Search results for "decay"

showing 10 items of 2087 documents

Observable Majoron emission in neutrinoless double beta decay

1992

We consider a class of simplest Majoron models where neutrino- majoron couplings can be in the range $g \sim 10^{-5}-10^{-3}$ leading to the observability of neutrinoless double beta decay with majoron emission. The majoron is a singlet of the electroweak gauge symmetry, thus avoiding conflict with the LEP data on Z decay, which rules out the triplet and doublet majoron models.

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayHigh Energy Physics::ExperimentSinglet stateNeutrinoNuclear ExperimentMajoronGauge symmetry
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Neutrinoless double beta decay in supersymmetry with bilinear R-parity breaking

1998

We reanalyze the contributions to neutrinoless double beta ($\znbb$) decay from supersymmetry with explicit breaking of R-parity. Although we keep both bilinear and trilinear terms, our emphasis is put on bilinear R-parity breaking terms, because these mimic more closely the models where the breaking of R-parity is spontaneous. Comparing the relevant Feynman diagrams we conclude that the usual mass mechanism of double beta decay is the dominant one. From the non-observation of $\znbb$ decay we set limits on the bilinear R-parity breaking parameters of typically a (few) 100 $keV$. Despite such stringent bounds, we stress that the magnitude of R-parity violating phenomena that can be expected…

PhysicsNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesBilinear interpolationFísicaSupersymmetryFirst generationThird generationHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Double beta decayR-paritysymbolsFeynman diagramBeta (velocity)High Energy Physics::Experiment
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NUCLEAR MATRIX ELEMENTS FOR DOUBLE BETA DECAY

2008

The neutrinoless double beta (0νββ) decay of atomic nuclei plays a key role in the search for massive Majorana neutrinos and their mass scale. To extract the necessary information from the measured data the nuclear-structure effects have to be accounted for by computation of the associated nuclear matrix elements (NME's). In this article the NME's for the light-neutrino exchange mechanism are discussed. They are computed by using the proton-neutron quasiparticle random-phase approximation (pnQRPA). Recent developments in this field relate to the handling of the nucleon-nucleon short-range correlations and independent experimental probes of the wave functions relevant for the NME's.

PhysicsNuclear and High Energy PhysicsParticle physicsField (physics)ComputationNuclear TheoryGeneral Physics and AstronomyNuclear physicsMAJORANADouble beta decayAtomic nucleusQuasiparticleBeta (velocity)NeutrinoNuclear ExperimentInternational Journal of Modern Physics E
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Tri-bimaximal neutrino mixing and neutrinoless double beta decay

2008

We present a tri-bimaximal lepton mixing scheme where the neutrinoless double beta decay rate (bb0v) has a lower bound which correlates with the ratio alpha = Dmsol/Dmatm well determined by current data, as well as with the unknown Majorana CP phase phi12 characterizing the solar neutrino sub-system. For the special value phi12 = pi/2 (opposite CP-sign neutrinos) the bb0v rate vanishes at tree level when Dmsol/Dmatm = 3/80, only allowed at 3 sigma. For all other cases the rate is nonzero, and lies within current and projected experimental sensitivities close to phi12=0. We suggest two model realizations of this scheme in terms of an A4xZ2 and A4xZ4 flavour symmetries.

PhysicsNuclear and High Energy PhysicsParticle physicsFísicaFOS: Physical sciencesTree (descriptive set theory)MAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayCP violationSensitivity (control systems)NeutrinoNeutrino oscillationLepton
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Search forWWandWZResonances Decaying to Electron, MissingET, and Two Jets inpp¯Collisions ats=1.96  TeV.

