2013
DOI: 10.1093/ptep/ptt067
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Revisiting the Higgs sector of a 3-3-1 model in light of the 126 GeV signal at the LHC

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Cited by 11 publications
(6 citation statements)
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“…A detailed analysis of the scalar spectrum could supply interesting results with regard to their masses and couplings. In the case of 3-3-1 models with no exotic electric charges, the author succeded in proving that only two physical Higgses survive the SSB [18,32], while the third one comes out massless and sterile (with no couplings at all). Some of them could also be put forward as plausible DM candidates.…”
Section: Boson Mass Spectrummentioning
confidence: 99%
“…A detailed analysis of the scalar spectrum could supply interesting results with regard to their masses and couplings. In the case of 3-3-1 models with no exotic electric charges, the author succeded in proving that only two physical Higgses survive the SSB [18,32], while the third one comes out massless and sterile (with no couplings at all). Some of them could also be put forward as plausible DM candidates.…”
Section: Boson Mass Spectrummentioning
confidence: 99%
“…For the new massive fermions, the resulting couplings overlap with those obtained in the literature in the canonical approach. With regard to the SSB mechanism SU(n) L ⊗ U(1) Y → U(1) em induced in one step conceived by Cotȃescu in the general method [70], the author also proved its compatibility [33,40] with the Higgs mechanism in two steps largely used in the literature for 3-3-1 and 3-4-1 models. For each particular model inferred in section 4, one can work out a specific phenomenology (see for instance the author's papers [26,33,59]).…”
Section: A Palcumentioning
confidence: 88%
“…With regard to the SSB mechanism SU(n) L ⊗ U(1) Y → U(1) em induced in one step conceived by Cotȃescu in the general method [70], the author also proved its compatibility [33,40] with the Higgs mechanism in two steps largely used in the literature for 3-3-1 and 3-4-1 models. For each particular model inferred in section 4, one can work out a specific phenomenology (see for instance the author's papers [26,33,59]). One more advantage of this method resides in the fact that the diagonalization of the neutral bosons' matrix with the SM-restriction between W and Z allows for getting b = f(a) and thus the whole mass spectrum becomes a one-parameter spectrum (see for example [26,33,59].…”
Section: A Palcumentioning
confidence: 88%
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