{
  "annotation_id": "0a4f5c3c-5520-4ffa-a12b-bffc87d22046",
  "date_created": "2026-03-02T18:00:18.962000Z",
  "date_modified": "2026-03-02T18:00:18.962000Z",
  "file_hash": "224fe0d5899a3084689baeaa22e333c6de698fb34c80c05ad4f848c3d2102915",
  "private": false,
  "record": {
    "abstract": "We express nuclear structure functions $F_i^A$ as generalized convolutions of\nthe structure function of a nucleon and of a nucleus, composed of\npoint-nucleons. In computations of the latter we include Final State\nInteractions and results for $F_2^A$ are compared with a few directly measured\ndata on C and Fe. The above $F_i^A$ are primarily used for predictions of the\nTJNAF 89-008 inclusive scattering experiment of 4 GeV electrons on various\ntargets. Those cover a broad angular, and correspondingly wide $x,Q^2$ range,\nwhere the nucleon-inelastic part dominates large sections of the covered\nkinematics. The same model has been applied to the study of hitherto neglected\nFinal State Interaction effects in the nuclear component in EMC ratios in the\nregion $0.85\\lesssim x\\lesssim 0.25$.",
    "arxiv_id": "nucl-th/9702012",
    "authors": [
      "A. S. Rinat",
      "M. F. Taragin"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0375-9474(97)00167-X",
    "journal_ref": "Nucl.Phys. A620 (1997) 417-437; Erratum-ibid. A624 (1997) 773-775",
    "title": "Predictions for the 4 GeV TJNAF inclusive electron scattering experiment   and for FSI effects in EMC ratios",
    "url": "https://arxiv.org/abs/nucl-th/9702012"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "8d21087d-7ac8-497f-bceb-f829555ba2fb",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}