The real-space Chern number of ensembles of Bloch states is robust and symmetry-forced to be nonzero in twisted TMDs and twisted bilayer graphene.
Polarization-driven band topology evolution in twisted MoTe$_2$ and WSe$_2$
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abstract
Motivated by recent experimental observations of opposite Chern numbers in $R$-type twisted MoTe$_2$ and WSe$_2$ homobilayers, we perform large-scale density-functional-theory (DFT) calculations with machine learning force fields to investigate moir\'e band topology from large to small twist angles in both materials. We find that the Chern numbers of the moir\'e frontier bands change sign as a function of twist angle, and this change is driven by the competition between moir\'{e} ferroelectricity and piezoelectricity. Our large-scale calculations, enabled by machine learning methods, reveal crucial insights into interactions across different scales in twisted bilayer systems. The interplay between atomic-level relaxation effects and moir\'e-scale electrostatic potential variation opens new avenues for the design of intertwined topological and correlated states, including the possibility of mimicking higher Landau-level physics in the absence of a magnetic field.
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Robustness of real-space topology in moir\'e systems
The real-space Chern number of ensembles of Bloch states is robust and symmetry-forced to be nonzero in twisted TMDs and twisted bilayer graphene.