Topological Phase Transitions in the Repulsively Interacting Haldane-Hubbard Model

被引:77
|
作者
Vanhala, Tuomas I. [1 ,2 ]
Siro, Topi [1 ]
Liang, Long [1 ]
Troyer, Matthias [2 ]
Harju, Ari [1 ]
Torma, Paivi [1 ,3 ]
机构
[1] Aalto Univ, Dept Appl Phys, COMP Ctr Excellence, Helsinki, Finland
[2] ETH, Theoret Phys, CH-8093 Zurich, Switzerland
[3] ETH, Inst Quantum Elect, CH-8093 Zurich, Switzerland
基金
瑞士国家科学基金会; 欧洲研究理事会; 芬兰科学院;
关键词
SQUARE LATTICE; SPIN LIQUID; MONTE-CARLO; QUANTUM; REALIZATION;
D O I
10.1103/PhysRevLett.116.225305
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Using dynamical mean-field theory and exact diagonalization we study the phase diagram of the repulsive Haldane-Hubbard model, varying the interaction strength and the sublattice potential difference. In addition to the quantum Hall phase with Chern number C = 2 and the band insulator with C = 0 present already in the noninteracting model, the system also exhibits a C = 0 Mott insulating phase, and a C = 1 quantum Hall phase. We explain the latter phase by a spontaneous symmetry breaking where one of the spin components is in the Hall state and the other in the band insulating state.
引用
收藏
页数:6
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