Search results for "Matrix"

showing 10 items of 3205 documents

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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Low energy collective modes of deformed superfluid nuclei within the finite amplitude method

2013

Background: The major challenge for nuclear theory is to describe and predict global properties and collective modes of atomic nuclei. Of particular interest is the response of the nucleus to a time-dependent external field that impacts the low-energy multipole and beta-decay strength. Purpose: We propose a method to compute low-lying collective modes in deformed nuclei within the finite amplitude method (FAM) based on the quasiparticle random-phase approximation (QRPA). By using the analytic property of the response function, we find the QRPA amplitudes by computing the residua of the FAM amplitudes by means of a contour integration around the QRPA poles in a complex frequency plane. Metho…

PhysicsNuclear and High Energy Physicsta114Nuclear TheoryIsoscalarNuclear TheoryMagnetic monopoleFOS: Physical sciencesMethods of contour integrationNuclear Theory (nucl-th)Matrix (mathematics)Classical mechanicsQuantum mechanicsAtomic nucleusQuasiparticleMultipole expansionNuclear ExperimentNuclear density
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Double charge exchange reactions as a probe for neutrinoless double beta decay nuclear matrix elements

2020

Abstract The formalism to describe heavy-ion double charge exchange (DCE) processes in the eikonal and small-momentum transfer approximations introduced in Phys. Rev. C 98, 061601(R) (2018) is briefly discussed. It is also shown that, under the previous approximations, the heavy-ion DCE cross-section can be factorized in terms of a reaction and a nuclear part. A double charge exchange effective potential is explicitly derived in the closure approximation and also for the first time the explicit form of the DCE nuclear matrix elements, that are of the form of double Gamow-Teller and double Fermi. The recent hypothesis of a linear correlation between double Gamow-Teller neutrinoless double be…

PhysicsNuclear physicsHistoryDouble beta decayNuclear TheoryhiukkasfysiikkaydinfysiikkaNuclear ExperimentNuclear matrixComputer Science ApplicationsEducationCharge exchangeJournal of Physics: Conference Series
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Weak-interaction and nuclear-structure aspects of nuclear double beta decay

1998

Abstract Weak-interaction and nuclear-structure aspects of double beta decay are reviewed. Starting from effective electroweak lagrangians, decay rates for the two-neutrino and neutrinoless modes of the nuclear double beta decay transitions are defined and second-order perturbative expressions for the nuclear decay amplitudes are given. Nuclear matrix elements of the relevant operators are presented, as extracted from data and from shell-model and QRPA calculations as well as from other theoretical approximations. The analysis is performed both for the two-neutrino and neutrinoless modes of the decay. The expressions for ground-state-to-ground-state and ground-state-to-excited-state transit…

PhysicsNuclear physicsMatrix (mathematics)Particle physicsDouble beta decayElectroweak interactionNuclear structureGeneral Physics and AstronomyVertex functionHigh Energy Physics::ExperimentWeak interactionRandom phase approximationRadioactive decayPhysics Reports
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Nuclear matrix elements and the neutrinoless double beta decay

2005

Systematics of the nuclear matrix elements related to the neutrinoless double beta ( 0 ν β β ) decay are discussed. The calculation of the related nuclear matrix elements in the framework of the proton-neutron quasiparticle random-phase approximation (pnQRPA) is analyzed. In particular, the extraction of a proper value of the proton-neutron particle-particle interaction parameter in this theory is addressed. The relevance of different multipoles in the multipole decomposition of the 0 ν β β matrix element is also discussed.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsDouble beta decayNuclear TheoryQuasiparticleBeta (velocity)Matrix elementNuclear ExperimentMultipole expansionNuclear matrixAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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Hyperon Semileptonic Decays and CKM Unitarity

