{
  "annotation_id": "45c8ae25-d6e6-42fe-ac9a-6502fe27d24c",
  "date_created": "2026-03-02T18:00:15.357000Z",
  "date_modified": "2026-03-02T18:00:15.357000Z",
  "file_hash": "68271c356f918644ad721c2f720f6455a51f3e8aa5637025dd33f01511d3b492",
  "private": false,
  "record": {
    "abstract": "A Quark-Meson Coupling (QMC) model is extended to finite nuclei in the\nrelativistic mean-field or Hartree approximation. The ultra-relativistic quarks\nare assumed to be bound in non-overlapping nucleon bags, and the interaction\nbetween nucleons arises from a coupling of vector and scalar meson fields to\nthe quarks. We develop a perturbative scheme for treating the spatial\nnonuniformity of the meson fields over the volume of the nucleon as well as the\nnucleus. Results of calculations for spherical nuclei are given, based on a fit\nto the equilibrium properties of nuclear matter. Several possible extensions of\nthe model are also considered.",
    "arxiv_id": "nucl-th/9602031",
    "authors": [
      "Peter G. Blunden",
      "Gerald A. Miller"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.54.359",
    "journal_ref": "Phys.Rev.C54:359-370,1996",
    "title": "Quark-meson coupling model for finite nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9602031"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "4528fa21-74f6-4c1b-952a-1ddd7e9c96b2",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}