b\u9078\u51fa
    <\/strong>\u89e3\u8aac\u8a18\u4e8b\uff1a”    Pressure-Tuned Classical\u2013Quantum Crossover in Magnetic Field-Induced Quantum Phase Transitions of a Triangular-Lattice Antiferromagnet<\/a>“

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  12. Daisuke Yamamoto<\/em><\/strong> and Katsuhiro Morita
    Engineering of a Low-Entropy Quantum Simulator for Strongly Correlated Electrons Using Cold Atoms with SU(N)-Symmetric Interactions<\/a>
    Physical Review Letters 132<\/strong>, 213401 (2024).
    Published 20 May 2024
    DOI: 10.1103\/PhysRevLett.132.213401

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  13. Ko Gondaira, Nobuo Furukawa, and Daisuke Yamamoto<\/em><\/strong>
    Dynamics of Interacting Bosons on the Sawtooth Lattice with a Flat Band<\/a>
    Journal of the Physical Society of Japan 93<\/strong>, 074004 (2024).
    Published 24 June 2024
    DOI: 10.7566\/JPSJ.93.074004

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  14. Motoaki Bamba, Koji Hashimoto, Keiju Murata, Daichi Takeda, and Daisuke Yamamoto<\/em><\/strong>
    Spacetime-localized response in quantum critical spin systems: Insights from holography<\/a>
    Physical Review D 109<\/strong>, 126003 (2024)
    Published 5 June, 2024
    DOI: 10.1103\/PhysRevD.109.126003

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  15. Giacomo Marmorini<\/em><\/strong>, Shigehiro Yasui, and Muneto Nitta
    Pulsar glitches from quantum vortex networks<\/a>
    Scientific Reports 14<\/strong>, 7857 (2024).
    Published: 03 April 2024
    DOI: 10.1038\/s41598-024-56383-w

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  16. Sebasti\u00e1n E. Ramos-Onsins, Giacomo Marmorini<\/em><\/strong>, Guillaume Achaz, and Luca Ferretti
    A General Framework for Neutrality Tests Based on the Site Frequency Spectrum<\/a>
    Genes 14<\/strong>, 1714 (2023).
    Published: 28 August 2023
    DOI: 10.3390\/genes14091714

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  17. Hayato Motegi, Giacomo Marmorini<\/em><\/strong>, Nobuo Furukawa, and Daisuke Yamamoto<\/em><\/strong>
    Thermal Ising transition in two-dimensional SU(3) Fermi lattice gases with population imbalance<\/a>
    Phys. Rev. Research 5<\/strong>, L022056 (2023).
    Published: 20 June 2023
    DOI: 10.1103\/PhysRevResearch.5.L022056

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  18. Kazuki Okada, Hidekazu Tanaka, Nobuyuki Kurita, Daisuke Yamamoto<\/em><\/strong>, Akira Matsuo, and Koichi Kindo
    Field-orientation dependence of quantum phase transitions in the S=1\/2 triangular-lattice antiferromagnet Ba3CoSb2O9<\/a>
    Physical Review B 106<\/strong>, 104415 (2022).
    Published: 15 September 2022
    DOI: 10.1103\/PhysRevB.106.104415

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  19. Daisuke Yamamoto<\/em><\/strong>, Kotaro Bannai, Nobuo Furukawa, and Carlos A. R. S\u00e1 de Melo
    Supersolid devil’s staircases of spin-orbit-coupled bosons in optical lattices<\/a>
    Physical Review Research 4<\/strong>, L032023 (2022).
    Published 12 August 2022
    DOI: 10.1103\/PhysRevResearch.4.L032023

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  20. X. Z. Liu, O. Prokhnenko, M. Bartkowiak, A. Gazizulina, D. Yamamoto<\/em><\/strong>, A. Matsuo, K. Kindo, K. Okada, N. Kurita, and H. Tanaka
    Ground state of the S=1\/2 triangular lattice Heisenberg-like antiferromagnet Ba3CoSb2O9 in an out-of-plane magnetic field<\/a>
    Physical Review B 105<\/strong>, 214433 (2022).
    Published 27 June 2022
    DOI: 10.1103\/PhysRevB.105.214433

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  21. Yuki Miyazaki<\/em><\/strong>, Giacomo Marmorini<\/em><\/strong>, Nobuo Furukawa, and Daisuke Yamamoto<\/em><\/strong>
    Linear Flavor-Wave Analysis of SU(4)-Symmetric Tetramer Model with Population Imbalance
    <\/a>Journal of the Physical Society of Japan 91<\/strong>, 073702 (2022).
    Published June 23, 2022
    DOI: 10.7566\/JPSJ.91.073702

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  22. Yoshihiro Machida, Ippei Danshita, Daisuke Yamamoto<\/em><\/strong>, and Kenichi Kasamatsu
    Quantum droplet of a two-component Bose gas in an optical lattice near the Mott insulator transition<\/a>
    Physical Review A 105<\/strong>, L031301 (2022).
    Published 2 March 2022
    DOI: 10.1103\/PhysRevA.105.L031301

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  23. Daisuke Yamamoto<\/em><\/strong>, Takahiro Sakurai, Ryosuke Okuto, Susumu Okubo, Hitoshi Ohta, Hidekazu Tanaka, and Yoshiya Uwatoko
    Continuous control of classical-quantum crossover by external high pressure in the coupled chain compound CsCuCl3<\/sub><\/a>
    Nature Communications 12<\/strong>, Article number: 4263 (2021).
    Published: 12 July 2021
    DOI: 10.1038\/s41467-021-24542-6

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  24. O. Prokhnenko, G. Marmorini, S. E. Nikitin, D. Yamamoto<\/em><\/strong>, A. Gazizulina, M. Bartkowiak, A. N. Ponomaryov, S. A. Zvyagin, H. Nojiri, I. F. D\u00edaz-Ortega, L. M. Anovitz, A. I. Kolesnikov, and A. Podlesnyakurukawa
    High-field spin-flop state in green dioptase<\/a>
    Physical Review B 103<\/strong>, 014427 (2021).
    Published 19 January 2021
    DOI: 10.1103\/PhysRevB.103.014427

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  25. Daisuke Yamamoto<\/em><\/strong>, Chihiro Suzuki, Giacomo Marmorini, Sho Okazaki, and Nobuo Furukawa
    Quantum and Thermal Phase Transitions of the Triangular SU(3) Heisenberg Model under Magnetic Fields<\/a>
    Physical Review Letters 125<\/strong>, 057204 (2020).
    Published 31 July 2020
    DOI: 10.1103\/PhysRevLett.125.057204

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  26. Daisuke Yamamoto<\/em><\/strong>, Takeshi Fukuhara, and Ippei Danshita
    Frustrated Quantum Magnetism with Bose Gases in Triangular Optical Lattices at Negative Absolute Temperatures<\/a>
    Communications Physics 3<\/strong>, Article number: 56 (2020).
    Published 20 March 2020
    DOI: 10.1038\/s42005-020-0323-5

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  27. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, Masahiro Tabata, Kazuki Sakakura, and Ippei Danshita
    Magnetism driven by the interplay of fluctuations and frustration in the easy axis triangular XXZ model with transverse fields<\/a>
    Physical Review B 100<\/strong>, 140410(R) (2019).
    Published 21 October 2019
    DOI: 10.1103\/PhysRevB.100.140410

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  28. X. Z. Liu, O. Prokhnenko, M. Bartkowiak, D. Yamamoto<\/em><\/strong>, N. Kurita, and H. Tanaka
    Microscopic Evidence of a Quantum Magnetization Process in S = 1\/2 Triangular Lattice Heisenberg-like Antiferromagnet Ba3<\/sub>CoSb2<\/sub>O9<\/sub><\/a>
    Physical Review B 100<\/strong>, 094436 (2019).
    Published 20 September 2019
    DOI: 10.1103\/PhysRevB.100.094436

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  29. Nobuyuki Kurita, Daisuke Yamamoto<\/em><\/strong>, Takuya Kanesaka, Nobuo Furukawa, Seiko Ohira-Kawamura, Kenji Nakajima, and Hidekazu Tanaka
    Localized magnetic excitations in the fully frustrated dimerized magnet Ba2<\/sub>CoSi2<\/sub>O6<\/sub>Cl2<\/sub><\/a>
    Physical Review Letters 123<\/strong>, 027206 (2019).
    Published 11 July 2019
    DOI: 10.1103\/PhysRevLett.123.027206

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    2018\u5e74\u4ee5\u524d<\/summary>
    \n
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    1. Shunji Tsuchiya, Daisuke Yamamoto<\/em><\/strong>, Ryosuke Yoshii, and Muneto Nitta
      Hidden Charge-Conjugation, Parity, Time-Reversal Symmetries and Higgs Modes in Superconductors <\/a>
      Physical Review B 98<\/strong>, 094503 (2018).
      Published 4 September 2018
      DOI: 10.1103\/PhysRevB.98.094503

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    2. Masahito Mochizuki, Masaya Kobayashi, Reoya Okabe, and Daisuke Yamamoto <\/em><\/strong>
      Spin model for nontrivial types of magnetic order in inverse-perovskite antiferromagnets<\/a>
      Physical Review B (Rapid Communications) 97<\/strong>, 060401(R) (2018).
      Published 5 February 2018
      DOI: 10.1103\/PhysRevB.97.060401

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    3. Daisuke Yamamoto<\/em><\/strong>, I. B. Spielman, and C. A. R. S\u00e1 de Melo
      Quantum Phases of Two-Component Bosons with Spin-Orbit Coupling in Optical Lattices <\/a>
      Physical Review A (Rapid Communications) 96<\/strong>, 061603(R) (2017).
      Published 26 December 2017
      DOI: 10.1103\/PhysRevA.96.061603

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    4. Daisuke Yamamoto<\/em><\/strong>, Hiroshi Ueda, Ippei Danshita, Giacomo Marmorini, Tsutomu Momoi, and Tokuro Shimokawa
      Exact diagonalization and cluster mean-field study of triangular-lattice XXZ antiferromagnets near saturation <\/a>
      Physical Review B 96<\/strong>, 014431 (2017).
      Published 25 July 2017
      DOI: 10.1103\/PhysRevB.96.014431

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    5. Shinpei Goto, Susumu Kurihara, and Daisuke Yamamoto <\/em><\/strong>
      Incommensurate spiral magnetic order on anisotropic triangular lattice: Dynamical mean field study in a spin-rotating frame <\/a>
      Physical Review B 94<\/strong>, 245145 (2016).
      Published 28 December 2016
      DOI: 10.1103\/PhysRevB.94.245145

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    6. Giacomo Marmorini, Daisuke Yamamoto<\/em><\/strong>, and Ippei Danshita
      Umbrella-coplanar transition in the triangular XXZ model with arbitrary spin <\/a>
      Physical Review B 93<\/strong>, 224402 (2016).
      Published 1 June 2016
      DOI: 10.1103\/PhysRevB.93.224402

      <\/li>\n
    7. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Ippei Danshita
      Magnetization process of spin-1\/2 Heisenberg antiferromagnets on a layered triangular lattice <\/a>
      Journal of the Physical Society of Japan 85<\/strong>, 024706 (2016).
      Published January 12, 2016
      DOI: 10.7566\/JPSJ.85.024706

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    8. Hiroki Yamamura and Daisuke Yamamoto <\/em><\/strong>
      Collective Excitation and Stability of Flowing Gapless Fermi Superfluids<\/a>
      Journal of the Physical Society of Japan 84<\/strong>, 044003 (2015).
      Published March 19, 2015
      DOI: 10.7566\/JPSJ.84.044003

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    9. Keisuke Masuda and Daisuke Yamamoto <\/em><\/strong>
      Variational cluster approach to s-wave pairing in heavy-fermion superconductors <\/a>
      Physical Review B 91<\/strong>, 104508 (2015).
      Published 12 March 2015
      DOI: 10.1103\/PhysRevB.91.104508

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    10. Ippei Danshita, Daisuke Yamamoto<\/em><\/strong>, and Yasuyuki Kato
      Cubic-quintic nonlinearity in superfluid Bose-Bose mixtures in optical lattices: Heavy solitary waves, barrier-induced criticality, and current-phase relations<\/a>
      Physical Review A 91<\/strong>, 013630 (2015).
      Published 30 January 2015
      DOI: 10.1103\/PhysRevA.91.013630

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    11. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Ippei Danshita
      Microscopic Model Calculations for the Magnetization Process of Layered Triangular-Lattice Quantum Antiferromagnets <\/a>
      Physical Review Letters 114<\/strong>, 027201 (2015).
      (Research Highlight of \u201fRIKEN RESEARCH\u201d)
      Published 16 January 2015
      DOI: 10.1103\/PhysRevLett.114.027201

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    12. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Ippei Danshita
      Quantum Phase Diagram of the Triangular-Lattice XXZ Model in a Magnetic Field <\/a>
      Physical Review Letters 112<\/strong>, 127203 (2014); ibid, 112<\/strong>, 259901 (2014).
      Published 26 March 2014
      DOI: 10.1103\/PhysRevLett.112.127203

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    13. Yasuyuki Kato, Daisuke Yamamoto<\/em><\/strong>, and Ippei Danshita
      Quantum tricriticality at the superfluid-insulator transition of binary Bose mixtures<\/a>
      Physical Review Letters 112<\/strong>, 055301 (2014).
      (Research Highlight of \u201fRIKEN RESEARCH\u201d)
      Published 3 February 2014
      DOI: 10.1103\/PhysRevLett.112.055301

      <\/li>\n
    14. Daisuke Yamamoto<\/em><\/strong>, Takeshi Ozaki, Carlos A. R. S\u00e1 de Melo, and Ippei Danshita
      First-Order Phase Transition and Anomalous Hysteresis of Binary Bose Mixtures in an Optical Lattice<\/a>
      Journal of Low Temperature Physics 175<\/strong>, 258 (2014).
      Published: 04 December 2013
      DOI: 10.1007\/s10909-013-0989-0

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    15. Daisuke Yamamoto<\/em><\/strong>, Takeshi Ozaki, Carlos A. R. S\u00e1 de Melo, and Ippei Danshita
      First-order phase transition and anomalous hysteresis of Bose gases in optical lattices<\/a>
      Physical Review A 88<\/strong>, 033624 (2013).
      Published 20 September 2013
      DOI: 10.1103\/PhysRevA.88.033624

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    16. Daisuke Yamamoto<\/em><\/strong> and Ippei Danshita
      Magnon Supersolid and Anomalous Hysteresis in Spin Dimers on a Triangular Lattice <\/a>
      Physical Review B 88<\/strong>, 014419 (2013).
      Published 19 July 2013
      DOI: 10.1103\/PhysRevB.88.014419

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    17. Daisuke Yamamoto<\/em><\/strong>, Chika Sato, Tetsuro Nikuni, Shunji Tsuchiya
      Flow-Induced Charge Modulations in Superfluid Atomic Fermions Loaded into an Optical Kagome Lattice <\/a>
      Physical Review Letters 110<\/strong>, 145304 (2013).
      Published 4 April 2013
      DOI: 10.1103\/PhysRevLett.110.145304

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    18. Keisuke Masuda and Daisuke Yamamoto <\/em><\/strong>
      Formation of Cooper pairs between conduction and localized electrons in heavy-fermion superconductors <\/a>
      Physical Review B 87<\/strong>, 014516 (2013).
      Published 29 January 2013
      DOI: 10.1103\/PhysRevB.87.014516

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    19. Daisuke Yamamoto<\/em><\/strong>, Akiko Masaki, and Ippei Danshita
      Quantum phases of hardcore bosons with long-range interactions on a square lattice<\/a>
      Physical Review B 86<\/strong>, 054516 (2012).
      Published 27 August 2012
      DOI: 10.1103\/PhysRevB.86.054516

      <\/li>\n
    20. Daisuke Yamamoto<\/em><\/strong>, Ippei Danshita, and Carlos A. R. S\u00e1 de Melo
      Dipolar bosons in triangular optical lattices: Quantum phase transitions and anomalous hysteresis <\/a>
      Physical Review A (Rapid Communications) 85<\/strong>, 021601(R) (2012).
      Published 3 February 2012
      DOI: 10.1103\/PhysRevA.85.021601

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    21. Ippei Danshita and Daisuke Yamamoto <\/em><\/strong>
      Critical velocity of flowing supersolids of dipolar Bose gases in optical lattices <\/a>
      Physical Review A 82<\/strong>, 013645 (2010).
      Published 30 July 2010
      DOI: 10.1103\/PhysRevA.82.013645

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    22. Jun Nakabayashi, Daisuke Yamamoto<\/em><\/strong>, and Susumu Kurihara
      Band-Selective Filter in a Zigzag Graphene Nanoribbon
      <\/a>Physical Review Letters 102<\/strong>, 066803 (2009).
      (Research Highlight of \u201fNPG Asia Materials\u201d)
      Published 10 February 2009
      DOI: 10.1103\/PhysRevLett.102.066803

      <\/li>\n
    23. Daisuke Yamamoto <\/em><\/strong>
      Correlated cluster mean-field theory for spin systems
      <\/a>Physical Review B 79<\/strong>, 144427 (2009).
      Published 24 April 2009
      DOI: 10.1103\/PhysRevB.79.144427

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    24. Yoshihiro Yunomae, Daisuke Yamamoto<\/em><\/strong>, Ippei Danshita, Nobuhiko Yokoshi, and Shunji Tsuchiya
      Instability of superfluid Fermi gases induced by a roton-like density mode in optical lattices <\/a>
      Physical Review A 80<\/strong>, 063627 (2009).
      Published 29 December 2009
      DOI: 10.1103\/PhysRevA.80.063627

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    25. Daisuke Yamamoto<\/em><\/strong>, Synge Todo, and Susumu Kurihara
      Green’s function theory for spin-1\/2 ferromagnets with an easy plane exchange anisotropy<\/a>
      Physical Review B 78<\/strong>, 024440 (2008).
      Published 30 July 2008
      DOI: 10.1103\/PhysRevB.78.024440

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    26. Daisuke Yamamoto<\/em><\/strong> and Susumu Kurihara
      Antiferromagnetism in two-dimensional t-J model: A pseudospin representation <\/a>
      Physical Review B 75<\/strong>, 134520 (2007).
      Published 30 April 2007
      DOI: 10.1103\/PhysRevB.75.134520
      <\/li>\n<\/ol>\n

      <\/p>\n<\/div><\/details><\/div>\n<\/div>\n\n\n\n

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      \n
      \u56fd\u969b\u4f1a\u8b70\u30d7\u30ed\u30b7\u30fc\u30c7\u30a3\u30f3\u30b0\u30b9\u7b49<\/summary>
      \n
        \n
      1. Y. Miyazaki, D. Yamamoto<\/em><\/strong>, G. Mormorini, and N. Furukawa
        Field-induced phase transitions of tetramer-singlet states in synthetic SU(4) magnets<\/a>
        AIP Advances 11<\/strong>, 025202 (2021).

