Search results for "nuclear structure"

showing 10 items of 401 documents

Hyperfine anomaly in gold and magnetic moments of $I^{\pi}$ $= 11/2^{−}$ gold isomers

2020

Physical review / C 101(3), 034308 (2020). doi:10.1103/PhysRevC.101.034308

Nuclear Physics - Experimentddc:530Physics::Atomic Physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Structure530
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Spectroscopy of low-spin states in $^{157}\mathrm{Dy}$: Search for evidence of enhanced octupole correlations

2019

Low-spin states of 157Dy have been studied using the JUROGAM II array, following the 155Gd ({\alpha}, 2n) reaction at a beam energy of 25 MeV. The level scheme of 157Dy has been expanded with four new bands. Rotational structures built on the [523]5/2- and [402]3/2+ neutron orbitals constitute new additions to the level scheme as do many of the inter- and intra-band transitions. This manuscript also reports the observation of cross I- to (I-1)- and I- to (I-1)+ E1 dipole transitions inter-linking structures built on the [523]5/2- (band 5) and [402]3/2+ (band 7) neutron orbitals. These interlacing band structures are interpreted as the bands of parity doublets with simplex quantum number s =…

Nuclear Theory (nucl-th)Nuclear Theorynuclear spin and parityshell modelFOS: Physical sciencescollective levelscollective modelsNuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ydinfysiikkaNuclear Structurenuclear structure and decaysNuclear Experiment
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Extended shell model calculation for even N = 82 isotones with a realistic effective interaction

1996

The shell model within the $2s1d0g_{7/2}0h_{11/2}$ shell is applied to calculate nuclear structure properties of the even Z=52 - 62, N=82 isotones. The results are compared with experimental data and with the results of a quasiparticle random-phase approximation (QRPA) calculation. The interaction used in these calculations is a realistic two-body G-matrix interaction derived from modern meson-exchange potential models for the nucleon-nucleon interaction. For the shell model all the two-body matrix elements are renormalized by the $\hat{Q}$-box method whereas for the QRPA the effective interaction is defined by the G-matrix.

Nuclear Theory (nucl-th)PhysicsNuclear and High Energy PhysicsMatrix (mathematics)Nuclear TheorySHELL modelNuclear TheoryShell (structure)Nuclear structureQuasiparticleFOS: Physical sciencesNuclear ExperimentMolecular physics
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In-beam gamma-ray and electron spectroscopy of $^{249,251}$Md

2020

The odd-Z Md251 nucleus was studied using combined γ-ray and conversion-electron in-beam spectroscopy. Besides the previously observed rotational band based on the [521]1/2− configuration, another rotational structure has been identified using γ-γ coincidences. The use of electron spectroscopy allowed the rotational bands to be observed over a larger rotational frequency range. Using the transition intensities that depend on the gyromagnetic factor, a [514]7/2− single-particle configuration has been inferred for this band, i.e., the ground-state band. A physical background that dominates the electron spectrum with an intensity of ≃60% was well reproduced by simulating a set of unresolved ex…

Nuclear Theory (nucl-th)nucl-th[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryNuclear Physics - TheoryFOS: Physical sciencesNuclear Physics - Experimentddc:530Nuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear StructureNuclear Experiment
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Evolution of Octupole Deformation in Radium Nuclei from Coulomb Excitation of Radioactive $^{222}$Ra and $^{228}$Ra Beams

2020

There is sparse direct experimental evidence that atomic nuclei can exhibit stable pear shapes arising from strong octupole correlations. In order to investigate the nature of octupole collectivity in radium isotopes, electric octupole ($E3$) matrix elements have been determined for transitions in $^{222,228}$Ra nuclei using the method of sub-barrier, multi-step Coulomb excitation. Beams of the radioactive radium isotopes were provided by the HIE-ISOLDE facility at CERN. The observed pattern of $E$3 matrix elements for different nuclear transitions is explained by describing $^{222}$Ra as pear-shaped with stable octupole deformation, while $^{228}$Ra behaves like an octupole vibrator.

