How to Evade a No-Go Theorem in Flavor Symmetries

dc.creatorKoide, Yoshio
dc.date2008-01-23
dc.date.accessioned2026-07-07T11:55:27Z
dc.date.available2026-07-07T11:55:27Z
dc.descriptionA no-go theorem in flavor symmetries is reviewed. The theorem asserts that we cannot bring any flavor symmetry into mass matrix model in which number of Higgs scalars is, at most, one for each sector (e.g. H_u and H_d for up- and down-quark sectors, respectively). Such the strong constraint comes from the SU(2)_L symmetry. Possible three options to evade the theorem are discussed.
dc.description10 pages, no figure, talk given at International Workshop on Grand Unified Theories: Current Status and Future Prospects, Kusatsu, Japan, December 17 - 19, 2007
dc.identifierhttps://arxiv.org/abs/0801.3491
dc.identifierhttp://arxiv.org/abs/0801.3491
dc.identifierAIPConf.Proc.1015:80-86,2008
dc.identifierdoi:10.1063/1.2939063
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/205248
dc.subjectHigh Energy Physics - Phenomenology
dc.titleHow to Evade a No-Go Theorem in Flavor Symmetries
dc.typetext

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