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      2. K. Takagi, D. Yamamoto<\/em><\/strong>, H. Kitano, and N. Furukawa
        Phase retrapping effects on switching characteristic in intrinsic Josephson junctions<\/a>
        AIP Conference Proceedings 2319<\/strong>, 070004 (2021).

        <\/li>\n
      3. Keisuke Masuda and Daisuke Yamamoto<\/em><\/strong>
        Interorbital Cooper Pairing with s-Wave Symmetry in Heavy-Fermion Systems
        JPS Conf. Proc., The Physical Society of Japan, Vol. 3, 015024 (2014).

        <\/li>\n
      4. Keisuke Masuda and Daisuke Yamamoto<\/em><\/strong>
        Cooper pairing between conduction and localized electrons in heavy-fermion systems
        Journal of the Korean Physical Society, Korean Physical Society, Vol. 63, 459 (2013).

        <\/li>\n
      5. Daisuke Yamamoto<\/em><\/strong>, Ippei Danshita, and Carlos A. R. S\u00e1 de Melo
        Anomalous hysteretic behavior in a system of dipolar Bose gases
        Journal of Physics: Conference Series, IOP Publishing Ltd, Vol. 400, 012083 (2012).

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      6. Keisuke Masuda and Daisuke Yamamoto<\/em><\/strong>
        Cooper Pairing of Fermions with Unequal Masses in Heavy-Fermion Systems
        Journal of the Physical Society of Japan, The Physical Society of Japan, Vol. 81, SB010 (2012).

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      7. Daisuke Yamamoto<\/em><\/strong> and Ippei Danshita
        Stability of superflow in supersolid phases of lattice bosons with dipole-dipole interaction
        Journal of Physics: Conference Series, IOP Publishing Ltd, Vol. 273, 012020 (2011).

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      8. Takao Nomura, Daisuke Yamamoto<\/strong><\/em>, Susumu Kurihara
        Electric Field Effects in Zigzag Edged Graphene Nanoribbons
        Journal of Physics: Conference Series, IOP Publishing Ltd, Vol. 200, 062015 (2010).

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      9. Daisuke Yamamoto <\/em><\/strong>
        Cluster Mean-Field Approach Including Correlation Effects between Clusters
        Journal of Physics: Conference Series, IOP Publishing Ltd, Vol. 200, 022072 (2010).

        <\/li>\n
      10. Yoshihiro Yunomae, Ippei Danshita, Daisuke Yamamoto<\/em><\/strong>, Nobuhiko Yokoshi, and Shunji Tsuchiya
        Stability of superfluid Fermi gases in optical lattices
        Foundations of Quantum Mechanics in the Light of New Technology, Advanced Research Laboratory Hitachi Ltd, 41 (2009).

        <\/li>\n
      11. Daisuke Yamamoto<\/em><\/strong>, Synge Todo, and Susumu Kurihara
        Application of the Green’s Function Method to an Easy-Plane Heisenberg Model
        Journal of Physics: Conference Series, IOP Publishing Ltd, Vol. 150, 042234 (2009).

        <\/li>\n
      12. Yoshihiro Yunomae, Ippei Danshita, Daisuke Yamamoto<\/em><\/strong>, Nobuhiko Yokoshi, and Shunji Tsuchiya
        Current-Induced Instability of Superfluid Fermi Gases in Optical Lattices
        Journal of Physics: Conference Series, IOP Publishing Ltd, Vol. 150, 032128 (2009).

        <\/li>\n
      13. \u5c71\u672c\u5927\u8f14<\/strong>
        \u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u306b\u304a\u3051\u308b\u30b0\u30ea\u30fc\u30f3\u95a2\u6570\u6cd5\u3000\uff0dt-J\u30e2\u30c7\u30eb\u306e\u64ec\u30b9\u30d4\u30f3\u8868\u793a\uff0d \u7269\u6027\u7814\u7a76
        \u7269\u6027\u7814\u7a76\u520a\u884c\u4f1a\u300191-3\u53f7\u3001pp.299-331 (2008).

        <\/li>\n
      14. Yuki Terakawa, Nobuhiko Yokoshi, Kenji Kamide, Daisuke Yamamoto<\/em><\/strong>, and Susumu Kurihara
        Effect of quantum fluctuations on Bose-Einstein condensation of bilayer atomic gases in rapid rotation
        Laser Physics, MAIK Nauka, Vol. 18, No. 5, pp.641-647 (2008).

        <\/li>\n
      15. Daisuke Yamamoto<\/em><\/strong> and Susumu Kurihara
        Pseudospin representation of the two-dimentional t-J model
        Physica B: Condensed Matter, Elsevier B.V., Vol. 403, 1112 (2008).<\/li>\n<\/ol>\n

        <\/p>\n<\/div><\/details><\/div>\n<\/div>\n\n\n\n

        \u6700\u8fd1\u306e\u5b66\u4f1a\u767a\u8868\u7b49<\/h2>\n\n\n\n
          \n
        1. (\u30dd\u30b9\u30bf\u30fc)\u00a0\u5c71\u6839\u8f1d\u4e5f\u3001\u5c71\u672c\u5927\u8f14<\/strong>
          \u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53CsFeCl3<\/sub>\u306b\u304a\u3051\u308b\u5f37\u78c1\u5834\u78c1\u6027\u306e\u7406\u8ad6\u89e3\u6790
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a 2026\u5e74\u6625\u5b63\u5927\u4f1a
          \u9818\u57df3\u300125pPSC-18\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012026\u5e743\u670825\u65e5

          <\/li>\n\n\n\n
        2. (\u30dd\u30b9\u30bf\u30fc)\u00a0\u5c71\u672c\u5927\u8f14<\/strong>
          \u7269\u8cea\u30fb\u60c5\u5831\u30fb\u6642\u7a7a\u3092\u7d71\u5408\u3059\u308b\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u57fa\u76e4\u306e\u5275\u51fa
          JST\u3055\u304d\u304c\u3051\u91cf\u5b50\uff13\u9818\u57df\u5408\u540c\u30bb\u30df\u30ca\u30fc
          AP\u5e02\u30f6\u8c37\u3001\u6771\u4eac\u30012026\u5e742\u670820\u65e5

          <\/li>\n\n\n\n
        3. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u98fd\u548c\u3092\u8d85\u3048\u305f\u305d\u306e\u5148\u306b – \u4e09\u4f53\u76f8\u4e92\u4f5c\u7528\u304c\u62d3\u304f\u65b0\u3057\u3044\u78c1\u6027
          \u7b2c20\u56de\u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u4f1a
          \u6d77\u5ce1\u30d3\u30e5\u30fc\u3057\u3082\u306e\u305b\u304d\u3001\u5c71\u53e3\u30012025\u5e7412\u670813\u65e5

          <\/li>\n\n\n\n
        4. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u7269\u8cea\u30fb\u60c5\u5831\u30fb\u6642\u7a7a\u3092\u7d71\u5408\u3059\u308b\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u57fa\u76e4\u306e\u5275\u51fa
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u7269\u8cea\u3068\u60c5\u5831\u306e\u91cf\u5b50\u5354\u594f\u300d\u7b2c6\u56de\u9818\u57df\u4f1a\u8b70
          \u5357\u7d00\u767d\u6d5c\u30de\u30ea\u30aa\u30c3\u30c8\u30db\u30c6\u30eb\u3001\u548c\u6b4c\u5c71\u30012025\u5e7411\u67085\u65e5

          <\/li>\n\n\n\n
        5. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>, \u4e8c\u672c\u6728\u514b\u65ed, \u6728\u7530\u5b5d\u5247, \u9cf4\u6d77\u5eb7\u96c4, \u6c5f\u85e4\u512a\u6a39, \u677e\u672c\u6b63\u8302, \u6817\u7530\u4f38\u4e4b, \u7530\u4e2d\u79c0\u6570, \u91d1\u9053\u6d69\u4e00, \u4e0a\u5e8a\u7f8e\u4e5f, \u8429\u539f\u653f\u5e78
          \u9ad8\u5727\u30fb\u5f37\u78c1\u5834\u4e0b\u306eCsFeCl3<\/sub>\u306b\u304a\u3051\u308b\u4e09\u4f53\u30b9\u30d4\u30f3\u76f8\u4e92\u4f5c\u7528\u306e\u5275\u767a\u3068\u30e1\u30bf\u78c1\u6027\u8ee2\u79fb\u6a5f\u69cb\u306e\u89e3\u660e
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2025\u5e74\uff08\u7b2c80\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df3\u300116pSK312-5\u3001\u5e83\u5cf6\u5927\u5b66\u30012025\u5e749\u670816\u65e5

          <\/li>\n\n\n\n
        6. (\u53e3\u982d)
          M2 \u4eca\u5ddd\u5927\u5b99<\/strong>\u3000SU(N)\u6a21\u578b\u306b\u304a\u3051\u308b\u6642\u7a7a\u3068\u7a7a\u9593\u306b\u5c40\u5728\u3057\u305f\u5c40\u6240\u5fdc\u7b54\u306e\u6570\u5024\u89e3\u6790\u306b\u5411\u3051\u3066
          M2 \u67ff\u539f\u7965\u5e78<\/strong>\u3000Qudit \u306b\u5bfe\u3059\u308b\u5727\u7e2e\u30bb\u30f3\u30b7\u30f3\u30b0\u91cf\u5b50\u72b6\u614b\u30c8\u30e2\u30b0\u30e9\u30d5\u30a3\uff1a\u57fa\u5e95\u306e\u30b3\u30d2\u30fc\u30ec\u30f3\u30b9\u3068\u884c\u5217\u518d\u69cb\u6210\u52b9\u7387
          M2 \u677e\u91ce\u4f51\u7d00<\/strong>\u3000\u30b9\u30d4\u30f3\u7cfb\u306b\u3088\u308b\u30d6\u30e9\u30c3\u30af\u30db\u30fc\u30eb\u306e\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3
          M1 \u5c71\u6839\u8f1d\u4e5f<\/strong>\u3000\u91cf\u5b50\u78c1\u6027\u4f53 CsFeCl3 \u306e\u5f37\u78c1\u5834\u30e1\u30bf\u78c1\u6027\u306e\u89e3\u660e\u306b\u5411\u3051\u3066
          M1 \u7acb\u82b1\u5343\u62d3<\/strong>\u3000\u5149\u683c\u5b50\u4e2d\u306e\u4e8c\u6210\u5206 Bose \u7c92\u5b50\u306b\u304a\u3051\u308b Stark \u591a\u4f53\u5c40\u5728
          B4 \u4f50\u85e4\u614e\u592a\u90ce\u3000<\/strong>\u975e\u30d6\u30e9\u30d9\u30fc\u683c\u5b50\u4e0a\u306b\u304a\u3051\u308b Bose-Hubbard \u6a21\u578b\u306e\u57fa\u5e95\u72b6\u614b
          B4<\/strong> \u5317\u5cf6\u6d77<\/strong>\u3000\u30b9\u30d4\u30f3\u7cfb\u3092\u7528\u3044\u305f\u66f2\u304c\u3063\u305f\u6642\u7a7a\u306e\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3
          B4 \u95a2\u6839\u548c\u8f1d<\/strong>\u3000\u30ab\u30b4\u30e1\u53cd\u5f37\u78c1\u6027\u4f53\u306b\u304a\u3051\u308b\u78c1\u5316\u30d7\u30e9\u30c8\u30fc\u69cb\u9020\u306e\u30dc\u30bd\u30f3\u7cfb\u985e\u4f3c\u76f8\u306e\u63a2\u7a76\u306b\u5411\u3051\u3066
          B4 \u5fb3\u690d\u529f\u592a\u90ce<\/strong>\u3000\u7f6e\u63db\u5bfe\u79f0\u5316\u5bc6\u5ea6\u884c\u5217\u3067\u306e\u6e2c\u5b9a\u8a98\u8d77\u76f8\u8ee2\u79fb\u306e\u89b3\u6e2c\u53ef\u80fd\u6027
          2025\u91cf\u5b50\u7269\u6027\u82e5\u624b\u4ea4\u6d41\u7814\u7a76\u4f1a
          \u30db\u30c6\u30eb\u30ea\u30b9\u30c6\u30eb\u6d5c\u540d\u6e56\u3001\u6d5c\u677e\u5e02\u3001\u9759\u5ca1\u30012025\u5e748\u670827\u65e5-29\u65e5

          <\/li>\n\n\n\n
        7. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Daichi Imagawa<\/strong>, Keiju Murata, and Daisuke Yamamoto<\/strong>
          Numerical Analysis of AdS\/CFT Inspired Phenomena in a Quantum Critical Spin System
          30th International Conference on Low Temperature Physics (LT30)
          Bilbao Exhibition Centre, Bilbao, Spain, August 9, 2025

          <\/li>\n\n\n\n
        8. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Yoshiyuki Kakihara<\/strong>, Daisuke Yamamoto<\/strong>, and Giacomo Marmorini<\/strong>
          Efficiency Analysis of Compressed Sensing Quantum State Tomography for Qudit Systems
          30th International Conference on Low Temperature Physics (LT30)
          Bilbao Exhibition Centre, Bilbao, Spain, August 11, 2025

          <\/li>\n\n\n\n
        9. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Yuki Matsuno<\/strong>, Keiju Murata, and Daisuke Yamamoto<\/strong>
          Simulating Hawking Radiation from Evolving Black Holes with Quantum Many-Body Systems
          30th International Conference on Low Temperature Physics (LT30)
          Bilbao Exhibition Centre, Bilbao, Spain, August 9, 2025

          <\/li>\n\n\n\n
        10. (\u56fd\u969b, \u53e3\u982d) Giacomo Marmorini<\/strong>, Takeshi Fukuhara, and Daisuke Yamamoto<\/strong>
          Spiral quantum state tomography of quantum many-body states and entanglement measurement
          30th International Conference on Low Temperature Physics (LT30)
          Bilbao Exhibition Centre, Bilbao, Spain, August 12, 2025

          <\/li>\n\n\n\n
        11. (\u56fd\u969b, \u53e3\u982d) Daisuke Yamamoto<\/strong> and Katsuhiro Morita
          Entropy engineering in SU(N) cold atoms for simulating strongly correlated electron systems
          30th International Conference on Low Temperature Physics (LT30)
          Bilbao Exhibition Centre, Bilbao, Spain, August 13, 2025

          <\/li>\n\n\n\n
        12. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u72b6\u614b\u540c\u5b9a\u304a\u3088\u3073\u91cf\u5b50\u3082\u3064\u308c\u306e\u5b9a\u91cf\u5316\u6cd5\u306e\u958b\u767a
          \u3055\u304d\u304c\u3051\u300c\u91cf\u5b50\u60c5\u5831\u51e6\u7406\u300d\u9818\u57df\u516c\u958b\u30b7\u30f3\u30dd\u30b8\u30a6\u30e0
          \u65e5\u672c\u79d1\u5b66\u672a\u6765\u9928\u3001\u6771\u4eac\u30012025\u5e742\u67086\u65e5

          <\/li>\n\n\n\n
        13. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u591a\u4f53\u7cfb\u306b\u304a\u3051\u308b\u30a8\u30f3\u30bf\u30f3\u30b0\u30eb\u30e1\u30f3\u30c8\u691c\u51fa\u3068\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3
          \u3055\u304d\u304c\u3051\u91cf\u5b50\uff13\u9818\u57df\u5408\u540c\u30bb\u30df\u30ca\u30fc
          \u65e5\u672c\u79d1\u5b66\u672a\u6765\u9928\u3001\u6771\u4eac\u30012025\u5e742\u67085\u65e5

          <\/li>\n\n\n\n
        14. (\u62db\u5f85\u8b1b\u6f14, \u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u5f37\u78c1\u5834\u30fb\u9ad8\u5727\u74b0\u5883\u4e0b\u306b\u304a\u3051\u308b\u91cf\u5b50\u52b9\u679c\u304c\u751f\u307f\u51fa\u3059\u65b0\u5947\u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u78c1\u6027\u306e\u7406\u8ad6\u7684\u958b\u62d3\u3068\u5b9f\u9a13\u30c7\u30fc\u30bf\u89e3\u6790\uff08\u5f37\u78c1\u5834\u30d5\u30a9\u30fc\u30e9\u30e0\u30d5\u30ed\u30f3\u30c6\u30a3\u30a2\u5968\u52b1\u8cde\u53d7\u8cde\u8b1b\u6f14\uff09
          \u7b2c19\u56de\u5f37\u78c1\u5834\u30d5\u30a9\u30fc\u30e9\u30e0\u7dcf\u4f1a
          \u6771\u4eac\u5927\u5b66\u7269\u6027\u7814\u7a76\u6240\u3001\u5343\u8449\u30012024\u5e7412\u670819\u65e5

          <\/li>\n\n\n\n
        15. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u91cf\u2f26\u30b9\u30d4\u30f3\u7cfb\u3092\u2f64\u3044\u305f\u66f2\u304c\u3063\u305f\u6642\u7a7a\u306e\u91cf\u2f26\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3
          \u7b2c20\u56de\u91cf\u5b50\u30b9\u30d4\u30f3\u7814\u7a76\u4f1a
          \u3042\u304d\u305f\u82b8\u8853\u6751 \u6e29\u6cc9\u3086\u307d\u307d\u3001\u79cb\u7530\u30012024\u5e7412\u670813\u65e5

