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arxiv: 2403.03713 · v1 · pith:BZGM4R62new · submitted 2024-03-06 · ⚛️ nucl-th

Nuclear magnetism in the deformed halo nucleus ³¹Ne

classification ⚛️ nucl-th
keywords halomagnetismnuclearnucleusdeformedboundcorecurrent
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Based on the point-coupling density functional, the time-odd deformed relativistic Hartree-Bogoliubov theory in continuum (TODRHBc) is developed. Then the effects of nuclear magnetism on halo phenomenon are explored by taking the experimentally suggested deformed halo nucleus $^{31}$Ne as an example. For $^{31}$Ne, nuclear magnetism contributes 0.09 MeV to total binding energy, and the breaking of Kramers degeneracy results in 0-0.2 MeV splitting in canonical single-particle spectra. The blocked neutron level has a dominant component of $p$ wave and it is marginally bound. However, if we ignore nuclear magnetism, the level becomes unbound. This shows a subtle mechanism that nuclear magnetism changes the single-particle energies, causing a nucleus to become bound. Based on the TODRHBc results, a prolate one-neutron halo is formed around the near-spherical core in $^{31}$Ne. The nucleon current is mostly contributed by the halo rather than the core, except near the center of the nucleus. A layered structure in the neutron current distribution is observed and studied in detail.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Deformed neutron halo nuclei and soft dipole excitations in the 40<A<90 mass region

    nucl-th 2026-05 unverdicted novelty 5.0

    DRHBc calculations identify unique density features in possible s- and p-wave deformed halo nuclei and demonstrate that low-energy dipole response sensitively probes halo components and deformation in the 40<A<90 region.

  2. Deformed neutron halo nuclei and soft dipole excitations in the 40<A<90 mass region

    nucl-th 2026-05 unverdicted novelty 4.0

    DRHBc calculations on three candidate nuclei show unique density features in deformed halos and indicate that low-energy dipole response is sensitive to halo wave-function components and deformation.