Search results for "nuclear structure"

showing 10 items of 401 documents

Effects of one valence proton on seniority and angular momentum of neutrons in neutron-rich Sb51122–131 isotopes

2019

Background: Levels fulfilling the seniority scheme and relevant isomers are commonly observed features in semimagic nuclei; for example, in Sn isotopes (Z=50). Seniority isomers in Sn, with dominantly pure neutron configurations, directly probe the underlying neutron-neutron (νν) interaction. Furthermore, an addition of a valence proton particle or hole, through neutron-proton (νπ) interaction, affects the neutron seniority as well as the angular momentum. Purpose: Benchmark the reproducibility of the experimental observables, like the excitation energies (EX) and the reduced electric-quadrupole transition probabilities [B(E2)], with the results obtained from shell-model interactions for ne…

PhysicsAngular momentumValence (chemistry)Isotope010308 nuclear & particles physicsFissionNuclear TheoryNuclear structure7. Clean energy01 natural sciencesNeutron number0103 physical sciencesAGATANeutronAtomic physicsNuclear Experiment010306 general physicsPhysical Review C
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Nucleon Pairing and Seniority

2007

Until now we have been dealing with particle and hole aspects of nuclear structure. In this second part of the book we go farther away from a closed major shell. Still near the beginning or end of a major shell we encounter vibrational, spherical open-shell nuclei that cannot be described in terms of a few particles or holes. Farther towards the middle of the shell the spherical shape will give way to permanent deformation signalled by rotational bands analogous to those of diatomic molecules. Microscopic description of such nuclei requires a deformed mean field as the starting point. Deformed nuclei will not be considered in any detail in this book.

PhysicsClassical mechanicsMean field theoryDeformation (mechanics)PairingNuclear TheoryPhysics::Atomic and Molecular ClustersShell (structure)Nuclear structureParticleNucleonDiatomic molecule
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Nonlocal energy density functionals for low-energy nuclear structure

2014

We introduce a finite-range pseudopotential built as an expansion in derivatives up to next-to-next-to-next-to-leading order (N$^3$LO) and we calculate the corresponding nonlocal energy density functional (EDF). The coupling constants of the nonlocal EDF, for both finite nuclei and infinite nuclear matter, are expressed through the parameters of the pseudopotential. All central, spin-orbit, and tensor terms of the pseudopotential are derived both in the spherical-tensor and Cartesian representation. At next-to-leading order (NLO), we also derive relations between the nonlocal EDF expressed in the spherical-tensor and Cartesian formalism. Finally, a simplified version of the finite-range pse…

PhysicsCoupling constantNuclear and High Energy PhysicsEnergy density functionalNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear structureFOS: Physical sciencesNuclear matterlaw.inventionPseudopotentialNuclear Theory (nucl-th)Low energylawEnergy densityCartesian coordinate systemComputer Science::Operating SystemsMathematical physics
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Spin-orbit and tensor mean-field effects on spin-orbit splitting including self-consistent core polarizations

2008

A new strategy of fitting the coupling constants of the nuclear energy density functional is proposed, which shifts attention from ground-state bulk to single-particle properties. The latter are analyzed in terms of the bare single-particle energies and mass, shape, and spin core-polarization effects. Fit of the isoscalar spin-orbit and both isoscalar and isovector tensor coupling constants directly to the f5/2-f7/2 spin-orbit splittings in 40Ca, 56Ni, and 48Ca is proposed as a practical realization of this new programme. It is shown that this fit requires drastic changes in the isoscalar spin-orbit strength and the tensor coupling constants as compared to the commonly accepted values but i…

PhysicsCoupling constantNuclear and High Energy PhysicsIsovectorNuclear TheoryBand gapIsoscalarBinding energyNuclear TheoryNuclear structureFOS: Physical sciencesPolarization (waves)Nuclear Theory (nucl-th)Mean field theoryAtomic physics
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Group O(4) in the Nuclear IBA Model

1994

The group O(4) is established as a link in the group chains of the interacting-boson model (IBA) of nuclear structure. It is obtained as a subgroup of O(5) by excluding the m = 0 component of the d boson. Since only the third component of the angular momentum is then conserved, O(4) symmetry is limited to intrinsic states. No O(3) can be sandwiched between this O(4) and the physical O(2). Branching rules are derived for groups U(4), O(4) and O(2). The dynamic-symmetry contributions of O(4) and U(4) to the energy are given. The structure \(O\left( 4 \right) \approx O\left( 3 \right) \times O\left( 3 \right) \supset O\left( 3 \right)\)is established

