Search results for "decay"

showing 10 items of 2087 documents

Double beta decay: an interface between nuclear, particle and atomic physics

2013

General properties of the nuclear matrix elements (NMEs) related to the various modes of neutrinoless double β decays are examined and analyzed. The decays include the electron-emitting double beta-minus decays β−β− and the various positron-emitting/electron capture decays. Special interest is devoted to the neutrinoless double electron capture decay with a resonance condition.

PhysicsHistoryParticle physicsElectron captureResonance (particle physics)Beta decayComputer Science ApplicationsEducationNuclear physicsDouble beta decayParticleHigh Energy Physics::ExperimentAtomic physicsNuclear ExperimentRandom phase approximationJournal of Physics: Conference Series
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Probing the Majorana nature of the neutrino with neutrinoless double beta decay

2009

11th International Conference on Topics in Astroparticle and Underground Physics (TAUP 2009). Rome, ITALY, JUL 01-05, 2009

PhysicsHistoryParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesComputer Science ApplicationsEducationHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Double beta decayHigh Energy Physics::ExperimentNeutrinoMixing (physics)Lepton
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Simultaneous analysis of neutrinoless double beta decay and LHC pp-cross sections: limits on the left-right mixing angle

2015

The extension of the Standard Model of electroweak interactions, to accommodate massive neutrinos and/or right-handed currents, is one of the fundamental questions to answer in the cross-field of particle and nuclear physics. The consequences of such extensions would reflect upon nuclear decays, like the very exotic nuclear double-beta-decay, as well as upon high-energy proton-proton reactions of the type performed at the LHC accelerator. In this talk we shall address this question by looking at the results reported by the ATLAS and CMS collaborations, where the excitation and decay of a heavy-mass boson may be mediated by a heavy-mass neutrino in proton-proton reactions leading to two jets…

PhysicsHistoryParticle physicsLarge Hadron ColliderElectroweak interactionNuclear TheoryHigh Energy Physics::PhenomenologyFísicaneutrinoless double beta decayComputer Science ApplicationsEducationStandard ModelNuclear physicsdouble-beta-decayDouble beta decayLHC acceleratorHigh Energy Physics::ExperimentLHCNeutrinoNuclear ExperimentMixing (physics)Ciencias ExactasLeptonBoson
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Double beta decay and the quest for Majorana neutrinos

2020

Abstract The observation of neutrinoless double beta (0νββ) decay remains crucial for understanding lepton number violation. The inverse half-life for 0νββ-decay is given by the product of a phase space factor (PSF), a nuclear matrix element (NME), which both rely on theoretical description, and a function f containing the physics beyond the standard model. Phase space factors and nuclear matrix elements have been evaluated, or are under evaluation, systematically for all processes of interest. The nuclear matrix elements have been calculated within the framework of the microscopic interacting boson model (IBM-2), and phase space factors have been evaluated using exact Dirac electron wave f…

PhysicsHistoryParticle physicsMAJORANADouble beta decayHigh Energy Physics::ExperimenthiukkasfysiikkaNeutrinoydinfysiikkaComputer Science ApplicationsEducationJournal of Physics: Conference Series
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Nuclear and weak interaction aspects of neutrinoless double beta decay: Recent results

2012

The determination of the value of the light neutrino mass, as well as the determination of the nature of the neutrino, are two of the fundamental questions which motivate the experimental search of signals of neutrinoless double beta decay transitions. Here, we shall review some of the the essentials of the theory, based on both nuclear structure and elementary particle physics, relevant for the understanding of the problem.

PhysicsHistoryParticle physicsNuclear structureFísicaexperimental searchElementary particleWeak interactionComputer Science ApplicationsEducationElementary particle physicsNuclear physicsDouble beta decayHigh Energy Physics::Experimentelementary particleNeutrinolight neutrino massValue (mathematics)
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Physics of nuclear processes triggered by the interplay of strong and weak interactions

2012

Neutrinoless double beta (0νββ) decay of nuclei is a process that requires the neutrino to be a massive Majorana particle and thus cannot proceed in the standard model of electro-weak interactions. Recent results of the neutrino-oscillation experiments have produced accurate information on the mixing of neutrinos and their squared mass differences. The 0νββ decay takes place in atomic nuclei where it can be observed, at least in principle, by underground neutrino experiments. The information about the weak-interaction observables, like the neutrino mass, has to be filtered from the data through the nuclear matrix elements (NMEs). In this article recent work of the Jyv¨askyl¨a group on the N…

