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Sasaki, Kento; Domon, Kaoru; Ono, Yoshiaki; Yamada, Takemi, E-mail: f18a009f@mail.cc.niigata-u.ac.jp
Proceedings of the international conference on strongly correlated electron systems (SCES2019)2020
Proceedings of the international conference on strongly correlated electron systems (SCES2019)2020
AbstractAbstract
[en] The spinless two-band Hubbard model simulating a electron-hole system is investigated on the basis of the dynamical mean-field theory to elucidate the strong correlation effects on the excitonic phase. We calculate the local excitonic susceptibility χloc and the renormalization factor Z as functions of the energy level splitting Δ and the Coulomb interaction V between conduction and valence electrons and find that χloc is enhanced around the semimetal-to-semiconductor transition where the excitonic phase is expected to be realized. Remarkably, strongly correlated electronic states with Z ∼ 0 are observed for large V in the semimetallic region close to the semimetal-to-semiconductor transition where the both conduction and valence electrons are far away from the half-filling in contrast to the case with the Mott transition. (author)
Source
Hotta, Takashi (ed.) (Tokyo Metropolitan University, Hachioji, Tokyo (Japan)); Katsufuji, Takuro (ed.) (Waseda University, Tokyo (Japan)); [1157 p.]; ISBN 978-4-89027-142-9;
; 2020; p. 011070.1-011070.4; SCES2019: International conference on strongly correlated electron systems; Okayama (Japan); 23-28 Sep 2019; Available from DOI: https://doi.org/10.7566/JPSCP.30.011070; 12 refs., 1 fig.

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