Search results for "Majoron"

showing 10 items of 50 documents

Lepton flavour violating decay of the Z0 in the scalar triplet model

1987

Abstract The lepton flavour violating Z→μme, Z→μτ and Z→eτ decays are evaluated in the framework of the majoron triplet model of Gelmini and Roncadelli. The process is dominated by the diagrams with charged scalars in the loops, so the GIM cancellation is avoided. We obtain branching ratios for Z→μτ and Z→eτ which might be detectable at SLC and/or LEP.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsFlavourScalar (mathematics)High Energy Physics::PhenomenologyFísicaHigh Energy Physics::ExperimentLeptonMajoronParticle Physics - Phenomenology
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Leptogenesis from oscillations and dark matter

2019

An extension of the Standard Model with Majorana singlet fermions in the 1–100 GeV range can explain the light neutrino masses and give rise to a baryon asymmetry at freeze-in of the heavy states, via their CP-violating oscillations. In this paper we consider extending this scenario to also explain dark matter. We find that a very weakly coupled B−L gauge boson, an invisible QCD axion model, and the singlet majoron model can simultaneously account for dark matter and the baryon asymmetry.

Particle physicsPhysics and Astronomy (miscellaneous)Dark matterFOS: Physical scienceslcsh:AstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics7. Clean energy01 natural sciencesStandard ModelHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetrylcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsEngineering (miscellaneous)AxionMajoronPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyLeptogenesislcsh:QC770-798High Energy Physics::ExperimentNeutrinoThe European Physical Journal C
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Detailed studies of $^{100}$Mo two-neutrino double beta decay in NEMO-3

2019

The full data set of the NEMO-3 experiment has been used to measure the half-life of the two-neutrino double beta decay of $^{100}$Mo to the ground state of $^{100}$Ru, $T_{1/2} = \left[ 6.81 \pm 0.01\,\left(\mbox{stat}\right) ^{+0.38}_{-0.40}\,\left(\mbox{syst}\right) \right] \times10^{18}$ y. The two-electron energy sum, single electron energy spectra and distribution of the angle between the electrons are presented with an unprecedented statistics of $5\times10^5$ events and a signal-to-background ratio of ~80. Clear evidence for the Single State Dominance model is found for this nuclear transition. Limits on Majoron emitting neutrinoless double beta decay modes with spectral indices of …

Particle physicsS029MTPhysics and Astronomy (miscellaneous)FOS: Physical sciencesElementary particle[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exinvariance: Lorentz01 natural sciences7. Clean energyneutrinoless double beta decaydecay modesPhysics Particles & Fieldsdouble-beta decay: (0neutrino)SEARCHDouble beta decay0103 physical sciencesground stateNuclear Experiment (nucl-ex)010306 general physics0206 Quantum PhysicsEngineering (miscellaneous)Nuclear ExperimentMajoronS076H2NPhysicsScience & TechnologyHALF-LIFE010308 nuclear & particles physicsPhysicsMO-100High Energy Physics::PhenomenologyNuclear & Particles PhysicsMajoronviolation: Lorentznucleus: transitionSTATESstatisticsPhysical Sciences0202 Atomic Molecular Nuclear Particle and Plasma Physicsspectralelectron: energy spectrumHigh Energy Physics::ExperimentNeutrinoGround stateEnergy (signal processing)Radioactive decayLepton
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Majorons and supernova cooling

1990

We consider the role of Majoron emission in supernova cooling and its implications for the neutrino mass and lifetime in generic single Majoron models. It is found that, for ${\ensuremath{\nu}}_{\ensuremath{\tau}}$ with mass $m$, if the lifetime for the decay ${\ensuremath{\nu}}_{\ensuremath{\tau}}\ensuremath{\rightarrow}\mathrm{Majoron}+{\ensuremath{\nu}}_{e,\ensuremath{\mu}}$ is shorter than ${10}^{\ensuremath{-}7}$ (m/MeV) sec, then Majorons are so strongly trapped by the inverse process that the resulting Majoron luminosity is small enough not to destabilize the observed ${\ensuremath{\nu}}_{e}$ pulse from SN 1987A. For ${\ensuremath{\nu}}_{\ensuremath{\tau}}$ with a longer lifetime, th…

PhysicsAstrofísicaParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyInverseElementary particlePartícules (Física nuclear)LuminosityNuclear physicsSupernovaHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentEnergy (signal processing)LeptonMajoron
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Bounds on new Majoron models from the Heidelberg-Moscow experiment

1996

In recent years several new Majoron models were invented to avoid shortcomings of the classical models while leading to observable decay rates in double beta experiments. We give the first experimental half life bounds on double beta decays with new Majoron emission and derive bounds on the effective neutrino--Majoron couplings from the data of the $^{76}Ge$ HEIDELBERG--MOSCOW experiment. While stringent half life limits for all decay modes and the coupling constants of the classical models were obtained, small matrix elements and phase space integrals \cite{hir95,pae95} result in much weaker limits on the effective coupling constants of the new Majoron models.

