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Elastic deformations and Wigner-Weyl formalism in graphene

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arxiv 1905.11097 v1 pith:GSF772VO submitted 2019-05-27 cond-mat.mes-hall hep-lat

classification cond-mat.mes-hallhep-lat
keywords deformationselasticformalismallowsgraphenepresencewigner-weylbinding
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abstract

We discuss the tight-binding models of solid state physics with the $Z_2$ sublattice symmetry in the presence of elastic deformations, and their important particular case -the tight binding model of graphene. In order to describe the dynamics of electronic quasiparticles we explore Wigner-Weyl formalism. It allows to calculate the two-point Green's function in the presence of both slowly varying external electromagnetic fields and the inhomogeneous modification of the hopping parameters resulted from the elastic deformations. The developed formalism allows us to consider the influence of elastic deformations and the variations of magnetic field on the quantum Hall effect.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Hall conductivity as the topological invariant in phase space in the presence of interactions and non-uniform magnetic field

    cond-mat.mes-hall 2019-08 conditional novelty 6.0 of 10

    Interactions do not renormalize the phase-space topological expression for the Hall conductivity in a 2+1D tight-binding model with non-uniform magnetic field, to all orders of perturbation theory.

  2. Topological invariant responsible for the integer QHE and non-commutative geometry

    cond-mat.mes-hall 2026-06 unverdicted novelty 5.0 of 10

    The integer quantum Hall invariant N3 is expressed as a K-theory/cyclic-cohomology pairing; it vanishes on finite lattices and is only conditionally integer in the infinite-lattice limit.

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