Abstract

A positive temperature analogue of the scattering length of a potential VV can be defined via integrating the difference of the heat kernels of −Δ-Δ and −Δ+12V-Δ+ \frac 12 V, with ΔΔ the Laplacian. An upper bound on this quantity is a crucial input in the derivation of a bound on the critical temperature of a dilute Bose gas \cite{SU}. In \cite{SU} a bound was given in the case of finite range potentials and sufficiently low temperature. In this paper, we improve the bound and extend it to potentials of infinite range.

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