Search results for "SIP"

showing 10 items of 1280 documents

Giant Monopole Resonances and nuclear incompressibilities studied for the zero-range and separable pairing interactions

2012

Background: Following the 2007 precise measurements of monopole strengths in tin isotopes, there has been a continuous theoretical effort to obtain a precise description of the experimental results. Up to now, there is no satisfactory explanation of why the tin nuclei appear to be significantly softer than 208Pb. Purpose: We determine the influence of finite-range and separable pairing interactions on monopole strength functions in semi-magic nuclei. Methods: We employ self-consistently the Quasiparticle Random Phase Approximation on top of spherical Hartree-Fock-Bogolyubov solutions. We use the Arnoldi method to solve the linear-response problem with pairing. Results: We found that the dif…

PhysicsNuclear and High Energy Physicsta114Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsMagnetic monopolechemistry.chemical_elementFOS: Physical sciencesNuclear matter01 natural sciencesSeparable spaceNuclear Theory (nucl-th)chemistryPairingQuantum mechanics0103 physical sciencesIsotopes of tinPhysical SciencesQuasiparticle010306 general physicsRandom phase approximationTin
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Multipole modes in deformed nuclei within the finite amplitude method

2015

Background: To access selected excited states of nuclei, within the framework of nuclear density functional theory, the quasiparticle random phase approximation (QRPA) is commonly used. Purpose: We present a computationally efficient, fully self-consistent framework to compute the QRPA transition strength function of an arbitrary multipole operator in axially-deformed superfluid nuclei. Methods: The method is based on the finite amplitude method (FAM) QRPA, allowing fast iterative solution of QRPA equations. A numerical implementation of the FAM-QRPA solver module has been carried out for deformed nuclei. Results: The practical feasibility of the deformed FAM module has been demonstrated. I…

PhysicsNuclear and High Energy Physicsta114quasiparticle random phase approximationNuclear TheoryOperator (physics)Nuclear Theorydeformed nucleiFOS: Physical sciencesSpace (mathematics)Nuclear Theory (nucl-th)Quantum electrodynamicsQuadrupoleQuasiparticleMultipole expansionRandom phase approximationAxial symmetryNuclear ExperimentNuclear densityexcited states
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First identification of rotational band structures inRe9175166

2015

Despite that it is more than 100 years since the atomic nucleus was first dis- covered by Ernest Rutherford and coworkers, many of its features still elude our understanding. The fact that the fundamental interactions between the nuclear constituents; nucleons, and ultimately quarks, are not yet known in detail, and the complexity of the nuclear many-body system compound the great challenges facing theoretical interpretations of experimental data. It is therefore important to focus on distinct phenomena where experimental mea- surements can be compared with theoretical predictions, providing stringent tests of theory. One such area is the nuclear phenomenology of collective excitations rela…

PhysicsNuclear physicsNuclear and High Energy PhysicsAngular momentumExcited stateNuclear TheoryAtomic nucleusQuasiparticleSemiclassical physicsNeutronNucleonGround statePhysical Review C
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Microscopic study of muon-capture transitions in nuclei involved in double-beta-decay processes

2003

Abstract Total and partial ordinary muon-capture (OMC) rates to 1 + and 2 − states are calculated in the framework of the proton–neutron quasiparticle random-phase approximation (pnQRPA) for several nuclei involved in double-beta-decay processes. The aim is to obtain information on intermediate states involved in double-beta-decay transitions having these nuclei as either daughter or parent nuclei. It is found that the OMC observables, just like the 2 νββ -decay amplitudes, strongly depend on the particle–particle part of the proton–neutron interaction. First experiments measuring the partial OMC rates for nuclei involved in double beta decays have recently been performed.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsAmplitudeDouble beta decayNuclear TheoryQuasiparticleObservableBeta (velocity)Nuclear ExperimentMuon captureNuclear Physics A
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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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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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Perturbative analysis of the 2νββ decays of 100Mo and 116Cd

2003

We have performed a theoretical analysis of the ground-state-to-ground-state transitions in 100Mo and 116Cd, based on the quasiparticle random-phase approximation and on a straightforward perturbative scheme. The results show that the single-state dominance found in the realistic calculations of the nuclear matrix elements, which is consistent with data, can be viewed as a result of the interference between few two-quasiparticle configurations.

