{
  "annotation_id": "5d9e95db-b7ed-4891-abac-0c300a284f53",
  "date_created": "2026-03-02T18:00:01.599000Z",
  "date_modified": "2026-03-02T18:00:01.599000Z",
  "file_hash": "fa6de7af1f369ef4e0ff296c39e329e635515ef62e1e601ecbc279c7f8d777af",
  "private": false,
  "record": {
    "abstract": "Full Coupled Channels Calculations were performed for the $^{16}O(d,n)^{17}F$\nand $^{16}O(d,p)^{17}O$ transfer reactions at several deuteron incident\nenergies from $E_{lab}=2.29$ MeV up to 3.27 MeV. A strong polarization effect\nbetween the entrance channel and the transfer channels\n$^{16}O(d,n)^{17}F(1/2^{+},0.495)$ and $^{16}O(d,p)^{17}O(1/2^{+},0.87)$ was\nobserved. This polarization effect had to be taken into account in order to\nobtain realistic spectroscopic factors from these reactions.",
    "arxiv_id": "nucl-th/0409004",
    "authors": [
      "M. Assuncao",
      "R. Lichtenthaler",
      "V. Guimaraes",
      "A. Lepine-Szily",
      "G. F. Lima",
      "A. M. Moro"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.70.054601",
    "journal_ref": "Phys.Rev. C70 (2004) 054601",
    "title": "Higher order effects in the $^{16}O(d,p)^{17}O$ and $^{16}O(d,n)^{17}F$   transfer reactions",
    "url": "https://arxiv.org/abs/nucl-th/0409004"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "eab04dc4-3acd-4e63-9bab-971d9186560c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}