2009

We present a search for WW and WZ production in final states that contain a charged lepton (electron or muon) and at least two jets, produced in {radical}(s)=1.96 TeV pp collisions at the Fermilab Tevatron, using data corresponding to 1.2 fb{sup -1} of integrated luminosity collected with the CDF II detector. Diboson production in this decay channel has yet to be observed at hadron colliders due to the large single W plus jets background. An artificial neural network has been developed to increase signal sensitivity, as compared with an event selection based on conventional cuts. We set a 95% confidence level upper limit of {sigma}{sub WW}xBR(W{yields}l{nu}{sub l},W{yields}jets)+{sigma}{sub…

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonMuon010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyElementary particleCoupling (probability)01 natural sciencesStandard ModelNuclear physicsMassless particleParticle decay0103 physical sciencesProduction (computer science)High Energy Physics::ExperimentSensitivity (control systems)010306 general physicsLeptonBosonPhysical Review Letters
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A realistic model of neutrino masses with a large neutrinoless double beta decay rate

2011

The minimal Standard Model extension with the Weinberg operator does accommodate the observed neutrino masses and mixing, but predicts a neutrinoless double beta ($0\nu\beta\beta$) decay rate proportional to the effective electron neutrino mass, which can be then arbitrarily small within present experimental limits. However, in general $0\nu\beta\beta$ decay can have an independent origin and be near its present experimental bound; whereas neutrino masses are generated radiatively, contributing negligibly to $0\nu\beta\beta$ decay. We provide a realization of this scenario in a simple, well defined and testable model, with potential LHC effects and calculable neutrino masses, whose two-loop…

PhysicsNuclear and High Energy PhysicsParticle physicsHiggs PhysicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesType (model theory)Quantum numberPartícules (Física nuclear)Neutrino physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Standard-Model ExtensionDouble beta decayBeyond Standard ModelHigh Energy Physics::ExperimentConnection (algebraic framework)NeutrinoElectron neutrinoLepton
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Final State Interactions in Kaon Decays

2001

27 páginas, 1 figura, 2 tablas.-- PACS: 13.25.Es; 11.30.Er; 13.85.Fb; 11.55.Fv.-- arXiv:hep-ph/0007208v1

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Lattice (hep-lat)Phase (waves)FOS: Physical sciencesFísicaState (functional analysis)Final state interactionsStandard ModelHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics - LatticeKaon decays
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Status and implications of neutrino masses: a brief panorama

2015

15 pages.- 10 figures

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeElectroweak interactionDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstronomy and AstrophysicsFlavor symmetryAstrophysics::Cosmology and Extragalactic AstrophysicsAtomic and Molecular Physics and OpticsCosmologyNeutrino mixing and oscillationsHigh Energy Physics - PhenomenologyQuark-lepton unificationHigh Energy Physics - Phenomenology (hep-ph)Double beta decayHiggs bosonCP violationSeesaw mechanismHigh Energy Physics::ExperimentNeutrinoLepton
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Correlation between flavour violating decay of long-lived slepton and tau in the coannihilation scenario with Seesaw mechanism

2011

We investigate flavour violating decays of the long-lived lightest slepton and the tau lepton in the coannihilation region of the Minimal Supersymmetric Standard Model with a Seesaw mechanism to generate neutrino masses. We consider a situation where the mass difference between the lightest neutralino, as the Lightest Supersymmetric particle (LSP), and the lightest slepton, as the Next-to-LSP, is smaller than the mass of tau lepton. In this situation, the lifetime of the lightest slepton is very long and it is determined by lepton flavour violating (LFV) couplings because the slepton mainly consists of the lighter stau and the flavour conserving 2-body decay is kinematically forbidden. We s…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesLightest Supersymmetric ParticleNuclear physicsParticle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismNeutralinoGrand Unified TheoryHigh Energy Physics::ExperimentNeutrinoMinimal Supersymmetric Standard ModelLepton
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Inverse tribimaximal type-III seesaw mechanism and lepton flavor violation

2009

We present a type-III version of inverse seesaw or, equivalently an inverse version of type-III seesaw. Naturally small neutrino masses arise at low-scale from the exchange of neutral fermions transforming as hyperchargeless SU(2) triplets. In order to implement tri-bimaximal lepton mixing we supplement the minimal SU(3)xSU(2)xU(1) gauge symmetry with an A4-based flavor symmetry. Our scenario induces lepton flavour violating (LFV) three body decays that can proceed at the tree level, while radiative li to lj gamma decays and mu-e conversion in nuclei are also expected to be sizeable. LFV decays are related by the underlying flavor symmetry and the new fermions are also expected to be access…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyRadiative decayInverseFísicaType (model theory)Particle decaySeesaw mechanismHigh Energy Physics::ExperimentNeutrinoLepton
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