Master actions for massive spin-3 particles in D = 2 + 1

dc.contributor.authorMendonça, Elias Leite [UNESP]
dc.contributor.authorDalmazi, Denis [UNESP]
dc.contributor.institutionUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2018-12-11T17:02:12Z
dc.date.available2018-12-11T17:02:12Z
dc.date.issued2016-04-01
dc.description.abstractWe present here a relationship between massive self-dual models for spin-3 particles in (Formula presented.) via the master action procedure. Starting with a first-order model (in the derivatives) (Formula presented.) we have constructed a master action which interpolates between a sequence of four self-dual models (Formula presented.) where (Formula presented.). By analyzing the particle content of the mixing terms, we give additional arguments that explain why it is apparently impossible to jump from the fourth-order model to a higher-order model. We have also analyzed similarities and differences between the fourth-order K-term in the spin-2 case and the analogous fourth-order term in the spin-3 context.en
dc.description.affiliationUNESP Campus de Guaratinguetá DFQ, Avenida Dr. Ariberto Pereira da Cunha, 333
dc.description.affiliationUnespUNESP Campus de Guaratinguetá DFQ, Avenida Dr. Ariberto Pereira da Cunha, 333
dc.identifierhttp://dx.doi.org/10.1140/epjc/s10052-016-3957-4
dc.identifier.citationEuropean Physical Journal C, v. 76, n. 4, 2016.
dc.identifier.doi10.1140/epjc/s10052-016-3957-4
dc.identifier.file2-s2.0-84962714632.pdf
dc.identifier.issn1434-6052
dc.identifier.issn1434-6044
dc.identifier.lattes5325671871600272
dc.identifier.orcid0000-0002-1380-9672
dc.identifier.scopus2-s2.0-84962714632
dc.identifier.urihttp://hdl.handle.net/11449/172792
dc.language.isoeng
dc.relation.ispartofEuropean Physical Journal C
dc.relation.ispartofsjr2,022
dc.relation.ispartofsjr2,022
dc.rights.accessRightsAcesso aberto
dc.sourceScopus
dc.titleMaster actions for massive spin-3 particles in D = 2 + 1en
dc.typeArtigo
unesp.author.lattes5325671871600272[1]
unesp.author.orcid0000-0002-1380-9672[1]

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