Abstract:
Schrödinger and Bargmann–Fock representations in non-Archimedean quantum mechanics are realized in the spaces L2(Kn,dx) and L2(Zn,e−zzdzdˉz) (K is a non-Archimedean field, and Z=K(√τ) is its quadratic extension) by means of the calculus of pseudodifferential operators.
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