Abstract
A stronger version of the Bogoliubov inequality is used to derive an upper bound for the anomalous average ¦<o(x)>|s of an interacting nonrelativislic Bose fielda(x) at a finite temperature. This bound is ¦a(x)2|s <pR, whereR satisfies 1 -R = (RT/2T c v/2, withv the dimensionality, andT c the critical temperature in the absence of interactions. The formation of nonzero averages is closely related to the Bose-Einstein condensation and ¦<a(X)>|·2 is often believed to coincide with the mean densitypa of the condensate. We have found nonrigorous arguments supporting the inequality po ⩾ ¦<a(X)>|·2, which parallels the result of Griffiths in the case of spin systems.
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Roepstorff, G. Bounds for a Bose condensate in dimensions v ⩾ 3. J Stat Phys 18, 191–206 (1978). https://doi.org/10.1007/BF01014310
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DOI: https://doi.org/10.1007/BF01014310