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Anderson's Theorem for Correlated Insulating States in Twisted Bilayer Graphene
Kryštof Kolář1, Gal Shavit2, Christophe Mora3
1Dahlem Center for Complex Quantum Systems and Fachbereich Physik, Freie Universität Berlin, 14195 Berlin, Germany.
The Kramers intervalley coherent (K-IVC) state in twisted bilayer graphene is robust against certain perturbations, but sensitive to others. This Anderson theorem helps explain the sample-dependent insulating phases observed in experiments.
Area of Science:
- Condensed matter physics
- Materials science
- Quantum mechanics
Background:
- Correlated insulating phases in magic-angle twisted bilayer graphene show significant sample dependence.
- The Kramers intervalley coherent (K-IVC) state is a leading candidate for these insulating phases at even fillings.
- Understanding the stability of these states against disorder is crucial for experimental realization.
Purpose of the Study:
- To derive an Anderson theorem for the K-IVC state in twisted bilayer graphene.
- To investigate the robustness of the K-IVC state against various perturbations.
- To classify the stability of the K-IVC state against experimentally relevant conditions.
Main Methods:
- Theoretical derivation of an Anderson theorem.
- Analysis of the K-IVC state's response to PT-odd and PT-even perturbations.
- Classification of stability based on perturbation types.
Main Results:
- An Anderson theorem governing the K-IVC state's robustness against disorder was derived.
- The K-IVC gap is robust against PT-odd local perturbations.
- PT-even perturbations can induce subgap states, reducing or eliminating the gap.
Conclusions:
- The K-IVC state's stability is characterized by its distinct response to PT-odd and PT-even perturbations.
- The derived Anderson theorem provides a framework for understanding sample dependence in twisted bilayer graphene.
- This theoretical insight helps distinguish the K-IVC state from other potential insulating ground states.
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