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arxiv: hep-ph/9811282 · v2 · pith:REGA3GUSnew · submitted 1998-11-09 · ✦ hep-ph

Neutrino Oscillations and Other Key Issues in Supersymmetric SU(4)_c times SU(2)_L times SU(2)_R

classification ✦ hep-ph
keywords neutrinosymmetrytimesmassoscillationsexplanationissuesmssm
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We try to gain an understanding of the recent Superkamiokande data on neutrino oscillations and several other important phenomenological issues within the framework of supersymmetric $SU(4)_c \times SU(2)_L \times SU(2)_R$ ($\equiv G_{422}$). By supplementing $G_{422}$ with a U(1)-${\cal R}$ symmetry, we can provide an explanation of the magnitude $M_G$ ($\sim 10^{16}$ GeV) of the $G_{422}$- symmetry breaking scale, resolve the MSSM $\mu $ problem, and understand why proton decay has not been seen ($\tau_p \gg 10^{34}$ yr). The family dependent ${\cal R}$ - symmetry also helps provide an explanation of the charged fermion mass hierarchies as well as the magnitudes of the CKM matrix elements. Several additional heavy states in the mass range $10^4-10^7$ GeV are predicted, and the MSSM parameter $\tan \beta $ turns out to be of order unity. The atmospheric neutrino problem is explained through $\nu_{\mu}-\nu_{\tau}$ mixing with $\sin^2 2\theta_{\mu \tau}\simeq 1$. The resolution of the solar neutrino puzzle is via the small angle MSW oscillations and necessarily requires a sterile neutrino $\nu_s$ which, thanks to the ${\cal R}$ - symmetry, has a tiny mass.

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