Theory of broken symmetry quantum Hall states in the Landau level of Graphene
arXiv:2210.03752 · doi:10.1103/PhysRevB.107.045132
Abstract
We study many-body ground states for the partial integer fillings of the Landau level in graphene, by constructing a model that accounts for the lattice scale corrections to the Coulomb interactions. Interestingly, in contrast to the Landau level, this model contains not only pure delta function interactions but also some of its derivatives. Due to this we find several important differences with respect to the Landau level. For example at quarter filling when only a single component is filled, there is a degeneracy lifting of the quantum hall ferromagnets and ground states with entangled spin and valley degrees of freedom can become favourable. Moreover at half-filling of the Landau level, we have found a new phase that is absent in the Landau level, that combines characteristics of the Kekulé state and an antiferromagnet. We also find that according to the parameters extracted in a recent experiment, at half-filling of the Landau level graphene is expected to be in a delicate competition between an AF and a CDW state, but we also discuss why the models for these recent experiments might be missing some important terms.
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Cited by in corpus (8)
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- Spin-valley entangled quantum Hall states in graphene
- Phase diagram of the quantum Hall state in bilayer graphene
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