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Please use this identifier to cite or link to this item: http://acervodigital.unesp.br/handle/11449/130456
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dc.contributor.authorAldrovandi, R.-
dc.contributor.authorKraenkel, Roberto André-
dc.date.accessioned2014-05-27T06:35:49Z-
dc.date.accessioned2016-10-25T21:21:12Z-
dc.date.available2014-05-27T06:35:49Z-
dc.date.available2016-10-25T21:21:12Z-
dc.date.issued1989-12-01-
dc.identifierhttp://scitation.aip.org/content/aip/journal/jmp/30/8/10.1063/1.528273-
dc.identifier.citationJournal of Mathematical Physics, v. 30, n. 8, p. 1866-1870, 1989.-
dc.identifier.issn0022-2488-
dc.identifier.urihttp://hdl.handle.net/11449/130456-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/130456-
dc.description.abstractThe basic field equations of a field theory are not always derivable from a Lagrangian. Lagrangian theories are perturbatively coherent, in the sense that they have well-defined vertices. Non-Lagrangian theories may be coherent or not. Coherent theories are, in principle, quantizable by perturbative methods. The general condition for a theory to have well-defined vertices is given. © 1989 American Institute of Physics.en
dc.description.sponsorshipFundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)-
dc.format.extent1866-1870-
dc.language.isoeng-
dc.publisherAmerican Institute of Physics (AIP)-
dc.sourceScopus-
dc.titlePerturbative coherence in field theoryen
dc.typeoutro-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.description.affiliationInstitute de Física Teórica Universidade Estadual Paulista, Rua Pamplona, 145, 01405, São Paulo-
dc.description.affiliationFAPESP, São Paulo-
dc.description.affiliationUnespInstitute de Física Teórica Universidade Estadual Paulista, Rua Pamplona, 145, 01405, São Paulo-
dc.identifier.doihttp://dx.doi.org/10.1063/1.528273-
dc.identifier.wosWOS:A1989AH02700026-
dc.rights.accessRightsAcesso restrito-
dc.identifier.file2-s2.0-3043002427.pdf-
dc.relation.ispartofJournal of Mathematical Physics-
dc.identifier.scopus2-s2.0-3043002427-
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