Physics – High Energy Physics – High Energy Physics - Phenomenology
Scientific paper
2004-08-10
Physics
High Energy Physics
High Energy Physics - Phenomenology
2 pages, talk at theYITP Workshop 2004 "Progress in Particle Physics"
Scientific paper
It 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.
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