Search results for "Discrete and Finite Symmetries"

showing 3 items of 3 documents

Bilinear R-parity violation with flavor symmetry

2012

Bilinear R-parity violation (BRPV) provides the simplest intrinsically supersymmetric neutrino mass generation scheme. While neutrino mixing parameters can be probed in high energy accelerators, they are unfortunately not predicted by the theory. Here we propose a model based on the discrete flavor symmetry Lambda(4) with a single R-parity violating parameter, leading to (i) correct Cabbibo mixing given by the Gatto-Sartori-Tonin formula, and a successful unification-like b-tau mass relation, and (ii) a correlation between the lepton mixing angles theta(13) and theta(23) in agreement with recent neutrino oscillation data, as well as a (nearly) massless neutrino, leading to absence of neutri…

Particle physicsNuclear and High Energy PhysicsSupersymmetric Standard ModelFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)R-parityDouble beta decay0103 physical sciencesDiscrete and Finite SymmetriesNeutrino Physics010306 general physicsNeutrino oscillationMixing (physics)Physics010308 nuclear & particles physicsComputer Science::Information RetrievalMass generationHigh Energy Physics::PhenomenologyFísicaMassless particleHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard ModelHigh Energy Physics::ExperimentNeutrinoLepton
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The minimal adjoint-SU (5) x Z(4) GUT model

2013

An extension of the adjoint SU (5) model with a flavour symmetry based on the Z(4) group is investigated. The Z(4) symmetry is introduced with the aim of leading the up-and down-quark mass matrices to the Nearest-Neighbour-Interaction form. As a consequence of the discrete symmetry embedded in the SU (5) gauge group, the charged lepton mass matrix also gets the same form. Within this model, light neutrinos get their masses through type-I, type-III and one-loop radiative seesaw mechanisms, implemented, respectively, via a singlet, a triplet and an octet from the adjoint fermionic 24 fields. It is demonstrated that the neutrino phenomenology forces the introduction of at least three 24 fermio…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsProton decayHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica01 natural sciencesSymmetry (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryGauge group0103 physical sciencesHiggs bosonDiscrete and Finite SymmetriesHigh Energy Physics::ExperimentNeutrino PhysicsGUTNeutrino010306 general physicsLeptonDiscrete symmetry
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Probing CPT in transitions with entangled neutral kaons

2015

In this paper we present a novel CPT symmetry test in the neutral kaon system based, for the first time, on the direct comparison of the probabilities of a transition and its CPT reverse. The required interchange of in ↔ out states for a given process is obtained exploiting the Einstein-Podolsky-Rosen correlations of neutral kaon pairs produced at a ϕ-factory. The observable quantities have been constructed by selecting the two semileptonic decays for flavour tag, the ππ and 3π 0 decays for CP tag and the time orderings of the decay pairs. The interpretation in terms of the standard Weisskopf-Wigner approach to this system, directly connects CPT violation in these observables to the violati…

PhysicsNuclear and High Energy PhysicsParticle physicsCPT symmetryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableQuantum entanglementDiscrete and finite symmetries; Kaon Physics; CP violationMass matrixHigh Energy Physics - PhenomenologyKaon Physicssymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)CP violationsymbolsCP violationDiscrete and finite symmetriesHigh Energy Physics::ExperimentEPR paradoxSensitivity (control systems)Spurious relationshipJournal of High Energy Physics
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