{
  "annotation_id": "1a838892-6621-4a70-bebf-7574bc6905e7",
  "date_created": "2026-03-02T18:00:15.529000Z",
  "date_modified": "2026-03-02T18:00:15.529000Z",
  "file_hash": "202018ebae8d8072366c5aede2a1d23d86d9b526981dc5187ed71f9df1841a3c",
  "private": false,
  "record": {
    "abstract": "We extend the formulation of relativistic Coulomb sum rules to account for\nthe average effects of nuclear binding on the initial and final states of\nejected nucleons. Relativistic interactions are included by using a Dirac\nrepresentation adapted from a vector-scalar field theory. The scalar field\nreduces the effective nucleon mass $M^*$ and increases the relativistic effects\nof recoil and Fermi motion. We consider two models for the off-shell behavior\nof the nuclear electromagnetic current, and demonstrate that the sum rule is\naccurate for applications to data over the interesting range of $M^*$ and three\nmomentum $q$. We further indicate that the form of the sum rule is sufficiently\ngeneral to accommodate a broad class of off-shell form factor models.",
    "arxiv_id": "nucl-th/9412030",
    "authors": [
      "D. S. Koltun",
      "T. C. Ferree"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.52.901",
    "journal_ref": "Phys.Rev.C52:901-914,1995",
    "title": "Nuclear Binding Effects in Relativistic Coulomb Sum Rules",
    "url": "https://arxiv.org/abs/nucl-th/9412030"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c0acc8e1-0a0e-4e62-a2ba-6fbe3cbefecc",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}