Search results for "Double Beta Decay"

showing 10 items of 317 documents

Role of Single-Particle Energies in Microscopic Interacting Boson Model Double Beta Decay Calculations

2021

Single-particle level energies form a significant input in nuclear physics calculations where single-particle degrees of freedom are taken into account, including microscopic interacting boson model investigations. The single-particle energies may be treated as input parameters that are fitted to reach an optimal fit to the data. Alternatively, they can be calculated using a mean field potential, or they can be extracted from available experimental data, as is done in the current study. The role of single-particle level energies in the microscopic interacting boson model calculations is discussed with special emphasis on recent double beta decay calculations.

Physicslcsh:QC793-793.5single-particle energieslcsh:Elementary particle physicsDegrees of freedom (physics and chemistry)General Physics and Astronomyhiukkasfysiikkaneutrinoless double beta decayNuclear physicsMean field theorymicroscopic interacting boson modelDouble beta decayParticleInteracting boson modelydinfysiikka
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Occupation probabilities of single particle levels using the microscopic interacting boson model: Application to some nuclei of interest in neutrinol…

2016

We have developed a new method to calculate the occupancies of single particle levels in atomic nuclei. This method has been developed in the context of the microscopic interacting boson model, in which neutron and proton degrees of freedom are treated explicitly. The energies of the single particle levels constitute a very important input for the calculation of the occupancies in this method. In principle these energies can be considered as input parameters that can be fitted to reproduce the experimental occupancies. Instead of fitting, in this study we have extracted the single particle energies from experimental data on nuclei with a particle more or one particle less than a shell closu…

Physicsta114Proton010308 nuclear & particles physicsNuclear TheoryDegrees of freedom (physics and chemistry)double beta decayContext (language use)01 natural sciences7. Clean energyNuclear physicssingle particle levelsParticle decayatomic nucleimicroscopic interacting boson model0103 physical sciencesAtomic nucleusParticleNeutronInteracting boson modelAtomic physics010303 astronomy & astrophysicsPhysical Review C
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Neutrinoless double beta decay and QCD running at low energy scales

2018

There is a common belief that the main uncertainties in the theoretical analysis of neutrinoless double beta ($0\nu\beta\beta$) decay originate from the nuclear matrix elements. Here, we uncover another previously overlooked source of potentially large uncertainties stemming from non-perturbative QCD effects. Recently perturbative QCD corrections have been calculated for all dimension 6 and 9 effective operators describing $0\nu\beta\beta$-decay and their importance for a reliable treatment of $0\nu\beta\beta$-decay has been demonstrated. However, these perturbative results are valid at energy scales above $\sim 1$ GeV, while the typical $0\nu\beta\beta$-scale is about $\sim 100$ MeV. In vi…

Quantum chromodynamicsPhysicsCoupling constantParticle physics010308 nuclear & particles physicsScalar (mathematics)Perturbative QCDFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesTensorPerturbation theory (quantum mechanics)010306 general physicsPhysical Review
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Neutrino masses and mixing: a flavour symmetry roadmap

2012

Over the last ten years tri-bimaximal mixing has played an important role in modeling the flavour problem. We give a short review of the status of flavour symmetry models of neutrino mixing. We concentrate on non-Abelian discrete symmetries, which provide a simple way to account for the TBM pattern. We discuss phenomenological implications such as neutrinoless double beta decay, lepton flavour violation as well as theoretical aspects such as the possibility to explain quarks and leptons within a common framework, such as grand unified models

QuarkParticle physicsNuclear TheoryHigh Energy Physics::LatticeFlavourFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesneutrino mixingNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciences010306 general physicsMixing (physics)Physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaNeutrino massesCommon frameworkSymmetry (physics)High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoflavour symmetryLeptonFortschritte der Physik
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The neutrinoless double beta decay of 76Ge, 82Se, 86Kr, 114Cd, 128, 130Te and 134, 136Xe in the framework of a relativistic quark confinement model