          <\/li>\n\n\n\n
        16. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u7269\u8cea\u30fb\u60c5\u5831\u30fb\u6642\u7a7a\u3092\u7d71\u5408\u3059\u308b\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u57fa\u76e4\u306e\u5275\u51fa
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u7269\u8cea\u3068\u60c5\u5831\u306e\u91cf\u5b50\u5354\u594f\u300d\u7b2c5\u56de\u9818\u57df\u4f1a\u8b70
          AP\u5927\u962a\u6dc0\u5c4b\u6a4b\u3001\u5927\u962a\u30012024\u5e7410\u670829\u65e5

          <\/li>\n\n\n\n
        17. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Honami Fukushima<\/strong>, Kotaro Tamaoka, Hiroshi Ueda, and Daisuke Yamamoto<\/strong>
          Pseudo entanglement entropy as a probe of quantum phase transitions: Matrix product state approach
          Quantum Extreme Universe: Matter, Information, and Gravity
          Okinawa Institute of Science and Technology, Okinawa, Japan, Oct 21, 2024

          <\/li>\n\n\n\n
        18. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Giacomo Marmorini<\/strong>, Takeshi Fukuhara, and Daisuke Yamamoto<\/strong>
          Measurement of entanglement in a many-body quantum simulator via spiral quantum state tomography
          Quantum Extreme Universe: Matter, Information, and Gravity
          Okinawa Institute of Science and Technology, Okinawa, Japan, Oct 21, 2024

          <\/li>\n\n\n\n
        19. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          <\/strong>Measuring entanglement entropy in quantum many-body systems via spiral quantum state
          tomography
          \u5b66\u8853\u5909\u9769(\uff21)\u300c\u6975\u9650\u5b87\u5b99\u300d\u7b2c4\u56de\u9818\u57df\u4f1a\u8b70
          \u5927\u962a\u5927\u5b66\u3001\u5927\u962a\u30012024\u5e749\u670827\u65e5

          <\/li>\n\n\n\n
        20. (\u53e3\u982d) \u4eca\u5ddd\u5927\u5b99, \u5c71\u672c\u5927\u8f14<\/strong>
          1\u6b21\u5143\u91cf\u5b50\u30b9\u30d4\u30f3\u6a21\u578b\u306b\u304a\u3051\u308b\u6642\u9593\u3068\u7a7a\u9593\u306b\u5c40\u5728\u3057\u305f\u5468\u671f\u5fdc\u7b54\u306e\u6570\u5024\u89e3\u6790\uff1aAdS\/CFT\u5bfe\u5fdc\u306e\u898b\u5730\u304b\u3089
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2024\u5e74\uff08\u7b2c79\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1\u300116aS202-1\u3001\u5317\u6d77\u9053\u5927\u5b66\u30012024\u5e749\u670816\u65e5

          <\/li>\n\n\n\n
        21. (\u53e3\u982d) \u798f\u5cf6\u5e06\u5948\u7f8e<\/strong>, <\/strong>\u7389\u5ca1\u5e78\u592a\u90ce, \u4e0a\u7530\u5b8f, \u5c71\u672c\u5927\u8f14<\/strong>
          \u91cf\u5b50\u76f8\u8ee2\u79fb\u73fe\u8c61\u306b\u304a\u3051\u308b\u64ec\u30a8\u30f3\u30bf\u30f3\u30b0\u30eb\u30e1\u30f3\u30c8\u30fb\u30a8\u30f3\u30c8\u30ed\u30d4\u30fc\u306e\u632f\u308b\u821e\u3044\uff1a\u884c\u5217\u7a4d\u72b6\u614b\u3092\u7528\u3044\u305f\u89e3\u6790
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2024\u5e74\uff08\u7b2c79\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1\u300116aS202-2\u3001\u5317\u6d77\u9053\u5927\u5b66\u30012024\u5e749\u670816\u65e5

          <\/li>\n\n\n\n
        22. (\u53e3\u982d) \u67ff\u539f\u7965\u5e78, \u5c71\u672c\u5927\u8f14, Giacomo Marmorini<\/strong>
          Qudit\u306b\u5bfe\u3059\u308b\u5727\u7e2e\u30bb\u30f3\u30b7\u30f3\u30b0\u91cf\u5b50\u72b6\u614b\u30c8\u30e2\u30b0\u30e9\u30d5\u30a3\uff1a\u4e00\u822c\u5316Gell-Mann\u57fa\u5e95\u3068Heisenberg-Weyl\u57fa\u5e95\u306e\u6bd4\u8f03
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2024\u5e74\uff08\u7b2c79\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1\u300116aS202-3\u3001\u5317\u6d77\u9053\u5927\u5b66\u30012024\u5e749\u670816\u65e5

          <\/li>\n\n\n\n
        23. (\u53e3\u982d) \u5bae\ufa11\u512a\u5e0c, Giacomo Marmorini<\/strong>, \u53e4\u5ddd\u4fe1\u592b, \u5c71\u672c\u5927\u8f14<\/strong>
          \u5bc6\u5ea6\u884c\u5217\u306e\u7f6e\u63db\u4e0d\u5909\u90e8\u5206\u306b\u3088\u308b\u91cf\u5b50\u76f8\u306e\u7279\u5fb4\u4ed8\u3051
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2024\u5e74\uff08\u7b2c79\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1\u300116aS202-4\u3001\u5317\u6d77\u9053\u5927\u5b66\u30012024\u5e749\u670816\u65e5

          <\/li>\n\n\n\n
        24. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u5f37\u76f8\u95a2\u7269\u6027\u306e\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u3068\u30b9\u30d1\u30a4\u30e9\u30eb\u57fa\u5e95\u91cf\u5b50\u30c8\u30e2\u30b0\u30e9\u30d5\u30a3
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2024\u5e74\uff08\u7b2c79\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df3 \u5171\u50ac\u30b7\u30f3\u30dd\u30b8\u30a6\u30e0\u8b1b\u6f14\u300117pS101-7\u3001\u5317\u6d77\u9053\u5927\u5b66\u30012024\u5e749\u670817\u65e5

          <\/li>\n\n\n\n
        25. (\u53e3\u982d)
          \u798f\u5cf6\u5e06\u5948\u7f8e<\/strong>\u3000\u91cf\u2f26\u591a\u4f53\u7cfb\u306b\u304a\u3051\u308b\u64ec\u30a8\u30f3\u30bf\u30f3\u30b0\u30eb\u30e1\u30f3\u30c8\u30fb\u30a8\u30f3\u30c8\u30ed\u30d4\u30fc\u306e\u6570\u5024\u89e3\u6790
          \u7a32\u8449\u9999\u5948<\/strong>\u3000\u5468\u671f\u5909\u8abf\u3055\u308c\u305f\u2f00\u6b21\u5143Bose-Hubbard\u6a21\u578b\u306e\u65b0\u305f\u306a\u91cf\u2f26\u76f8\u8ee2\u79fb\u306e\u958b\u62d3
          \u4eca\u5ddd\u5927\u5b99<\/strong>\u3000\u91cf\u2f26\u30b9\u30d4\u30f3\u6a21\u578b\u306b\u304a\u3051\u308b\u5c40\u6240\u7684\u306a\u5468\u671f\u5fdc\u7b54\u306e\u91cf\u2f26\u30a2\u30cb\u30fc\u30ea\u30f3\u30b0\u30de\u30b7\u30f3\u5b9f\u88c5\u306b\u5411\u3051\u3066
          \u67ff\u539f\u7965\u5e78<\/strong>\u3000\u2fae\u30d1\u30a6\u30ea\u57fa\u5e95\u306b\u304a\u3051\u308bqudit\u306b\u5bfe\u3059\u308b\u5727\u7e2e\u30bb\u30f3\u30b7\u30f3\u30b0\u91cf\u2f26\u72b6\u614b\u30c8\u30e2\u30b0\u30e9\u30d5\u30a3
          \u2f2d\u6839\u8f1d\u4e5f\u3000<\/strong>\u91cf\u2f26\u78c1\u6027\u4f53CsFeCl3<\/sub>\u306e\u5f37\u78c1\u5834\u30e1\u30bf\u78c1\u6027\u8ee2\u79fb\u306b\u304a\u3051\u308b\u30a8\u30cd\u30eb\u30ae\u30fc\u6e96\u4f4d\u554f\u984c
          \u9234\u2f4a\u6c99\u5f25\u2fb9<\/strong>\u3000\u91cf\u2f26\u78c1\u6027\u4f53CsFeCl3<\/sub>\u306e\u5f37\u78c1\u5834\u30e1\u30bf\u78c1\u6027\u8ee2\u79fb\u306b\u304a\u3051\u308b\u78c1\u6c17\u79e9\u5e8f\u306e\u89e3\u660e\u306b\u5411\u3051\u3066
          \u2ec4\u2f2d\u5609\u2fb3<\/strong>\u3000\u5b87\u5b99\u7269\u7406\u5b66\u306e\u91cf\u2f26\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u306b\u5411\u3051\u3066
          \u5c45\u9644\u84ee<\/strong>\u3000\u6df7\u5408\u72b6\u614b\u306b\u304a\u3051\u308b\u6e2c\u5b9a\u8a98\u8d77\u76f8\u8ee2\u79fb
          \u5bae\ufa11\u512a\u5e0c<\/strong>\u3000R\u00e9nyi entropy for the permutationally invariant part of density matrix across a quantum phase transition
          2024\u91cf\u5b50\u7269\u6027\u82e5\u624b\u4ea4\u6d41\u7814\u7a76\u4f1a
          \u30db\u30c6\u30eb\u30fb\u30b5\u30f3\u30df\u5036\u697d\u90e8\u3001\u71b1\u6d77\u5e02\u3001\u9759\u5ca1\u30012024\u5e748\u670827\u65e5-29\u65e5

          <\/li>\n\n\n\n
        26. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Honami Fukushima<\/strong>, Kotaro Tamaoka, Hiroshi Ueda, and Daisuke Yamamoto<\/strong>
          Pseudo Entanglement Entropy Across a Quantum Phase Transition
          International Conference on Magnetism 2024
          Bologna congress center, Bologna, Italy, July 1, 2024

          <\/li>\n\n\n\n
        27. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Giacomo Marmorini <\/strong>and Daisuke Yamamoto<\/strong>
          Quantum \u03a8 phase in hexagonal antiferromagnets at high magnetic fields
          International Conference on Magnetism 2024
          Bologna congress center, Bologna, Italy, July 2, 2024

          <\/li>\n\n\n\n
        28. (\u56fd\u969b\u3001\u53e3\u982d) Daisuke Yamamoto<\/strong>
          Synthetic Magnets with Ultracold Atoms: Exploration of Diverse Phases under Time-Periodic Driving
          International Conference on Magnetism 2024
          Bologna congress center, Bologna, Italy, July 2, 2024

          <\/li>\n\n\n\n
        29. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u72b6\u614b\u540c\u5b9a\u304a\u3088\u3073\u91cf\u5b50\u3082\u3064\u308c\u306e\u5b9a\u91cf\u5316\u6cd5\u306e\u958b\u767a
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u9769\u65b0\u7684\u306a\u91cf\u5b50\u60c5\u5831\u51e6\u7406\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c10\u56de\u9818\u57df\u4f1a\u8b70
          \u6307\u5bbf\u3053\u3053\u308d\u306e\u6e6f\u3001\u9e7f\u5150\u5cf6\u30012024\u5e745\u670816\u65e5

          <\/li>\n\n\n\n
        30. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Yoshiyuki<\/strong> Kakihara<\/strong>, Daisuke Yamamoto<\/strong>, and Giacomo Marmorini<\/strong>
          Compressed Sensing Quantum State Tomography for Qudits: Gell-Mann vs. Heisenberg-Weyl Basis
          Quantum Simulation of Novel Phenomena with Ultracold Atoms and Molecules
          YITP, Kyoto university, Kyoto, Japan, April 23, 2024

          <\/li>\n\n\n\n
        31. (\u56fd\u969b, \u53e3\u982d) Daisuke Yamamoto<\/strong>
          Exploration of Diverse Phases in Bose-Hubbard Systems under Dual Time-Periodic Driving
          Quantum Simulation of Novel Phenomena with Ultracold Atoms and Molecules
          YITP, Kyoto university, Kyoto, Japan, April 23, 2024

          <\/li>\n\n\n\n
        32. (\u62db\u5f85\u8b1b\u6f14, \u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u591a\u4f53\u7cfb\u3067\u306e\u91cf\u5b50\u72b6\u614b\u30c8\u30e2\u30b0\u30e9\u30d5\u30a3\u30fc\u306e\u52b9\u7387\u5316\u3068\u76f8\u8ee2\u79fb\u73fe\u8c61\u3078\u306e\u9069\u7528
          OIST mini meeting\uff1a\u7570\u5206\u91ce\u878d\u5408\u306b\u3088\u308b\u65b0\u305f\u306a\u79d1\u5b66\u306e\u5275\u9020
          OIST center building B503\u3001OIST\u3001\u6c96\u7e04\u30012024\u5e742\u670820\u65e5

          <\/li>\n\n\n\n
        33. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Daisuke Yamamoto<\/strong>
          Quantum Phases of Frustrated Bose Gases in an Optical Lattice under Dual Periodic Driving
          International Conference on Highly Frustrated Magnetism
          D2P63, IIT Madras, Chennai, India, January 11, 2024

          <\/li>\n\n\n\n
        34. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Giacomo<\/strong> Marmorini<\/strong>
          Does the PDO anomaly in CsCuCl3<\/sub> signal a quantum phase transition?
          International Conference on Highly Frustrated Magnetism
          D2P8, IIT Madras, Chennai, India, January 11, 2024

          <\/li>\n\n\n\n
        35. (\u53e3\u982d) Daisuke Yamamoto<\/strong>
          Holographic teleportation in artificial quantum spin systems
          “Extreme Universe” circular meeting, Online, December 19, 2023

          <\/li>\n\n\n\n
        36. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u72b6\u614b\u540c\u5b9a\u304a\u3088\u3073\u91cf\u5b50\u3082\u3064\u308c\u306e\u5b9a\u91cf\u5316\u6cd5\u306e\u958b\u767a
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u9769\u65b0\u7684\u306a\u91cf\u5b50\u60c5\u5831\u51e6\u7406\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c9\u56de\u9818\u57df\u4f1a\u8b70
          AP\u5e02\u30f6\u8c37\u3001\u6771\u4eac\u30012023\u5e7411\u670829\u65e5

          <\/li>\n\n\n\n
        37. (\u56fd\u969b, \u53e3\u982d) Giacomo<\/strong> Marmorini<\/strong>
          Possible measurement of entanglement in a many-body quantum simulator via spiral quantum state tomography
          YIPQS long-term workshop “Quantum Information, Quantum Matter and Quantum Gravity”
          Yukawa Institute for Theoretical Physics, Kyoto University, September 29, 2023

          <\/li>\n\n\n\n
        38. (\u56fd\u969b, \u30dd\u30b9\u30bf\u30fc) Yuki Miyazaki<\/strong>
          Evaluation of Quantum Entanglement via Permutationally Invariant Quantum State Tomography
          YIPQS long-term workshop “Quantum Information, Quantum Matter and Quantum Gravity”
          Yukawa Institute for Theoretical Physics, Kyoto University, September 26, 2023

          <\/li>\n\n\n\n
        39. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          2\u91cd\u5468\u671f\u99c6\u52d5\u5149\u683c\u5b50\u3092\u7528\u3044\u305fFloquet\u30a8\u30f3\u30b8\u30cb\u30a2\u30ea\u30f3\u30b0\u306b\u3088\u308bBose\u7c92\u5b50\u7cfb\u306e\u91cf\u5b50\u76f8\u306e\u958b\u62d3
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2023\u5e74\uff08\u7b2c78\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1\u300116aC200-11\u3001\u6771\u5317\u5927\u5b66\u30012023\u5e749\u670816\u65e5

          <\/li>\n\n\n\n
        40. (\u53e3\u982d) 2023\u91cf\u5b50\u7269\u6027\u82e5\u624b\u4ea4\u6d41\u7814\u7a76\u4f1a
          \u798f\u5cf6\u5e06\u5948\u7f8e<\/strong>\u3000\u91cd\u529b\u53cc\u5bfe\u306b\u304a\u3051\u308b\u30a8\u30f3\u30bf\u30f3\u30b0\u30eb\u30e1\u30f3\u30c8\u30a8\u30f3\u30c8\u30ed\u30d4\u30fc\u306e\u4e00\u822c\u5316\u3068\u30c6\u30f3\u30bd\u30eb\u30cd\u30c3\u30c8\u30ef\u30fc\u30af\u306b\u3088\u308b\u89e3\u6790
          \u7a32\u8449\u9999\u5948<\/strong>\u3000\u4e8c\u91cd\u5909\u8abf\u3055\u308c\u305f\u4e00\u6b21\u5143Bose-Hubbard\u6a21\u578b\u306e\u65b0\u305f\u306a\u91cf\u5b50\u76f8
          \u4eca\u5ddd\u5927\u5b99<\/strong>\u3000AdS\/CFT\u5bfe\u5fdc\u3068\u91cf\u5b50\u591a\u4f53\u7cfb\u306e\u30c0\u30a4\u30ca\u30df\u30af\u30b9
          \u6c5f\u85e4\u512a\u6a39<\/strong>\u3000\u30ab\u30a4\u30e9\u30ea\u30c6\u30a3\u611f\u53d7\u7387\u306b\u3088\u308b\u91cf\u5b50\u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53\u306e\u5f37\u78c1\u5834\u76f8\u306e\u6570\u5024\u5bfe\u89d2\u5316\u89e3\u6790
          \u67ff\u539f\u7965\u5e78<\/strong>\u3000Qutrit\u7cfb\u306b\u304a\u3051\u308b\u5727\u7e2e\u30bb\u30f3\u30b7\u30f3\u30b0\u306b\u3088\u308b\u91cf\u5b50\u72b6\u614b\u30c8\u30e2\u30b0\u30e9\u30d5\u30a3\u30fc

