Search results for "Beta Decay"

showing 10 items of 501 documents

The Next White (NEW) detector

2018

[EN] Conceived to host 5 kg of xenón at a pressure of 15 bar in the ¿ducial volume,the NEXTWhite (NEW)apparatus is currently the largest high pressure xenon gas TPC using electroluminescent ampli¿cation in the world. It is also a 1:2 scale model of the NEXT-100 detector scheduled to start searching for ßß0¿ decays in 136Xe in 2019. Both detectors measure the energy of the event using a plane of photomultipliers located behind a transparent cathode. They can also reconstruct the trajectories of charged tracks in the dense gas of the TPC with the help of a plane of silicon photomultipliers located behind the anode. A sophisticated gas system, common to both detectors, allows the high gas puri…

Physics - Instrumentation and DetectorsXenon010308 nuclear & particles physicsEuropean researchLibrary scienceFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)7. Clean energy01 natural sciencesHigh-pressure xenon chambersTECNOLOGIA ELECTRONICATime Projection Chamber (TPC)Political science0103 physical sciencesmedia_common.cataloged_instanceEuropean unionNeutrinoless double beta decay010306 general physicsInstrumentationMathematical Physicsmedia_commonNEXT-100 experiment
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Majorana parameters of the interacting boson model of nuclear structure and their implication for 0νββ decay

2021

photonuclear reactionsnuclear spinelectromagnetic transitionsparitylifetimeswidthscollective modelspesonance reactionsneutrinoless double beta decay
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Electron capture decay of116Inand nuclear structure of doubleβdecays

1998

Quasiparticle-random-phase-approximation (QRPA) calculations of double $\ensuremath{\beta}$ decays have not been able to reproduce data in the $A=100$ system. We propose the $A=116$ system---because of its smaller deformation---as a simpler system to test QRPA calculations. We present results of two experiments we performed, which determine the electron-capture-decay branch of ${}^{116}\mathrm{In}$ to be $(2.27\ifmmode\pm\else\textpm\fi{}0.63)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}2}%$, from which we deduce $\mathrm{log}{ft=4.39}_{\ensuremath{-}0.15}^{+0.10}$. We present QRPA calculations and compare their predictions to experimental data. Finally we use these calculations to…

PhysicsNuclear and High Energy PhysicsParticle physicsElectron captureExcited stateDouble beta decayRadiative captureNuclear structureBeta (velocity)Atomic physicsRandom phase approximationQuasi particlesPhysical Review C
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Single and Double Beta-DecayQValues among the TripletZr96,Nb96, andMo96

2016

The atomic mass relations among the mass triplet ^{96}Zr, ^{96}Nb, and ^{96}Mo have been determined by means of high-precision mass measurements using the JYFLTRAP mass spectrometer at the IGISOL facility of the University of Jyvaskyla. We report Q values for the ^{96}Zr single and double β decays to ^{96}Nb and ^{96}Mo, as well as the Q value for the ^{96}Nb single β decay to ^{96}Mo, which are Q_{β}(^{96}Zr)=163.96(13), Q_{ββ}(^{96}Zr)=3356.097(86), and Q_{β}(^{96}Nb)=3192.05(16)  keV. Of special importance is the ^{96}Zr single β-decay Q value, which has never been determined directly. The single β decay, whose main branch is fourfold unique forbidden, is an alternative decay path to the…

QuenchingCoupling constantPhysics010308 nuclear & particles physicsQ valueGeneral Physics and AstronomyMass spectrometry7. Clean energy01 natural sciencesAtomic massMain branchDouble beta decay0103 physical sciencesUniquenessAtomic physics010306 general physicsPhysical Review Letters
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Neutrino phenomenology and stable dark matter with A4

2011

We present a model based on the A4 non-abelian discrete symmetry leading to a predictive five-parameter neutrino mass matrix and providing a stable dark matter candidate. We found an interesting correlation among the atmospheric and the reactor angles which predicts theta_23 ~ pi/4 for very small reactor angle and deviation from maximal atmospheric mixing for large theta_13. Only normal neutrino mass spectrum is possible and the effective mass entering the neutrinoless double beta decay rate is constrained to be |m_ee| > 4 10^{-4} eV.

