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states in the electronic structure of the intermediate-valence superconductor CeIr
藤森 伸一; 川崎 郁斗; 竹田 幸治; 山上 浩志; 雀部 矩正*; 佐藤 芳樹*; 清水 悠晴*; 仲村 愛*; Maruya, A.*; 本間 佳哉*; et al.
Electronic Structure (Internet), 5(4), p.045009_1 - 045009_7, 2023/11
The electronic structure of the 
-based superconductor 
was studied by photoelectron spectroscopy. The energy distribution of the 
state was revealed by the 
resonant photoelectron spectroscopy. The state was mostly distributed in the vicinity of the Fermi energy, suggesting the itinerant character of the state. The contribution of the state to the density of states (DOS) at the Fermi energy was estimated to be nearly half of that of the
states, implying that the state has aconsiderable contribution to the DOS at the Fermi energy. The 
core-level and X-ray absorption spectra were analyzed based on a single-impurity Anderson model. The number of the state in the ground state was estimated to be 0.8-0.9, which is much larger than the values obtained in the previous studies (i.e., 0-0.4).
Si in paramagnetic phase; Three-dimensional angle resolved photoelectron spectroscopy study藤森 伸一; 竹田 幸治; 山上 浩志; 山本 悦嗣; 芳賀 芳範
Electronic Structure (Internet), 3(2), p.024008_1 - 024008_8, 2021/06
The three-dimensional (3D) electronic structure of the hidden order compound 
in a paramagnetic phase was revealed using a 3D angle-resolved photoelectron spectroscopy where the electronic structure of the entire Brillouin zone is obtained by scanning both incident photon energy and detection angles of photoelectrons. The quasi-particle bands with enhanced contribution from the 
state were observed near 
, formed by the hybridization with the 
states. The energy dispersion of the quasi-particle band is significantly depend on
, indicating that they inherently have a 3D nature. The band-structure calculation qualitatively explain the characteristic features of the band structure and Fermi surface although the electron correlation effect strongly renormalizes the quasi-particle bands. The 3D and strongly-correlated nature of the quasi-particle bands in is an essential ingredient for modeling its hidden-order transition.