2005

We perform a new numerical analysis of hyperon semileptonic decays emphasizing the systematic uncertainties. The poor understanding of SU(3) symmetry breaking effects at second order in the vector form factor translates into a large error of |V(us)|. Using our determination |V(us)| = 0.226 +/- 0.005 together with those coming from other sources we test the unitarity of the CKM matrix.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)UnitarityCabibbo–Kobayashi–Maskawa matrixHyperonForm factor (quantum field theory)FOS: Physical sciencesSymmetry breakingAtomic and Molecular Physics and Optics
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Description of the two-neutrino ββ decay of100Mo by pnMAVA

2009

The microscopic anharmonic vibrator approach (MAVA) is a scheme where the one- and two-phonon states of an even–even nucleus are treated consistently by using a realistic microscopic nuclear Hamiltonian. This model has recently been extended to describe odd–odd nuclei by adding proton–neutron phonons in a scheme called the proton–neutron MAVA (pnMAVA). In this paper, we apply pnMAVA to compute the nuclear matrix elements corresponding to the two-neutrino double beta (2νββ) decay of 100Mo to the ground state and the first excited 0+ state of 100Ru in a realistic single-particle space. We also compute the GT− and GT+ Gamow–Teller strength functions and compare them with the plain pnQRPA (prot…

PhysicsNuclear physicsNuclear and High Energy PhysicsProtonExcited stateDouble beta decayNuclear TheoryQuasiparticleNeutronNeutrinoNuclear ExperimentTransition rate matrixGround stateJournal of Physics G: Nuclear and Particle Physics
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Electroweak effects in the extraction of the CKM angle γ from B→Dπ decays

2015

The angle γ of the standard CKM unitarity triangle can be determined from tree-level B-meson decays essentially without hadronic uncertainties. We calculate the second-order electroweak corrections for the B→Dπ modes and show that their impact on the determination of γ could be enhanced by an accidental cancellation of poorly known hadronic matrix elements. However, we do not expect the resulting shift in γ to exceed |δγDπ/γ|≲O(10−4).

PhysicsNuclear physicsParticle physicsMatrix (mathematics)Nuclear and High Energy PhysicsUnitarityExtraction (chemistry)HadronElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experimentlcsh:Physicslcsh:QC1-999Physics Letters B
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Fine structure in fragment mass-energy distribution from 238U+40Ar (275 MeV)

2003

Existence of a new feature in fragment mass-energy distribution is reported. Careful analysis of the data obtained in the reaction 238U + 40Ar (275 MeV) shows that small but statistically significant ripples visible already in the gross mass spectrum come from extended and regular 2D patterns in the TKE vs. mass matrix. Intensity distributions of these patterns coincide with the location of heavy clusters such as 78Ni, 108Mo, or 132Sn. Presumably, the observed patterns show the dominant trajectories in the elongation vs. mass-asymmetry space of the decaying system. This information, unknown in the past, can shed a new light even on the previously well-studied reactions.

PhysicsNuclear reactionDistribution (mathematics)Fragment (logic)Mass spectrumSpace (mathematics)Mass matrixMolecular physicsIntensity (heat transfer)Spectral line
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Parallel implementation of the MAGPACK package for the analysis of high-nuclearity spin clusters

2010

Abstract Molecular clusters are formed by a finite number of exchange-coupled paramagnetic centers and they are model systems between molecules and extended solids. In order to simulate their properties and extrapolate to solids, the size of the systems to be treated should be as large as possible. In this context, the use of efficient parallel codes is essential. We present the parallel programs ParAni and ParIso , for anisotropic and isotropic models, that enable the calculation of large energy matrices in parallel and the subsequent computation of the relevant spectral information. The evaluation of the matrix elements is based on the serial package Magpack that uses the irreducible tens…

PhysicsParamagnetismMagnetic anisotropyMatrix (mathematics)Theoretical computer scienceHardware and ArchitectureIsotropyGeneral Physics and AstronomyContext (language use)TensorEigenvalues and eigenvectorsComputational physicsSpin-½Computer Physics Communications
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