Orbital Chern Insulator at $ν=-2$ in Twisted MoTe$_{2}$

Fuente: arXiv
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Main Authors: Fan, Feng-Ren, Xiao, Cong, Yao, Wang
Format: Preprint
Published: 2023
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author Fan, Feng-Ren
Xiao, Cong
Yao, Wang
author_facet Fan, Feng-Ren
Xiao, Cong
Yao, Wang
contents In twisted MoTe$_{2}$, latest transport measurement has reported observation of 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 antiferromagtic 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 range of $D$ where this antiferronagnet is the ground state, the orbital magnetization allows magnetic field initialization of the spin antiferromagnetic order and the Chern number.
format Preprint
id arxiv_https___arxiv_org_abs_2308_11454
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Orbital Chern Insulator at $ν=-2$ in Twisted MoTe$_{2}$
Fan, Feng-Ren
Xiao, Cong
Yao, Wang
Strongly Correlated Electrons
Materials Science
In twisted MoTe$_{2}$, latest transport measurement has reported observation of 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 antiferromagtic 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 range of $D$ where this antiferronagnet is the ground state, the orbital magnetization allows magnetic field initialization of the spin antiferromagnetic order and the Chern number.
title Orbital Chern Insulator at $ν=-2$ in Twisted MoTe$_{2}$
topic Strongly Correlated Electrons
Materials Science
url https://arxiv.org/abs/2308.11454