†Observation of Current-Induced Lattice Distortion in Spin–Orbit Coupled Iridium Oxide Ca5Ir3O12: K. Kadohiro, H. Hanate, M. Hayashida, T. Hasegawa, H. Nakao, Y. Okamoto, K. Miyazaki, S. Tsutsui and K. Matsuhira, J. Phys. Soc. Jpn. 94, 023601(1-4) (2025).
Optimal Carrier Concentration of Low-Temperature Thermoelectric Material M4SiTe4 (M = Ta, Nb) from First-Principles Calculations: G. Tomitaka, S. Kawano, Y. Okamoto and K. Matsuhira, J. Phys. Soc. Jpn. 94, 114705 (2025).
*Superconductivity in Hexagonal Zr6CoAl2-Type Zr6RuBi2 and Zr6FeBi2: K. Yuchi, D. Nishio-Hamane, K. Kojima, K. Moriyama, R. Okuma and Y. Okamoto, J. Phys. Soc. Jpn. 94, 013701(1-5) (2025).
*Superconductivity in Ternary Zirconium Telluride Zr6RuTe2: K. Yuchi, H. Matsumoto, D. Nishio-Hamane, K. Moriyama, K. Kojima, R. Okuma, J.-I. Yamaura and Y. Okamoto, J. Phys. Soc. Jpn. 94, 085001(1-2) (2025).
Anisotropic superconducting gap probed by Te125 NMR in noncentrosymmetric Sc6MTe2 (M = Fe, Co): K. Doi, H. Takei, Y. Shinoda, Y. Okamoto, D. Hirai, K. Takenaka, T. Matsushita, Y. Kobayashi and Y. Shimizu, Phys. Rev. B 111, 214502(1-7) (2025).
