Ergodic Properties of the Quantum Ideal Gas in the Maxwell-Boltzmann Statistics

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dc.creatorLenci, Marco
dc.date1996-05-09
dc.date.accessioned2026-07-07T09:07:55Z
dc.date.available2026-07-07T09:07:55Z
dc.descriptionIt is proved that the quantization of the Volkovyski-Sinai model of ideal gas (in the Maxwell-Boltzmann statistics) enjoys at the thermodynamical limit the properties of mixing and ergodicity with respect to the quantum canonical Gibbs state. Plus, the average over the quantum state of a pseudo-differential operator is exactly the average over the classical canonical measure of its Weyl symbol.
dc.description35 pages, LaTeX
dc.identifierhttps://arxiv.org/abs/chao-dyn/9605005
dc.identifierhttp://arxiv.org/abs/chao-dyn/9605005
dc.identifierJ. Math. Phys. 37 (1996), no. 10, 5136-5157
dc.identifierdoi:10.1063/1.531684
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/150538
dc.subjectChaotic Dynamics
dc.subjectExactly Solvable and Integrable Systems
dc.subjectQuantum Physics
dc.titleErgodic Properties of the Quantum Ideal Gas in the Maxwell-Boltzmann Statistics
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