M. Tsunekawa
Osaka University
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Featured researches published by M. Tsunekawa.
Journal of the Physical Society of Japan | 2005
S. Suga; Akira Sekiyama; S. Imada; A. Shigemoto; A. Yamasaki; M. Tsunekawa; Claudia Dallera; L. Braicovich; Tien Lin Lee; Osamu Sakai; Takao Ebihara; Yoshichika Onuki
By use of high-resolution soft X-rays, intrinsic temperature dependences of bulk Yb 4f photoelectron spectra were obtained for fractured surfaces of high-purity YbAl 3 single crystals. The spectra ...
Physical Review B | 2004
Akira Sekiyama; Shinya Kasai; M. Tsunekawa; Y. Ishida; M. Sing; Akinori Irizawa; A. Yamasaki; S. Imada; Takayuki Muro; Y. Saitoh; Y. Ōnuki; Tsuyoshi Kimura; Yoshinori Tokura; S. Suga
We report the Fermi surfaces of the superconductor
Physical Review Letters | 1996
T. Susaki; Akira Sekiyama; K. Kobayashi; T. Mizokawa; A. Fujimori; M. Tsunekawa; Takayuki Muro; Tomohiro Matsushita; S. Suga; H. Ishii; Takaaki Hanyu; Akio Kimura; Hirofumi Namatame; M. Taniguchi; Tsuneaki Miyahara; Fumitoshi Iga; M. Kasaya; Hisatomo Harima
{\mathrm{Sr}}_{2}{\mathrm{RuO}}_{4}
Physical Review Letters | 1996
T. Susaki; A. Sekiyama; K. Kobayashi; T. Mizokawa; A. Fujimori; M. Tsunekawa; Takayuki Muro; Tomohiro Matsushita; S. Suga; H. Ishii; Takaaki Hanyu; Akio Kimura; H. Namatame; M. Taniguchi; Tsuneaki Miyahara; Fumitoshi Iga; M. Kasaya; Hisatomo Harima
and the nonsuperconductor
Journal of the Physical Society of Japan | 1998
Shigemasa Suga; Akira Ochiai; Takashi Suzuki; H. Harada; Akira Sekiyama; Tomohiro Matsushita; Takeshi Iwasaki; Akio Kimura; M. Tsunekawa; Takayuki Muro; Shigenori Ueda; Hiroshi Daimon; S. Imada; Hirofumi Namatame; M. Taniguchi; Hiroyoshi Ishii; Tsuneaki Miyahara; Takaaki Hanyu; Atsushi Fujimori
{\mathrm{Sr}}_{1.8}{\mathrm{Ca}}_{0.2}{\mathrm{RuO}}_{4}
Journal of the Physical Society of Japan | 2005
A. Yamasaki; Akira Sekiyama; S. Imada; M. Tsunekawa; Claudia Dallera; L. Braicovich; Tien Lin Lee; Akira Ochiai; S. Suga
probed by bulk-sensitive high-energy angle-resolved photoemission. It is found that there is one square-shaped hole-like, one square-shaped electron-like, and one circle-shaped electron-like Fermi surface in both compounds. These results provide direct evidence for nesting instability giving rise to magnetic fluctuations. Our study clarifies that the electron correlation effects are changed with composition depending on the individual band.
Physical Review B | 2013
Martin Sperlich; Christian König; G. Güntherodt; A. Sekiyama; G. Funabashi; M. Tsunekawa; S. Imada; A. Shigemoto; K Okada; A. Higashiya; Makina Yabashi; Kenji Tamasaku; Tetsuya Ishikawa; V. Renken; T. Allmers; M. Donath; S. Suga
We have studied the low-energy electronic structure of a Kondo insulator YbB{sub 12} by high-resolution photoemission spectroscopy. A {open_quote}{open_quote}Kondo peak{close_quote}{close_quote} is observed {approximately}25 meV below the Fermi level, which agrees well with the Kondo temperature, whereas the gap at the Fermi level is found much smaller, indicating that the magnetic properties at higher temperatures (75 K) are indeed determined by the Kondo effect in spite of the gap formation at lower temperatures. A renormalized band picture is presented to describe the coexistence of the Kondo peak and the transport gap as well as the highly asymmetric line shape of the Kondo peak. {copyright} {ital 1996 The American Physical Society.}
Solid State Communications | 1997
M. Tsunekawa; S. Suga; A. Kimura; Tomohiro Matsushita; Takayuki Muro; S. Ueda; Hiroshi Daimon; S. Imada; Takeshi Nakatani; Y. Saitoh; T. Iwasaki; Akira Sekiyama; A. Fujimori; H. Ishii; Tsuneaki Miyahara; Takaaki Hanyu; Hirofumi Namatame; M. Taniguchi; E. Shigemasa; O. Sakai; Ryu Takayama; Rikio Settai; Hisashi Azuma; Yoshichika Onuki
We have studied the low-energy electronic structure of a Kondo insulator YbB{sub 12} by high-resolution photoemission spectroscopy. A {open_quote}{open_quote}Kondo peak{close_quote}{close_quote} is observed {approximately}25 meV below the Fermi level, which agrees well with the Kondo temperature, whereas the gap at the Fermi level is found much smaller, indicating that the magnetic properties at higher temperatures (75 K) are indeed determined by the Kondo effect in spite of the gap formation at lower temperatures. A renormalized band picture is presented to describe the coexistence of the Kondo peak and the transport gap as well as the highly asymmetric line shape of the Kondo peak. {copyright} {ital 1996 The American Physical Society.}
Journal of the Physical Society of Japan | 2005
A. Yamasaki; S. Imada; Akira Sekiyama; M. Tsunekawa; Claudia Dallera; L. Braicovich; Tien Lin Lee; H. Sugawara; Hideyuki Sato; Rikio Settai; Yoshichika Onuki; S. Suga
Clear changes of the Yb 4f photoemission spectra with temperature are observed in Yb 4 As 3 by high resolution photoemission spectroscopy. The photoemission intensity is very low at the Fermi level and decreases as the temperature is lowered in accord with the narrowing of the 4f spectra. Bulk and surface contributions are deconvoluted in the 4f 13 final state spectra. In comparison with the corresponding results in Yb 4 (As 1- x Sb x ) 3 , the spectral changes of Yb 4 As 3 with temperature are confirmed to be beyond simple thermal broadening effects and related to the charge ordering effects. Although the change from the charge ordering temperature ( T t ) down to about T t /2 is consistent with a theoretical prediction, the change below it is rather unusual and may be ascribed to the incompleteness of the charge ordering effect. Spectral changes with Yb 4 Sb 3 -substitution are qualitatively discussed.
Journal of Experimental and Theoretical Physics | 2008
E. E. Kokorina; E. Z. Kuchinskii; I. A. Nekrasov; Z. V. Pchelkina; M. V. Sadovskii; Akira Sekiyama; S. Suga; M. Tsunekawa
The bulk and surface electronic structures of Sm 4 As 3 have been investigated by hard and soft X-ray photoemission spectroscopies (PESs). PES with a wide range of photon energies ( h νs) between 220 and 2450 eV demonstrates the absence of valence mixing in both high- and low-temperature phases, that is, the valence of Sm ions is definitely trivalent in the bulk and divalent on the surface. Atomic multiplet calculations taking into account the bulk and surface spectral weights at each h ν well reproduce the experimental valence band PES and Sm 3 d core-level spectra, supporting the valence difference between bulk and surface in Sm 4 As 3 .