Search results for "Matrix element"

showing 10 items of 72 documents

Precision thrust cumulant moments atN3LL

2012

We consider cumulant moments (cumulants) of the thrust distribution using predictions of the full spectrum for thrust including O(alpha_s^3) fixed order results, resummation of singular N^3LL logarithmic contributions, and a class of leading power corrections in a renormalon-free scheme. From a global fit to the first thrust moment we extract the strong coupling and the leading power correction matrix element Omega_1. We obtain alpha_s(m_Z) = 0.1141 \pm (0.0004)_exp \pm (0.0014)_hadr \pm (0.0007)_pert, where the 1-sigma uncertainties are experimental, from hadronization (related to Omega_1) and perturbative, respectively, and Omega_1 = 0.372 \pm (0.044)_exp \pm (0.039)_pert GeV. The n-th th…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsElectron–positron annihilationFOS: Physical sciencesOrder (ring theory)01 natural sciencesOmegaHigh Energy Physics - ExperimentNuclear Theory (nucl-th)CombinatoricsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Power correctionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesStrong couplingHigh Energy Physics::ExperimentMatrix element010306 general physicsNuclear theoryPhysical Review D
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ISOSPIN MIXING IN THE VICINITY OF THE N = Z LINE

2010

We present the isospin- and angular-momentum-projected nuclear density functional theory (DFT) and its applications to the isospin-breaking corrections to the superallowed beta-decay rates in the vicinity of the N=Z line. A preliminary value obtained for the Cabbibo-Kobayashi-Maskawa matrix element, |V_{ud}|=0.97463(24), agrees well with the recent estimate by Towner and Hardy [Phys. Rev. C{\bf 77}, 025501 (2008)]. We also discuss new opportunities to study the symmetry energy by using the isospin-projected DFT.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theoryta114Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyNuclear matterSymmetry (physics)Nuclear Theory (nucl-th)IsospinMatrix elementNuclear Experiment (nucl-ex)Nuclear ExperimentFunctional theoryNuclear ExperimentNuclear densityMixing (physics)Line (formation)International Journal of Modern Physics E
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Gluonic contributions in the chiral hyperbag

1990

Abstract We incorporate into a non-perturbative chiral bag model scheme the gluons and the η' in a perturbative fashion. We analyze in this context the proton matrix element for the flavor singlet axial current, where due account is taken of the anomaly, and the delta-nucleon mass difference. Our results show that the contribution due to the gluons is significant for large bag radii and that they are crucial in order to establish the Cheshire cat principle.

PhysicsNuclear and High Energy PhysicsParticle physicsQuantization (physics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryAxial currentMatrix elementSinglet stateNuclear ExperimentGluonNuclear Physics A
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Electron capture on116In and implications for nuclear structure related to double-βdecay

2013

The electron capture decay branch of ${}^{116}$In has been measured to be $[2.46\ifmmode\pm\else\textpm\fi{}0.44(\mathrm{stat}.)\ifmmode\pm\else\textpm\fi{}0.39(\mathrm{syst}.)]\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$ using Penning trap-assisted decay spectroscopy. The corresponding Gamow-Teller transition strength is shown to be compatible with the most recent value extracted from the $(p,n)$ charge-exchange reaction, providing a resolution to longstanding discrepancies. This transition can now be used as a reliable benchmark for nuclear-structure calculations of the matrix element for the neutrinoless double-$\ensuremath{\beta}$ decay of ${}^{116}$Cd and other nuclides.

PhysicsNuclear and High Energy PhysicsParticle physicsTransition strengthElectron captureNuclear structureMatrix elementNuclideSpectroscopyPhysical Review C
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Spin-dipole nuclear matrix elements for double beta decays and astro-neutrinos

2014

Spin-dipole (SD) nuclear matrix elements (NMEs) M±(SD2) for unique first forbidden β±2−→0+ ground-state-to-ground-state transitions are studied by using effective microscopic two-nucleon interactions in realistic single-particle model spaces. The observed values of the NMEs Mexp±(SD2) are compared with the values of the single-quasiparticle NMEs Mqp±(SD2) without nucleon spin–isospin (στ) correlation and the QRPA NMEs MQRPA±(SD2) with the στ correlation. The observed SD matrix elements are found to be reduced by the factor k≈0.2 with respect to Mqp±(SD2) and by the factor kNM≈0.5 with respect to MQRPA±(SD2). We then infer that the SD NME is reduced considerably partly by the nucleon στ corr…

PhysicsNuclear and High Energy PhysicsParticle physicsta114Renormalization of the axial-vector weak coupling constantPhysics::Medical PhysicsNuclear Theorycoupling constantdouble beta decayrenormalization of the axial-vector weakDouble beta decayspin-dipole matrix elementNuclear physicsDipoleMatrix (mathematics)Double beta decaySpin-dipole matrix elementBeta (velocity)Neutrinounique forbidden beta decayNuclear ExperimentSpin (physics)NucleonUnique forbidden beta decayPhysics Letters B
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Proton spin and the cheshire cat principle

1991

Abstract We discuss the proton matrix element of the flavor-singlet axial current (FSAC), often referred to as proton spin, in terms of the chiral bag model with due account of the axial anomaly and quantum number fractionation. We conclude that the contribution due to gluons is significant for large bag radii and that it is crucial in order to establish the Cheshire cat principle.

PhysicsNuclear and High Energy PhysicsProtonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQuantum numberAtomic and Molecular Physics and OpticsGluonQuantum electrodynamicsProton spin crisisAxial currentMatrix elementAnomaly (physics)Nuclear Physics B - Proceedings Supplements
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Effects of orbital occupation on 0νββ nuclear matrix element

2009

We have used the recently measured neutron occupancies in the 76 Ge and 76 Se nuclei as a guideline to define the neutron quasiparticle states in the 1p0f0g shell. The adjacent odd-mass nuclei help define the corresponding proton quasiparticle states. We insert the obtained quasiparticles in a proton-neutron quasiparticle random-phase approximation (pnQRPA) calculation of the nuclear matrix element of the neutrinoless double beta (0 νββ ) decay of 76 Ge. It is found that the resulting value of the 0 νββ matrix element is not far from the recently reported shell-model result.

PhysicsNuclear and High Energy PhysicsProtonNuclear TheoryShell (structure)Nuclear matrixAtomic and Molecular Physics and OpticsNuclear physicsCondensed Matter::SuperconductivityBeta (plasma physics)QuasiparticleMatrix elementNeutronElement (category theory)Atomic physicsNuclear ExperimentNuclear Physics B - Proceedings Supplements
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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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New determination of double-β-decay properties in48Ca: High-precisionQββ-value measurement and improved nuclear matrix element calculations

2014

We report a direct measurement of the Q-value of the neutrinoless double-beta-decay candidate 48Ca at the TITAN Penning-trap mass spectrometer, with the result that Q = 4267.98(32) keV. We measured the masses of both the mother and daughter nuclides, and in the latter case found a 1 keV deviation from the literature value. In addition to the Q-value, we also present results of a new calculation of the neutrinoless double-beta-decay nuclear matrix element of 48Ca. Using diagrammatic many-body perturbation theory to second order to account for physics outside the valence space, we constructed an effective shell-model double-beta-decay operator, which increased the nuclear matrix element by ab…

PhysicsNuclear and High Energy PhysicsValence (chemistry)010308 nuclear & particles physicsMass spectrometryNuclear matrix01 natural sciencesNuclear physics0103 physical sciencesMatrix elementNuclideNuclear Experiment010306 general physicsNuclear theoryPhysical Review C
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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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