Abstract

The construction of the flux operator in the Fock space of harmonic oscillator eigenfunctions is outlined. In one dimension, the flux operator is found to be F=( iω/√π) exp[− a +2/√2] [|1><0|−|0><1|] exp[− a 2/2]. Two approaches for the temperature propagation are discussed, and the thermal flux eigenvalues for a double well potential are presented.

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