Search results for " shell"

showing 10 items of 307 documents

Three beta-decaying states in 128In and 130In resolved for the first time using Penning-trap techniques

2020

Isomeric states in 128In and 130In have been studied with the JYFLTRAP Penning trap at the IGISOL facility. By employing state-of-the-art ion manipulation techniques, three different beta-decaying states in 128In and 130In have been separated and their masses measured. JYFLTRAP was also used to select the ions of interest for identification at a post-trap decay spectroscopy station. A new beta-decaying high-spin isomer feeding the isomer in 128Sn has been discovered in 128In at 1797.6(20) keV. Shell-model calculations employing a CD-Bonn potential re-normalized with the perturbative G-matrix approach suggest this new isomer to be a 16⁺ spin-trap isomer. In 130In, the lowest-lying (10⁻) isom…

Nuclear and High Energy PhysicsPenning trapAstronomy & Astrophysics01 natural sciencesIonPhysics Particles & Fieldsbeta-decay spectroscopyIsomersShell model0103 physical sciencesPhysics::Atomic and Molecular ClustersNuclear Experiment010306 general physicsSpectroscopyCouplingPhysicsScience & TechnologyNUCLEI010308 nuclear & particles physicsPhysicsPRECISION MASS-SPECTROMETRYNuclear shell modelR-PROCESSshell modelpenning trapRAMSEY METHODPenning traplcsh:QC1-999Physics NuclearExcited stateBeta (plasma physics)Physical SciencesSHELL-MODELTRANSITION-PROBABILITIESisomersAtomic physicsBeta-decay spectroscopylcsh:PhysicsIon cyclotron resonancePhysics Letters B
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Search for two-neutrino double electron capture of $^{124}$Xe with XENON100

2017

Two-neutrino double electron capture is a rare nuclear decay where two electrons are simultaneously captured from the atomic shell. For $^{124}$Xe this process has not yet been observed and its detection would provide a new reference for nuclear matrix element calculations. We have conducted a search for two-neutrino double electron capture from the K-shell of $^{124}$Xe using 7636 kg$\cdot$d of data from the XENON100 dark matter detector. Using a Bayesian analysis we observed no significant excess above background, leading to a lower 90 % credibility limit on the half-life $T_{1/2}>6.5\times10^{20}$ yr. We also evaluated the sensitivity of the XENON1T experiment, which is currently bein…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectron captureenergy resolutionFOS: Physical scienceschemistry.chemical_elementelectron: captureElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBayesianX-rayneutrinoXenon0103 physical sciencesSensitivity (control systems)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)010306 general physics[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear ExperimentPhysicsnucleus: decayTime projection chamberphotomultiplier010308 nuclear & particles physicsbackgroundInstrumentation and Detectors (physics.ins-det)dark matter: detectorAtomic shellsensitivitytime projection chamberGran SassoxenonchemistryNeutrinoAtomic physicsRadioactive decayexperimental results
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Nuclear charge radii of 62−80Zn and their dependence on cross-shell proton excitations

2019

Nuclear charge radii of 62−80Zn have been determined using collinear laser spectroscopy of bunched ion beams at CERN-ISOLDE. The subtle variations of observed charge radii, both within one isotope and along the full range of neutron numbers, are found to be well described in terms of the proton excitations across the Z=28 shell gap, as predicted by large-scale shell model calculations. It comprehensively explains the changes in isomer-to-ground state mean square charge radii of 69−79Zn, the inversion of the odd-even staggering around N=40 and the odd-even staggering systematics of the Zn charge radii. With two protons above Z=28, the observed charge radii of the Zn isotopic chain show a cum…