Nuclear and High Energy PhysicsParticle physicsLepton mixingDark matterDiscrete symmetriesFOS: Physical sciencesElementary particle01 natural sciences7. Clean energyNuclear physicsEffective mass (solid-state physics)High Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesDark matterNeutrinoless double beta decay010306 general physicsNeutrino oscillationPhysics010308 nuclear & particles physicsFlavor symmetriesNeutrino massesMassless particleHigh Energy Physics - PhenomenologyMass spectrumNeutrinoPhysics Letters B
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Mitigation of backgrounds from cosmogenic 137 Xe in xenon gas experiments using 3 He neutron capture

2020

[EN] Xe-136 is used as the target medium for many experiments searching for 0 nu beta beta. Despite underground operation, cosmic muons that reach the laboratory can produce spallation neutrons causing activation of detector materials. A potential background that is difficult to veto using muon tagging comes in the form of Xe-137 created by the capture of neutrons on Xe-136. This isotope decays via beta decay with a half-life of 3.8 min and a Q(beta) of similar to 4.16 MeV. This work proposes and explores the concept of adding a small percentage of He-3 to xenon as a means to capture thermal neutrons and reduce the number of activations in the detector volume. When using this technique we f…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsScintillation and light emission processesGas and liquid scintillatorsFOS: Physical scienceschemistry.chemical_element01 natural sciences7. Clean energyHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICANuclear physicsGaseous detectorsSolidHigh Energy Physics - Experiment (hep-ex)XenonDouble beta decay0103 physical sciencesIsotopes of xenonSpallationNeutron010306 general physicsPhysics010308 nuclear & particles physicsFísicaInstrumentation and Detectors (physics.ins-det)Beta DecayNeutron temperatureNeutron capturechemistryScintillatorsRadioactive decayJournal of Physics G: Nuclear and Particle Physics
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β−-delayed spectroscopy of neutron-rich tantalum nuclei: Shape evolution in neutron-rich tungsten isotopes

2009

The low-lying structure of W-188,W-190,W-192 has been studied following beta decays of the neutron-rich mother nuclei Ta-188,Ta-190,Ta-192 produced following the projectile fragmentation of a 1-GeV-per-nucleon Pb-208 primary beam on a natural beryllium target at the GSI Fragment Separator. The beta-decay half-lives of Ta-188, Ta-190, and Ta-192 have been measured, with gamma-ray decays of low-lying states in their respective W daughter nuclei, using heavy-ion beta-gamma correlations and a position-sensitive silicon detector setup. The data provide information on the low-lying excited states in W-188, W-190, and W-192, which highlight a change in nuclear shape at W-190 compared with that of …

PhysicsNuclear and High Energy PhysicsProtonIsotopeNuclear TheoryTantalumchemistry.chemical_elementNuclear physicschemistryDouble beta decayNeutronBerylliumAtomic physicsNuclear ExperimentNucleonRadioactive decayPhysical Review C
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MQPM description of the structure and beta decays of the odd Mo and Tc isotopes

2010

The odd-mass isotopes A=95,97 of molybdenum are of interest for neutrino-physics applications. The microscopic quasiparticle-phonon model (MQPM) is used to calculate energy and decay characteristics of these nuclei and their beta-decay partners (Tc95 and Tc97). A realistic single-particle valence space and two-body interaction are used in the calculations. The computed results are compared with available data. The obtained energy spectra are also compared with earlier calculations. We present the first ever calculations for the rates of allowed and forbidden β+/EC decay transitions in these nuclei. In general our computed numbers agree rather well with the available data.

PhysicsNuclear and High Energy PhysicsDecay schemeValence (chemistry)Isotopechemistry.chemical_elementBeta decaySpectral lineNuclear physicschemistryMolybdenumDouble beta decayPositron emissionAtomic physicsNuclear Physics A
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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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New contributions to supersymmetric mechanism of neutrinoless double beta decay

1995

The neutrinoless double beta ($\znbb$) decay is analyzed within the Minimal Supersymmetric Standard Model with explicit R-parity violation (\rp MSSM). We have found new supersymmetric contributions to this process and give the complete set of relevant Feynman diagrams. Operators describing $0^+ \longrightarrow 0^+$ nuclear transitions induced by the supersymmetric interactions of the \rp MSSM are derived. These operators can be used for calculating the $\znbb$ decay rate applying any specific nuclear model wave functions.

PhysicsNuclear and High Energy PhysicsParticle physicssymbols.namesakeDouble beta decayHigh Energy Physics::PhenomenologysymbolsFeynman diagramFísicaBeta (velocity)High Energy Physics::ExperimentWave functionMinimal Supersymmetric Standard Model
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