Hamiltonian quantization of the non-anomalous generalized Schwinger model

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dc.contributor.authorDutra, Alvaro de Souza [UNESP]
dc.contributor.authorNatividade, C. P. [UNESP]
dc.contributor.institutionUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2014-05-27T11:18:01Z
dc.date.available2014-05-27T11:18:01Z
dc.date.issued1995-09-01
dc.description.abstractWe quantize a generalized version of the Schwinger model, where the two chiral sectors couples with different strengths to the U(1) gauge field. Starting from a theory which includes a generalized Wess-Zumino term, we obtain the equal time commutation relation for physical fields, both the singular and non-singular cases are considered. The photon propagators are also computed in their gauge dependent and invariant versions. © 1995 Springer-Verlag.en
dc.description.affiliationDepartamento de Física e Química Universidade Estadual Paulista, Campus de Guaratinguetá, 12500-00, SP
dc.description.affiliationUnespDepartamento de Física e Química Universidade Estadual Paulista, Campus de Guaratinguetá, 12500-00, SP
dc.format.extent517-522
dc.identifierhttp://dx.doi.org/10.1007/BF01556380
dc.identifier.citationZeitschrift für Physik C Particles and Fields, v. 66, n. 3, p. 517-522, 1995.
dc.identifier.doi10.1007/BF01556380
dc.identifier.issn0170-9739
dc.identifier.issn1434-6052
dc.identifier.lattes6314084638411003
dc.identifier.scopus2-s2.0-33750426807
dc.identifier.urihttp://hdl.handle.net/11449/64633
dc.identifier.wosWOS:A1995QV77200023
dc.language.isoeng
dc.relation.ispartofZeitschrift fur Physik C: Particles and Fields
dc.relation.ispartofsjr2,022
dc.rights.accessRightsAcesso restrito
dc.sourceScopus
dc.titleHamiltonian quantization of the non-anomalous generalized Schwinger modelen
dc.typeArtigo
dcterms.licensehttp://www.springer.com/open+access/authors+rights
unesp.author.lattes6314084638411003[1]
unesp.author.orcid0000-0003-3027-1066[1]
unesp.campusUniversidade Estadual Paulista (Unesp), Faculdade de Engenharia, Guaratinguetápt

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Artigos - Física e Química - FEG