3-3-1 models at electroweak scale

dc.contributorUniversidade Estadual Paulista (UNESP)
dc.creatorDias, A. G.
dc.creatorMontero, J. C.
dc.creatorPleitez, V.
dc.date2014-05-20T14:06:45Z
dc.date2014-05-20T14:06:45Z
dc.date2006-06-01
dc.date.accessioned2017-04-05T21:38:58Z
dc.date.available2017-04-05T21:38:58Z
dc.identifierPhysics Letters B. Amsterdam: Elsevier B.V., v. 637, n. 1-2, p. 85-89, 2006.
dc.identifier0370-2693
dc.identifierhttp://hdl.handle.net/11449/23441
dc.identifier10.1016/j.physletb.2006.04.015
dc.identifierWOS:000238007500017
dc.identifier2-s2.0-33646344471.pdf
dc.identifier2-s2.0-33646344471
dc.identifier0000-0001-5279-8438
dc.identifierhttp://dx.doi.org/10.1016/j.physletb.2006.04.015
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/868597
dc.descriptionWe show that in 3-3-1 models there exist a natural relation among the SU(3)(L) coupling constant g, the electroweak mixing angle theta(W), the mass of the W, and one of the vacuum expectation values, which implies that those models can be realized at low energy scales and, in particular, even at the electroweak scale. So that, being that symmetries realized in Nature, new physics may be really just around the corner. (c) 2006 Elsevier B.V. All rights reserved.
dc.languageeng
dc.publisherElsevier B.V.
dc.relationPhysics Letters B
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subject3-3-1 model
dc.subjectneutral currents
dc.title3-3-1 models at electroweak scale
dc.typeOtro


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