Search results for "Isotone"

showing 10 items of 16 documents

Level scheme ofZr101and structure of theN=61 Sr, Zr, and Mo isotones

1995

The neutron-rich nucleus $_{40}^{101}\mathrm{Zr}_{61}$ has been studied at the isotope separator ISOLDE via the \ensuremath{\beta} decay of $^{101}\mathrm{Y}$. A detailed level scheme has been obtained from \ensuremath{\gamma}-ray singles, \ensuremath{\gamma}-\ensuremath{\gamma}-t and \ensuremath{\beta}-\ensuremath{\gamma}-t coincidence measurements. The level structure of $^{101}\mathrm{Zr}$ is similar to that of its isotone $^{103}\mathrm{Mo}$ showing that, in contrast to their Sr neighbors, the Zr isotopes do not reach maximum of deformation immediately at its onset. This result is rather well reproduced by particle-rotor coupling calculations. A level systematics for the deformed N=61 i…

Nuclear physicsPhysicsNuclear and High Energy PhysicsExcited stateIsotoneNuclear structureLevel structureAtomic physicsNuclear ExperimentRadioactive decayPhysical Review C
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Behavior of the nuclear charge radii systematics in thes-dshell from muonic atom measurements

1992

The present work extends the systematics of nuclear charge radii obtained by the method of muonic atoms to nuclei with 8\ensuremath{\le}Z,N\ensuremath{\le}20. The accuracy of the measured muonic Lyman transition energies of generally \ensuremath{\le}10 eV leads to a precision in the model-independent nuclear charge radii differences of 2--3 am for the isotope shifts and 4--9 am for isotone shifts. Both isotope and isotone shifts within the s-d shell behave ``anomalously'' with respect to the systematics of heavier nuclei. However, such behavior is predicted on theoretical grounds, if mixing in the s-d shells and the strong deformation of some of the nuclei in this region are considered. We …

PhysicsNuclear and High Energy PhysicsIsotopeScatteringIsotoneNuclear TheoryShell (structure)Charge densityCharge (physics)Effective nuclear chargePhysics::Atomic PhysicsAtomic physicsNuclear ExperimentExotic atomPhysical Review C
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Shell evolution of $N=40$ isotones towards $^{60}$Ca: First spectroscopy of $^{62}$Ti

2020

7 pags., 4 figs., 1 tab.

Nuclear and High Energy PhysicsNuclear TheoryNuclear TheoryAb initioFOS: Physical sciencesShell evolution[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesShell evolution ; Radioactive beams ; Gamma-ray spectroscopyNuclear Theory (nucl-th)Gamma-ray spectroscopy; Radioactive beams; Shell evolution0103 physical sciencesddc:530Gamma-ray spectroscopyNuclear Experiment (nucl-ex)010306 general physicsSpectroscopyNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsIsland of inversionIsotonePhysicsStarke Wechselwirkung und exotische Kerne – Abteilung BlaumFísicalcsh:QC1-999Excited stateQuadrupoleAtomic physicsNucleonGround statelcsh:PhysicsRadioactive beams
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Shape coexistence in theN=59 isotone97Sr

1988

Experimental evidence for shape coexistence in the N=59 isotone97Sr is presented. The ground state and the lowest excited levels are confirmed to be spherical. At 585.1 keV, a K=3/2 rotational band built on the v[422 3/2] Nilsson configuration has been identified. Nilsson orbital assignments for three further levels of deformed origin are proposed. The results are compared to RPA shell-model predictions.

PhysicsNuclear and High Energy PhysicsExcited stateIsotoneNuclear TheoryNuclear fusionElementary particleAtomic physicsGround stateZeitschrift f�r Physik A Atomic Nuclei
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Coulomb Excitation of Neutron-Rich Zn Isotopes: First Observation of the21+State inZn80

2007

Neutron-rich, radioactive Zn isotopes were investigated at the Radioactive Ion Beam facility REX-ISOLDE (CERN) using low-energy Coulomb excitation. The energy of the 2(1)+ state in 78Zn could be firmly established and for the first time the 2+ --> 0(1)+ transition in 80Zn was observed at 1492(1) keV. B(E2,2(1)+ --> 0(1)+) values were extracted for (74,76,78,80)Zn and compared to large scale shell model calculations. With only two protons outside the Z=28 proton core, 80Zn is the lightest N=50 isotone for which spectroscopic information has been obtained to date. Two sets of advanced shell model calculations reproduce the observed B(E2) systematics. The results for N=50 isotones indicate a g…

PhysicsLarge Hadron ColliderProtonIon beamIsotope010308 nuclear & particles physicsIsotoneNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementCoulomb excitationZinc01 natural scienceschemistry0103 physical sciencesPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear Experiment010306 general physicsPhysical Review Letters
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Isomers inPd128andPd126: Evidence for a Robust Shell Closure at the Neutron Magic Number 82 in Exotic Palladium Isotopes

