{
  "annotation_id": "d972b405-ada1-4591-8d4e-ed19d3724b8d",
  "date_created": "2026-03-02T18:00:04.808000Z",
  "date_modified": "2026-03-02T18:00:04.808000Z",
  "file_hash": "c7105da3133fb80dd7fe8f5675ac60de1a5b932bdaf79e4c2830ee52dac5e664",
  "private": false,
  "record": {
    "abstract": "A comparative study is performed of a deformed mean field theory, represented\nby the cranked Nilsson-Strutinsky (CNS) model, and the spherical shell model.\nEnergy spectra, occupation numbers, B(E2)-values, and spectroscopic quadrupole\nmoments in the light pf shell nuclei are calculated in the two models and\ncompared. The result is also compared to available experimental data which are\ngenerally well described by the shell model. Although the Nilsson-Strutinsky\ncalculation does not include pairing, both the subshell occupation numbers and\nquadrupole properties are found to be rather similar in the two models. It is\nalso shown that ``unpaired\u0027\u0027 shell model calculations produce very similar\nenergies as the CNS at all spins. The role of the pairing energy in the\ndescription of backbending and signature splitting in odd-mass nuclei is also\ndiscussed.",
    "arxiv_id": "nucl-th/0502057",
    "authors": [
      "A. Juodagalvis",
      "I. Ragnarsson",
      "S. Aberg"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.73.044327",
    "journal_ref": "Phys.Rev. C73 (2006) 044327",
    "title": "The Cranked Nilsson-Strutinsky versus the Spherical Shell Model: A   Comparative Study of pf-Shell Nuclei",
    "url": "https://arxiv.org/abs/nucl-th/0502057"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "794e71b1-434f-4529-b5d0-30c30e9c0613",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}