Abstract

The strong correlation effects on topological insulator are studied in a two-sublattice system with an onsite single-particle energy difference ΔΔ between two sublattices. At Δ=0Δ=0, increasing the onsite interaction strength UU drives the transition from the quantum spin Hall insulating state to the non-topological antiferromagnetic Mott-insulating (AFMI) state. When ΔΔ is larger than a certain value, a topologically trivial band insulator or AFMI at small values of UU may change into a quantum anomalous Hall state with antiferromagnetic ordering at intermediate values of UU. Further increasing UU drives the system back into the topologically trivial state of AFMI. The corresponding phenomena is observable in the solid state and cold atom systems. We also propose a scheme to realize and detect these effects in cold atom systems.

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