{
  "annotation_id": "4f8a2298-5cd9-49c0-90bc-de5affc0dcf5",
  "date_created": "2026-03-02T18:00:04.390000Z",
  "date_modified": "2026-03-02T18:00:04.390000Z",
  "file_hash": "4ed071626b9dcf5c5ae7533ddc175bad436504136324ffb51664b8d12d81cc7e",
  "private": false,
  "record": {
    "abstract": "The semiclassical Coulomb excitation interaction is at times expressed in the\nLorentz gauge in terms of the electromagnetic fields and a contribution from\nthe scalar electric potential. We point out that the potential term can make\nspurious contributions to excitation cross sections, especially when the the\ndecay of excited states is taken into account. We show that, through an\nappropriate gauge transformation, the excitation interaction can be expressed\nin terms of the electromagnetic fields alone.",
    "arxiv_id": "nucl-th/0509036",
    "authors": [
      "B. V. Carlson",
      "L. F. Canto",
      "M. S. Hussein"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.72.041603",
    "journal_ref": "Phys.Rev. C72 (2005) 041603",
    "title": "The Semiclassical Coulomb Interaction",
    "url": "https://arxiv.org/abs/nucl-th/0509036"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "4f42ceb7-cdc2-46ec-9908-558e51e5e5d1",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}