Geometrical phase,generalized quasienergy and Floquet operator as invariants

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dc.creatorMan'ko, V. I.
dc.date1992-12-21
dc.date.accessioned2026-07-07T04:19:06Z
dc.date.available2026-07-07T04:19:06Z
dc.descriptionFor time-periodical quantum systems generalized Floquet operator is found to be integral of motion.Spectrum of this invariant is shown to be quasienergy spectrum.Analogs of invariant Floquet operators are found for nonperiodical systems with several characteristic times.Generalized quasienergy states are introduced for these systems. Geometrical phase is shown to be integral of motion.
dc.description4 pages,Latex,DSF-T-92/26,INFN-NA-IV-92/26
dc.identifierhttps://arxiv.org/abs/hep-th/9212122
dc.identifierhttp://arxiv.org/abs/hep-th/9212122
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/53458
dc.subjectHigh Energy Physics - Theory
dc.titleGeometrical phase,generalized quasienergy and Floquet operator as invariants
dc.typetext

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