Second order gauge theory

dc.contributorUniversidade Estadual Paulista (Unesp)
dc.contributorInst Fomento & Coordenacao Ind
dc.date.accessioned2014-05-20T14:07:59Z
dc.date.accessioned2022-10-05T15:02:55Z
dc.date.available2014-05-20T14:07:59Z
dc.date.available2022-10-05T15:02:55Z
dc.date.created2014-05-20T14:07:59Z
dc.date.issued2007-05-01
dc.identifierAnnals of Physics. San Diego: Academic Press Inc. Elsevier B.V., v. 322, n. 5, p. 1211-1232, 2007.
dc.identifier0003-4916
dc.identifierhttp://hdl.handle.net/11449/23840
dc.identifier10.1016/j.aop.2006.07.006
dc.identifierWOS:000246274500009
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/3897094
dc.description.abstractA gauge theory of second order in the derivatives of the auxiliary field is constructed following Utiyama's program. A novel field strength G = partial derivative F + fAF arises besides the one of the first order treatment, F = partial derivative A - partial derivative A + fAA. The associated conserved current is obtained. It has a new feature: topological terms are determined from local invariance requirements. Podolsky Generalized Eletrodynamics is derived as a particular case in which the Lagrangian of the gauge field is L-P alpha G(2). In this application the photon mass is estimated. The SU(N) infrared regime is analysed by means of Alekseev-Arbuzov-Baikov's Lagrangian. (c) 2006 Elsevier B.V. All rights reserved.
dc.languageeng
dc.publisherElsevier B.V.
dc.relationAnnals of Physics
dc.relation2.367
dc.relation0,987
dc.rightsAcesso restrito
dc.sourceWeb of Science
dc.subjectgauge theory
dc.subjecthigher order field theory
dc.titleSecond order gauge theory
dc.typeArtigo


Este ítem pertenece a la siguiente institución