{
  "annotation_id": "13510729-08ff-46ad-bc18-894c4dfdd183",
  "date_created": "2026-03-02T18:00:28.036000Z",
  "date_modified": "2026-03-02T18:00:28.036000Z",
  "file_hash": "4b9e7295d7b6d8c7e9a30564bdf010178b0743d6345b5975623cdf10f19ab7fa",
  "private": false,
  "record": {
    "abstract": "Rotational behavior inducing triaxiality is discussed for 48Cr in the cranked\nNilsson-Strutinsky (CNS) model, as well as in the spherical shell model. It is\nshown that the low-spin region up to about I=8, has a prolate well-deformed\nshape. At higher spins the shape is triaxial with a \"negative-gamma\"\ndeformation, that is, with rotation around the classically forbidden\nintermediate axis. By comparing calculated B(E2)-values and spectroscopic\nquadrupole moments in the CNS with spherical shell model results and\nexperimental data, the triaxial rotation around the intermediate axis is\nconfirmed.",
    "arxiv_id": "nucl-th/9909079",
    "authors": [
      "A. Juodagalvis",
      "I. Ragnarsson",
      "S. Aberg"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0370-2693(00)00214-8",
    "journal_ref": "Phys.Lett. B477 (2000) 66-72",
    "title": "Triaxiality in 48Cr",
    "url": "https://arxiv.org/abs/nucl-th/9909079"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "cc1eadd7-6886-467e-802d-c9a7185b7703",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}