PhysicsCouplingCoupling constantNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableMatrix (mathematics)Double beta decayPhase spaceNuclear Experiment (nucl-ex)NeutrinoNuclear ExperimentNuclear ExperimentMajoron
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Measurement of the double-βdecay half-life ofNd150and search for neutrinoless decay modes with the NEMO-3 detector

2009

The half-life for double-{beta} decay of {sup 150}Nd has been measured by the NEMO-3 experiment at the Modane Underground Laboratory. Using 924.7 days of data recorded with 36.55 g of {sup 150}Nd, we measured the half-life for 2{nu}{beta}{beta} decay to be T{sub 1/2}{sup 2{nu}}=(9.11{sub -0.22}{sup +0.25}(stat.){+-}0.63(syst.))x10{sup 18} yr. The observed limit on the half-life for neutrinoless double-{beta} decay is found to be T{sub 1/2}{sup 0{nu}}>1.8x10{sup 22} yr at 90% confidence level. This translates into a limit on the effective Majorana neutrino mass of <4.0-6.3 eV if the nuclear deformation is taken into account. We also set limits on models involving Majoron emission, right-hand…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElementary particle7. Clean energy01 natural sciencesBeta decayNuclear physicsMAJORANADouble beta decay0103 physical sciencesNeutrino010306 general physicsRadioactive decayMajoronLeptonPhysical Review C
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A(4)-based neutrino masses with Majoron decaying dark matter

2010

We propose an A(4) flavor-symmetric SU(3) circle times SU(2) circle times U(1) seesaw model where lepton number is broken spontaneously. A consistent two-zero texture pattern of neutrino masses and mixing emerges from the interplay of type-I and type-II seesaw contributions, with important phenomenological predictions. We show that, if the Majoron becomes massive, such seesaw scenario provides a viable candidate for decaying dark matter, consistent with cosmic microwave background lifetime constraints that follow from current WMAP observations. We also calculate the subleading one-loop-induced decay into photons which leads to a monoenergetic emission line that may be observed in future x-r…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelCosmic microwave backgroundDark matterHigh Energy Physics::PhenomenologyCosmic background radiationFísicaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciences7. Clean energyLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesNeutrino010306 general physicsMajoronParticle Physics - Phenomenology
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Spontaneous proton decay and the origin of Peccei-Quinn symmetry

2019

We propose a new interpretation of Peccei-Quinn symmetry within the Standard Model, identifying it with the axial $B + L$ symmetry i.e. $U(1)_{PQ} \equiv U(1)_{\gamma_5(B+L)}$. This new interpretation retains all the attractive features of Peccei-Quinn solution to strong CP problem but in addition also leads to several other new and interesting consequences. Owing to the identification $U(1)_{PQ} \equiv U(1)_{\gamma_5(B+L)}$ the axion also behaves like Majoron inducing small seesaw masses for neutrinos after spontaneous symmetry breaking. Another novel feature of this identification is the phenomenon of spontaneous (and also chiral) proton decay with its decay rate associated with the axion…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsProton decaySpontaneous symmetry breakingPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural scienceslcsh:QC1-999Symmetry (physics)Standard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesStrong CP problem010306 general physicsAxionlcsh:PhysicsMajoron
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Dark matter as the origin of neutrino mass in the inverse seesaw mechanism

2021

We propose that neutrino masses are "seeded" by a dark sector within the inverse seesaw mechanism. This way we have a new, "hidden", variant of the scotogenic scenario for radiative neutrino masses. We discuss both explicit and dynamical lepton number violation. In addition to invisible Higgs decays with majoron emission, we discuss in detail the pheneomenolgy of dark matter, as well as the novel features associated to charged lepton flavour violation, and neutrino physics.

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)PhysicsQC1-999High Energy Physics::PhenomenologyDark matterFOS: Physical sciencesLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismRadiative transferHiggs bosonHigh Energy Physics::ExperimentNeutrinoAstrophysics - Cosmology and Nongalactic AstrophysicsMajoronLeptonPhysics Letters B
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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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