Experimental determination of band structures of CeCoSi by an angle-resolved photoelectron spectroscopy
ORAL
Abstract
Strongly correlated electron systems exhibit various physical properties closely related to charge, spin, and orbital degrees of freedom; in f-electron systems, multipoles, which are combinations of spin and orbital degrees of freedom, play a major role. The centrosymmetric CeCoSi, which belongs to the non-symmorphic space group (P4/nmm), has attracted much attention from the viewpoint of the odd-parity multipoles below the phase transition temperature T0. Recently, a Ce 4f-driven antiferroquadrupolar order below T0 was proposed by a detailed study using single crystal samples, followed by a complete phase diagram and further clarification of the finite T0 ~12 K even at ambient pressure [1,2]. Subsequently, 59Co NMR revealed anomalies suggestive of quadrupolar order [3], and odd-parity multipole order was theoretically proposed [4]. However, a fundamental question has remained unsolved as to why the localized Ce 4f state is so sensitive to external pressure and why the T0 increases substantially. Here, we report the direct observation of the Fermi surfaces and electronic band dispersions of CeCoSi by angle-resolved photoelectron spectroscopy (ARPES) utilizing synchrotron radiation. The photon energy-dependent ARPES result shows that two- and three-dimensional Fermi surfaces coexist, being consistent with the result of the first-principles calculation. By the Ce 3d-4f resonant photoelectron spectroscopy and the high-resolution ARPES, Ce 4f level is found to be located quite close to the Fermi level (~10 meV), which explains why the pressure-sensitive feature of the phase transition.
[1] H. Tanida, Y. Muro, and T. Matsumura, J. Phys. Soc. Jpn. 87, 023705 (2018).
[2] H. Tanida, K. Mitsumoto, Y. Muro, T. Fukuhara, Y. Kawamura, A. Kondo, K. Kindo, Y. Matsumoto,T. Namiki, T. Kuwai, and T. Matsumura, J. Phys. Soc. Jpn. 88, 054716 (2019).
[3] M. Manago, H. Kotegawa, H. Tou, H. Harima, and H. Tanida, J. Phys. Soc. Jpn. 90, 023702 (2021).
[4] M. Yatsushiro, and S. Hayami, J. Phys. Soc. Jpn. 89, 013703 (2019).
[1] H. Tanida, Y. Muro, and T. Matsumura, J. Phys. Soc. Jpn. 87, 023705 (2018).
[2] H. Tanida, K. Mitsumoto, Y. Muro, T. Fukuhara, Y. Kawamura, A. Kondo, K. Kindo, Y. Matsumoto,T. Namiki, T. Kuwai, and T. Matsumura, J. Phys. Soc. Jpn. 88, 054716 (2019).
[3] M. Manago, H. Kotegawa, H. Tou, H. Harima, and H. Tanida, J. Phys. Soc. Jpn. 90, 023702 (2021).
[4] M. Yatsushiro, and S. Hayami, J. Phys. Soc. Jpn. 89, 013703 (2019).
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Presenters
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Akio Kimura
Graduate School of Advanced Science and Engineering, Hiroshima Univ., Hiroshima Univ, Hiroshima University
Authors
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Akio Kimura
Graduate School of Advanced Science and Engineering, Hiroshima Univ., Hiroshima Univ, Hiroshima University
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Tomoki Yoshikawa
Hiroshima University
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Yuto Fukushima
Hiroshima University
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Takashi Kono
Hiroshima University
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Munisa Nurmamat
Hiroshima University
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Masashi Arita
HiSOR, Hiroshima Univ., Hiroshima University
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Keisuke Mitsumoto
Toyama Prefectural University
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Hiroshi Tanida
Toyama Prefectural University