          <\/li>\n\n\n\n
        41. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u72b6\u614b\u540c\u5b9a\u304a\u3088\u3073\u91cf\u5b50\u3082\u3064\u308c\u306e\u5b9a\u91cf\u5316\u6cd5\u306e\u958b\u767a
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u9769\u65b0\u7684\u306a\u91cf\u5b50\u60c5\u5831\u51e6\u7406\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c8\u56de\u9818\u57df\u4f1a\u8b70
          \u5357\u7d00\u767d\u6d5c\u30de\u30ea\u30aa\u30c3\u30c8\u30db\u30c6\u30eb\u3001\u548c\u6b4c\u5c71\u30012023\u5e745\u670823\u65e5

          <\/li>\n\n\n\n
        42. (\u62db\u5f85\u8b1b\u6f14, \u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          SU(N)\u78c1\u6027\u3068\u51b7\u5374\u539f\u5b50\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30bf
          \u6975\u9650\u5b87\u5b99\u30ef\u30fc\u30af\u30b7\u30e7\u30c3\u30d7\uff5e\u5b9f\u9a13\u3068\u7406\u8ad6\u306e\u5354\u594f\u306b\u5411\u3051\u3066\uff1a\u56fa\u4f53\u7269\u8cea\u7cfb\u304b\u3089\u91cf\u5b50\u30fb\u51b7\u5374\u6c17\u4f53\u7cfb\u307e\u3067
          \u6771\u5927\u99d2\u5834\u30ad\u30e3\u30f3\u30d1\u30b9\u3001\u6771\u4eac\u30012023\u5e745\u670816\u65e5

          <\/li>\n\n\n\n
        43. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>, \u68ee\u7530\u514b\u6d0b
          SU(N)\u539f\u5b50\u6c17\u4f53\u3068\u975e\u4e00\u69d8\u5916\u5834\u3092\u7528\u3044\u305f\u5149\u683c\u5b50\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30bf\u306e\u52b9\u7387\u7684\u51b7\u5374
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2023\u5e74\u6625\u5b63\u5927\u4f1a
          \u9818\u57df1\u300123aA1-8\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012023\u5e743\u670823\u65e5

          <\/li>\n\n\n\n
        44. (\u53e3\u982d) \u53cb\u6210\u672a\u4e45<\/strong>, \u4e0a\u7530\u5b8f, \u4e0b\u5ddd\u7d71\u4e45\u6717, \u5c71\u672c\u5927\u8f14<\/strong>
          \u6570\u5024\u5bfe\u89d2\u5316\u306b\u3088\u308b\u81ea\u767a\u7684\u5bfe\u79f0\u6027\u306e\u7834\u308c\u306e\u89e3\u6790\uff1a\u91cf\u5b50\u30b9\u30d4\u30f3\u30bd\u30eb\u30d0\u30fcQS3
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2023\u5e74\u6625\u5b63\u5927\u4f1a
          \u9818\u57df3\u300124aC1-10\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012023\u5e743\u670824\u65e5

          <\/li>\n\n\n\n
        45. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u72b6\u614b\u540c\u5b9a\u304a\u3088\u3073\u91cf\u5b50\u3082\u3064\u308c\u306e\u5b9a\u91cf\u5316\u6cd5\u306e\u958b\u767a
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u9769\u65b0\u7684\u306a\u91cf\u5b50\u60c5\u5831\u51e6\u7406\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c7\u56de\u9818\u57df\u4f1a\u8b70
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012022\u5e7412\u670820\u65e5

          <\/li>\n\n\n\n
        46. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>, \u68ee\u7530\u514b\u6d0b
          SU(N)\u78c1\u6027\u3092\u7528\u3044\u305f\u5f37\u76f8\u95a2\u96fb\u5b50\u7cfb\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30bf\u306e\u65ad\u71b1\u51b7\u5374
          \u7b2c\uff11\uff18\u56de\u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u4f1a
          \u30b5\u30f3\u30b7\u30fc\u30db\u30fc\u30eb\u6d5c\u5742\u3001\u5175\u5eab\u30012022\u5e7412\u670816\u65e5

          <\/li>\n\n\n\n
        47. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14, \u99ac\u5834\u572d\u90fd, Giacomo Marmorini<\/strong>
          \u5927\u57df\u7684\u64cd\u4f5c\u306b\u3088\u308b\u30b9\u30d1\u30a4\u30e9\u30eb\u89b3\u6e2c\u57fa\u5e95\u3092\u7528\u3044\u305f\u5149\u683c\u5b50\u7cfb\u306e\u5bc6\u5ea6\u884c\u5217\u518d\u69cb\u7bc9
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2022\u5e74\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df1\u300112aW934-12\u3001\u6771\u4eac\u5de5\u696d\u5927\u5b66\u30012022\u5e749\u670812\u65e5

          <\/li>\n\n\n\n
        48. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u8c37\u5cfb\u4ecb
          \u4e00\u6b21\u5143\u5149\u683c\u5b50\u4e2dSU(3)\u51b7\u5374\u539f\u5b50\u6c17\u4f53\u306b\u304a\u3051\u308b\u5916\u5834\u52b9\u679c\u3068\u30b9\u30d4\u30f3\u30cd\u30de\u30c6\u30a3\u30c3\u30af\u6db2\u4f53
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2022\u5e74\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df1\u300113pW933-7\u3001\u6771\u4eac\u5de5\u696d\u5927\u5b66\u30012022\u5e749\u670813\u65e5

          <\/li>\n\n\n\n
        49. (\u53e3\u982d) 2022\u91cf\u5b50\u7269\u6027\u82e5\u624b\u4ea4\u6d41\u7814\u7a76\u4f1a
          \u99ac\u5834 \u572d\u90fd<\/strong>\u3000\u3000Behavior of pseudo-entropy across a quantum phase transition
          \u5bae\u8d8a \u2f24\u8f1d<\/strong>\u3000\u3000\u30db\u30c3\u30d4\u30f3\u30b0\u306e\u7b26\u53f7\u53cd\u8ee2\u3068 Bose-Hubbard model \u306e\u6642\u9593\u767a\u5c55
          \u2ed1\u2f95\u5ddd \u5ee3\u5ef6<\/strong>\u3000S=1\/2 \u7c60\u2f6c\u683c\u2f26\u53cd\u5f37\u78c1\u6027\u4f53 Cs2Cu3SnF12\u306e\u52b1\u8d77\u30a8\u30cd\u30eb\u30ae\u30fc\u306b\u304a\u3051\u308b\u8ca0\u306e\u91cf\u2f26\u518d\u898f\u683c\u5316\u73fe\u8c61\u306e\u89e3\u660e\u306b\u5411\u3051\u3066
          \u53cb\u6210 \u672a\u4e45<\/strong>\u3000\u3000\u53b3\u5bc6\u5bfe\u2f93\u5316\u306b\u304a\u3051\u308b\u2f83\u767a\u7684\u5bfe\u79f0\u6027\u306e\u7834\u308c
          \u2f95\u5ddd \u8a69\u685c\u8389<\/strong>\u3000\u51b7\u5374\u30ea\u30e5\u30fc\u30c9\u30d9\u30ea\u539f\u2f26\u91cf\u2f26\u30b7\u30df\u30e5\u30ec\u30fc\u30bf\u3068\u30b5\u30a4\u30f3\u2f06\u4e57\u5909\u5f62
          \u5ca9\u6df5 \u5468\u5e73<\/strong>\u3000\u3000DMRG \u3092\u2f64\u3044\u305f 1 \u6b21\u5143 SU(3)Heisenberg \u9396\u306e\u57fa\u5e95\u72b6\u614b\u306e\u89e3\u660e

          <\/li>\n\n\n\n
        50. (invited, oral) Daisuke Yamamoto<\/em><\/strong>
          Supersolid Devil’s staircases of spin-orbit-coupled bosons in optical lattices
          Connections between cold atoms and nuclear matter: From low to high energy
          European Centre for Theoretical Studies in Nuclear Physics and Related Areas (ECT*)
          Trento, Italy, June 7, 2022

          <\/li>\n\n\n\n
        51. (poster) Daisuke Yamamoto<\/em><\/strong>, Takahiro Sakurai, Ryosuke Okuto, Susumu Okubo, Hitoshi Ohta, Hidekazu Tanaka, and Yoshiya Uwatoko
          <\/em><\/strong>Classical-Quantum Crossover by External Pressure in the Coupled-Chain Triangular-Lattice Antiferromaget CsCuCl3<\/sub>
          The 29th International Conference on Low Temperature Physics
          Hokkaido University, Sapporo, Japan, August 20, 2022

          <\/li>\n\n\n\n
        52. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u72b6\u614b\u540c\u5b9a\u304a\u3088\u3073\u91cf\u5b50\u3082\u3064\u308c\u306e\u5b9a\u91cf\u5316\u6cd5\u306e\u958b\u767a
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u9769\u65b0\u7684\u306a\u91cf\u5b50\u60c5\u5831\u51e6\u7406\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c6\u56de\u9818\u57df\u4f1a\u8b70
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012022\u5e745\u670825\u65e5

          <\/li>\n\n\n\n
        53. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>\u3001\u6afb\u4e95\u656c\u535a\u3001\u5927\u4e45\u4fdd\u664b\u3001\u592a\u7530\u4ec1\u3001\u7530\u4e2d\u79c0\u6570\u3001\u4e0a\u5e8a\u7f8e\u4e5f
          Pressure effects on the magnetic transition temperature of CsCuCl3: CMF+TPQ analysis
          \u7b2c\uff11\uff17\u56de\u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u4f1a
          \u6c96\u7e04\u770c\u90a3\u8987\u5e02\u3068\u3082\u304b\u305c\u632f\u8208\u4f1a\u9928\u3001\u6c96\u7e04\u30012022\u5e744\u670822\u65e5

          <\/li>\n\n\n\n
        54. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>\u3001\u576a\u4e95\u4f51\u4ecb<\/strong>\u3001\u6afb\u4e95\u656c\u535a\u3001\u5927\u4e45\u4fdd\u664b\u3001\u592a\u7530\u4ec1
          \u7d50\u5408\u30b9\u30d4\u30f3\u9396\u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53CsCuCl3<\/sub>\u306e\u5727\u529b\u306b\u3088\u308b\u6b21\u5143\u6027\u3068\u71b1\u63fa\u3089\u304e\u306e\u5909\u5316
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2022\u5e74\uff08\u7b2c77\u56de\uff09\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df3\u300117aT11-7\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012022\u5e743\u670817\u65e5

          <\/li>\n\n\n\n
        55. (\u53e3\u982d\u3001\u62db\u5f85\u8b1b\u6f14) \u5c71\u672c\u5927\u8f14<\/strong>
          \u5f37\u78c1\u5834\u3068\u7570\u65b9\u6027\u306b\u3088\u308b\u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53\u306e\u591a\u5f69\u306a\u78c1\u6c17\u76f8\u3068\u5727\u529b\u306b\u3088\u308b\u91cf\u5b50\u6027\u306e\u5236\u5fa1
          \u7b2c\uff11\uff10\u56de\u5f37\u78c1\u5834\u30b3\u30e9\u30dc\u30e9\u30c8\u30ea\u30fc\u30aa\u30f3\u30e9\u30a4\u30f3\u30bb\u30df\u30ca\u30fc
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012022\u5e741\u670819\u65e5

          <\/li>\n\n\n\n
        56. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          \u4eba\u5de5\u91cf\u5b50\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u72b6\u614b\u540c\u5b9a\u304a\u3088\u3073\u91cf\u5b50\u3082\u3064\u308c\u306e\u5b9a\u91cf\u5316\u6cd5\u306e\u958b\u767a
          JST\u3055\u304d\u304c\u3051\u7814\u7a76\u9818\u57df\u300c\u9769\u65b0\u7684\u306a\u91cf\u5b50\u60c5\u5831\u51e6\u7406\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c5\u56de\u9818\u57df\u4f1a\u8b70
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012021\u5e7411\u670818\u65e5

          <\/li>\n\n\n\n
        57. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>\u3001\u4f34\u5185\u5149\u592a\u90ce\u3001\u53e4\u5ddd\u4fe1\u592b\u3001Carlos S\u00e1 de Melo
          \u30b9\u30d4\u30f3\u8ecc\u9053\u76f8\u4e92\u4f5c\u7528\u3059\u308b\u5149\u683c\u5b50\u4e2d\u30dc\u30fc\u30b9\u6c17\u4f53\u306b\u304a\u3051\u308b\u300c\u60aa\u9b54\u306e\u968e\u6bb5\u300d\u8d85\u56fa\u4f53
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2021\u5e74\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df1\u300120aA2-7\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012021\u5e749\u6708

          <\/li>\n\n\n\n
        58. (\u53e3\u982d) 2021\u91cf\u5b50\u7269\u6027\u82e5\u624b\u4ea4\u6d41\u7814\u7a76\u4f1a
          \u576a\u4e95 \u4f51\u4ecb<\/strong>\u3000\u3000\u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53 CsCuCl3 <\/sub>\u306e N\u00e9el \u6e29\u5ea6\u306e\u5727\u529b\u4f9d\u5b58\u6027\u306b\u3064\u3044\u3066
          \u6d77\u8001\u539f \u660c\u5e73<\/strong>\u3000\u91cf\u5b50\u4e09\u89d2\u53cd\u5f37\u78c1\u6027\u4f53 Ba3<\/sub>CoSb2<\/sub>O9<\/sub> \u306e\u78c1\u6c17\u98fd\u548c\u76f4\u524d\u306e\u76f8\u306e\u89e3\u660e
          \u4e03\u6d77 \u5149\u4e00<\/strong>\u3000\u3000\u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u539f\u5b50\u6c17\u4f53\u306e\u8d85\u6d41\u52d5\u30fbMott \u7d76\u7e01\u4f53\u76f8\u8ee2\u79fb
          \u5409\u67f3 \u5065\u592a<\/strong>\u3000\u3000SU(3)\u30c8\u30e9\u30a4\u30de\u30fc\u306e\u56fa\u6709\u72b6\u614b\u3068\u65b0\u305f\u306a\u591a\u8272\u91cf\u5b50\u78c1\u6027\u306e\u958b\u62d3
          \u99ac\u5834 \u572d\u90fd<\/strong>\u3000\u3000\u91cf\u5b50\u72b6\u614b\u30c8\u30e2\u30b0\u30e9\u30d5\u30a3\u306b\u3088\u308b\u5bc6\u5ea6\u884c\u5217\u306e\u518d\u69cb\u6210\u3068\u305d\u306e\u8a55\u4fa1

          <\/li>\n\n\n\n
        59. (oral) Hayato Motegi, Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Nobuo Furukawa
          Phase diagram of the SU(3) Fermi gases with population imbalance in square optical lattices
          2021 APS March Meeting
          Online, March 2021.

          <\/li>\n\n\n\n
        60. (poster) Hayato Motegi, Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Nobuo Furukawa
          Phase diagram of the SU(3) Heisenberg model with tunable single-ion anisotropy
          The International Conference on Highly Frustrated Magnetism 2021 (WHFM 2021)
          Online, January 2021.

          <\/li>\n\n\n\n
        61. (poster) Giacomo Marmorini, Daisuke Yamamoto<\/em><\/strong>, Chihiro Suzuki, Sho Okazaki, and Nobuo Furukawa
          Mixed dipolar-nematic order and half-vortex topological transitions of the triangular SU(3) Heisenberg model under magnetic fields
          The International Conference on Highly Frustrated Magnetism 2021 (WHFM 2021)
          Online, January 2021.

          <\/li>\n\n\n\n
        62. (\u53e3\u982d) \u5bae\ufa11\u512a\u5e0c\u3001\u5c71\u672c\u5927\u8f14<\/strong>\u3001Giacomo Marmorini\u3001\u53e4\u5ddd\u4fe1\u592b
          \u5149\u8d85\u683c\u5b50\u4e2d\u306eSU(N) Fermi\u539f\u5b50\u6c17\u4f53\u306b\u304a\u3051\u308b\u6210\u5206\u6570\u306e\u4e0d\u5747\u8861\u304c\u8a98\u8d77\u3059\u308b\u91cf\u5b50\u76f8
          \u7b2c3\u56de\u51b7\u5374\u539f\u5b50\u7814\u7a76\u4f1a\u30a2\u30c8\u30e0\u306e\u4f1a
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012021\u5e748\u670810\u65e5-11\u65e5

          <\/li>\n\n\n\n
        63. (\u53e3\u982d) \u5bae\ufa11\u512a\u5e0c\u3001\u5c71\u672c\u5927\u8f14<\/strong>\u3001Giacomo Marmorini\u3001\u53e4\u5ddd\u4fe1\u592b
          \u5149\u8d85\u683c\u5b50\u4e2d\u306e SU(N) Fermi\u539f\u5b50\u6c17\u4f53\u306b\u304a\u3051\u308b\u6210\u5206\u6570\u306e\u4e0d\u5747\u8861\u304c\u8a98\u8d77\u3059\u308b\u91cf\u5b50\u76f8
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c76\u56de\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1\u300113pA2-9\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012021\u5e743\u670812\u65e5-15\u65e5
          \u5b66\u751f\u512a\u79c0\u767a\u8868\u8cde\u3092\u53d7\u8cde\uff08\u5bae\ufa11\u512a\u5e0c\uff09<\/strong>

          <\/li>\n\n\n\n
        64. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>
          SU(3)\u30b9\u30d4\u30f3\u6a21\u578b\u306b\u304a\u3051\u308b\u30cd\u30de\u30c6\u30a3\u30c3\u30af\u306a\u30b9\u30d4\u30f3\u30c0\u30a4\u30dd\u30fc\u30eb\u79e9\u5e8f
          \u7b2c15\u56de\u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u4f1a
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012021\u5e741\u6708

          <\/li>\n\n\n\n
        65. (poster) Yuki Miyazaki, Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini and Nobuo Furukawa
          Field-induced Phase Transitions of Tetramer-Singlet States in Synthetic SU(4) Magnets
          Magnetism and Magnetic Materials 2020 Virtual Conference
          F5-12, Online, November 2020.