Nuclear and High Energy PhysicsProtonShell closureNuclear TheoryAstronomy & Astrophysics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530ISOTOPE SHIFTS01 natural sciences7. Clean energyMolecular physicsEffective nuclear chargePhysics Particles & FieldsIonNaturvetenskap0103 physical sciencesNuclear Physics - Experimentddc:530Neutron010306 general physicsSpectroscopyNuclear ExperimentCumulative effectPhysicsScience & TechnologyIsotopeCorrelations010308 nuclear & particles physicsPhysicsNuclear structurelcsh:QC1-999Physique atomique et nucléaireNuclear deformationZincPhysics NuclearNuclear charge radiiPhysical SciencesCorrelations ; Nuclear charge radii ; Nuclear deformation ; Shell closure ; ZincPräzisionsexperimente - Abteilung BlaumNatural Scienceslcsh:Physics
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Study of isomeric states in $^{198,200,202,206}$Pb and $^{206}$Hg populated in fragmentation reactions

2018

International audience; Isomeric states in isotopes in the vicinity of doubly-magic 208Pb were populatedfollowing reactions of a relativistic 208Pb primary beam impinging on a9Be fragmentation target. Secondary beams of 198,200,202,206Pb and 206Hg wereisotopically separated and implanted in a passive stopper positioned in thefocal plane of the GSI Fragment Separator. Delayed γ rays were detected withthe Advanced Gamma Tracking Array (AGATA). Decay schemes were reevaluatedand interpreted with shell-model calculations. The momentumdependentpopulation of isomeric states in the two-nucleon hole nuclei206Pb/206Hg was found to differ from the population of multi neutron-holeisomeric states in 198…

Nuclear and High Energy Physicsisomeric decaysAstrophysics::High Energy Astrophysical PhenomenaPopulationNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesFragmentation (mass spectrometry)Subatomic Physics0103 physical sciencesGamma spectroscopyGamma-ray spectroscopy010306 general physicseducationNuclear ExperimentPhysicseducation.field_of_studyIsotope010308 nuclear & particles physicsNuclear shell modeldirect reactionsrelativistic projectile fragmentationelectromagnetic transitionsnuclear shell modelAGATAPreSPEC-AGATAAtomic physicsBeam (structure)
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Evolution of nuclear structure in neutron-rich odd-Zn isotopes and isomers

2017

Collinear laser spectroscopy was performed on Zn (Z=30) isotopes at ISOLDE, CERN. The study of hyperfine spectra of nuclei across the Zn isotopic chain, N=33–49, allowed the measurement of nuclear spins for the ground and isomeric states in odd-A neutron-rich nuclei up to N=50. Exactly one long-lived (&

Nuclear and High Energy Physicsshell closureShell closureNuclear TheoryLasermagnetic dipole moment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesQuadrupole momentMagnetic dipole momentNaturvetenskap0103 physical sciencesPhysics::Atomic and Molecular ClustersDalton Nuclear InstituteNuclear Physics - Experimentddc:530NeutronPhysics::Atomic Physics010306 general physicsNuclear ExperimentHyperfine structurePhysicsValence (chemistry)quadrupole momentMagnetic moment010308 nuclear & particles physicsNuclear structurePhysique atomique et nucléairelcsh:QC1-999laserZincResearchInstitutes_Networks_Beacons/dalton_nuclear_instituteZinc ; Magnetic dipole moment ; Quadrupole moment ; Laser ; Shell closureQuadrupoleNuclear magnetic momentPräzisionsexperimente - Abteilung BlaumAtomic physicsNatural SciencesMagnetic dipolelcsh:Physics
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Spins, Electromagnetic Moments, and Isomers of $^{107-129}Cd$

2013

The neutron-rich isotopes of cadmium up to the N=82 shell closure have been investigated by high-resolution laser spectroscopy. Deep-UV excitation at 214.5 nm and radioactive-beam bunching provided the required experimental sensitivity. Long-lived isomers are observed in 127Cd and 129Cd for the first time. One essential feature of the spherical shell model is unambiguously confirmed by a linear increase of the 11/2- quadrupole moments. Remarkably, this mechanism is found to act well beyond the h11/2 shell. The neutron-rich isotopes of cadmium up to the N=82 shell closure have been investigated by high-resolution laser spectroscopy. Deep-uv excitation at 214.5 nm and radioactive-beam bunchin…

