Search results for "matrix elements"

showing 10 items of 33 documents

Neutrino-nuclear responses for astro-neutrinos, single beta decays and double beta decays

2019

Abstract Neutrino–nuclear responses associated with astro-neutrinos, single beta decays and double beta decays are crucial in studies of neutrino properties of interest for astro-particle physics. The present report reviews briefly recent studies of the neutrino–nuclear responses from both experimental and theoretical points of view in order to obtain a consistent understanding of the many facets of the neutrino–nuclear responses. Subjects discussed in this review include (i) experimental studies of neutrino–nuclear responses by means of single beta decays, charge-exchange nuclear reactions, muon- photon- and neutrino–nuclear reactions, and nucleon-transfer reactions, (ii) implications of a…

Nuclear reactionParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoastrofysiikkasingle beta decaysNuclear TheoryGeneral Physics and Astronomyneutrino-nucleus interactionsnuclear matrix elements01 natural sciences7. Clean energyastro-neutrinosNucleosynthesisDouble beta decay0103 physical sciencesBeta (velocity)Nuclear Experiment010306 general physicsPhysicsdouble beta decaysMuonta114010308 nuclear & particles physicsHigh Energy Physics::Phenomenologymuon captureneutriinotMuon capturephoto-nuclear reactionsHigh Energy Physics::Experimentcharge-exchange reactionsNeutrinoPhysics Reports
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Electron spectra in forbidden β decays and the quenching of the weak axial-vector coupling constant gA

2017

Evolution of the electron spectra with the effective value of the weak axial-vector coupling constant ${g}_{\mathrm{A}}$ was followed for 26 first-, second-, third-, fourth- and fifth-forbidden ${\ensuremath{\beta}}^{\ensuremath{-}}$ decays of odd-$A$ nuclei by calculating the involved nuclear matrix elements (NMEs) in the framework of the microscopic quasiparticle-phonon model (MQPM). The next-to-leading-order terms were included in the $\ensuremath{\beta}$-decay shape factor of the electron spectra. The spectrum shapes of third- and fourth-forbidden nonunique decays were found to depend strongly on the value of ${g}_{\mathrm{A}}$, while first- and second-forbidden decays were mostly unaff…

PhysicsCoupling constantta114010308 nuclear & particles physicsElectron spectrabeetasäteilyExcitation spectranuclear matrix elements01 natural sciencesSpectral linespektritsymbols.namesakeMean field theoryDouble beta decay0103 physical sciencesforbidden beta-decaysymbolselectron spectraAtomic physics010306 general physicsHamiltonian (quantum mechanics)PseudovectorPhysical Review C
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Nuclear matrix elements for double beta decay in the QRPA approach: a critical review

2009

The calculation of nuclear matrix elements (NME) for double beta decay transitions (DBD) relies upon several approximations. The purpose of this note is to review some of these approximations, and their impact upon the NME. We shall present our results, which have been obtained in the framework of the proton-neutron quasiparticle random phase approximation (pnQRPA), and we shall focus on short range correlations, pairing, and symmetry effects.

PhysicsHistoryFísicaSymmetry (physics)Computer Science ApplicationsEducationNuclear physicsTheoretical physicsRange (mathematics)Double beta decayPairingNuclear matrix elementsQuasiparticleNeutrinoless double beta decayRandom phase approximationPairing correlations
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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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Consistent large-scale shell-model analysis of the two-neutrino ββ and single β branchings in 48Ca and 96Zr

2020

Abstract Two-neutrino double-beta-decay matrix elements M 2 ν and single beta-decay branching ratios were calculated for 48Ca and 96Zr in the interacting nuclear shell model using large single-particle valence spaces with well-tested two-body Hamiltonians. For 48Ca the matrix element M 2 ν = 0.0511 is obtained, which is 5.5% smaller than the previously reported value of 0.0539. For 96Zr this work reports the first large-scale shell-model calculation of the nuclear matrix element, yielding a value M 2 ν = 0.0747 with extreme single-state dominance. These matrix elements, combined with the available ββ-decay half-life data, yield effective values of the weak axial coupling which in turn are u…

PhysicsNuclear and High Energy Physics48CaYield (engineering)Valence (chemistry)010308 nuclear & particles physicsmatrix elementsSHELL modelNuclear shell modelshell modeldouble-beta decayBranching (polymer chemistry)01 natural sciencesMolecular physicslcsh:QC1-999axial-vector coupling96ZrDouble beta decay0103 physical sciencesMatrix elementHigh Energy Physics::ExperimentNeutrino010306 general physicsydinfysiikkalcsh:PhysicsPhysics Letters B
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Nuclear matrix elements of ββ decay from β-decay data

2005

Abstract The evaluation of the nuclear matrix elements (NME) of the two-neutrino double beta ( 2 ν β β ) decay and neutrinoless double beta ( 0 ν β β ) decay using the proton–neutron quasiparticle random-phase approximation (pnQRPA) is addressed. In particular, the extraction of a proper value of the proton–neutron particle–particle interaction parameter, g pp , of this theory is analyzed in detail. Evidence is shown, that it can be misleading to use the experimental half-life of the 2 ν β β decay to extract a value for g pp . Rather, arguments are given in favour of using the available data on single beta decay for this purpose.

