EVOLUTION OF NEUTRON SHELL STRUCTURE OF N = 14, 16 ISOTONES

The evolution of the single-particle characteristics of neutron and proton-excess isotones with the new magic numbers N = 14, 16 in the Z range from 8 to 20 in the dispersive optical model was traced. The calculated energy gaps N = 14 and 16 widened with the increase in excess of protons and neutrons respectively. At the same time, the deviation of half-sum of the single-particle energies of the last predominantly occupied and the first predominantly unoccupied states from the Fermi energy decreased. The widening of the gaps enhanced under the assumption of an increase in the diffuseness of the Hartree–Fock component of the dispersive optical model potential with an increase in the neutron excess over the range of Z numbers considered. The bubble structure manifests clearly in the neutron density distribution of the proton-unstable nucleus Са.

Publication Details

Journal
Ядерная физика / Physics of Atomic Nuclei
Published
2025-01-01
DOI
https://doi.org/10.7868/s3034628225010164
Primary Topic
Nuclear physics research studies
Type
article
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article

EVOLUTION OF NEUTRON SHELL STRUCTURE OF N = 14, 16 ISOTONES

Ядерная физика / Physics of Atomic Nuclei
Nuclear physics research studies
article

EVOLUTION OF NEUTRON SHELL STRUCTURE OF N = 14, 16 ISOTONES

article en

Abstract

The evolution of the single-particle characteristics of neutron and proton-excess isotones with the new magic numbers N = 14, 16 in the Z range from 8 to 20 in the dispersive optical model was traced. The calculated energy gaps N = 14 and 16 widened with the increase in excess of protons and neutrons respectively. At the same time, the deviation of half-sum of the single-particle energies of the last predominantly occupied and the first predominantly unoccupied states from the Fermi energy decreased. The widening of the gaps enhanced under the assumption of an increase in the diffuseness of the Hartree–Fock component of the dispersive optical model potential with an increase in the neutron excess over the range of Z numbers considered. The bubble structure manifests clearly in the neutron density distribution of the proton-unstable nucleus Са.

Ядерная физика / Physics of Atomic NucleiVol. 88(1)
Openalex Percentile: Top 87%
Nuclear physics research studies
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