1991

The half-life of the 0+ → 0+ neutrinoless double beta decay is calculated for 76Ge, 82Se, 86Kr, 114Cd, 128, 130Te and 134, 136Xe and the upper limit for the effective neutrino mass of 3.0 eV is deduced from available experimental data. In addition, the contribution of the right-handed charged weak currents to the effective weak hamiltonian is estimated. The relevant parameters attain the values |〈Λ〉| < 4.1 × 10−6 and |〈ν〉| < 6.6 × 10−8. The nucleonic weak current is treated starting from the current quark level and evaluating the quark current using relativistic quark wave functions obtained from a Dirac equation with a harmonic confinement potential. The nuclear matrix elements of the thus…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsCurrent quarkNuclear physicssymbols.namesakeDirac equationDouble beta decaysymbolsHigh Energy Physics::ExperimentColor confinementNeutrinoWave functionRandom phase approximationNuclear Physics A
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Neutrinoless double beta decay in the dualized standard model

2001

The Dualized Standard Model offers a {\it raison d'\^etre} for 3 fermion generations and an explanation for their distinctive mass and mixing patterns, reproducing to a reasonable accuracy the empirical mixing matrix and mass spectrum for both quarks and leptons in terms of just a few parameters. With its parameters thus fixed, the result is a highly predictive framework. In particular, it is shown that it gives explicit parameter-free predictions for neutrinoless double beta decays. For $^{76}Ge$, it predicts a half-life of $10^{28}-10^{30}$ years, which satisfies the present experimental lower bound of $1.8 \times 10^{25}$ years.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesFísicaFermionUpper and lower boundsStandard ModelHigh Energy Physics - PhenomenologyMatrix (mathematics)High Energy Physics - Phenomenology (hep-ph)Double beta decayMixing (physics)LeptonPhysical Review D
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New leptoquark mechanism of neutrinoless double beta decay

1996

A new mechanism for neutrinoless double beta ($\znbb$) decay based on leptoquark exchange is discussed. Due to the specific helicity structure of the effective four-fermion interaction this contribution is strongly enhanced compared to the well-known mass mechanism of $\znbb$ decay. As a result the corresponding leptoquark parameters are severely constrained from non-observation of $\znbb$-decay. These constraints are more stringent than those derived from other experiments.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesLepton numberHelicityNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayLeptoquarkBeta (velocity)High Energy Physics::ExperimentNeutrinoLepton
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Confined quarks and the neutrinoless ββ decay

1990

Abstract The half life of the neutrinoless double beta decay of 76Ge into the ground state of 76Se is calculated in a relativistic quark confinement model. The neutron-proton quasi-particle random phase approximation is used to evaluate the nuclear matrix elements involved in the decay amplitude. We avoid the closure approximation, but compare our results with this approximation. From the experimental half life we deduce an upper limit for the Majorana mass of the neutrino and estimate the right-handed contribution to the charged weak current.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryForm factor (quantum field theory)Nuclear physicsMAJORANADouble beta decayHigh Energy Physics::ExperimentColor confinementNeutrinoRandom phase approximationGround statePhysics Letters B
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Supersymmetry and neutrinoless double beta decay.

1996

Neutrinoless double beta decay ($\znbb$) induced by superparticle exchange is investigated. Such a supersymmetric (SUSY) mechanism of $\znbb$ decay arises within SUSY theories with R-parity non-conservation (\rp). We consider the minimal supersymmetric standard model (MSSM) with explicit \rp terms in the superpotential (\rp MSSM). The decay rate for the SUSY mechanism of $\znbb$ decay is calculated. Numerical values for nuclear matrix elements for the experimentally most interesting isotopes are calculated within pn-QRPA. Constraints on the \rp MSSM parameter space are extracted from current experimental half-life limits. The most stringent limits are derived from data on $^{76}$Ge. It is s…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsSuperpotentialHigh Energy Physics::PhenomenologyForm factor (quantum field theory)FOS: Physical sciencesSuperpartnerFísicaSupersymmetryStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Double beta decayHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelPhysical review. D, Particles and fields
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Relating quarks and leptons with the T7 flavour group

2015

In this letter we present a model for quarks and leptons based on T7 as flavour symmetry, predicting a canonical mass relation between charged leptons and down-type quarks proposed earlier. Neutrino masses are generated through a Type-I seesaw mechanism, with predicted correlations between the atmospheric mixing angle and neutrino masses. Compatibility with oscillation results lead to lower bounds for the lightest neutrino mass as well as for the neutrinoless double beta decay rates, even for normal neutrino mass hierarchy.

QuarkPhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicalcsh:QC1-999Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismDouble beta decayddc:530High Energy Physics::ExperimentNeutrinoNeutrino oscillationlcsh:PhysicsLepton
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