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

Abstract

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 ($U_{\text{A/B}}$) 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 $U_{\text{A}}$ and $U_{\text{B}}$. 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.

8 pages, 5 figures

References in corpus (4)

• Observation of antiferromagnetic correlations in the Hubbard model with ultracold atoms
• Correlation effects in two-dimensional topological insulators
• Interaction effects and quantum phase transitions in topological insulators
• Spontaneous symmetry breaking of an interacting Chern insulator on a topological square lattice

Cited by in corpus (1)

• The antiferromagnetic Chern insulator phase in the Kane-Mele-Hubbard model