Y. Matsumoto

collaborators

3 papers

cond-mat.str-el2026

Non-magnetic ground state in A $_{2}$ WCl $_{6}$ (A = Cs, Rb, K): A face-centered cubic system of spin-orbit-entangled $J$ = 2 states

T. Takayama, K. Ishii, S. Bette +10

Heavy transition metal compounds with strong spin-orbit coupling appeared as a platform for $d$ -electron multipolar physics. We report the electronic, magnetic, and structural prop…

cond-mat.str-el2025

Magnetic ground state of the dimer-based hexagonal perovskite Ba $_{3}$ ZnRu $_{2}$ O $_{9}$

S. Hayashida, H. Gretarsson, P. Puphal +7

We investigate the magnetic ground state of single crystals of the ruthenium-dimer-based hexagonal perovskite Ba $_{3}$ ZnRu $_{2}$ O $_{9}$ using magnetic susceptibility and resonant i…

cond-mat.supr-con2025

Interplay between Multipolar Order and Multipole-Induced Superconductivity in PrTi $_{2}$ Al $_{20}$

Akito Sakai, Yosuke Matsumoto, Mingxuan Fu +5

Multipolar moments entail a new route to tackle frontier problems in superconductivity (SC). A key progress in the search for multipolar SC is the discovery of Pr $T r_{2}$ Al $_{20}$ ($…

Non-magnetic ground state in A2​WCl6​ (A = Cs, Rb, K): A face-centered cubic system of spin-orbit-entangled J = 2 states

Magnetic ground state of the dimer-based hexagonal perovskite Ba3​ZnRu2​O9​

Interplay between Multipolar Order and Multipole-Induced Superconductivity in PrTi2​Al20​

Non-magnetic ground state in A $_{2}$ WCl $_{6}$ (A = Cs, Rb, K): A face-centered cubic system of spin-orbit-entangled $J$ = 2 states

Magnetic ground state of the dimer-based hexagonal perovskite Ba $_{3}$ ZnRu $_{2}$ O $_{9}$

Interplay between Multipolar Order and Multipole-Induced Superconductivity in PrTi $_{2}$ Al $_{20}$