Search results for "Tribimaximal mixing"

showing 4 items of 4 documents

S-4 as a natural flavor symmetry for lepton mixing

2008

Group theoretical arguments seem to indicate the discrete symmetry S4 as the minimal flavour symmetry compatible with tribimaximal neutrino mixing. We prove in a model independent way that indeed S4 can realize exact tribimaximal mixing through different symmetry breaking patterns. We present two models in which lepton tribimaximal mixing is realized in different ways and for each one we discuss the superpotential that leads to the correct breaking of the flavor symmetry.

Tribimaximal mixingPhysicsNuclear and High Energy PhysicsParticle physicsSpontaneous symmetry breakingSuperpotentialHigh Energy Physics::PhenomenologyFOS: Physical sciencesSymmetry (physics)High Energy Physics - PhenomenologyExplicit symmetry breakingHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSymmetry breakingMixing (physics)Discrete symmetryPhysical Review D
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Model for T2K indication with maximalθ23and trimaximalθ12

2011

Recently T2K experiment gives hint in favor of large reactor angle ${\ensuremath{\theta}}_{13}$. Most of the models, with tribimaximal mixing at the leading order, can not reproduce such a large mixing angle since they predict typically corrections for the reactor angle of the order ${\ensuremath{\theta}}_{13}\ensuremath{\sim}{\ensuremath{\lambda}}_{C}^{2}$, where ${\ensuremath{\lambda}}_{C}\ensuremath{\sim}0.2$. In this paper, we discuss the possibility to achieve large ${\ensuremath{\theta}}_{13}$ within the T2K region with maximal atmospheric mixing angle, ${sin}^{2}{\ensuremath{\theta}}_{23}=1/2$, and trimaximal solar mixing angle, ${sin}^{2}{\ensuremath{\theta}}_{12}=1/3$, through th…

Tribimaximal mixingPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsOrder (ring theory)LambdaMass matrix01 natural sciences0103 physical sciencesNeutrinoSymmetry (geometry)010306 general physicsMixing (physics)LeptonPhysical Review D
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Indication of electron neutrino appearance from an accelerator-produced off-axis muon neutrino beam

2011

The T2K experiment observes indications of $\nu_\mu\rightarrow \nu_e$ appearance in data accumulated with $1.43\times10^{20}$ protons on target. Six events pass all selection criteria at the far detector. In a three-flavor neutrino oscillation scenario with $|\Delta m_{23}^2|=2.4\times10^{-3}$ eV$^2$, $\sin^2 2\theta_{23}=1$ and $\sin^2 2\theta_{13}=0$, the expected number of such events is 1.5$\pm$0.3(syst.). Under this hypothesis, the probability to observe six or more candidate events is 7$\times10^{-3}$, equivalent to 2.5$\sigma$ significance. At 90% C.L., the data are consistent with 0.03(0.04)$<\sin^2 2\theta_{13}<$ 0.28(0.34) for $\delta_{\rm CP}=0$ and a normal (inverted) hierarchy.

Particle physicsFOS: Physical sciencesGeneral Physics and Astronomyddc:500.2CHOOZ01 natural sciencesParticle identificationHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)neutrino14.60.Pq 13.15.+g 25.30.Pt 95.55.Vj0103 physical sciencesneutrino oscillationMuon neutrino[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNeutrino oscillationGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSPhysicsNOνATribimaximal mixinghep-ex010308 nuclear & particles physicsT2K experimentFísicaT2K Collaborationparticle identificationElectron neutrinoexperimental resultsPhysical Review Letters
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Underlying A_4 Symmetry for the Neutrino Mass Matrix and the Quark Mixing Matrix

2002

The discrete non-Abelian symmetry $A_4$, valid at some high-energy scale, naturally leads to degenerate neutrino masses, without spoiling the hierarchy of charged-lepton masses. Realistic neutrino mass splittings and mixing angles (one of which is necessarily maximal and the other large) are then induced radiatively in the context of softly broken supersymmetry. The quark mixing matrix is also calculable in a similar way. The mixing parameter $U_{e3}$ is predicted to be imaginary, leading to maximal CP violation in neutrino oscillations. Neutrinoless double beta decay and $\tau \to \mu \gamma$ should be in the experimentally accessible range.

PhysicsTribimaximal mixingParticle physicsNuclear and High Energy PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaMass matrixHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)
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