Nuclear TheoryAtomic Physics (physics.atom-ph)Nuclear TheoryFOS: Physical sciencesnuclear structure and decaysPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)electromagnetic transitionsPhysics::Accelerator Physicscollective levelsPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)ydinfysiikkaNuclear ExperimentNuclear Experiment
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Competition between Allowed and First-Forbidden β Decay : The Case of Hg208→Tl208

2020

The β decay of 208Hg into the one-proton hole, one neutron-particle 20881Tl127 nucleus was investigated at CERN-ISOLDE. Shell-model calculations describe well the level scheme deduced, validating the proton-neutron interactions used, with implications for the whole of the N>126, Z<82 quadrant of neutron-rich nuclei. While both negative and positive parity states with spin 0 and 1 are expected within the Qβ window, only three negative parity states are populated directly in the β decay. The data provide a unique test of the competition between allowed Gamow-Teller and Fermi, and first-forbidden β decays, essential for the understanding of the nucleosynthesis of heavy nuclei in the rapid neut…

Nuclear TheoryNuclear Experimentydinfysiikkanuclear structure and decays
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Evidence for a spin-aligned neutron-proton paired phase from the level structure of (92)Pd

2011

4 páginas, 4 figuras.-- El Pdf es la versión pre-print.-- et al.

Nuclear TheoryProton[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]pairingNuclear Theory (nucl-th)Magic number (programming)spin-alignementPhysics::Atomic and Molecular ClustersNuclear forceNeutronNuclear structureNuclear Experiment (nucl-ex)Spin (physics)Nuclear ExperimentNuclear ExperimentPhysicsMultidisciplinaryta114Nuclear structureNuclear shell modelAtomic nucleusFísica nuclearAtomic physics
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Mirror and triplet displacement energies within nuclear DFT: : numerical stability

2017

Isospin-symmetry-violating class II and III contact terms are introduced into the Skyrme energy density functional to account for charge dependence of the strong nuclear interaction. The two new coupling constants are adjusted to available experimental data on triplet and mirror displacement energies, respectively. We present preliminary results of the fit, focusing on its numerical stability with respect to the basis size.

Nuclear TheorySYMMETRYNuclear TheoryFOS: Physical sciencesGeneral Physics and Astronomy114 Physical sciences01 natural sciencesDisplacement (vector)strong nuclear forceNuclear Theory (nucl-th)0103 physical sciences010306 general physicsdisplacement energiesdensity functional theoryPARAMETRIZATIONCoupling constantPhysicsta114Energy density functionalBasis (linear algebra)010308 nuclear & particles physicstiheysfunktionaaliteoriaCharge (physics)Nuclear interactionnuclear structureAtomic physicsisospin-symmetry breakingNumerical stability
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First candidates for $\gamma$ vibrational bands built on the $[505]11/{2}^{-}$ neutron orbital in odd-$A$ Dy isotopes

2020

Rotational structures have been measured using the Jurogam II and GAMMASPHERE arrays at low spin following the 155Gd({\alpha},2n)157Dy and 148Nd(12C, 5n)155Dy reactions at 25 and 65 MeV, respectively. We report high-K bands, which are conjectured to be the first candidates of a K{\pi}= 2+ {\gamma} vibrational band, built on the [505]11/2- neutron orbital, in both odd-A 155, 157Dy isotopes. The coupling of the first excited K=0+ states or the so-called \b{eta} vibrational bands at 661 and 676 keV in 154Dy and 156Dy to the [505]11/2- orbital, to produce a K{\pi}=11/2- band, was not observed in both 155Dy and 157Dy, respectively. The implication of these findings on the interpretation of the f…

Nuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear StructureNuclear Experiment
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Impact of the surface energy coefficient on the deformation properties of atomic nuclei as predicted by Skyrme energy density functionals

2018

Background: In the framework of nuclear energy density functional (EDF) methods, many nuclear phenomena are related to the deformation of intrinsic states. Their accurate modeling relies on the correct description of the change of nuclear binding energy with deformation. The two most important contributions to the deformation energy have their origin in shell effects that are correlated to the spectrum of single-particle states, and the deformability of nuclear matter, that can be characterized by a model-dependent surface energy coefficient asurf. Purpose: With the goal of improving the global performance of nuclear EDFs through the fine-tuning of their deformation properties, the purpose …

Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryFOS: Physical sciencesNuclear Structure01 natural sciences7. Clean energySpectral lineNuclear Theory (nucl-th)nuclear physics0103 physical sciences010306 general physicsNuclear Experimentdensity functional theoryPhysicsta114010308 nuclear & particles physicstiheysfunktionaaliteoriaOrder (ring theory)Moment of inertiaNuclear matterPhysique atomique et nucléaireIsospinAtomic nucleusNuclear binding energyAtomic physicsydinfysiikkaEnergy (signal processing)
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