{
  "annotation_id": "0173968d-4599-4b75-8aa0-6c57d019e8c8",
  "date_created": "2026-03-02T18:00:14.496000Z",
  "date_modified": "2026-03-02T18:00:14.496000Z",
  "file_hash": "fc71ea16486e1f8f45f55f1a34cd4498bdf58ab32b73d568782219f48ee281e0",
  "private": false,
  "record": {
    "abstract": "The quark-meson coupling model, based on a mean field description of\nnon-overlapping nucleon bags bound by the self-consistent exchange of $\\sigma$,\n$\\omega$ and $\\rho$ mesons, is extended to investigate the properties of finite\nnuclei. Using the Born-Oppenheimer approximation to describe the interacting\nquark-meson system, we derive the effective equation of motion for the nucleon,\nas well as the self-consistent equations for the meson mean fields. The model\nis first applied to nuclear matter, after which we show some initial results\nfor finite nuclei.",
    "arxiv_id": "nucl-th/9509034",
    "authors": [
      "P. A. M. Guichon",
      "K. Saito",
      "E. Rodionov",
      "A. W. Thomas"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1016/0375-9474(96)00033-4",
    "journal_ref": "Nucl.Phys.A601:349-379,1996",
    "title": "The role of nucleon structure in finite nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9509034"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "a28abc28-6f93-47f2-8681-34bd9f736d35",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}