dc.contributorUniversidade Federal de Santa Catarina (UFSC)
dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2014-05-20T14:06:36Z
dc.date.accessioned2022-10-05T15:00:05Z
dc.date.available2014-05-20T14:06:36Z
dc.date.available2022-10-05T15:00:05Z
dc.date.created2014-05-20T14:06:36Z
dc.date.issued2002-05-31
dc.identifierJournal of Physics A-mathematical and General. Bristol: Iop Publishing Ltd, v. 35, n. 21, p. 4633-4640, 2002.
dc.identifier0305-4470
dc.identifierhttp://hdl.handle.net/11449/23379
dc.identifier10.1088/0305-4470/35/21/311
dc.identifierWOS:000176286200013
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/3896767
dc.description.abstractFollowing the discussion-in state-space language-presented in a preceding paper, we work on the passage from the phase-space description of a degree of freedom described by a finite number of states (without classical counterpart) to one described by an infinite (and continuously labelled) number of states. With this it is possible to relate an original Schwinger idea to the Pegg-Barnett approach to the phase problem. In phase-space language, this discussion shows that one can obtain the Weyl-Wigner formalism, for both Cartesian and angular coordinates, as limiting elements of the discrete phase-space formalism.
dc.languageeng
dc.publisherIop Publishing Ltd
dc.relationJournal of Physics A: Mathematical and General
dc.rightsAcesso restrito
dc.sourceWeb of Science
dc.titleSchwinger and Pegg-Barnett approaches and a relationship between angular and Cartesian quantum descriptions: II. Phase spaces
dc.typeArtigo


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