Particle fluctuations in systems with Bose-Einstein condensate

TL;DR

This paper clarifies misconceptions about particle fluctuations in Bose-Einstein condensates, emphasizing the importance of gauge symmetry breaking and correcting the notion of catastrophic fluctuations in the condensed phase.

Contribution

It demonstrates that proper gauge symmetry breaking eliminates condensate fluctuations and resolves the grand canonical catastrophe misconception.

Findings

No catastrophic fluctuations in the condensed phase when gauge symmetry is broken.

Ideal Bose gas has no condensate fluctuations, only anomalous uncondensed particle fluctuations.

Canonical and grand canonical ensembles with broken gauge symmetry are equivalent in particle number scaling.

Abstract

Particle fluctuations in systems, exhibiting Bose-Einstein condensation, are reviewed in order to clarify the basic points that attract high interest and often confront misunderstanding. It is explained that the so-called ``grand canonical catastrophe", claiming the occurrence of catastrophic particle fluctuations in the condensed phase, treated by grand canonical ensemble, does not exist. What exists is the incorrect use of the grand canonical ensemble, where gauge symmetry is not broken, while the correct description of the condensed phase necessarily requires gauge symmetry breaking. The ideal Bose gas has no catastrophic condensate fluctuations, and moreover there are no condensate fluctuations at all, as soon as gauge symmetry is broken. However it does have anomalous fluctuations of uncondensed particles, which implies its instability. For interacting particles, there are no condensate fluctuations, as soon as gauge symmetry is broken, and anomalous fluctuations of uncondensed particles, when correctly calculated, do not appear. Particle fluctuations in the systems of trapped atoms are discussed. Canonical ensemble and grand canonical ensemble with broken gauge symmetry are equivalent with respect to the number of particle scaling.