Abstract
We propose a new version of Wigner-Weyl calculus for tight-binding lattice models. It allows to express various physical quantities through Weyl symbols of operators and Green's functions. In particular, Hall conductivity in the presence of varying and arbitrarily strong magnetic field is represented using the proposed formalism as a topological invariant.
Original language | English |
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Article number | 114999 |
Journal | Nuclear Physics B |
Volume | 954 |
DOIs | |
State | Published - May 2020 |