{
  "annotation_id": "86933358-d333-419a-8a49-b86308489500",
  "date_created": "2026-03-02T18:00:04.619000Z",
  "date_modified": "2026-03-02T18:00:04.619000Z",
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  "record": {
    "abstract": "Mean field methods to calculate the nuclear mass are extended into the high\nspin regime to calculate the nuclear binding energy as a function of proton\nnumber, neutron number and angular momentum. Comparing the trend as a function\nof mass number for a selection of high-spin states, a similar agreement between\ntheory and experiment is obtained as for ground state masses.",
    "arxiv_id": "nucl-th/0503080",
    "authors": [
      "B. G. Carlsson",
      "I. Ragnarsson"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1088/0031-8949/2006/T125/030",
    "journal_ref": "Phys.Scripta T125 (2006) 130-133",
    "title": "Calculating the nuclear mass at finite angular momenta",
    "url": "https://arxiv.org/abs/nucl-th/0503080"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ca09d4ec-e36d-4c60-b26a-e582407a8882",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}