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Neutrino masses, mixing, and oscillations in the S4 model of permutation symmetry
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Citations
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References
1984
Year
Neutrino PropertyNuclear PhysicsPhysicsSimplest Possible SchemeNatural SciencesLong Baseline Neutrino ExperimentParticle PhysicsQuantum Field TheoryS4 ModelSymmetry (Physics)Neutrino PhysicNeutrino MassesMixing MatrixPermutation Symmetry
In the ${\mathrm{S}}_{4}$ model, we work out the simplest possible scheme for neutrino masses. We find that ${\ensuremath{\nu}}_{e}$ and ${\ensuremath{\nu}}_{\ensuremath{\mu}}$ have dominant massless components but not ${\ensuremath{\nu}}_{\ensuremath{\tau}}$. The mixing matrix is completely determined and ${\ensuremath{\nu}}_{e}\ensuremath{-}{\ensuremath{\nu}}_{\ensuremath{\tau}}$ and ${\ensuremath{\nu}}_{\ensuremath{\mu}}\ensuremath{-}{\ensuremath{\nu}}_{\ensuremath{\tau}}$ oscillations are possible with known mixing angles and only one $\ensuremath{\delta}{m}^{2}$.
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