          <\/li>\n\n\n\n
        66. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>\u3001\u6afb\u4e95\u656c\u535a\u3001\u5927\u4e45\u4fdd\u664b\u3001\u592a\u7530\u4ec1
          \u5727\u529b\u3092\u7528\u3044\u305f\u7d50\u5408\u30b9\u30d4\u30f3\u9396\u7269\u8cea\u306e\u91cf\u5b50\u6027\u306e\u5236\u5fa1\uff1aCsCuCl3\u306e\u5834\u5408
          \u7b2c\uff14\u56de\u30b9\u30d4\u30f3\u7cfb\u7269\u7406\u7814\u7a76\u4f1a \u300c\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u306e\u958b\u62d3\u524d\u7dda\u300d
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012020\u5e7411\u6708

          <\/li>\n\n\n\n
        67. (\u53e3\u982d\u3001\u62db\u5f85\u8b1b\u6f14) \u5c71\u672c\u5927\u8f14<\/strong>
          \u78c1\u5834\u4e2dSU(3) Heisenberg\u6a21\u578b\u306e\u91cf\u5b50\u76f8\u3068\u96a0\u308c\u305f\u30cd\u30de\u30c6\u30a3\u30c3\u30af\u6027\u3092\u6301\u3064\u30b9\u30d4\u30f3\u30c0\u30a4\u30dd\u30fc\u30eb\u79e9\u5e8f
          \u30aa\u30f3\u30e9\u30a4\u30f3CMT\u30bb\u30df\u30ca\u30fc\uff08\u7b2c25\u56de\uff09
          \u30aa\u30f3\u30e9\u30a4\u30f3\u30012020\u5e7411\u6708

          <\/li>\n\n\n\n
        68. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>\u3001Giacomo Marmorini\u3001\u53e4\u5ddd\u4fe1\u592b
          \u4e09\u89d2\u5149\u683c\u5b50\u4e2d\u306eSU(3) Fermi\u539f\u5b50\u6c17\u4f53\u306b\u304a\u3051\u308b\u78c1\u5834\u52b9\u679c\u3068\u3086\u3089\u304e\u306b\u3088\u308b\u79e9\u5e8f\u5316
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2020\u5e74\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df1\u30018aA2-11\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012020\u5e749\u6708

          <\/li>\n\n\n\n
        69. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>\u3001\u6afb\u4e95\u656c\u535a\u3001\u5927\u4e45\u4fdd\u664b\u3001\u592a\u7530\u4ec1
          \u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53CsCuCl3\u306e\u9ad8\u5727\u4e0b\u78c1\u5316\u904e\u7a0b\u306b\u5bfe\u3059\u308b\u7406\u8ad6\u89e3\u6790\u3068\u91cf\u5b50\u6027\u306e\u5236\u5fa1II
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2020\u5e74\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df3\u30019aC1-7\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u30012020\u5e749\u6708

          <\/li>\n\n\n\n
        70. (\u53e3\u982d) \u4f34\u5185\u5149\u592a\u90ce\u3001\u5c71\u672c\u5927\u8f14<\/strong>\u3001\u53e4\u5ddd\u4fe1\u592b
          \u5149\u683c\u5b50\u4e2d\u306e\u30b9\u30d4\u30f3\u8ecc\u9053\u76f8\u4e92\u4f5c\u7528\u3092\u6301\u3064Bose\u539f\u5b50\u6c17\u4f53\u306b\u304a\u3051\u308b\u60aa\u9b54\u306e\u968e\u6bb5\u3068\u8d85\u6d41\u52d5\u81e8\u754c\u901f\u5ea6
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2020\u5e74\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df1\u30018pA2-3\u3001 \u30aa\u30f3\u30e9\u30a4\u30f3\u30012020\u5e749\u6708

          <\/li>\n\n\n\n
        71. (\u53e3\u982d) <\/strong>\u8302\u6728\u96bc\u4eba\u3001\u5c71\u672c\u5927\u8f14<\/strong>\u3001Giacomo Marmorini\u3001\u53e4\u5ddd\u4fe1\u592b
          \u6b63\u65b9\u5149\u683c\u5b50\u4e2d\u306eSU(3)Fermi\u539f\u5b50\u6c17\u4f53\u306b\u304a\u3051\u308b\u6210\u5206\u6570\u4e0d\u5747\u8861\u304c\u751f\u3080\u65b0\u305f\u306a\u78c1\u6c17\u79e9\u5e8f
          \u65e5\u672c\u7269\u7406\u5b662020\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df1\u30018pA2-10\u3001\u30aa\u30f3\u30e9\u30a4\u30f3\u3001 2020\u5e749\u6708

          <\/li>\n\n\n\n
        72. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14<\/strong>\u3001\u6afb\u4e95\u656c\u535a\u3001\u5965\u85e4\u6dbc\u4ecb\u3001\u5927\u4e45\u4fdd\u664b\u3001\u592a\u7530\u4ec1
          \u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53CsCuCl3\u306e\u9ad8\u5727\u5316\u78c1\u5316\u904e\u7a0b\u306b\u5bfe\u3059\u308b\u7406\u8ad6\u89e3\u6790\u3068\u91cf\u5b50\u6027\u306e\u5236\u5fa1
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c75\u56de\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df3\u300118pE24-5\u3001\u540d\u53e4\u5c4b\u5927\u5b66\u30012020\u5e743\u6708

          <\/li>\n\n\n\n
        73. (\u53e3\u982d) <\/strong>\u8302\u6728\u96bc\u4eba, \u5c71\u672c\u5927\u8f14<\/strong>, Giacomo Marmorini, \u53e4\u5ddd\u4fe1\u592b
          \u5149\u683c\u5b50\u4e2d\u306e\u30a2\u30eb\u30ab\u30ea\u571f\u985e ( \u69d8 )Fermi \u539f\u5b50\u6c17\u4f53\u306e SU(3) \u8272\u79e9\u5e8f\u3068\u6210 \u5206\u6570\u4e0d\u5747\u8861\u306e\u52b9\u679c
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c75\u56de\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1\u300118pK27-4\u3001\u540d\u53e4\u5c4b\u5927\u5b66\u30012020\u5e743\u6708

          <\/li>\n\n\n\n
        74. (\u53e3\u982d) \u592a\u7530\u967d\u3001\u5c71\u672c\u5927\u8f14\u3001<\/strong>\u53e4\u5ddd\u4fe1\u592b
          \u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53Mn(OH)2\u306e\u6e29\u5ea6-\u78c1\u5834\u76f8\u6d25\u306b\u5bfe\u3059\u308b\u30e2\u30f3\u30c6\u30ab\u30eb\u30ed\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3\u89e3\u6790
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c75\u56de\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df3\u300118pE24-5\u3001\u540d\u53e4\u5c4b\u5927\u5b66\u30012020\u5e743\u6708

          <\/li>\n\n\n\n
        75. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14
          <\/strong>\u8ca0\u6e29\u5ea6\u539f\u5b50\u6c17\u4f53\u3092\u7528\u3044\u305f\u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u91cf\u5b50\u78c1\u6027\u306e\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3
          \u7b2c14\u56de\u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u4f1a
          \u79cb\u7530\u82b8\u8853\u6751\u30012020\u5e741\u6708

          <\/li>\n\n\n\n
        76. (invited, oral) Daisuke Yamamoto
          <\/em><\/strong>Magnetic Phase Diagram of the SU(3) Heisenberg Model with Ultracold Fermions in a Triangular Optical Lattice
          14th Asia-Pacific Physics Conference
          Borneo Convention Centre Kuching, Sarawak, Malaysia, November 2019.

          <\/li>\n\n\n\n
        77. (oral) Kazuki Takagi, Daisuke Yamamoto<\/em><\/strong>, Haruhisa Kitano, and Nobuo Furukawa
          Phase Retrapping Effects on Switching Characteristic in Intrinsic Josephson Junctions
          14th Asia-Pacific Physics Conference
          Borneo Convention Centre Kuching, Sarawak, Malaysia, November 2019.

          <\/li>\n\n\n\n
        78. (invited, oral) Daisuke Yamamoto <\/em><\/strong>
          Quantum Simulation of Frustrated Quantum Magnetism with Bose Gases at Negative Absolute Temperatures
          The Fourth Kyoto-Beijing-Tokyo Workshop on Ultracold Atomic Gases
          Kyoto University, September 2019.

          <\/li>\n\n\n\n
        79. (oral) Daisuke Yamamoto,<\/em><\/strong> Takeshi Fukuhara, and Ippei Danshita
          Synthetic Frustrated Quantum Systems with Bose Gases in Triangular Lattices at Negative Absolute Temperatures
          International Conference on Strongly Correlated Electron Systems (SCES 2019)
          Okayama Convention Center, Okayama, September 2019.

          <\/li>\n\n\n\n
        80. (poster) Giacomo Marmorini, Daisuke Yamamoto,<\/em><\/strong> Masahiro Tabata, Kazuki Sakakura, and Ippei Danshita
          Frustrated Magnetism with Coherently-Coupled Binary Fermi Gases in Triangular Optical Lattices
          The Fourth Kyoto-Beijing-Tokyo Workshop on Ultracold Atomic Gases
          Kyoto University, October 2019.

          <\/li>\n\n\n\n
        81. (poster) Chihiro Suzuki, Daisuke Yamamoto,<\/em><\/strong> and Nobuo Furukawa
          Quantum and Thermal Effects of the Triangular SU(3) Heisenberg Model in a Magnetic Field
          The Fourth Kyoto-Beijing-Tokyo Workshop on Ultracold Atomic Gases
          Kyoto University, October 2019.

          <\/li>\n\n\n\n
        82. (poster) Kazuki Takagi, Daisuke Yamamoto<\/em><\/strong>, and Nobuo Furukawa
          Slave Boson Mean Field Analysis of Superconductivity in the SU(3) t-J model
          The Fourth Kyoto-Beijing-Tokyo Workshop on Ultracold Atomic Gases
          Kyoto University, October 2019.

          <\/li>\n\n\n\n
        83. (poster) Kotaro Bannai, Daisuke Yamamoto,<\/em><\/strong> and Nobuo Furukawa
          Chiral soliton crystal and superfluid critical velocity in ultracold Bose gases with spin-orbit coupling
          The Fourth Kyoto-Beijing-Tokyo Workshop on Ultracold Atomic Gases
          Kyoto University, October 2019.

          <\/li>\n\n\n\n
        84. (poster) Chihiro Suzuki, Daisuke Yamamoto,<\/em><\/strong> and Nobuo Furukawa
          Quantum and Thermal Phase Diagrams of the Triangular-Lattice SU(3) Heisenberg Model in a Magnetic Field
          International Conference on Strongly Correlated Electron Systems (SCES 2019)
          Okayama Convention Center, Okayama, September 2019.
          SCES2019 poster award (Chihiro Suzuki)
          <\/strong>
          <\/li>\n\n\n\n
        85. (poster) Prokhnenko, X. Z. Liu, Daisuke Yamamoto,<\/em><\/strong> M. Bartkowiak, N. Kurita, and H. Tanaka
          Neutron scattering investigation of frustrated quantum magnet Ba3CoSb2O9 in magnetic fields up to 25.9T
          International Conference on Strongly Correlated Electron Systems (SCES 2019)
          Okayama Convention Center, Okayama, September 2019.

          <\/li>\n\n\n\n
        86. (poster) N. Kurita, Daisuke Yamamoto,<\/em><\/strong> T. Kanesaka, N. Furukawa, S. Ohira-Kawamura, K. Nakajima, K. Nawa, T. J. Sato, and H. Tanaka
          Localized Magnetic Excitations of the Strongly Frustrated Dimerized Magnets
          International Conference on Strongly Correlated Electron Systems (SCES 2019)
          Okayama Convention Center, Okayama, September 2019.

          <\/li>\n\n\n\n
        87. (poster) Daisuke Yamamoto,<\/em><\/strong> Takeshi Fukuhara, and Ippei Danshita
          Theoretical Modeling of Cold-Atom Simulations for Frustrated Quantum Magnetism
          IAS Workshop on Quantum Simulation of Novel Phenomena with Ultracold Atoms
          Hong Kong, China, May 2019.

          <\/li>\n\n\n\n
        88. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14\u3001<\/strong>\u9234\u6728\u5343\u5c0b\u3001\u53e4\u5ddd\u4fe1\u592b
          SU(N) Heisenberg\u6a21\u578b\u306b\u304a\u3051\u308b\u78c1\u5316\u904e\u7a0b\u3068\u63fa\u3089\u304e\u306b\u3088\u308b\u79e9\u5e8f\u5316
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a2019\u5e74\u79cb\u5b63\u5927\u4f1a
          \u9818\u57df3, 13aD11-10\u3001\u5c90\u961c\u5927\u5b66\u30012019\u5e749\u6708

          <\/li>\n\n\n\n
        89. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14,<\/strong> \u798f\u539f\u6b66, \u6bb5\u4e0b\u4e00\u5e73
          \u4e09\u89d2\u5149\u683c\u5b50\u4e2d\u306e\u8ca0\u6e29\u5ea6\u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8Bose\u539f\u5b50\u6c17\u4f53\u306e\u91cf\u5b50\u76f8\u8ee2\u79fb
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c74\u56de\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df1, 15pF202-5\u3001\u4e5d\u5dde\u5927\u5b66\u30012019\u5e743\u6708

          <\/li>\n\n\n\n
        90. (\u53e3\u982d) \u9ad8\u6728\u4e00\u6a39, \u5c71\u672c\u5927\u8f14,<\/strong> \u5317\u91ce\u6674\u4e45, \u53e4\u5ddd\u4fe1\u592b
          \u56fa\u6709\u30b8\u30e7\u30bb\u30d5\u30bd\u30f3\u63a5\u5408\u7cfb\u306e\u30b9\u30a4\u30c3\u30c1\u30f3\u30b0\u7279\u6027\u306b\u304a\u3051\u308b\u4f4d\u76f8\u518d\u6355\u6349\u52b9\u679c\u306e\u89e3\u6790
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c74\u56de\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df6, 14aK404-13\u3001\u4e5d\u5dde\u5927\u5b66\u30012019\u5e743\u6708

          <\/li>\n\n\n\n
        91. (\u30dd\u30b9\u30bf\u30fc) \u5ddd\u53e3\u6052\u3001\u5c71\u672c\u5927\u8f14<\/strong>\u3001\u53e4\u5ddd\u4fe1\u592b
          \u30d5\u30e9\u30c3\u30c8\u30d0\u30f3\u30c9\u3092\u3082\u3064\u5149\u683c\u5b50\u4e2d\u30dc\u30fc\u30b9\u539f\u5b50\u6c17\u4f53\u306e\u91cf\u5b50\u72b6\u614b
          \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c74\u56de\u5e74\u6b21\u5927\u4f1a
          \u9818\u57df11, 17aPS-46\u3001\u4e5d\u5dde\u5927\u5b66\u30012019\u5e743\u6708

          <\/li>\n\n\n\n
        92. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14 <\/strong>
          \u4e2d\u6027\u5b50\u6563\u4e71\u306e\u5fae\u8996\u7684\u89e3\u6790\u306b\u3088\u308b\u91cf\u5b50\u78c1\u6027\u306e\u5b9a\u91cf\u7684\u7406\u89e3\uff1aBa2CoSi2O6Cl2\u3068Ba3CoSb2O9
          \u7b2c2\u56de\u30b9\u30d4\u30f3\u7cfb\u7269\u7406\u7814\u7a76\u4f1a
          \u5206\u5b50\u30d5\u30a9\u30c8\u30b5\u30a4\u30a8\u30f3\u30b9\u7814\u7a76\u30bb\u30f3\u30bf\u30fc\u3001\u795e\u6238\u5927\u5b66\u30012019\u5e741\u6708

          <\/li>\n\n\n\n
        93. (\u53e3\u982d) \u5c71\u672c\u5927\u8f14
          <\/strong>\u78c1\u5834\u4e2dSU(N)\u91cf\u5b50\u30b9\u30d4\u30f3\u6a21\u578b\u306b\u304a\u3051\u308b\u91cf\u5b50\u30fb\u71b1\u63fa\u3089\u304e\u8a98\u8d77\u76f8\u8ee2\u79fb
          \u7b2c13\u56de\u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u4f1a
          \u6771\u6d77\u6751\u7523\u696d\u30fb\u60c5\u5831\u30d7\u30e9\u30b6\u300c\u30a2\u30a4\u30f4\u30a3\u30eb(iVil)\u300d\u30012019\u5e741\u6708
          <\/li>\n<\/ol>\n\n\n\n
          \n
          2018\u5e74\u4ee5\u524d\uff08\u56fd\u969b, oral\uff09<\/summary>
          \n
            \n
          1. Daisuke Yamamoto<\/em><\/strong>
            Synthetic triangular antiferromagnets with ultracold fermions in optical lattices
            Tensor Network States: Algorithms and Applications (TNSAA)
            R-CCS Kobe, Japan, December 2018.

            <\/li>\n
          2. (invited) Daisuke Yamamoto<\/em><\/strong>
            Exploring Quantum Frustrated Magnetism with Cold-Atom Quantum Simulators
            Recent Trends in Cold and Ultracold Matter
            Day 1: Session III, Guwahati, India, March 2018

            <\/li>\n
          3. (invited) Daisuke Yamamoto<\/em><\/strong>
            Strong Field-Induced Phase Transitions in Frustrated Quantum Magnets
            Trends in Theory of Correlated Materials (TTCM2017)
            Session 8, Tsukuba, Japan, September 2017.

            <\/li>\n
          4. Daisuke Yamamoto<\/em><\/strong>, Hiroshi Ueda, Ippei Danshita, Giacomo Marmorini, Tsutomu Momoi, and Tokuro Shimokawa
            Quantum phases of triangular-lattice spin-S XXZ antiferromagnets near saturation
            International Conference on Low Temperature Physics (LT28)
            Magn.076, Gothenburg, Sweden, August 2017.

