Entropy-enhanced fractional quantum anomalous Hall effect
Abstract
Strongly interacting electrons in a topologically nontrivial band may form exotic phases of matter. An especially intriguing example of which is the fractional quantum anomalous Hall phase, recently discovered in twisted transition metal dichalcogenides and in moiré graphene multilayers. However, it has been shown to be destabilized in certain filling factors at sub-100 mK temperatures in pentalayer graphene, in favor of a novel integer quantum anomalous Hall phase [Z. Lu, Extended quantum anomalous Hall states in graphene/hBN moiré superlattices, arXiv:2408.10203]. We propose that the culprit stabilizing the fractional phase at higher temperatures is its rich edge state structure. Possessing a multiplicity of chiral modes on its edge, the fractional phase has lower free energy at higher temperatures due to the excess edge mode entropy. We make distinct predictions under this scenario, including the system-size dependency of the fractional phase entropic enhancement, and how the phase boundaries change as a function of temperature.
Copyright and License
© 2024 American Physical Society.
Acknowledgement
G.S. acknowledges enlightening discussions with Gil Refael, as well as support from the Walter Burke Institute for Theoretical Physics at Caltech, and from the Yad Hanadiv Foundation through the Rothschild fellowship.
Supplemental Material
Supplemental Material (PDF):
The Supplementary Materials contain the derivation of the phase boundary from the expression for the free energy, details of the tight binding model for pentalayer graphene, and definition of the quantum Fubini-Study metric.
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Additional details
- Walter Burke Institute for Theoretical Physics
- Yad Hanadiv
- Accepted
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2024-11-05Accepted
- Caltech groups
- Institute for Quantum Information and Matter, Walter Burke Institute for Theoretical Physics
- Publication Status
- Published