PhysicsNuclear and High Energy PhysicsHalf-lifeProton–neutron interactionBeta decayDouble beta decayNuclear physicsDouble beta decayNuclear matrix elementsQuasiparticleQuasiparticle random-phase approximationBeta (velocity)High Energy Physics::ExperimentNeutrinoRandom phase approximationNuclear ExperimentEigenvalues and eigenvectorsPhysics Letters B
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New information on β-delayed neutron emission from Be-12, Be-14

1999

17 pages, 3 tables, 5 figures, 1 appendix.-- PACS nrs.: 23.40.Hc; 27.20.+n.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderRadioactivity: Be-12 Be-14 (from 1 GeV p on UC target selective mass separation)Astrophysics::High Energy Astrophysical PhenomenaConfidence intervalNuclear physics6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Neutron long countersBe-12 Be-14 deduced P(n) values Be-14 deduced P(xn) valuesHigh Energy Physics::ExperimentNeutronMeasured βn nn time correlations[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nuclear ExperimentDelayed neutronRadioactive beam[PACS] Relation with nuclear matrix elements and nuclear structureBe-12 Be-14 (from 1 GeV p on UC target selective mass separation) [Radioactivity]
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Short-range correlations and neutrinoless double beta decay

2007

In this work we report on the effects of short-range correlations upon the matrix elements of neutrinoless double beta decay. We focus on the calculation of the matrix elements of the neutrino-mass mode of neutrinoless double beta decays of 48Ca and 76Ge. The nuclear-structure components of the calculation, that is the participant nuclear wave functions, have been calculated in the shell-model scheme for 48Ca and in the proton-neutron quasiparticle random-phase approximation (pnQRPA) scheme for 76Ge. We compare the traditional approach of using the Jastrow correlation function with the more complete scheme of the unitary correlation operator method (UCOM). Our results indicate that the Jast…

PhysicsNuclear and High Energy PhysicsNuclear TheoryOperator (physics)Nuclear TheoryNuclear structureUnitary correlation operator methodFOS: Physical sciencesFísicaNuclear physicsNuclear Theory (nucl-th)Matrix (mathematics)Correlation functionDouble beta decayNuclear matrix elementsNeutronHigh Energy Physics::ExperimentNeutrinoless double beta decayWave functionRandom phase approximationNuclear ExperimentShort-range correlations
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Recursive method for computing matrix elements for two-body interactions

2015

A recursive method for the efficient computation of two-body matrix elements is presented. The method consists of a set of recursion relations for the computationally demanding radial integral and adds one more tool to the set of computational methods introduced by Horie and Sasaki [H. Horie and K. Sasaki, Prog. Theor. Phys. 25, 475 (1961)]. The neutrinoless double-$\ensuremath{\beta}$ decay will serve as the primary application and example, but the method is general and can be applied equally well to other kinds of nuclear structure calculations involving matrix elements of two-body interactions.

PhysicsNuclear and High Energy PhysicsPure mathematicstwo-body interactionsRecursionta114BETA (programming language)matrix elementsRadial integralComputationNuclear structureSet (abstract data type)Matrix (mathematics)computational physicscomputercomputer.programming_language
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Magnetic Hexadecapole γ Transitions and Neutrino-Nuclear Responses in Medium-Heavy Nuclei

2016

Neutrino-nuclear responses in the form of squares of nuclear matrix elements, NMEs, are crucial for studies of neutrino-induced processes in nuclei. In this work we investigate magnetic hexadecapole (M4) NMEs in medium-heavy nuclei. The experimentally derived NMEs,MEXP(M4), deduced from observed M4γtransition half-lives are compared with the single-quasiparticle (QP) NMEs,MQP(M4), and the microscopic quasiparticle-phonon model (MQPM) NMEsMMQPM(M4). The experimentally derived M4 NMEs are found to be reduced by a coefficientk≈0.29with respect toMQP(M4) and byk≈0.33with respect toMMQPM(M4). The M4 NMEs are reduced a little by the quasiparticle-phonon correlations of the MQPM wave functions but…

PhysicsNuclear and High Energy Physicsta114Article Subjectneutrino-nuclear responses010308 nuclear & particles physicsNuclear Theorymedium-heavy nucleinuclear matrix elements01 natural scienceslcsh:QC1-999Nuclear physicsgamma transitionBeta (plasma physics)0103 physical sciencesNeutrino010306 general physicsQuadrupole magnetWave functionlcsh:PhysicsOrder of magnitude
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