6533b7d9fe1ef96bd126c38e
RESEARCH PRODUCT
Phenomenology of maximal and near-maximal lepton mixing
Yosef NirYosef NirCarlos Pena-garayM. C. Gonzalez-garciaAlexei Yu. Smirnovsubject
Nuclear and High Energy PhysicsParticle physicsAstrofísica nuclearRadiació solarSolar neutrinomedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaAstrophysicsAsymmetryPartícules (Física nuclear)High Energy Physics - ExperimentNuclear physicsDouble beta decayPhenomenological theory (Physics)Solar radiationmedia_commonParticles (Nuclear physics)PhysicsHigh Energy Physics::PhenomenologyFísicaObservableLeptonsSupernovaHigh Energy Physics - PhenomenologyLeptons (Nuclear physics)Fenomenologia (Física)High Energy Physics::ExperimentNuclear astrophysicsNeutrinoPhenomenology (particle physics)Leptondescription
We study the phenomenological consequences of maximal and near-maximal mixing of the electron neutrino with other ($x$=tau and/or muon) neutrinos. We describe the deviations from maximal mixing in terms of a parameter $\epsilon\equiv1-2\sin^2\theta_{ex}$ and quantify the present experimental status for $|\epsilon|<0.3$. We find that the global analysis of solar neutrino data allows maximal mixing with confidence level better than 99% for $10^{-8}$ eV$^2\lsim\Delta m^2\lsim2\times10^{-7}$ eV$^2$. In the mass ranges $\Delta m^2\gsim 1.5\times10^{-5}$ eV$^2$ and $4\times10^{-10}$ eV$^2\lsim\Delta m^2\lsim2\times10^{-7}$ eV$^2$ the full interval $|\epsilon|<0.3$ is allowed within 4$\sigma$(99.995 % CL). We suggest ways to measure $\epsilon$ in future experiments. The observable that is most sensitive to $\epsilon$ is the rate [NC]/[CC] in combination with the Day-Night asymmetry in the SNO detector. With theoretical and statistical uncertainties, the expected accuracy after 5 years is $\Delta \epsilon\sim 0.07$. We also discuss the effects of maximal and near-maximal $\nu_e$-mixing in atmospheric neutrinos, supernova neutrinos, and neutrinoless double beta decay.
year | journal | country | edition | language |
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2000-12-08 |