過去のセミナー
<12/2025>- 12月10日 (水)
- Mr. Hiroto Tanaka (Condensed Matter Theory Group)
- " Surface acoustic wave-driven valley current generation in intervalley coherent states"
<11/2025>
- 11月12日 (水)
- Mr. Musashi Kato (Condensed Matter Theory Group)
- " The effects of interactions on exceptional points in bosonic systems"
<10/2025>
- 10月29日 (水)
- Mr. Yuma Hirobe (Condensed Matter Theory Group)
- " Anomalous Scaling Laws for Quantum-Geometric Superfluid Weight"
- 10月15日 (水)
- Mr. Yuta Shigedomi (Condensed Matter Theory Group)
- " Liouvillian skin effects in two-dimensional electron systems"
<7/2025>
- 7月16日 (水)
- Mr. Kanta Kudo (Condensed Matter Theory Group)
- " Multipole fluctuation by quantum geometry"
<6/2025>
- 6月18日 (水)
- Dr. Indrasen Ghosh (Condensed Matter Theory Group)
- "Introduction to entanglement in the Sachdev-Ye-Kitaev model at Large-N"
- 6月4日 (水)
- Mr. Hiroto Tanaka (Condensed Matter Theory Group)
- "Linear and Nonlinear Optical Responses in Topological Superconductors: Quantum Geometry and Collective Mode"
<5/2025>
- 5月28日 (水)
- Mr. Naratip Nunchot (Condensed Matter Theory Group)
- "Interplay between Coulomb interaction and disorder in the superconducting diode effect"
- 5月14日 (水)
- Dr. Makoto Shimizu (Condensed Matter Theory Group)
- "Electronic and Magnetic Structures of UTe2"
<4/2025>
- 4月23日 (水)
- Mr. Shu Hamanaka (Condensed Matter Theory Group)
- "Exact Multifractal Dimensions of Non-Hermitian Skin Modes on a Cayley Tree"
- 4月9日 (水)
- Mr. Shin Kaneshiro (Condensed Matter Theory Group)
- "Symplectic-Amoeba formulation of the non-Bloch band theory for one-dimensional two-band systems"
<1/2025>
- 1月22日 (水)
- Dr. Rina Tazai (YITP)
- "Theoretical study on loop current phase and non-reciprocal transport in Kagome Superconductors"
- 1月15日 (水)
- Mr. Jun Oike (Condensed Matter Theory Group)
- "Nonlinear magnetoelectric effect under magnetic octupole order"
- 1月8日 (水)
- Mr. Ryuji Hakuno (Condensed Matter Theory Group)
- "Magnetism and superconductivity in the two sublattice periodic Anderson model for UTe2"
