Classical field theory limit of 2D many-body quantum Gibbs states
Résumé
We prove that the grand-canonical Gibbs states of a large 2D bosonic system converge to the Gibbs measure of an interacting classical field theory, in a mean-field-type limit. Reduced density matrices of the quantum Gibbs state converge to their classical analogues, given by a nonlinear Schrödinger-Gibbs measure supported on distributions with low regularity. Tuning the chemical potential of the grand-canonical ensemble provides a counter-term for the diverging repulsive interactions, analogue to the Wick ordering of the limit classical theory.
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