            <\/li>\n
          5. Giacomo Marmorini, Daisuke Yamamoto<\/em><\/strong>, and Ippei Danshita
            New results for triangular-lattice quantum antiferromagnets in a magnetic field
            International Conference on Magnetism
            TU.C.3.O1, Barcelona, Spain, July 2015.

            <\/li>\n
          6. Daisuke Yamamoto<\/em><\/strong>, Keisuke Masuda, and Susumu Kurihara
            Frustrated Ultracold Bose Gases in a Kagome Optical Lattice
            Novel Quantum States in Condensed Matter
            WS-A6, Kyoto, Japan, November 2014.

            <\/li>\n
          7. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Ippei Danshita
            Phase Diagram of Spin-1\/2 Triangular-Lattice Antiferromagnets with Exchange Anisotropy and a Magnetic Field
            The APS March Meeting
            B4-11, Denver, USA, March 2014.

            <\/li>\n
          8. Yasuyuki Kato, Daisuke Yamamoto<\/em><\/strong>, and Ippei Danshita
            Quantum tricriticality at the superfluid-insulator transition of binary Bose mixtures: A quantum Monte-Carlo study
            The APS March Meeting
            Z35-13, Denver, USA, March 2014.

            <\/li>\n
          9. Daisuke Yamamoto<\/em><\/strong>, Takeshi Ozaki, Carlos A. R. S\u00e1 de melo, and Ippei Danshita
            First-order transition and hysteresis phenomena of Bose-Bose mixtures in an optical lattice
            2013 Joint Meeting of the APS Division of Atomic, Molecular and Optical Physics and the CAP Division of Atomic, Molecular and Optical Physics (DAMOP2013)
            N2, Quebec, Canada, June 2013.

            <\/li>\n
          10. Daisuke Yamamoto<\/em><\/strong> and Ippei Danshita
            Supersolids and Anomalous Hysteresis in Frustrated Spin-Dimer Model
            The APS March Meeting
            F15.3, Baltimore, USA, March 2013.

            <\/li>\n
          11. Daisuke Yamamoto<\/em><\/strong>, Ippei Danshita, and Carlos A. R. S\u00e1 de Melo
            Re-entrant first-order phase transitions and anomalous hysteresis of dipolar Bose gases in a triangular optical lattice
            The APS March Meeting
            D4.15, Boston, USA, February 2012.

            <\/li>\n
          12. Keisuke Masuda and Daisuke Yamamoto<\/em><\/strong>
            Cooper Pairing of Fermions with Unequal Masses in Heavy-Fermion Systems
            International workshop on heavy fermions (TOKIMEKI 2011)
            24-SO-4, Osaka, Japan, November 2011.

            <\/li>\n
          13. Yuki Terakawa, Nobuhiko Yokoshi, Kenji Kamide, Daisuke Yamamoto<\/em><\/strong>, and Susumu Kurihara
            Effect of quantum fluctuations on Bose-Einstein condensation of bilayer atomic gases in rapid rotation
            16th International Laser Physics Workshop (LPHYS ’07)
            Section 6.6.2, Leon, Mexico, August 2007.<\/li>\n<\/ol>\n<\/div><\/details><\/div>\n
            2018\u5e74\u4ee5\u524d\uff08\u56fd\u969b, poster\uff09 <\/summary>
            \n
              \n
            1. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, Masahiro Tabata, Kazuki Sakakura, and Ippei Danshita
              Quantum frustrated magnetism with fermions in triangular optical lattices: Theoretical proposal and prediction
              ITAMP Harvard Workshop, Fermions in Optical Lattices, Cambridge, USA, October 2018.

              <\/li>\n
            2. Masahiro Tabata, Daisuke Yamamoto<\/em><\/strong>, and Nobuo Furukawa
              Numerical analysis for Berezinskii-Kosterlitz-Thouless transitions with incommensurate orders
              International Conference on Highly Frustrated Magnetism (HFM2018)
              0.21, Davis, USA, July 2018.

              <\/li>\n
            3. Nobuyuki Kurita, Seiko Ohira-Kawamura, Kenji Nakajima, Daisuke Yamamoto<\/em><\/strong>, Takuya Kanesaka, Nobuo Furukawa, and Hidekazu Tanaka
              Localized magnetic excitations of the strongly frustrated dimerized quantum magnet
              International Conference on Highly Frustrated Magnetism (HFM2018)
              0.21, Davis, USA, July 2018.

              <\/li>\n
            4. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, Masahiro Tabata, and Ippei Danshita
              Novel Quantum and Thermal Phase Transitions of Easy-Axis Triangular Antiferromagnets in a Transverse Field
              International Conference on Magnetism (ICM2018)
              W4-04, San Francisco, USA, July 2018.

              <\/li>\n
            5. Sho Okazaki, Daisuke Yamamoto<\/em><\/strong>, Nobuo Furukawa
              Phase Transition Phenomena of the Antiferromagnetic Kagome XY Model with and without Next-Nearest-Neighbor Interactions
              International Conference on Magnetism (ICM2018)
              N13-01, San Francisco, USA, July 2018.

              <\/li>\n
            6. Takuya Kanesaka, Daisuke Yamamoto<\/em><\/strong>, and Nobuo Furukawa
              Magnetic Phase Diagram of Quantum Spin-Dimer Antiferromagnets on the Square and Triangular Lattices
              International Conference on Magnetism (ICM2018)
              N6-09, San Francisco, USA, July 2018.

              <\/li>\n
            7. Chihiro Suzuki, Daisuke Yamamoto<\/em><\/strong>, and Nobuo Furukawa
              Quantum Phases of the S=1 Triangular Bilinear-Biquadratic Model in a Magnetic Field
              International Conference on Magnetism (ICM2018)
              N6-06, San Francisco, USA, July 2018.

              <\/li>\n
            8. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, Masahiro Tabata, and Ippei Danshita
              Synthetic Frustrated Antiferromagnets with Coherently-Coupled Binary Fermi Gases in a Triangular Optical Lattice
              International Conference on Atomic Physics (26th ICAP)
              170, Barcelona, Spain, July 2018.

              <\/li>\n
            9. Hisashi Kawaguchi, Daisuke Yamamoto<\/em><\/strong>, and Nobuo Furukawa
              Supersolid Phase with Ultracold Bose Gases in an Optical Lieb Lattice
              International Conference on Atomic Physics (26th ICAP)
              164, Barcelona, Spain, July 2018.

              <\/li>\n
            10. Yutaka Saiki, Daisuke Yamamoto<\/em><\/strong>, and Nobuo Furukawa
              Quantum phase transition of a frustrated Bose-Hubbard model on triangular lattice: Density matrix renormalization group study
              International Conference on Atomic Physics (26th ICAP)
              180, Barcelona, Spain, July 2018.

              <\/li>\n
            11. Shimpei Goto and Daisuke Yamamoto<\/em><\/strong>
              Incommensurate spiral magnetic order in the Hubbard model on anisotropic triangular lattice
              International Conference on Low Temperature Physics (LT28)
              P.328, Gothenburg, Sweden, August 2017.

              <\/li>\n
            12. Masahiro Tabata, Daisuke Yamamoto<\/em><\/strong>, and Nobuo Furukawa
              Kosterlitz-Thouless transitions of incommensurate orders in frustrated Heisenberg models
              International Conference on Low Temperature Physics (LT28)
              P.536, Gothenburg, Sweden, August 2017.

              <\/li>\n
            13. Nobuyuki Kurita, Seiko Ohira-Kawamura, Kenji Nakajima, Daisuke Yamamoto<\/em><\/strong>, Takuya Kanesaka, Nobuo Furukawa, and Hidekazu Tanaka
              Localized Magnetic Excitations in the S = 1\/2 Fully Frustrated Dimerized Magnet Ba2CoSi2O6Cl2
              International Conference on Neutron Scattering (ICNS2017)
              TuP97, Daejeon, Korea, July 2017.

              <\/li>\n
            14. Daisuke Yamamoto<\/em><\/strong>, Hiroshi Ueda, Ippei Danshita, Giacomo Marmorini, Tsutomu Momoi, and Tokuro Shimokawa
              On the 0-\u03c0 transition of coplanar states in quantum triangular XXZ antiferromagnets near saturation
              The 8th International Conference on Highly Frustrated Magnetism 2016 (HFM 2016)
              Taipei, Taiwan, Sept. 7th-11th, 2016.

              <\/li>\n
            15. Daisuke Yamamoto<\/em><\/strong> and Makoto Naka
              Schwinger-boson study of Bose gases in a shaken triangular optical lattice
              International workshop on `Synthetic Quantum Magnetism’
              Max Planck, Germany, August 2015.

              <\/li>\n
            16. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Ippei Danshita
              High-Field Quantum Phase Transition Induced by Weak Three Dimensionality in Triangular-Lattice Antiferromagnets
              International Conference on Magnetism, TH.C-P54, Barcelona, Spain, July 2015.

              <\/li>\n
            17. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Ippei Danshita
              Quantum phase diagram of triangular-lattice antiferromagnets with XXZ anisotropy and magnetic field
              The 2014 International Conference on Highly Frustrated Magnetism (HFM2014)
              S10414, Cambridge, UK, July 2014.

              <\/li>\n
            18. Daisuke Yamamoto<\/em><\/strong>, Keisuke Masuda, and Susumu Kurihara
              Effects of phase and amplitude fluctuations on the ground state of a frustrated Bose-Hubbard system
              Higgs modes in condensed matter and quantum gases
              P27, Kyoto, Japan, Jun 2014.

              <\/li>\n
            19. Daisuke Yamamoto<\/em><\/strong>, Giacomo Marmorini, and Ippei Danshita
              Field-induced quantum phases of the XXZ model on the triangular lattice
              International Conference on Strongly Correlated Electron Systems (SCES2013)
              A011, Tokyo, Japan, August 2013.

              <\/li>\n
            20. Keisuke Masuda and Daisuke Yamamoto<\/em><\/strong>
              Interorbital Cooper pairing with s-wave symmetry in heavy-fermion systems
              International Conference on Strongly Correlated Electron Systems (SCES2013)
              A407, Tokyo, Japan, August 2013.

              <\/li>\n
            21. Daisuke Yamamoto<\/em><\/strong>, Takeshi Ozaki, Carlos A. R. S\u00e1 de Melo, and Ippei Danshita
              First-Order Phase Transition and Anomalous Hysteresis of Binary Bose Mixtures in an Optical Lattice
              International Symposium on Quantum Fluids and Solids (QFS2013)
              PS3.48, Matsue, Japan, August 2013.

              <\/li>\n
            22. Keisuke Masuda and Daisuke Yamamoto<\/em><\/strong>
              Cooper pairing between conduction and localized electrons in heavy-fermion systems
              International Conference on Magnetism (ICM2012)
              SB23, Busan, Korea, July 2012.

              <\/li>\n
            23. Hiroki Yamamura and Daisuke Yamamoto<\/em><\/strong>
              Instability of superfluid Fermi gases caused by bosonic excitations
              The 23rd International Conference on Atomic Physics (ICAP2012)
              Th-093, Palaiseau, France, July 2012.

              <\/li>\n
            24. Tomonori Fukase, Shunji Tsuchiya, Daisuke Yamamoto<\/em><\/strong>, and Tetsuro Nikuni
              Possibility of gapless superfluid states od Fermi atoms in triangular optical lattices
              The 23rd International Conference on Atomic Physics (ICAP2012)
              Tu-091, Palaiseau, France, July 2012.

              <\/li>\n
            25. Chika Sato, Daisuke Yamamoto<\/em><\/strong>, Shunji Tsutiya, and Tetsuro Nikuni \u300cFermi superfluid in a kagome optical lattice
              The 23rd International Conference on Atomic Physics (ICAP2012)
              Th-089, Palaiseau, France, July 2012.

              <\/li>\n
            26. Daisuke Yamamoto<\/em><\/strong>, Ippei Danshita, and Carlos A. R. S\u00e1 de Melo
              Quantum phases and anomalous hysteresis of dipolar Bose gases in a triangular optical lattice
              The 23rd International Conference on Atomic Physics (ICAP2012)
              Mo-079, Palaiseau, France, July 2012.

              <\/li>\n
            27. Daisuke Yamamoto<\/em><\/strong>, Ippei Danshita, and Carlos A. R. S\u00e1 de Melo
              Anomalous hysteresis of Bose gases in an optical lattice
              Workshop on Quantum Simulations with Ultracold Atoms
              Trieste, Italy, July 2012.

              <\/li>\n
            28. Daisuke Yamamoto<\/em><\/strong>, Ippei Danshita, and Carlos A. R. S\u00e1 de Melo
              Anomalous hysteretic behavior in a system of dipolar Bose gases
              26th International Conference on Low Temperature Physics (LT26)
              12P-A011, Beijing, China, August 2011.

              <\/li>\n
            29. Daisuke Yamamoto<\/em><\/strong> and Ippei Danshita
              Stability of Superflow in Supersolid Phases of Dipolar Bose Gases in Moving Optical Lattices
              22nd International Conference on Atomic Physics (ICAP2010)
              Th59, Cairns, Australia, July 2010.

              <\/li>\n
            30. Daisuke Yamamoto<\/em><\/strong> and Ippei Danshita
              Stability of superflow in supersolid phases of lattice bosons with dipole-dipole interaction
              International Conference on Strongly Correlated Electron Systems (SCES\u201910)
              M125, Santa Fe, USA, June 2010.

              <\/li>\n
            31. Daisuke Yamamoto<\/em><\/strong> and Ippei Danshita
              Supersolidity and Critical Velocity of Superflow in Lattice Boson Systems with Dipole-Dipole Interactions
              Ultracold Fermi Gas: Superfluidity and Strong-Correlation (USS-2010)
              P7,Tokyo, Japan, May 2010.

              <\/li>\n
            32. Takao Nomura, Daisuke Yamamoto<\/em><\/strong>, and Susumu Kurihara
              Electric Field Effects in Zigzag Graphene Nanoribbons
              The International Conference on Magnetism (ICM09)
              Th-B-6.10-03, Karlsruhe, Germany, July 2009.

              <\/li>\n
            33. Daisuke Yamamoto<\/em><\/strong>
              Cluster Mean-Field Approach Including Correlation Effects between Clusters
              The International Conference on Magnetism (ICM09)
              Th-C-2.6-02, Karlsruhe, Germany, July 2009.

              <\/li>\n
            34. Yoshihiro Yunomae, Ippei Danshita, Daisuke Yamamoto<\/em><\/strong>, Nobuhiko Yokoshi, and Shunji Tsuchiya
              Stability of superfluid Fermi gases in optical lattices
              The 9th International Symposium on Foundations of Quantum Mechanics in the Light of New Technology (ISQM-TOKYO\u201908)
              PII-22, Advanced Research Laboratory, Hitachi, Japan, August 2008.

              <\/li>\n
            35. Yoshihiro Yunomae, Ippei Danshita, Daisuke Yamamoto<\/em><\/strong>, Nobuhiko Yokoshi, and Shunji Tsuchiya
              Current-Induced Instability of Superfluid Fermi Gases in Optical Lattices
              25th international conference on Low Temperature Physics (LT25)
              LT1851, Amsterdam, Netherlands, August 2008.

              <\/li>\n
            36. Daisuke Yamamoto<\/em><\/strong>, Synge Todo, and Susumu Kurihara
              Application of the Green’s Function Method to an Easy-Plane Heisenberg Model
              25th international conference on Low Temperature Physics (LT25)
              LT1959, Amsterdam, Netherlands, August 2008.

              <\/li>\n
            37. Yuki Terakawa, Nobuhiko Yokoshi, Kenji Kamide, Daisuke Yamamoto<\/em><\/strong>, and Susumu Kurihara
              Quantum fluctuations on a bosonic Abrikosov lattice in bilayer system
              The 5th 21st century COE symposium on Physics of Self-organization System: Self-organization Phenomena in Condensed Matter
              M-15, Waseda University, September 2007.

              <\/li>\n
            38. Daisuke Yamamoto <\/em><\/strong>and Susumu Kurihara
              Pseudospin Representation of Constrained Electron Operators in the Two-Dimensional t-J Model
              The 5th 21st century COE symposium on Physics of Self-organization System: Self-organization Phenomena in Condensed Matter
              RA-13, Waseda University, September 2007.

              <\/li>\n
            39. Daisuke Yamamoto <\/em><\/strong>and Susumu Kurihara
              Pseudospin representation of the two-dimentional t-J model
              International Conference on Strongly Correlated Electron Systems (SCES\u201907)
              III-69, Houston, USA, May 2007.

