Bose-Einstein condensates in symmetry breaking states

dc.creatorCastin, Yvan
dc.creatorHerzog, Christopher
dc.date2000-12-04
dc.date2004-07-19
dc.date.accessioned2026-07-07T02:39:39Z
dc.date.available2026-07-07T02:39:39Z
dc.descriptionWe consider two models of interacting Bose gases: a gas of spin one particles in the ground state of a cubic box and a one-dimension Bose gas with contact interactions. We show how to calculate exact eigenstates of the corresponding N-body Hamiltonians. Both models share the property of not leading to the formation of a Bose-Einstein condensate, even at zero temperature, in the strict sense of the existence of a single one-particle state with a macroscopic population. We show that a lot of physical insight can be gained on these two model systems by using the usual Hartree-Fock mean field approach: in this approximation, that we test against the exact result, everything happens as if a single realization of the system was a Bose-Einstein condensate in a state phi breaking the rotational or translational symmetry, and varying in a random way for any new experimental realization.
dc.description24 pages, 2 figures, Lecture Notes of the Cargese School on Bose-Einstein condensates (July 2000); typos in Eqs.(72),(121) corrected
dc.identifierhttps://arxiv.org/abs/cond-mat/0012040
dc.identifierhttp://arxiv.org/abs/cond-mat/0012040
dc.identifierComptes Rendus de l'Academie des Sciences de Paris, tome 2, serie IV, p.419-443 (2001)
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/17096
dc.subjectSoft Condensed Matter
dc.titleBose-Einstein condensates in symmetry breaking states
dc.typetext

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