Realistic Quark and Lepton Masses through SO(10) Symmetry

preprint1995arXivOpen access

Abstract

In a recent paper a model of quark and lepton masses was proposed. Without any family symmetries almost all the qualitative and quantitative features of the quark and lepton masses and Kobayashi-Maskawa mixing angles are explained, primarily as consequences of various aspects of SO(10)SO(10) symmetry. Here the model is discussed in much greater detail. The threefold mass hierarchy as well as the relations mτ0≃mb0, mμ0≃3ms0, me0≃13md0, mu0/mt0≪md0/mb0, tanθC≃md0/ms0, Vcb≪ms0/mb0m_τ^0 \simeq m_b^0, ~m_μ^0 \simeq 3m_s^0,~ m_e^0 \simeq {1 \over 3} m_d^0, ~m_u^0/m_t^0 \ll m_d^0/m_b^0, ~{\rm tan}θ_C \simeq \sqrt{m_d^0/m_s^0},~ V_{cb} \ll \sqrt{m_s^0/m_b^0} and Vub∼VusVcbV_{ub} \sim V_{us}V_{cb} follow from a simple Yukawa structure at the unification scale. The model also gives definite predictions for tan⁡β\tan β, the neutrino mixing angles, and proton decay branching ratios. The (νμ−ντ)(ν_μ-ν_τ) mixing angle is typically large, tanββ is close to either mt0/mb0m_t^0/m_b^0 or mc0/ms0m_c^0/m_s^0, and proton decay is in the observable range, but there is a group theoretical suppression factor in the rate.

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