Bose-Einstein Condensation in a Harmonic Potential
W. J. Mullin (Department of Physics, Astronomy, University of, Massachusetts)

TL;DR
This paper explores Bose-Einstein condensation in harmonic traps, analyzing phase transitions, finite-size effects, and the differences between ideal and interacting gases across various dimensions.
Contribution
It provides a detailed analysis of BEC in harmonic potentials, including finite-size effects and the impact of interactions, extending understanding beyond the thermodynamic limit.
Findings
BEC occurs in harmonic traps for D≥2 in the thermodynamic limit.
Finite systems exhibit BEC below a pseudo-critical temperature without a true phase transition.
Momentum condensate fraction vanishes as 1/N^{1/2} in the thermodynamic limit.
Abstract
We examine several features of Bose-Einstein condensation (BEC) in an external harmonic potential well. In the thermodynamic limit, there is a phase transition to a spatial Bose-Einstein condensed state for dimension D greater than or equal to 2. The thermodynamic limit requires maintaining constant average density by weakening the potential while increasing the particle number N to infinity, while of course in real experiments the potential is fixed and N stays finite. For such finite ideal harmonic systems we show that a BEC still occurs, although without a true phase transition, below a certain ``pseudo-critical'' temperature, even for D=1. We study the momentum-space condensate fraction and find that it vanishes as 1/N^(1/2) in any number of dimensions in the thermodynamic limit. In D less than or equal to 2 the lack of a momentum condensation is in accord with the Hohenberg…
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