PhysicsCrystallographyCondensed matter physicsNuclear structureBoson
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Beta decay of neutron-rich Co: Probing single-particle states at and above the N=40 subshell closure

1999

Neutron-rich Co nuclei with A=66–70 were produced by the laser-ionization isotope-separation on-line method. The β decay from these nuclei has been studied. A case example is given by reporting on the observed decay scheme of 68Co. The half life of the ground-state decay of this nucleus was measured to be 0.21(3) seconds. In addition, a new β decaying isomer half life of 1.16(25) seconds was discovered. The level scheme of 68Ni has been significantly extended, and an interpretation of the observed levels is made by assuming that the N=40 gap has the characteristics of a shell closure.

PhysicsDecay schemeIsotopeNuclear TheoryNuclear structureHalf-lifeNeutronAtomic physicsNuclear ExperimentIsotopes of cobaltBeta decayRadioactive decayAIP Conference Proceedings
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One-neutron halo structure by the ratio method

2011

We present a new observable to study halo nuclei. This new observable is a particular ratio of angular distributions for elastic breakup and scattering. For one-neutron halo nuclei, it is shown to be independent of the reaction mechanism and to provide significant information about the structure of the projectile, including binding energy, partial-wave configuration, and radial wave function of the halo. This observable offers new capabilities for the study of nuclear structure far from stability.

PhysicsElastic scatteringNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsScatteringBinding energyNuclear TheoryNuclear structureFOS: Physical sciencesHalo nucleusObservable7. Clean energy01 natural sciencesNuclear physicsNuclear Theory (nucl-th)0103 physical sciencesNeutronHaloNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Experiment
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Infinite matter properties and zero-range limit of nonrelativistic finite-range interactions

2016

We discuss some infinite matter properties of two finite-range interactions widely used for nuclear structure calculations, namely Gogny and M3Y interactions. We show that some useful informations can be deduced for the central, tensor and spin-orbit terms from the spin-isospin channels and the partial wave decomposition of the symmetric nuclear matter equation of state. We show in particular that the central part of the Gogny interaction should benefit from the introduction of a third Gaussian and the tensor parameters of both interactions can be deduced from special combinations of partial waves. We also discuss the fact that the spin-orbit of the M3Y interaction is not compatible with lo…

PhysicsEquation of stateNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsGaussianNuclear TheoryNuclear structureFOS: Physical sciencesGeneral Physics and AstronomyNuclear matter01 natural sciencesNuclear Theory (nucl-th)Momentumsymbols.namesakeTheoretical physics0103 physical sciencessymbolsGauge theoryTensorLimit (mathematics)010306 general physics
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Frontiers of Heavy - Ion Physics and Superheavy Elements

2003

This contribution will focus on three topics of GSI nuclear structure research: super heavy elements, direct mass measurements in the storage ring, and the measurement of spallation cross section in reversed kinematics. The GSI project for an extended synchrotron facility will be outlined.

PhysicsFocus (computing)Nuclear and High Energy PhysicsFissionNuclear structureTransactinide elementSuperheavy ElementsSynchrotronlaw.inventionNuclear physicsCross section (physics)Nuclear Energy and EngineeringlawHeavy ionSpallationStorage ringJournal of Nuclear Science and Technology
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Nuclear structure dependence of fusion hindrance in heavy element synthesis

2018

The production of the heaviest elements in fusion-evaporation reactions is substantially limited by very low cross sections, as fusion cross sections (including fusion-fission) are greatly reduced by the competing quasifission mechanism. Using the Australian National University Heavy Ion Accelerator Facility and CUBE detector array, fission fragments from the $^{48}\mathrm{Ti}+^{204,208}\mathrm{Pb}$ and $^{50}\mathrm{Ti}+^{206,208}\mathrm{Pb}$ reactions have been measured, with the aim to investigate how the competition between quasifission and fusion-fission evolves with small changes in entrance-channel properties associated mainly with the nuclear structure. Analysis of mass-distribution…

PhysicsFusion010308 nuclear & particles physicsFissionNuclear TheoryNuclear structure7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesProduction (computer science)Heavy ionHeavy elementDetector arrayNuclear Experiment010306 general physicsPhysical Review C
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