PhysicsNuclear physicsNuclear and High Energy PhysicsQuantum mechanicsDouble beta decayHadronQuasiparticleNuclear fusionPerturbation theory (quantum mechanics)Random phase approximationInterference (wave propagation)The European Physical Journal A
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Neutrino scattering off the stable cadmium isotopes: neutral-current processes

2014

In this work we present computed cross sections for the incoherent neutral-current neutrino scattering off the stable cadmium isotopes. The main focus is on supernova neutrinos. The nuclear states of the even-mass and odd-mass cadmium isotopes have been constructed using the quasiparticle random-phase approximation and the microscopic quasiparticle-phonon model, respectively. The computed cross sections are folded with suitably parametrized Fermi–Dirac distributions of the supernova (anti)neutrinos energies to obtain realistic estimates of the nuclear responses to these neutrinos.

PhysicsNuclear physicsNuclear and High Energy PhysicsSupernovaParticle physicsNeutral currentAstrophysics::High Energy Astrophysical PhenomenaIsotopes of cadmiumQuasiparticleNeutrinoNeutrino scatteringJournal of Physics G: Nuclear and Particle Physics
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Collective 2$^{+1}$ excitations in$^{206}$Po and$^{208,210}$Rn

2016

In the present study, $B(E2; 2^{+}_{1}\rightarrow 0^{+}_{1})$ values have been measured in the 208,210Rn and 206Po nuclei through Coulomb excitation of re-accelerated radioactive beams in inverse kinematics at CERN-ISOLDE. These nuclei have been proposed to lie in, or at the boundary of the region where the seniority scheme should persist. However, contributions from collective excitations are likely to be present when moving away from the N=126 closed shell. Such an effect is confirmed by the observed increased collectivity of the $2^{+}_{1}\rightarrow 0^{+}_{1}$ transitions. Experimental results have been interpreted with the aid of theoretical studies carried out within the BCS-based QRP…

PhysicsNuclear reactionNuclear and High Energy Physics010308 nuclear & particles physicsHadronNuclear TheoryradonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesIsotopes of palladiumcollective excitationExcited state0103 physical sciencesQuasiparticlePhysics::Accelerator PhysicsAtomic physics010306 general physicsNuclear ExperimentOpen shellpoloniumExcitationexcited states
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High-Kfour-quasiparticle states inGd138

2011

States above the known ${K}^{\ensuremath{\pi}}={8}^{\ensuremath{-}}$ 6 $\ensuremath{\mu}$s isomer in $^{138}\mathrm{Gd}$ have been populated with the $^{106}\mathrm{Cd}$($^{36}\mathrm{Ar}$,$2p2n$) reaction at a beam energy of 180 MeV at the University of Jyv\"askyl\"a, Finland. The recoil-isomer tagging technique was utilized to correlate delayed $\ensuremath{\gamma}$-ray decays, detected in the GREAT focal plane spectrometer, with prompt decays measured in the JUROGAM II spectrometer at the target position. The lifetime of the ${K}^{\ensuremath{\pi}}={8}^{\ensuremath{-}}$ isomeric state has been remeasured as 6.2(2) $\ensuremath{\mu}$s. Two high-lying strongly coupled bands have been estab…

PhysicsNuclear reactionNuclear and High Energy PhysicsNeutron emissionLandé g-factorQuasiparticleState (functional analysis)Atomic physicsRadioactive decayHigh-κ dielectricDimensionless quantityPhysical Review C
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