PhysicsHistoryParticle physicsSterile neutrinoHigh Energy Physics::PhenomenologyBeta decayBeta-decay stable isobarsComputer Science ApplicationsEducationNuclear physicsMAJORANATheoretical nuclear physicsDouble beta decayAtomic nucleusteoreettinen ydinfysiikkaHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationNuclear Experiment
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The NEXT double beta decay experiment

2016

NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double-beta (ββ0v) decay experiment at Laboratorio Subterraneo de Canfranc (LSC). It is an electroluminescent Time Projection Chamber filled with high pressure 136Xe gas with separated function capabilities for calorimetry and tracking. Energy resolution and background suppression are the two key features of any neutrinoless double beta decay experiment. NEXT has both good energy resolution (< 1% FWHM) and an extra handle for background identification provided by track reconstruction. We expect a background rate of 4 × 10-4 counts keV-1 kg-1 yr-1, and a sensitivity to the Majorana neutrino mass of between 80-160 meV (depending on…

PhysicsHistoryParticle physicsTime projection chamberScale (ratio)010308 nuclear & particles physicsDetectorchemistry.chemical_elementTracking (particle physics)01 natural sciencesComputer Science ApplicationsEducationNuclear physicsMAJORANAXenonchemistryDouble beta decay0103 physical sciencesNeutrino010306 general physicsJournal of Physics: Conference Series
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Studies of astrophysically interesting nucleus23Al

2010

We have studied the β-delayed proton decay of 23Al with a novel detector setup at the focal plane of the MARS separator at the Texas A&M University to resolve existing controversies about the proton branching of the IAS in 23Mg and to determine the absolute proton branchings by combining our results to the latest βγ-decay data. We have made also a high precision mass measurement of the ground state of 23Al to establish more accurate proton separation energy of 23Al. Here the description of the used techniques along with preliminary results of the experiments are given.

PhysicsHistoryProton decayDetectorMars Exploration ProgramMass measurementComputer Science ApplicationsEducationNuclear physicsCardinal pointmedicine.anatomical_structuremedicineHigh Energy Physics::ExperimentGround stateNucleusJournal of Physics: Conference Series
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Single Particle Levels and ββ-Decay Matrix Elements in The Interacting Boson Model

2018

Recently a new method to calculate the occupancies of single particle levels in atomic nuclei was developed in the context of the microscopic interacting boson model, in which neutron and proton degrees of freedom are treated explicitly (IBM-2). The energies of the single particle levels constitute a very important input for the calculation of the occupancies in this method, and further they play important role in the calculation of double beta decay nuclear matrix elements. Here we discuss how the 0νββ, 0νhββ, and 2νββ-decay nuclear matrix elements (NMEs) are affected when the energies of single particle levels are changed. peerReviewed

PhysicsHistoryProtonNuclear TheoryDegrees of freedom (physics and chemistry)double beta decayContext (language use)nuclear matrix elementsComputer Science ApplicationsEducationNuclear physicsMatrix (mathematics)Double beta decayAtomic nucleusNeutronInteracting boson modelNuclear Experimentydinfysiikka
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βdecay of102Y produced in projectile fission of238U

2012

The population of 102Zr following the β decay of 102Y produced in the projectile fission of 238U at the GSI facility in Darmstadt, Germany has been studied. 102Y is known to ß decay into 102Zr via two states, one of high spin and the other low spin. These states preferentially populate different levels in the 102Zr daughter. In this paper the intensities of transitions in 102Zr observed are compared with those from the decay of the low-spin level studied at the TRISTAN facility at Brookhaven National Laboratory and of the high-spin level studied at the JOSEF separator at the Kernforschungsanlage Jülich.

PhysicsHistoryeducation.field_of_studyCluster decayFissionProjectilePopulationBeta decayddc:Computer Science ApplicationsEducationNuclear physicsSubatomic PhysicsHigh Energy Physics::ExperimentAtomic physicsNuclear ExperimentSpin (physics)National laboratoryeducationJournal of Physics: Conference Series
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