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Electron correlation effects near Van Hove singularities: Application to twisted bilayer graphene and supermetal

日程 : 2021年6月4日(金) 4:00 pm - 5:00 pm 場所 : Zoom 開催(事前登録を下記リンク先にてお願い致します) 講師 : 磯部 大樹 氏 所属 : 東京大学 大学院工学系研究科 物理工学専攻 世話人 : 加藤 岳生
e-mail: kato@issp.u-tokyo.ac.jp

Electron correlation decorates the condensed matter physics, bringing symmetry breaking and ordered phases. It becomes vital when many electrons are active, namely near a Van Hove singularity (VHS) where the density of states (DOS) diverges. Since a VHS accompanies the topological transition of the Fermi surface, tunable materials are desirable to observe VHS-related behaviors, for example, by strain or pressure. The seminar focuses on moiré superstructures made of van der Waals materials; twisted bilayer graphene allows band dispersion design by the stacking angle, and correlated insulating and superconducting states are observed near the so-called magic angle.

First, we introduce a theory that describes a possible mechanism for correlated insulating and superconducting states in twisted bilayer graphene [1]. Our analysis of a hot-spot model shows that d- or p-wave superconductivity and charge/spin-density wave emerge from Coulomb repulsion near VHS. We further investigate the tunable nature of twisted bilayer graphene, which invokes the notion of a high-order VHS [2]. We show that tuning a single tuning parameter, such as a twist angle of a moiré material, pressure, and strain, realizes a high-order VHS realizes a power-law divergence in the DOS in two dimensions, unlike the usual logarithmic one. We could attribute the origin of the so-called magic angle to the high-order VHS. Finally, we discuss correlation effects at a high-order VHS [3]. We perform a renormalization-group analysis to find a nontrivial metallic state, where various divergent susceptibilities coexist, but no long-range order appears. We term such a metallic state as a supermetal. Our controlled analysis at the interacting fixed point reveals that an interacting supermetal is a non-Fermi liquid.

[1] H. Isobe and L. Fu, Phys. Rev. Research 1, 033206 (2019).
[2] N. F. Q. Yuan, H. Isobe, and L. Fu, Nat. Commun. 10, 5769 (2019).
[3] H. Isobe, N. F. Q. Yuan, and L. Fu, Phys. Rev. X 8, 041041 (2018).

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(公開日: 2021年05月25日)