dc.contributorUniversidade Federal do ABC (UFABC)
dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2013-09-30T18:56:29Z
dc.date.accessioned2014-05-20T14:10:52Z
dc.date.available2013-09-30T18:56:29Z
dc.date.available2014-05-20T14:10:52Z
dc.date.created2013-09-30T18:56:29Z
dc.date.created2014-05-20T14:10:52Z
dc.date.issued2009-09-01
dc.identifierPhysical Review D. College Pk: Amer Physical Soc, v. 80, n. 5, p. 5, 2009.
dc.identifier1550-7998
dc.identifierhttp://hdl.handle.net/11449/24384
dc.identifier10.1103/PhysRevD.80.056007
dc.identifierWOS:000270384900114
dc.identifierWOS000270384900114.pdf
dc.identifier6783433390235727
dc.identifier0000-0001-5279-8438
dc.description.abstractOne way of avoiding the destabilization of the electroweak scale through a strong coupled regime naturally occurs in models with a Landau-like pole at the TeV scale. Hence, the quadratic divergence contributions to the scalar masses are not considered as a problem anymore since a new nonperturbative dynamic emerges at the TeV scale. This scale should be an intrinsic feature of the models, and there is no need to invoke any other sort of protection for the electroweak scale. In some models based on the SU(3)(C) circle times SU(3)(W) circle times U(1)(X) gauge symmetry, a nonperturbative dynamics arise and it stabilizes the electroweak scale.
dc.languageeng
dc.publisherAmer Physical Soc
dc.relationPhysical Review D
dc.rightsAcesso restrito
dc.sourceWeb of Science
dc.titleStabilization of the electroweak scale in 3-3-1 models
dc.typeArtículos de revistas


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