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  • Letter

Orbital Chern insulator at ν=−2 in twisted MoTe2

Feng-Ren Fan1,2,*, Cong Xiao3,1,2,*, and Wang Yao1,2,†

  • 1Department of Physics, The University of Hong Kong, Hong Kong, China
  • 2HKU-UCAS Joint Institute of Theoretical and Computational Physics at Hong Kong, China
  • 3Institute of Applied Physics and Materials Engineering, University of Macau, Taipa, Macau, China

  • *These authors contributed equally to this work.
  • †wangyao@hku.hk

Phys. Rev. B 109, L041403 – Published 10 January, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L041403

Abstract

In twisted MoTe2, the latest transport measurement has reported observation of the quantum anomalous Hall effect at hole filling ν=−1, which undergoes a topological phase transition to a trivial ferromagnet as layer hybridization gets suppressed by interlayer bias D. Here we show that this underlies the existence of an orbital Chern insulating state with gate (D) switchable sign in an antiferromagnetic spin background at hole filling ν=−2. From momentum-space Hartree-Fock calculations, we find this state has a topological phase diagram complementary to that of the ν=−1 one: by sweeping D from negative to positive, the Chern number of this ν=−2 state can be switched between +1, 0, and −1, accompanied by a sign change of a sizable orbital magnetization. In the range of D where this antiferromagnet is the ground state, the orbital magnetization allows magnetic field initialization of the spin antiferromagnetic order and the Chern number.

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