Topological phase in the extended Haldane-Hubbard model with sublattice-dependent repulsion

被引:0
|
作者
Wang, Bao-Qing [1 ,2 ]
Shao, Can [3 ]
Tohyama, Takami [4 ]
Luo, Hong-Gang [1 ,2 ,5 ]
Lu, Hantao [1 ,2 ]
机构
[1] Lanzhou Univ, Lanzhou Ctr Theoret Phys, Key Lab Quantum Theory & Applicat MoE, Lanzhou 730000, Peoples R China
[2] Lanzhou Univ, Key Lab Theoret Phys Gansu Prov, Lanzhou 730000, Peoples R China
[3] Nanjing Univ Sci & Technol, Dept Appl Phys, Nanjing 210094, Peoples R China
[4] Tokyo Univ Sci, Dept Appl Phys, Tokyo 1258585, Japan
[5] Beijing Computat Sci Res Ctr, Beijing 100084, Peoples R China
基金
中国国家自然科学基金;
关键词
REALIZATION; CATALOG;
D O I
10.1103/PhysRevB.110.035107
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We study the ground-state phase diagram of the half-filled extended Haldane-Hubbard model on the honeycomb lattice with sublattice-dependent on-site repulsion (UA/B) using the exact diagonalization (ED) and mean-field (MF) methods. The resulting phase diagram shows that there is a topologically nontrivial phase with the Chern number C = 1, emerging via the development of the imbalance between UA and UB. In this phase, the antiferromagnetic correlations are observed in the ED calculation, in line with the finite antiferromagnetic order obtained by the MF method. The spontaneous symmetry breaking of SU(2) spin rotation in the phase is also identified in the MF level. Distinct from previous studies in which the exotic C = 1 phase relies on the interplay between sublattice-dependent potentials and electronic interactions, our paper presents an alternative way by solely tuning the on-site interactions.
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页数:8
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