{
  "annotation_id": "41b8024e-bb38-4d60-9fce-bd5e9a423e00",
  "date_created": "2026-03-02T18:00:00.540000Z",
  "date_modified": "2026-03-02T18:00:00.540000Z",
  "file_hash": "699f530bc26dd771d2929323cf264429621512f50091235a4484a029a40bf1ef",
  "private": false,
  "record": {
    "abstract": "We calculate the electromagnetic form factors of a bound proton. The Chiral\nQuark-Soliton model provides the quark and antiquark substructure of the\nproton, which is embedded in nuclear matter. This procedure yields significant\nmodifications of the form factors in the nuclear environment. The sea quarks\nare almost completely unaffected, and serve to mitigate the valence quark\neffect. In particular, the ratio of the isoscalar electric to the isovector\nmagnetic form factor decreases by 20% at Q^2=1 GeV^2 at nuclear density, and we\ndo not see a strong enhancement of the magnetic moment.",
    "arxiv_id": "nucl-th/0407093",
    "authors": [
      "Jason R. Smith",
      "Gerald A. Miller"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.70.065205",
    "journal_ref": "Phys.Rev.C70:065205,2004",
    "title": "Chiral solitons in nuclei: Electromagnetic form factors",
    "url": "https://arxiv.org/abs/nucl-th/0407093"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "6a539936-4b18-4235-a06d-b8c98ec43ff0",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}