Skip to content
DraconiticResearch
Search Sources API
201,683 studies31 sourcesUpdated 57 min ago
PreprintarXiv licencearXiv

Probing alternating-parity bands in even-even nuclei within an axial quadrupole-octupole-hexadecapole collective model

Abstract

An analytic quadrupole octupole hexadecapole (QOH) axially symmetric model is used to provide a coherent framework for describing both octupole vibrations and octupole deformations in even-even nuclei. The model offers analytical solutions for the energy spectra and electric E1, E2 and E3 transition probabilities. The spectroscopic features are governed by three physically meaningful parameters: the stiffness constant c2, the hexadecapole deformation parameter ϕ02, and the sextic potential parameter α, directly linked to ϕ01π which represents the interplay between the quadrupole and octupole deformations for both even and odd angular momentum states. The model is applied across a broad range of nuclei including Ra, Th, Sm, Ba, U, Gd, Nd, Rn, Pu, Xe, and Ce isotopes, effectively capturing the characteristic properties of alternating parity bands. Detailed calculations of E1, E2, and E3 transition matrix elements have been performed for 220,222Rn, 222,224,228Ra, and 144,146Ba yielding results in good agreement with available experimental data.

Versions

Related

  1. Explicit and Parallelised Octupole and Hexadecapole Moment Interactions in Flexible Smooth Particle Mesh Ewald
    Matthew L. Brown, Michael K. Bane, Paul L. A. Popelier +1
    ChemRxivPreprintCC BYAtomic, molecular & optical physicsChemRxiv
  2. Semiclassical description of quadrupole-hexadecapole correlation in nuclear shape evolution
    Kenichiro Arita
    arXivPreprintCC BY 4.0Full textNuclear physicsarXiv
  3. Probing Collective and Individual Kondo Screening: Multi-Stage, Multi-Channel Kondo Effects in a C3-Symmetric Four-Impurity Model
    Danqing Hu, Jiangfan Wang, Zixiang Hu +1
    arXivPreprintCC BY-NC-SA 4.0Full textCondensed matterarXiv
  4. Octupole deformation in even-even Ra isotopes from covariant density functional theory with localized exchange terms in a three-dimensional lattice space
    Z.Y. Dong, Z.X. Ren, Q. Zhao +1
    Physics Letters BPeer-reviewedCC BY 4.0Full textNuclear physicsCrossref
  5. Two-Peak Heat Capacity Accounts for Rln (2) Entropy and Ground State Access in the Dipole-Octupole Pyrochlore Ce2Hf2 O7
    E.M. Smith, A. Fitterman, R. Schäfer +18
    Physical Review LettersPeer-reviewedLicence not statedFull text7 citedCondensed matterHAL
BibTeX
@misc{chabab2026probing,
  title = {{Probing alternating-parity bands in even-even nuclei within an axial quadrupole-octupole-hexadecapole collective model}},
  author = {M. Chabab and A. El Batoul and L. El Ouaourti},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.08294},
  eprint = {2610.08294},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.08294},
}
RIS
TY  - UNPB
TI  - Probing alternating-parity bands in even-even nuclei within an axial quadrupole-octupole-hexadecapole collective model
AU  - M. Chabab
AU  - A. El Batoul
AU  - L. El Ouaourti
PY  - 2026
DA  - 2026/10/06
PB  - arXiv
DO  - 10.48550/arxiv.2610.08294
UR  - https://arxiv.org/abs/2610.08294
AB  - An analytic quadrupole octupole hexadecapole (QOH) axially symmetric model is used to provide a coherent framework for describing both octupole vibrations and octupole deformations in even-even nuclei. The model offers analytical solutions for the energy spectra and electric E1, E2 and E3 transition probabilities. The spectroscopic features are governed by three physically meaningful parameters: the stiffness constant c_2, the hexadecapole deformation parameter ϕ_02, and the sextic potential parameter α, directly linked to ϕ_01^π which represents the interplay between the quadrupole and octupole deformations for both even and odd angular momentum states. The model is applied across a broad range of nuclei including Ra, Th, Sm, Ba, U, Gd, Nd, Rn, Pu, Xe, and Ce isotopes, effectively capturing the characteristic properties of alternating parity bands. Detailed calculations of E1, E2, and E3 transition matrix elements have been performed for ^220,222Rn, ^222,224,228Ra, and ^144,146Ba yielding results in good agreement with available experimental data.
ER  -