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Please use this identifier to cite or link to this item: http://acervodigital.unesp.br/handle/11449/65130
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dc.contributor.authorBoldo, J. L.-
dc.contributor.authorPimentel, B. M.-
dc.contributor.authorTomazelli, J. L.-
dc.date.accessioned2014-05-27T11:18:14Z-
dc.date.accessioned2016-10-25T18:14:30Z-
dc.date.available2014-05-27T11:18:14Z-
dc.date.available2016-10-25T18:14:30Z-
dc.date.issued1997-07-01-
dc.identifierhttp://dx.doi.org/10.1007/BF02435756-
dc.identifier.citationInternational Journal of Theoretical Physics, v. 36, n. 7, p. 1565-1574, 1997.-
dc.identifier.issn0020-7748-
dc.identifier.urihttp://hdl.handle.net/11449/65130-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/65130-
dc.description.abstractThe operator S in Fock space which describes the scattering and particle production processes in an external time-dependent electromagnetic potential A can be constructed from the one-particle S-matrix up to a physical phase λ[A]. In this work we determine this phase for QED in (2 + 1) dimensions by means of causality and show that no ultraviolet divergences arise, in contrast to the usual formalism of QED3.en
dc.format.extent1565-1574-
dc.language.isoeng-
dc.sourceScopus-
dc.titleCausal phase in QED3en
dc.typeoutro-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.description.affiliationInst. de Fis. Teórica Universidade Estadual Paulista, 01405-900, São Paulo, SP-
dc.description.affiliationUnespInst. de Fis. Teórica Universidade Estadual Paulista, 01405-900, São Paulo, SP-
dc.identifier.doi10.1007/BF02435756-
dc.identifier.wosWOS:A1997XT79900005-
dc.rights.accessRightsAcesso restrito-
dc.relation.ispartofInternational Journal of Theoretical Physics-
dc.identifier.scopus2-s2.0-0031475541-
Appears in Collections:Artigos, TCCs, Teses e Dissertações da Unesp

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