              <\/li>\n
            40. Daisuke Yamamoto<\/em><\/strong> and Susumu Kurihara
              Exact transformation for spin-charge separation of t-J model without constraints
              The 4th 21st century COE symposium on Physics of Self-organization System: Self-organization Phenomena in Condensed Matter
              CM-22, Waseda University, September 2006. <\/li>\n<\/ol>\n<\/div><\/details><\/div>\n
              2018\u5e74\u4ee5\u524d\uff08\u56fd\u5185, \u53e3\u982d\uff09 <\/summary>
              \n
                \n
              1. \u5c71\u672c\u5927\u8f14<\/strong>
                \u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53\u306e\u5f37\u78c1\u5834\u4e2d\u91cf\u5b50\u76f8\u56f3\u3068\u6700\u8fd1\u306e\u7406\u8ad6\u30fb\u5b9f\u9a13\u306e\u9032\u5c55
                \u7b2c1\u56de\u30b9\u30d4\u30f3\u7cfb\u7269\u7406\u7814\u7a76\u4f1a
                \u5206\u5b50\u30d5\u30a9\u30c8\u30b5\u30a4\u30a8\u30f3\u30b9\u7814\u7a76\u30bb\u30f3\u30bf\u30fc\u3001\u795e\u6238\u5927\u5b66\u30012018\u5e7411\u6708

                <\/li>\n
              2. \u5c71\u672c\u5927\u8f14<\/strong>, Giacomo Marmorimi, \u7530\u7551\u96c5\u535a, \u5742\u5009\u548c\u6a39, \u6bb5\u4e0b\u4e00\u5e73
                \u6a2a\u78c1\u5834\u4e2d\u306e\u5bb9\u6613\u8ef8\u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53\u306b\u304a\u3051\u308b\u91cf\u5b50\u63fa\u3089\u304e\u8a98\u8d77\u518d\u914d\u5411\u8ee2\u79fb\u30682\u6bb5\u968e\u71b1\u7684\u878d\u89e3\u8ee2\u79fb
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2018\u5e74\u79cb\u5b63\u5927\u4f1a
                \u9818\u57df3, 10pC201-9\u3001\u540c\u5fd7\u793e\u5927\u5b66\u30012018\u5e749\u6708

                <\/li>\n
              3. \u5ddd\u53e3\u6052, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                \u30d5\u30e9\u30c3\u30c8\u30d0\u30f3\u30c9\u4e2d\u306e\u6975\u4f4e\u6e29\u30dc\u30fc\u30b9\u539f\u5b50\u6c17\u4f53\u306b\u304a\u3051\u308b\u8d85\u56fa\u4f53\u72b6\u614b
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2018\u5e74\u79cb\u5b63\u5927\u4f1a
                \u9818\u57df1, 9aB102-8\u3001\u540c\u5fd7\u793e\u5927\u5b66\u30012018\u5e749\u6708
                \u5b66\u751f\u512a\u79c0\u767a\u8868\u8cde\u53d7\u8cde\uff08\u5ddd\u53e3\u6052\uff09<\/strong>

                <\/li>\n
              4. \u5c71\u672c\u5927\u8f14<\/strong>, \u4e2d\u60c7
                \u91cf\u5b50\u30b9\u30d4\u30f3J1-J2\u6a21\u578b\u306e\u78c1\u5316\u904e\u7a0b
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a
                \u9818\u57df3, 23aE26-5\u3001\u5ca9\u624b\u5927\u5b66\u30012017\u5e749\u6708

                <\/li>\n
              5. \u571f\u5c4b\u4fca\u4e8c, \u5c71\u672c\u5927\u8f14<\/strong>, \u65b0\u7530\u5b97\u571f
                BCS-BEC\u30af\u30ed\u30b9\u30aa\u30fc\u30d0\u30fc\u306b\u304a\u3051\u308b\u30d5\u30a7\u30eb\u30df\u539f\u5b50\u6c17\u4f53\u306e\u30d2\u30c3\u30b0\u30b9\u30e2\u30fc\u30c9\u306e\u632f\u308b\u821e\u3044II
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a
                \u9818\u57df1, 22aA10-9\u3001\u5ca9\u624b\u5927\u5b66\u30012017\u5e749\u6708

                <\/li>\n
              6. \u5c71\u672c\u5927\u8f14<\/strong>, \u4e0a\u7530\u5b8f, \u6bb5\u4e0b\u4e00\u5e73, Giacomo Marmorini, \u6843\u4e95\u52c9, \u4e0b\u5ddd\u7d71\u4e45\u6717
                \u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53\u306b\u304a\u3051\u308b\u5e0c\u8584\u30de\u30b0\u30ce\u30f3\u306eBose\u51dd\u7e2e\u3068\u78c1\u6c17\u79e9\u5e8f
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c72\u56de\u5e74\u6b21\u5927\u4f1a
                \u9818\u57df3, 20pC31-5\u3001\u5927\u962a\u5927\u5b66\u30012017\u5e743\u6708

                <\/li>\n
              7. \u571f\u5c4b\u4fca\u4e8c, \u5c71\u672c\u5927\u8f14<\/strong>, \u65b0\u7530\u5b97\u571f
                BCS-BEC\u30af\u30ed\u30b9\u30aa\u30fc\u30d0\u30fc\u306b\u304a\u3051\u308b\u30d5\u30a7\u30eb\u30df\u539f\u5b50\u6c17\u4f53\u306e\u30d2\u30c3\u30b0\u30b9\u30e2\u30fc\u30c9\u306e\u632f\u308b\u821e\u3044
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c72\u56de\u5e74\u6b21\u5927\u4f1a
                \u9818\u57df1, 18aC24-6\u3001\u5927\u962a\u5927\u5b66\u30012017\u5e743\u6708

                <\/li>\n
              8. \u5c71\u672c\u5927\u8f14<\/strong>, Carlos A. R. S\u00e1 de Melo
                \u30b9\u30d4\u30f3\u8ecc\u9053\u76f8\u4e92\u4f5c\u7528\u3059\u308bBose\u539f\u5b50\u6c17\u4f53\u306eMott\u7d76\u7e01\u4f53\u8ee2\u79fb\u3068\u91cf\u5b50\u76f8
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2016\u5e74\u79cb\u5b63\u5927\u4f1a
                \u9818\u57df1, 13aKJ-5\u3001\u91d1\u6ca2\u5927\u5b66\u30012016\u5e749\u6708

                <\/li>\n
              9. \u5c71\u672c\u5927\u8f14<\/strong>
                \u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u4e09\u89d2\u683c\u5b50\u78c1\u6027\u4f53\u306e\u78c1\u5316\u904e\u7a0b\u3068\u65b0\u5947\u91cf\u5b50\u76f8\u8ee2\u79fb\u306e\u7814\u7a76
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c71\u56de\u5e74\u6b21\u5927\u4f1a
                \u82e5\u624b\u5968\u52b1\u8cde\u53d7\u8cde\u8b1b\u6f14\u3001\u6771\u5317\u5b66\u9662\u5927\u5b66\u30012016\u5e743\u6708

                <\/li>\n
              10. \u5c71\u672c\u5927\u8f14<\/strong>, \u6817\u539f\u9032, \u4e2d\u60c7
                \u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8Bose-Hubbard\u7cfb\u306e\u591a\u6210\u5206Schwinger-boson\u8868\u793a\u3068\u91cf\u5b50\u76f8
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2015\u5e74\u79cb\u5b63\u5927\u4f1a
                16pBA-6\u3001\u95a2\u897f\u5b66\u9662\u30012015\u5e749\u6708

                <\/li>\n
              11. \u5c71\u672c\u5927\u8f14<\/strong>
                \u91cf\u5b50\u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u78c1\u6027\u7d76\u7e01\u4f53\u306e\u5fae\u8996\u7684\u89e3\u6790\u3068\u91cf\u5b50\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3
                \u57fa\u7814\u7814\u7a76\u4f1a\u300e\u91cf\u5b50\u5236\u5fa1\u6280\u8853\u306e\u767a\u5c55\u306b\u3088\u308a\u62d3\u304b\u308c\u308b\u91cf\u5b50\u60c5\u5831\u306e\u65b0\u6642\u4ee3\u300f
                \u4e00\u822c\u8b1b\u6f14\u3001\u4eac\u5927\u57fa\u7814\u30012015\u5e747\u6708

                <\/li>\n
              12. \u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u5897\u7530\u5553\u4ecb\uff0c\u6817\u539f\u9032
                \u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8Bose\u539f\u5b50\u6c17\u4f53\u306e\u91cf\u5b50\u76f8
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c70\u56de\u5e74\u6b21\u5927\u4f1a
                21aAG-1\u3001\u65e9\u7a32\u7530\u5927\u5b66\u30012015\u5e743\u6708

                <\/li>\n
              13. \u5c71\u672c\u5927\u8f14<\/strong>\uff0cGiacomo Marmorini\uff0c\u6bb5\u4e0b\u4e00\u5e73
                \u5c64\u72b6\u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53\u306e \u91cf\u5b50\u76f8\u8ee2\u79fb\u3068\u78c1\u5316\u904e\u7a0b
                \u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u7814\u7a76\u4f1a
                9-8\u3001\u798f\u4e95\u5927\u5b66\u30012015\u5e741\u6708

                <\/li>\n
              14. \u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u5897\u7530\u5553\u4ecb\uff0c\u6817\u539f\u9032
                \u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u3057\u305f\u30db\u30c3\u30d4\u30f3\u30b0\u3092\u6301\u3064\u5149\u683c\u5b50Bose\u7cfb\u306b\u304a\u3051\u308b\u91cf\u5b50\u7121\u79e9\u5e8f\u76f8\u306e\u53ef\u80fd\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2014\u5e74\u79cb\u5b63\u5927\u4f1a
                8aAW-6\u3001\u4e2d\u90e8\u5927\u5b66\u30012014\u5e749\u6708

                <\/li>\n
              15. \u5897\u7530\u5553\u4ecb, \u6817\u539f\u9032, \u5c71\u672c\u5927\u8f14<\/strong>
                flavor-wave\u5c55\u958b\u6cd5\u3092\u7528\u3044\u305fsoftcore Bose-Hubbard\u6a21\u578b\u306e\u89e3\u6790
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a2014\u5e74\u79cb\u5b63\u5927\u4f1a
                8aAW-5\u3001\u4e2d\u90e8\u5927\u5b66\u30012014\u5e749\u6708

                <\/li>\n
              16. \u5c71\u672c\u5927\u8f14<\/strong>\uff0cGiacomo Marmorini\uff0c\u6bb5\u4e0b\u4e00\u5e73
                \u4e09\u89d2\u683c\u5b50\u4e0a\u53cd\u5f37\u78c1\u6027\u30b9\u30d4\u30f3\u7cfb\u306e\u78c1\u5834\u4e2d\u91cf\u5b50\u76f8\u56f3:Ba3CoSb2O9\u306e\u78c1\u5316\u904e\u7a0b
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c69\u56de\u5e74\u6b21\u5927\u4f1a
                30aAF-8\u3001\u6771\u6d77\u5927\u5b66\u30012014\u5e743\u6708

                <\/li>\n
              17. \u52a0\u85e4\u5eb7\u4e4b\uff0c\u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u6bb5\u4e0b\u4e00\u5e73
                \u4e8c\u6210\u5206\u30dc\u30fc\u30ba\u30fb\u30cf\u30d0\u30fc\u30c9\u6a21\u578b\u306e\u91cf\u5b50\u4e09\u91cd\u81e8\u754c\u70b9\u8fd1\u508d\u306e\u81e8\u754c\u73fe\u8c61
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c69\u56de\u5e74\u6b21\u5927\u4f1a
                27aCF-1\u3001\u6771\u6d77\u5927\u5b66\u30012014\u5e743\u6708

                <\/li>\n
              18. \u6bb5\u4e0b\u4e00\u5e73\uff0c\u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u52a0\u85e4\u5eb7\u4e4b
                \u4e0d\u9023\u7d9a\u30e2\u30c3\u30c8\u7d76\u7e01\u4f53\u76f8\u8ee2\u79fb\u8fd1\u508d\u306b\u304a\u3051\u308b\u8d85\u6d41\u52d5\u30dc\u30fc\u30b9\u6df7\u5408\u6c17\u4f53\u306e\u660e\u7684\u6697\u30bd\u30ea\u30c8\u30f3\u3068\u6d41\u308c\u306e\u4f4d\u76f8\u7279\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c69\u56de\u5e74\u6b21\u5927\u4f1a
                27aCF-2\u3001\u6771\u6d77\u5927\u5b66\u30012014\u5e743\u6708

                <\/li>\n
              19. \u6771\u5927\u5fb3\uff0c\u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u6817\u539f\u9032
                \u4e8c\u6b21\u5143\u5149\u8d85\u683c\u5b50\u306b\u304a\u3051\u308bBEC\u306e\u8d85\u6d41\u52d5\u5b89\u5b9a\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c69\u56de\u5e74\u6b21\u5927\u4f1a
                27aCF-5\u3001\u6771\u6d77\u5927\u5b66\u30012014\u5e743\u6708

                <\/li>\n
              20. \u4e2d\u6751\u76f4\u4eba\uff0c\u6817\u539f\u9032\uff0c\u5c71\u672c\u5927\u8f14 <\/strong>
                \u5149\u683c\u5b50\u4e2d\u306b\u304a\u3051\u308b\u8d85\u6d41\u52d5\u30d5\u30a7\u30eb\u30df\u6df7\u5408\u6c17\u4f53\u306eFFLO\u76f8\u3068\u64ec\u30b9\u30d4\u30f3\u5f37\u78c1\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c69\u56de\u5e74\u6b21\u5927\u4f1a
                27pCF-12\u3001\u6771\u6d77\u5927\u5b66\u30012014\u5e743\u6708

                <\/li>\n
              21. \u5c71\u672c\u5927\u8f14<\/strong>\uff0cGiacomo Marmorini, \u6bb5\u4e0b\u4e00\u5e73
                \u4e09\u89d2\u683c\u5b50\u4e0a\u30b9\u30d4\u30f3-1\/2XXZ\u6a21\u578b\u306e\u78c1\u5834\u4e2d\u91cf\u5b50\u76f8\u56f3
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                25aKH-12\u3001\u5fb3\u5cf6\u5927\u5b66\u30012013\u5e749\u6708

                <\/li>\n
              22. \u5c71\u6751\u5b8f\u6a39\uff0c\u5c71\u672c\u5927\u8f14 <\/strong>
                \u5f31\u7d50\u5408\u8d85\u6d41\u52d5\u30d5\u30a7\u30eb\u30df\u6c17\u4f53\u306e\u52d5\u7684\u4e0d\u5b89\u5b9a\u5316
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                25aBA-1\u3001\u5fb3\u5cf6\u5927\u5b66\u30012013\u5e749\u6708

                <\/li>\n
              23. \u5897\u7530\u5553\u4ecb\uff0c\u5c71\u672c\u5927\u8f14<\/strong>
                \u5468\u671f\u30a2\u30f3\u30c0\u30fc\u30bd\u30f3\u6a21\u578b\u306b\u304a\u3051\u308b\u8ecc\u9053\u9593\u30da\u30a2\u30ea\u30f3\u30b0\u8d85\u4f1d\u5c0e\u3068\u53cd\u5f37\u78c1\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c68\u56de\u5e74\u6b21\u5927\u4f1a
                28pXZE-6\u3001\u5e83\u5cf6\u5927\u5b66\u30012013\u5e743\u6708

                <\/li>\n
              24. \u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u5c3e\u5d0e\u525b\uff0cCarlos A. R. S\u00e1 de Melo\uff0c\u6bb5\u4e0b\u4e00\u5e73
                \u5149\u683c\u5b50\u4e2d\u306eBose\u6df7\u5408\u6c17\u4f53\u306b\u304a\u3051\u308b\u8d85\u6d41\u52d5-Mott\u7d76\u7e01\u4f53\u4e00\u6b21\u8ee2\u79fb\u3068\u5c65\u6b74\u73fe\u8c61
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c68\u56de\u5e74\u6b21\u5927\u4f1a
                29aEE-1\u3001\u5e83\u5cf6\u5927\u5b66\u30012013\u5e743\u6708

                <\/li>\n
              25. \u5c71\u672c\u5927\u8f14<\/strong>, \u6bb5\u4e0b\u4e00\u5e73
                \u30b9\u30d4\u30f3\u4e8c\u91cf\u4f53\u5316\u5408\u7269\u306b\u304a\u3051\u308b\u30de\u30b0\u30ce\u30f3\u8d85\u56fa\u4f53\u76f8\u3068\u7570\u5e38\u306a\u5c65\u6b74\u73fe\u8c61
                \u57fa\u7814\u7814\u7a76\u4f1a\u300c\u91cf\u5b50\u30b9\u30d4\u30f3\u7cfb\u306e\u7269\u7406\u300d
                PS-A15\u3001\u4eac\u5927\u57fa\u7814\u30012012\u5e7411\u6708

                <\/li>\n
              26. \u4f50\u85e4\u611b\uff0c\u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u571f\u5c4b\u4fca\u4e8c\uff0c\u4e8c\u56fd\u5fb9\u90ce
                \u30ab\u30b4\u30e1\u5149\u5b66\u683c\u5b50\u4e2d\u306b\u304a\u3051\u308b\u30d5\u30a7\u30eb\u30df\u6c17\u4f53\u306e\u8d85\u6d41\u52d5
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                21aAL-5\u3001\u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66\u30012012\u5e749\u6708

                <\/li>\n
              27. \u6df1\u702c\u667a\u7d00\uff0c\u571f\u5c4b\u4fca\u4e8c\uff0c\u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u4e8c\u56fd\u5fb9\u90ce
                \u4e09\u89d2\u5149\u5b66\u683c\u5b50\u4e2d\u306e\u30d5\u30a7\u30eb\u30df\u8d85\u6d41\u4f53\u306b\u304a\u3051\u308b\u30ae\u30e3\u30c3\u30d7\u30ec\u30b9\u8d85\u6d41\u52d5\u306e\u53ef\u80fd\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                21aAL-3\u3001\u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66\u30012012\u5e749\u6708

                <\/li>\n
              28. \u5c71\u672c\u5927\u8f14 <\/strong>
                \u4e09\u89d2\u5149\u683c\u5b50\u4e2d\u306e\u7570\u7a2eFermi\u7c92\u5b50\u6df7\u5408\u6c17\u4f53\u306e\u91cf\u5b50\u76f8
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                21aAL-2\u3001\u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66\u30012012\u5e749\u6708

                <\/li>\n
              29. \u5c71\u6751\u5b8f\u6a39\uff0c\u5c71\u672c\u5927\u8f14<\/strong>
                \u8d85\u6d41\u52d5\u30d5\u30a7\u30eb\u30df\u6c17\u4f53\u306b\u304a\u3051\u308b\u96c6\u56e3\u52b1\u8d77\u3068\u5b89\u5b9a\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                21aAL-1\u3001\u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66\u30012012\u5e749\u6708

                <\/li>\n
              30. \u5897\u7530\u5553\u4ecb\uff0c\u5c71\u672c\u5927\u8f14<\/strong>
                \u91cd\u3044\u96fb\u5b50\u7cfb\u306b\u304a\u3051\u308bs\u6ce2\u8d85\u4f1d\u5c0e
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                20pGB-2\u3001\u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66\u30012012\u5e749\u6708

