Comments on a Flavor Symmetry

dc.creatorKoide, Yoshio
dc.date2004-08-10
dc.date.accessioned2026-07-07T03:53:07Z
dc.date.available2026-07-07T03:53:07Z
dc.descriptionIt is pointed out that if a flavor symmetry (a discrete symmetry, a U(1) symmetry, and so on) exists, we cannot obtain the observed CKM quark mixing matrix V_q and MNS lepton mixing matrix U_\ell, even if we can obtain reasonable mass spectra under the symmetry. Such the serious constraint is derived only from the SU(2)_L conditions, and we will not assume any explicit flavor symmetry and/or any explicit mass matrix forms. And then, we will discuss the meaning of the severe constraint.
dc.description2 pages, talk at theYITP Workshop 2004 "Progress in Particle Physics"
dc.identifierhttps://arxiv.org/abs/hep-ph/0408126
dc.identifierhttp://arxiv.org/abs/hep-ph/0408126
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/43713
dc.subjectHigh Energy Physics - Phenomenology
dc.titleComments on a Flavor Symmetry
dc.typetext

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