The observability of an additional discrete symmetry in the Standard Model

dc.creatorZubkov, M. A.
dc.date2006-09-04
dc.date2007-09-19
dc.date.accessioned2026-07-07T11:05:40Z
dc.date.available2026-07-07T11:05:40Z
dc.descriptionStandard Model may be defined with the additional discrete symmetry, i.e. with the gauge group $SU(3)\times SU(2) \times U(1)/{\cal Z}$ (${\cal Z} = Z_6$, $Z_3$ or $Z_2$) instead of the usual $SU(3)\times SU(2) \times U(1)$. It has the same perturbation expansion as the conventional one. However, it may describe nature in a different way at the energies compared to the triviality bound (of about 1 Tev). In this paper we present a possibility to observe this difference assuming that the gauge group of the Standard Model is embedded into the gauge group of an {\it a priory} unknown model, which describes physics at a Tev scale. This difference is related to the monopole content of the theory. We illustrate our results by consideration of the Petite Unification of quarks and leptons.
dc.descriptionLatex, 10 pages
dc.identifierhttps://arxiv.org/abs/hep-ph/0609029
dc.identifierhttp://arxiv.org/abs/hep-ph/0609029
dc.identifierPhys.Lett.B649:91-94,2007; Erratum-ibid.B655:91,2007
dc.identifierdoi:10.1016/j.physletb.2007.04.005; 10.1016/j.physletb.2007.09.026
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/189273
dc.subjectHigh Energy Physics - Phenomenology
dc.titleThe observability of an additional discrete symmetry in the Standard Model
dc.typetext

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