dc.contributorUniversidade Tecnológica Federal Do Paraná-UTFPR-DAFIS
dc.contributorUniversidade Federal do ABC (UFABC)
dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2014-05-27T11:29:29Z
dc.date.available2014-05-27T11:29:29Z
dc.date.created2014-05-27T11:29:29Z
dc.date.issued2013-05-10
dc.identifierPhysical Review D - Particles, Fields, Gravitation and Cosmology, v. 87, n. 9, 2013.
dc.identifier1550-7998
dc.identifier1550-2368
dc.identifierhttp://hdl.handle.net/11449/75380
dc.identifier10.1103/PhysRevD.87.095004
dc.identifierWOS:000318772100011
dc.identifier2-s2.0-84877936409
dc.identifier2-s2.0-84877936409.pdf
dc.description.abstractWe verify that SU(N)TC⊗ - SU(3) L⊗ - U(1)X models, where the gauge symmetry breaking is totally dynamical and promoted by the non-Abelian technicolor group and the strong Abelian interactions, are quite constrained by the LHC data. The theory contains a T quark self-energy involving the mixing between the neutral gauge bosons, which introduces the coupling between the light and heavy composite scalar bosons of the model. We determine the lightest scalar boson mass for these models from an effective action for composite operators, assuming details about the dynamics of the strong interaction theories. Comparing the value of this mass with the ATLAS and CMS observation of a new boson with a mass M∼125 GeV and considering the lower bound determined by the LHC Collaboration on the heavy neutral gauge boson (Z′) present in these models, we can establish constraints on the possible models. For example, if SU(N)TC≡SU(2)TC, with technifermions in the fundamental representation, the model barely survives the confrontation with the LHC data. © 2013 American Physical Society.
dc.languageeng
dc.relationPhysical Review D: Particles, Fields, Gravitation and Cosmology
dc.rightsAcesso restrito
dc.sourceScopus
dc.title125 GeV scalar boson and SU(NTC)⊗ - SU(3) L⊗ - U(1)X models
dc.typeArtículos de revistas


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