4.8 Article

Realization of topological Mott insulator in a twisted bilayer graphene lattice model

Journal

NATURE COMMUNICATIONS
Volume 12, Issue 1, Pages -

Publisher

NATURE PORTFOLIO
DOI: 10.1038/s41467-021-25438-1

Keywords

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Funding

  1. RGC of Hong Kong SAR of China [17303019, 17301420, AoE/P-701/20]
  2. MOST through the National Key Research and Development Program [2016YFA0300502]
  3. Strategic Priority Research Program of the Chinese Academy of Sciences [XDB33000000]
  4. NSFC [12074276, 11974036, 11834014, 12074024, 11774018]
  5. NSF [DMR-1916958]
  6. National High Magnetic Field Laboratory through NSF Grant [DMR-1157490]
  7. State of Florida
  8. Priority Academic Program Development (PAPD) of Jiangsu Higher Education Institutions

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This study investigates the correlated electron phenomena in magic-angle twisted bilayer graphene, proposing a Mott-Hubbard perspective and identifying a quantum phase transition in the lattice model. The results not only clarify the mechanism of the quantum anomalous Hall state, but also provide an example of the topological Mott insulator in the strong coupling limit.
Magic-angle twisted bilayer graphene has recently become a thriving material platform realizing correlated electron phenomena taking place within its topological flat bands. Several numerical and analytical methods have been applied to understand the correlated phases therein, revealing some similarity with the quantum Hall physics. In this work, we provide a Mott-Hubbard perspective for the TBG system. Employing the large-scale density matrix renormalization group on the lattice model containing the projected Coulomb interactions only, we identify a first-order quantum phase transition between the insulating stripe phase and the quantum anomalous Hall state with the Chern number of +/- 1. Our results not only shed light on the mechanism of the quantum anomalous Hall state discovered at three-quarters filling, but also provide an example of the topological Mott insulator, i.e., the quantum anomalous Hall state in the strong coupling limit.

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