“…In the high energy physics the topological invariants in momentum space were considered, say, in 46,47,48,49,50,43,51,52,53 . The Wigner-Weyl formalism in 27,29,31,32 was developed in the context of lattice field theory. The one-particle fermion Green's function G(p, q) was considered in momentum space M (p, q ∈ M).…”