Search results for "Matrix element"

showing 10 items of 72 documents

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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Parity nonconservation in the γ decay of polarized17/2−isomers inTc93

2005

The determination of the ${0}^{\ifmmode^\circ\else\textdegree\fi{}}\ensuremath{-}{180}^{\ifmmode^\circ\else\textdegree\fi{}}$ asymmetry (${A}_{\ensuremath{\gamma}}$), which arises because of the parity nonconserving matrix element, in the 751-keV \ensuremath{\gamma} decay of polarized $17/{2}^{\ensuremath{-}}$ isomers in $^{93}\mathrm{Tc}$ with respect to the direction of polarization is reported. A combined analysis of the present results together with those from our earlier work yields an effect of two standard deviations.

PhysicsNuclear and High Energy PhysicsCondensed matter physicsmedia_common.quotation_subjectGamma rayMatrix elementParity (physics)Atomic physicsAsymmetrymedia_commonPhysical Review C
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Two-neutrino ββ decay to excited states. The 0+ → 2+ decay of 136Xe

1993

Abstract A method to calculate the two-neutrino double beta decay (2vββ) to one-phonon excited states is presented. The formalism, which is based on the quasiparticle random phase approximation, is applied to the description of the 2vββ transition 136Xe (0 g.e. + ) → 136 Ba (2 1 + ). It is shown that the participant matrix element is not suppressed by the inclusion of renormalized particle-particle interactions.

PhysicsNuclear and High Energy PhysicsFormalism (philosophy of mathematics)Excited stateDouble beta decayQuasiparticleMatrix elementNeutrinoAtomic physicsRandom phase approximationPhysics 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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Simultaneous measurement of forward-backward asymmetry and top polarization in dilepton final states fromtt¯production at the Tevatron

2015

We present a simultaneous measurement of the forward-backward asymmetry and the top-quark polarization in t (t) over bar production in dilepton final states using 9.7 fb(-1) of proton-antiproton collisions at root s = 1.96 TeV with the D0 detector. To reconstruct the distributions of kinematic observables we employ a matrix element technique that calculates the likelihood of the possible t (t) over bar kinematic configurations. After accounting for the presence of background events and for calibration effects, we obtain a forward-backward asymmetry of A(t (t) over bar) = (15.0 +/- 6.4(stat) +/- 4.9(syst)) % and a top-quark polarization times spin analyzing power in the beam basis of kappa P…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectTevatronObservableForward backwardPolarization (waves)01 natural sciencesAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentMatrix elementNuclear Experiment010306 general physicsLeptonmedia_commonPhysical Review D
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Spontaneous CP violation and the B0 system

1998

We investigate effects of spontaneous breakdown of CP in $B^0_{d,s}-\overline{B^0}_{d,s}$ systems in left-right symmetric models. Assuming that the left-right contribution to the $B^0-\overline{B^0}$ matrix element $M_{12}$ can be at most equal to the standard model one we obtain a new lower bound, $M_H\gsim 12$ TeV, on the flavour changing Higgs boson mass. Most importantly, the convention independent parameter $Re(\overline{\epsilon}_B),$ which measures the amount of $\Delta B=2$ CP violation, can be enhanced by a factor of four or more for $B^0_d$ and almost by two orders of magnitude for $B^0_s$ systems when compared with the Standard Model predictions. Therefore, interesting possibilit…

PhysicsNuclear and High Energy PhysicsParticle physicsIndependent parameterHiggs bosonFísicaCP violationMatrix elementUpper and lower boundsOrder of magnitudeStandard ModelNuclear Physics B
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