Interacting Bose Gas in an Optical Lattice

dc.creatorZiegler, K.
dc.date2001-08-02
dc.date2001-10-23
dc.date.accessioned2026-07-07T02:42:19Z
dc.date.available2026-07-07T02:42:19Z
dc.descriptionA grand canonical system of hard-core bosons in an optical lattice is considered. The bosons can occupy randomly $N$ equivalent states at each lattice site. The limit $N\to\infty$ is solved exactly in terms of a saddle-point integration, representing a weakly-interacting Bose gas. At T=0 there is only a condensate in the limit $N\to\infty$. Corrections in 1/N increase the total density of bosons but suppress the condensate. This indicates a depletion of the condensate due to increasing interaction at finite values of N.
dc.description14 pages, 1 figure
dc.identifierhttps://arxiv.org/abs/cond-mat/0108041
dc.identifierhttp://arxiv.org/abs/cond-mat/0108041
dc.identifierJourn. Low Temp. Phys. 126, 1431 (2002)
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/18094
dc.subjectStatistical Mechanics
dc.titleInteracting Bose Gas in an Optical Lattice
dc.typetext

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