2013

The level structures of the very neutron-rich nuclei $^{128}\mathrm{Pd}$ and $^{126}\mathrm{Pd}$ have been investigated for the first time. In the $r$-process waiting-point nucleus $^{128}\mathrm{Pd}$, a new isomer with a half-life of $5.8(8)\text{ }\text{ }\ensuremath{\mu}\mathrm{s}$ is proposed to have a spin and parity of ${8}^{+}$ and is associated with a maximally aligned configuration arising from the ${g}_{9/2}$ proton subshell with seniority $\ensuremath{\upsilon}=2$. For $^{126}\mathrm{Pd}$, two new isomers have been identified with half-lives of 0.33(4) and $0.44(3)\text{ }\text{ }\ensuremath{\mu}\mathrm{s}$. The yrast ${2}^{+}$ energy is much higher in $^{128}\mathrm{Pd}$ than in…

Physics010308 nuclear & particles physicsYrastIsotoneNuclear TheoryGeneral Physics and Astronomy01 natural sciencesMagic number (programming)Isotopes of palladiumNeutron number0103 physical sciencesQuadrupoleLevel structureNeutronAtomic physics010306 general physicsPhysical Review Letters
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Five-valence-protonN=82isotone137Cs

1999

Yrast excitations in the N=82 isotone {sup 137}Cs have been identified for the first time in thick-target {gamma}-ray coincidence measurements for the system {sup 232}Th+{sup 136}Xe using the Gammasphere array. The {sup 137}Cs nuclei were produced in deep inelastic one-proton-transfer reactions. By-products of the main investigation were two well-developed rotational bands which were identified in heavy reaction partner products complementary to {sup 137}Cs and are tentatively assigned to the little studied nucleus {sup 231}Ac. There was no difficulty in placing the 11 observed {sup 137}Cs transitions in a yrast level scheme extending to an I{sup {pi}}=(31/2{sup {minus}}) level at 5494 keV.…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonExcited stateIsotoneYrastHadronGammasphereAtomic physicsNucleonPhysical Review C
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Assignment of levels in 208Fr and 10- isomers in the odd-odd isotones 206At and 208Fr

2009

Excited states in 208 Fr have been identified using the 197 Au( 16 O, 5n) 208 Fr reaction and a variety of time-correlated γ-ray and conversion electron spectroscopic techniques. Transitions above and below a τ = 623(16) ns 10 − isomer are placed in the level scheme. This isomer is analogous to that observed in the odd-odd isotone 206 At for which additional spectroscopic information is also obtained, including a precise lifetime of τ = 1173(30) ns. The γ-rays assigned to 208 Fr are the same as the main transitions erroneously assigned to 209 Fr in previous work.

PhysicsNuclear and High Energy PhysicsExcited stateIsotoneHadronNuclear fusionElectronAtomic physicsThe European Physical Journal A
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Level structure of 99Nb

1998

The β decay of 97Sr to 97Y has been investigated using ion-guide on-line mass separation and a 10 Ge-detector array to record γ−γ coincidences to a detection limit well below that of former studies. Similarities are found in the β-decay patterns of 99Zr and of its isotone 97Sr and also in the γ-ray decay rates and branchings of the corresponding levels in their respective daughters 99Nb and 97Y. This indicates a persisting influence of the d5/2 neutron shell closure for 99Nb. The level structure of 99Nb and the β-feeding pattern are discussed in the frame of the interacting boson-fermion plus broken pair model and the microscopic quasiparticle phonon model.

Physicsbeta decay nuclear stucture 99Nb interacting boson-fermion plus broken pair modelNuclear and High Energy PhysicsCondensed matter physicsPhononIsotoneShell (structure)Beta decayMolecular physicsNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.QuasiparticleLevel structureNeutronInteracting boson modelbeta decay; nuclear stucture; 99Nb; interacting boson-fermion plus broken pair model
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Half-Life Systematics across theN=126Shell Closure: Role of First-Forbidden Transitions in theβDecay of Heavy Neutron-Rich Nuclei

2014

This Letter reports on a systematic study of β-decay half-lives of neutron-rich nuclei around doubly magic Pb208. The lifetimes of the 126-neutron shell isotone Pt204 and the neighboring Ir200-202, Pt203, Au204 are presented together with other 19 half-lives measured during the "stopped beam" campaign of the rare isotope investigations at GSI collaboration. The results constrain the main nuclear theories used in calculations of r-process nucleosynthesis. Predictions based on a statistical macroscopic description of the first-forbidden β strength reveal significant deviations for most of the nuclei with N<126. In contrast, theories including a fully microscopic treatment of allowed and first…

PhysicsIsotopeIsotoneNuclear TheoryGeneral Physics and AstronomyBeta decayNuclear physicsNucleosynthesisDouble beta decayr-processNeutronAtomic physicsNuclear ExperimentSpectroscopyPhysical Review Letters
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