                <\/li>\n
              31. \u5c71\u672c \u5927\u8f14<\/strong>, \u6bb5\u4e0b \u4e00\u5e73
                \u30b9\u30d4\u30f3\u4e8c\u91cf\u4f53\u5316\u5408\u7269\u306b\u304a\u3051\u308b\u8d85\u56fa\u4f53\u76f8\u3068\u7570\u5e38\u306a\u5c65\u6b74\u73fe\u8c61
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                20pAC-11\u3001\u6a2a\u6d5c\u56fd\u7acb\u5927\u5b66\u30012012\u5e749\u6708

                <\/li>\n
              32. \u516b\u6728\u5ead\u6dbc\u5e73\uff0c\u5c71\u672c\u5927\u8f14<\/strong>\uff0c\u6bb5\u4e0b\u4e00\u5e73
                \u30dc\u30fc\u30b9\u30fb\u30cf\u30d0\u30fc\u30c9\u6a21\u578b\u306b\u304a\u3051\u308b\u8d85\u6d41\u52d5\u81e8\u754c\u901f\u5ea6\u306e\u5909\u5206\u30e2\u30f3\u30c6\u30ab\u30eb\u30ed\u6cd5\u306b\u3088\u308b\u89e3\u6790
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c67\u56de\u5e74\u6b21\u5927\u4f1a
                25aBE-5\u3001\u95a2\u897f\u5b66\u9662\u5927\u5b66\u30012012\u5e743\u6708

                <\/li>\n
              33. \u5c71\u672c \u5927\u8f14<\/strong>, \u6bb5\u4e0b \u4e00\u5e73
                Bose-Hubbard\u6a21\u578b\u306e\u8d85\u56fa\u4f53\u76f8\u767a\u73fe\u306b\u304a\u3051\u308b\u9577\u8ddd\u96e2\u76f8\u4e92\u4f5c\u7528\u306e\u5f79\u5272
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c67\u56de\u5e74\u6b21\u5927\u4f1a
                21pEE-2\u3001\u95a2\u897f\u5b66\u9662\u5927\u5b66\u30012012\u5e743\u6708

                <\/li>\n
              34. \u5c71\u672c \u5927\u8f14<\/strong>, \u6bb5\u4e0b \u4e00\u5e73, Carlos A. R. S\u00e1 de Melo
                \u5149\u5b66\u683c\u5b50\u4e2dBose \u6c17\u4f53\u306e\u30ea\u30a8\u30f3\u30c8\u30e9\u30f3\u30c8\u4e00\u6b21\u76f8\u8ee2\u79fb\u306b\u304a\u3051\u308b\u7570\u5e38\u306a\u5c65\u6b74\u73fe\u8c61
                Ultracold Gases: Superfluidity and Strong Correlations (USS-2012)
                B-3\u3001\u6771\u4eac\u7406\u79d1\u5927\u5b66\u30012012\u5e741\u6708

                <\/li>\n
              35. \u5c71\u672c \u5927\u8f14<\/strong>, \u6bb5\u4e0b \u4e00\u5e73
                \u5149\u683c\u5b50\u4e2d\u306eBose\u6c17\u4f53\u306b\u304a\u3051\u308b\u7570\u5e38\u306a\u5c65\u6b74\u73fe\u8c61
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                21pEE-2\u3001\u5bcc\u5c71\u5927\u5b66\u30012011\u5e749\u6708

                <\/li>\n
              36. \u5c71\u672c \u5927\u8f14<\/strong>, \u6bb5\u4e0b \u4e00\u5e73, Carlos A. R. S\u00e1 de Melo
                \u4e09\u89d2\u5149\u683c\u5b50\u4e2d\u306e\u53cc\u6975\u5b50\u76f8\u4e92\u4f5c\u7528\u3092\u6301\u3064\u30dc\u30fc\u30b9\u6c17\u4f53\u306e\u91cf\u5b50\u76f8
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                26aRD-6\u3001\u5927\u962a\u5e9c\u7acb\u5927\u5b66\u30012010\u5e749\u6708

                <\/li>\n
              37. \u5c71\u672c \u5927\u8f14<\/strong>, \u6bb5\u4e0b \u4e00\u5e73
                \u62e1\u5f35Bose-Hubbard\u6a21\u578b\u306b\u304a\u3051\u308b\u30ab\u30ec\u30f3\u30c8\u306b\u8a98\u8d77\u3055\u308c\u305f\u8d85\u56fa\u4f53\u76f8
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c65\u56de\u5e74\u6b21\u5927\u4f1a
                21aTB-3\u3001\u5ca1\u5c71\u5927\u5b66\u30012010\u5e743\u6708

                <\/li>\n
              38. \u6e6f\u524d \u6176\u5927\uff0c\u5c71\u672c \u5927\u8f14<\/strong>\uff0c\u6817\u539f \u9032\uff0c\u571f\u5c4b \u4fca\u4e8c
                \u5149\u683c\u5b50\u4e2d\u306b\u304a\u3051\u308b\u30a4\u30f3\u30d0\u30e9\u30f3\u30b9\u30d5\u30a7\u30eb\u30df\u6c17\u4f53\u306e\u5b89\u5b9a\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                26aZE-5\u3001\u718a\u672c\u5927\u5b66\u30012009\u5e749\u6708

                <\/li>\n
              39. \u6e6f\u524d \u6176\u5927, \u5c71\u672c \u5927\u8f14<\/strong>, \u6bb5\u4e0b \u4e00\u5e73, \u4f59\u8d8a \u4f38\u5f66, \u571f\u5c4b \u4fca\u4e8c
                \u4f4e\u6b21\u5143\u5149\u5b66\u683c\u5b50\u4e2d\u306b\u304a\u3051\u308b\u8d85\u6d41\u52d5\u30d5\u30a7\u30eb\u30df\u6c17\u4f53\u306e\u81e8\u754c\u901f\u5ea6
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c64\u56de\u5e74\u6b21\u5927\u4f1a
                28aSL-1\u3001\u7acb\u6559\u5927\u5b66\u30012009\u5e743\u6708

                <\/li>\n
              40. \u5c71\u672c \u5927\u8f14<\/strong>, \u6817\u539f \u9032
                \u30b9\u30d4\u30f3\u7cfb\u306b\u95a2\u3059\u308b\u76f8\u95a2\u30af\u30e9\u30b9\u30bf\u30fc\u5e73\u5747\u5834\u6cd5
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c64\u56de\u5e74\u6b21\u5927\u4f1a
                27pTJ-17\u3001\u7acb\u6559\u5927\u5b66\u30012009\u5e743\u6708

                <\/li>\n
              41. \u5e02\u539f \u907c\u5b50, \u6bb5\u4e0b \u4e00\u5e73, \u5c71\u672c \u5927\u8f14<\/strong>, \u4e8c\u56fd \u5fb9\u90ce
                \u4e8c\u91cd\u4e95\u6238\u578b\u30dd\u30c6\u30f3\u30b7\u30e3\u30eb\u4e2dBEC\u306e\u5b89\u5b9a\u6027
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u79cb\u5b63\u5927\u4f1a
                22aZD-1\u3001\u5ca9\u624b\u5927\u5b66\u30012008\u5e749\u6708

                <\/li>\n
              42. \u5c71\u672c \u5927\u8f14<\/strong>, \u6817\u539f \u9032
                \u78c1\u5834\u4e2d\u30cf\u30a4\u30bc\u30f3\u30d9\u30eb\u30b0\u5f37\u78c1\u6027\u4f53\u306b\u304a\u3051\u308b\u30b0\u30ea\u30fc\u30f3\u95a2\u6570\u6cd5
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c62\u56de\u5e74\u6b21\u5927\u4f1a
                24pTL-5\u3001\u5317\u6d77\u9053\u5927\u5b66\u30012007\u5e749\u6708

                <\/li>\n
              43. \u5c71\u672c \u5927\u8f14<\/strong>, \u6817\u539f \u9032
                \u64ec\u30b9\u30d4\u30f3\u8868\u793a\u3092\u7528\u3044\u305ft-J\u30e2\u30c7\u30eb\u306b\u304a\u3051\u308b\u53cd\u5f37\u78c1\u6027\u79e9\u5e8f
                \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u6625\u5b63\u5927\u4f1a
                18pXE-3\u3001\u9e7f\u5150\u5cf6\u5927\u5b66\u30012007\u5e743\u6708<\/li>\n<\/ol>\n<\/div><\/details><\/div>\n
                2018\u5e74\u4ee5\u524d\uff08\u56fd\u5185, \u30dd\u30b9\u30bf\u30fc\uff09 <\/summary>
                \n
                  \n
                1. \u5742\u5009\u548c\u6a39\u3001\u5c71\u672c\u5927\u8f14<\/strong>\u3001\u53e4\u5ddd\u4fe1\u592b
                  \u6b21\u8fd1\u63a5\u76f8\u4e92\u4f5c\u7528\u3092\u542b\u3080\u4e09\u89d2\u683c\u5b50\u53cd\u5f37\u78c1\u6027\u4f53\u306e\u76f8\u8ee2\u79fb\u73fe\u8c61
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2018\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df11, 12aPS-4\u3001\u540c\u5fd7\u793e\u5927\u5b66\u30012018\u5e749\u6708

                  <\/li>\n
                2. \u9234\u6728\u5343\u5c0b, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                  S=1\u4e09\u89d2\u683c\u5b50bilinear-biquadratic model\u306b\u304a\u3051\u308b\u6709\u9650\u78c1\u5834\u4e0b\u3067\u306e\u91cf\u5b50\u76f8\u56f3
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2018\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df3, 9aPS-75\u3001\u540c\u5fd7\u793e\u5927\u5b66\u30012018\u5e749\u6708

                  <\/li>\n
                3. \u91d1\u5742\u62d3\u54c9, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                  \u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u3057\u305fS=1\/2\u53cd\u5f37\u78c1\u6027\u30b9\u30d4\u30f3\u30c0\u30a4\u30de\u30fc\u30e2\u30c7\u30eb\u306e\u91cf\u5b50\u78c1\u6c17\u76f8\u56f3
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2018\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df3, 9aPS-74\u3001\u540c\u5fd7\u793e\u5927\u5b66\u30012018\u5e749\u6708

                  <\/li>\n
                4. \u5c0f\u6797\u8ce2\u4e5f, \u5ca1\u90e8\u73b2\u592e\u54c9, \u5c71\u672c\u5927\u8f14<\/strong>, \u671b\u6708\u7dad\u4eba
                  \u8ca0\u306e\u71b1\u81a8\u5f35\u3092\u793a\u3059\u9006\u30da\u30ed\u30d6\u30b9\u30ab\u30a4\u30c8\u578bMn\u7a92\u5316\u7269\u306e\u78c1\u6c17\u79e9\u5e8f\u3068\u76f8\u8ee2\u79fb\u306e\u7406\u8ad6\u7814\u7a76
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u5e74\u6b21\u5927\u4f1a
                  \u9818\u57df3, 22pPSA-24\u3001\u6771\u4eac\u7406\u79d1\u5927\u5b66\u30012018\u5e743\u6708

                  <\/li>\n
                5. S. Okazaki, D. Yamamoto<\/strong>, M. Tabata, N. Furukawa
                  Unbinding of fractional-vortex pairs in the classical XY model with optical Kagome lattice
                  CREST\u300c\u91cf\u5b50\u72b6\u614b\u306e\u9ad8\u5ea6\u306a\u5236\u5fa1\u306b\u57fa\u3065\u304f\u9769\u65b0\u7684\u91cf\u5b50\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c2\u56de\u516c\u958b\u30b7\u30f3\u30dd\u30b8\u30a6\u30e0
                  P20\u3001\u4eac\u90fd\u5927\u5b66\u30012017\u5e7412\u6708

                  <\/li>\n
                6. H. Kawaguchi, D. Yamamoto<\/strong>, N. Furukawa
                  Possible supersolids of ultracold Bose gases in an optical Lieb lattice
                  CREST\u300c\u91cf\u5b50\u72b6\u614b\u306e\u9ad8\u5ea6\u306a\u5236\u5fa1\u306b\u57fa\u3065\u304f\u9769\u65b0\u7684\u91cf\u5b50\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c2\u56de\u516c\u958b\u30b7\u30f3\u30dd\u30b8\u30a6\u30e0
                  P19\u3001\u4eac\u90fd\u5927\u5b66\u30012017\u5e7412\u6708

                  <\/li>\n
                7. D. Yamamoto<\/strong>, I. B. Spielman, C. A. R. S\u00e1 de Melo
                  Interacting ultracold Bose gases with synthetic spin-orbit coupling in an optical lattice
                  CREST\u300c\u91cf\u5b50\u72b6\u614b\u306e\u9ad8\u5ea6\u306a\u5236\u5fa1\u306b\u57fa\u3065\u304f\u9769\u65b0\u7684\u91cf\u5b50\u6280\u8853\u57fa\u76e4\u306e\u5275\u51fa\u300d\u7b2c2\u56de\u516c\u958b\u30b7\u30f3\u30dd\u30b8\u30a6\u30e0
                  P18\u3001\u4eac\u90fd\u5927\u5b66\u30012017\u5e7412\u6708

                  <\/li>\n
                8. \u5f8c\u85e4\u614e\u5e73, \u6817\u539f\u9032, \u5c71\u672c\u5927\u8f14<\/strong>
                  \u7a7a\u9593\u7570\u65b9\u7684\u4e8c\u6b21\u5143\u683c\u5b50\u306b\u304a\u3051\u308b\u4e0d\u6574\u5408\u30b9\u30d1\u30a4\u30e9\u30eb\u78c1\u6027\u76f8\u306e\u52d5\u7684\u5e73\u5747\u5834\u89e3\u6790
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a\u7b2c72\u56de\u5e74\u6b21\u5927\u4f1a
                  \u9818\u57df3, 17pC-PS-18\u3001\u5927\u962a\u5927\u5b66\u30012017\u5e743\u6708

                  <\/li>\n
                9. \u5ddd\u53e3\u6052, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                  \u30ea\u30fc\u30d7\u683c\u5b50\u30d5\u30e9\u30c3\u30c8\u30d0\u30f3\u30c9\u4e2d\u306e\u6975\u4f4e\u6e29\u30dc\u30fc\u30b9\u539f\u5b50\u6c17\u4f53\u306e\u8d85\u56fa\u4f53\u72b6\u614b
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df11, 24aPS-27\u3001\u5ca9\u624b\u5927\u5b66\u30012017\u5e749\u6708

                  <\/li>\n
                10. \u5ca1\ufa11\u7fd4, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                  \u30ab\u30b4\u30e1\u683c\u5b50\u4e0a\u53cd\u5f37\u78c1\u6027XY\u30e2\u30c7\u30eb\u306b\u304a\u3051\u308b\u5206\u6570\u6e26\u76f8\u8ee2\u79fb
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df11, 24aPS-7\u3001\u5ca9\u624b\u5927\u5b66\u30012017\u5e749\u6708

                  <\/li>\n
                11. \u7530\u7551\u96c5\u535a, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                  \u7a7a\u9593\u7570\u65b9\u6027\u3092\u6301\u3064\u78c1\u5834\u4e2d\u4e09\u89d2\u683c\u5b50\u30cf\u30a4\u30bc\u30f3\u30d9\u30eb\u30b0\u6a21\u578b\u306e\u30e2\u30f3\u30c6\u30ab\u30eb\u30ed\u30b7\u30df\u30e5\u30ec\u30fc\u30b7\u30e7\u30f3
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df3, 21aPS-49\u3001\u5ca9\u624b\u5927\u5b66\u30012017\u5e749\u6708

                  <\/li>\n
                12. \u91d1\u5742\u62d3\u54c9, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                  \u30b9\u30d4\u30f3\u30c0\u30a4\u30de\u30fc\u53cd\u5f37\u78c1\u6027\u4f53Ba2CoSi2O6Cl2\u306b\u304a\u3051\u308b\u5c40\u5728\u52b1\u8d77\u306b\u95a2\u3059\u308b\u7406\u8ad6\u7814\u7a76
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df3, 21aPS-73\u3001\u5ca9\u624b\u5927\u5b66\u30012017\u5e749\u6708

                  <\/li>\n
                13. \u9f4a\u6728\u96c4\u9ad8, \u5c71\u672c\u5927\u8f14<\/strong>, \u53e4\u5ddd\u4fe1\u592b
                  \u5bb9\u6613\u9762\u578bS=1\u30d5\u30e9\u30b9\u30c8\u30ec\u30fc\u30c8\u53cd\u5f37\u78c1\u6027\u4f53\u306e\u91cf\u5b50\u76f8\u8ee2\u79fb
                  \u65e5\u672c\u7269\u7406\u5b66\u4f1a2017\u5e74\u79cb\u5b63\u5927\u4f1a
                  \u9818\u57df3, 21aPS-46\u3001\u5ca9\u624b\u5927\u5b66\u30012017\u5e749\u6708<\/li>\n<\/ol>\n<\/div><\/details><\/div>\n<\/div>\n\n\n\n
                  \n
                  <\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"

                  \u6700\u8fd1\u306e\u51fa\u7248\u8ad6\u6587\u7b49 2018\u5e74\u4ee5\u524d Shunji Tsuchiya, Daisuke Yamamoto, Ryosuke Yoshii, and Muneto Nitta Hidden Charge-Conjugation […]<\/p>\n","protected":false},"author":1,"featured_media":100,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_coblocks_attr":"Arial,Arial","_coblocks_dimensions":"","_coblocks_responsive_height":"","_coblocks_accordion_ie_support":"","footnotes":""},"class_list":["post-138","page","type-page","status-publish","has-post-thumbnail","hentry"],"_links":{"self":[{"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/pages\/138","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/comments?post=138"}],"version-history":[{"count":229,"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/pages\/138\/revisions"}],"predecessor-version":[{"id":1885,"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/pages\/138\/revisions\/1885"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/media\/100"}],"wp:attachment":[{"href":"https:\/\/www.phys.chs.nihon-u.ac.jp\/yamamoto\/wp-json\/wp\/v2\/media?parent=138"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}