{
  "annotation_id": "4fff693a-2ce3-4a9a-afec-66494ea0fb0f",
  "date_created": "2026-03-02T18:00:11.541000Z",
  "date_modified": "2026-03-02T18:00:11.541000Z",
  "file_hash": "0c2ed15a2bd5d8706c721484edd317d0dd3bc1f5a9324c2517ec729c04ac7d45",
  "private": false,
  "record": {
    "abstract": "We apply a three-body model consisting of two valence neutrons and the core\nnucleus $^{14}$C in order to investigate the ground state properties and the\nelectronic quadrupole transition of the $^{16}$C nucleus. The discretized\ncontinuum spectrum within a large box is taken into account by using a\nsingle-particle basis obtained from a Woods-Saxon potential. The calculated\nB(E2) value from the first 2$^+$ state to the ground state shows good agreement\nwith the observed data with the core polarization charge which reproduces the\nexperimental B(E2) value for $^{15}$C. We also show that the present\ncalculation well accounts for the longitudinal momentum distribution of\n$^{15}$C fragment from the breakup of $^{16}$C nucleus. We point out that the\ndominant ($d_{5/2})^2$ configuration in the ground state of $^{16}$C plays a\ncrucial role for these agreement.",
    "arxiv_id": "nucl-th/0612040",
    "authors": [
      "K. Hagino",
      "H. Sagawa"
    ],
    "categories": [
      "nucl-th",
      "nucl-ex"
    ],
    "doi": "10.1103/PhysRevC.75.021301",
    "journal_ref": "Phys.Rev. C75 (2007) 021301",
    "title": "Three-body model calculations for 16C nucleus",
    "url": "https://arxiv.org/abs/nucl-th/0612040"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "664f7ddc-1cee-4654-93e3-da9b4e36026f",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}