{
  "annotation_id": "9d1a8e3f-d068-4167-b8d4-8ae5162f1f1d",
  "date_created": "2026-03-02T18:00:22.197000Z",
  "date_modified": "2026-03-02T18:00:22.197000Z",
  "file_hash": "83ce8eefc6bbca50006d7d5e53da801ae8bcbfede634c708d3ebfee98707faf2",
  "private": false,
  "record": {
    "abstract": "Relativistic Mean Field Theory is applied to the description of rotating\nnuclei. Since the previous formulation of Munich group was based on a special\nrelativistic transformation property of the spinor fields, we reformulate in a\nfully covariant manner using tetrad formalism. The numerical calculations are\nperformed for 3 zinc isotopes, including the newly discovered superdeformed\nband in $^{62}$Zn which is the first experimental observation in this mass\nregion.",
    "arxiv_id": "nucl-th/9712063",
    "authors": [
      "Hideki Madokoro",
      "Masayuki Matsuzaki"
    ],
    "categories": [
      "nucl-th"
    ],
    "title": "Relativistic Mean Field Description of Nuclear Collective Rotation -The   Superdeformed Rotational Bands in the A$\\sim$60 Mass Region-",
    "url": "https://arxiv.org/abs/nucl-th/9712063"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "6ef6e1fb-d41a-4704-a47d-6beac38ab974",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}