Nuclear momentsNuclear Theoryddc:550FOS: Physical sciencesPhysics::Accelerator PhysicsNuclear Physics - ExperimentNuclear Experiment (nucl-ex)Laser spectroscopyNuclear ExperimentNuclear shell model
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Properties of heavy nuclei measured at the GSI SHIP

2004

Abstract The nuclear shell model predicts that the next doubly magic shell-closure beyond 208 Pb is at a proton number Z = 114, 120, or 126 and at a neutron number N = 172 or 184. The outstanding aim of experimental investigations is the exploration of this region of spherical ‘Super-Heavy Elements’ (SHEs). The measured decay data reveal that for the heaviest elements, the dominant decay mode is α emission, not fission. Decay properties as well as reaction cross-sections are compared with results of theoretical investigations. Finally, plans are presented for the further development of the experimental set-up and the application of new techniques.At a higher sensitivity, the exploration of …

Nuclear physicsPhysicsNuclear and High Energy PhysicsFissionNeutron numberNuclear TheoryNuclear shell modelAtomic numberAtomic physicsNuclear ExperimentNuclear Physics A
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Shell-model study of partial muon-capture rates in light nuclei

1998

Abstract The nuclear shell model is used to study ordinary muon capture of light nuclei in the p, sd and p-sd shell-model spaces. Several well-established two-body interactions are applied to calculate the involved nuclear matrix elements and the emerging results are compared with each other. The resulting theoretical partial muon-capture rates are compared with experimental data and their stability against different model spaces and interactions studied. The effects of the induced-pseudoscalar strength, C p , on the capture rates is discussed. The relation between the allowed partial muon capture rates and the Gamow-Teller strength function is stressed.

Nuclear physicsPhysicsNuclear and High Energy PhysicsLight nucleusStrength functionNuclear TheorySHELL modelNuclear shell modelAtomic physicsNuclear matrixStability (probability)Muon captureNuclear Physics A
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Analysis of the 2νββ decay and muon capture reactions for the mass A = 46 and A = 48 nuclei using the nuclear shell model

2005

We discuss the two-neutrino double-beta decays of 46Ca and 48Ca by using the nuclear shell model with well-tested two-body interactions. We also discuss the ordinary muon-capture (OMC) reaction on the final nuclei, 46Ti and 48Ti, of these decays. The OMC leads to the virtual states of the intermediate nuclei, 46Sc and 48Sc, in these double-beta decays.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear shell modelHigh Energy Physics::ExperimentNuclear ExperimentAtomic and Molecular Physics and OpticsMuon captureNuclear Physics B - Proceedings Supplements
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Single-neutron orbits near 78 Ni: Spectroscopy of theN=49isotope 79 Zn

2015

Single-neutron states in the Z=30, N=49isotope 79Zn have been populated using the 78Zn(d,p)79Zn transfer reaction at REX-ISOLDE, CERN. The experimental setup allowed the combined detection of protons ejected in the reaction, and of γrays emitted by 79Zn. The analysis reveals that the lowest excited states populated in the reaction lie at approximately 1MeV of excitation, and involve neutron orbits above the N=50shell gap. From the analysis of γ-ray data and of proton angular distributions, characteristic of the amount of angular momentum transferred, a5/2+configuration was assigned to a state at 983keV. Comparison with large-scale-shell-model calculations supports a robust neutron N=50shell…

Nuclear reactionNuclear and High Energy PhysicsAngular momentumProtonAstrophysics::High Energy Astrophysical PhenomenaNuclear Theorygamma-Ray transitions[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesTransfer reactions0103 physical sciencesNuclear Physics - ExperimentNeutronNuclear structureNuclear Experiment010306 general physicsSpectroscopyComputingMilieux_MISCELLANEOUSN=50 shell closure[PHYS]Physics [physics]PhysicsElastic scatteringNUCLEIRICH ISOTOPES010308 nuclear & particles physicslcsh:QC1-999ELASTIC-SCATTERINGExcited stateAtomic physicsγ-Ray transitionsNucleonlcsh:PhysicsPhysics Letters B
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