{ "id": "cond-mat/0412034", "version": "v1", "published": "2004-12-01T20:14:29.000Z", "updated": "2004-12-01T20:14:29.000Z", "title": "Bose-Einstein Condensation as a Quantum Phase Transition in an Optical Lattice", "authors": [ "M. Aizenman", "E. H. Lieb", "R. Seiringer", "J. P. Solovej", "J. Yngvason" ], "comment": "To appear in the proceedings of QMath9, Giens, France, Sept. 12--16, 2004", "journal": "in: `Mathematical Physics of Quantum Mechanics, Selected and Refereed Lectures from QMath9', A. Joyce and and J. Ash (eds), Springer Lecture Notes in Physics, vol. 690 (2006)", "categories": [ "cond-mat.stat-mech", "cond-mat.other", "math-ph", "math.MP" ], "abstract": "One of the most remarkable recent developments in the study of ultracold Bose gases is the observation of a reversible transition from a Bose Einstein condensate to a state composed of localized atoms as the strength of a periodic, optical trapping potential is varied. In \\cite{ALSSY} a model of this phenomenon has been analyzed rigorously. The gas is a hard core lattice gas and the optical lattice is modeled by a periodic potential of strength $\\lambda$. For small $\\lambda$ and temperature Bose-Einstein condensation (BEC) is proved to occur, while at large $\\lambda$ BEC disappears, even in the ground state, which is a Mott-insulator state with a characteristic gap. The inter-particle interaction is essential for this effect. This contribution gives a pedagogical survey of these results.", "revisions": [ { "version": "v1", "updated": "2004-12-01T20:14:29.000Z" } ], "analyses": { "keywords": [ "quantum phase transition", "optical lattice", "hard core lattice gas", "ultracold bose gases", "bose einstein condensate" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2004cond.mat.12034A" } } }