{
  "annotation_id": "2028db9b-bb2a-4c2d-8237-7d3d88842133",
  "date_created": "2026-03-02T18:00:25.877000Z",
  "date_modified": "2026-03-02T18:00:25.877000Z",
  "file_hash": "3bcfa11bcfea352a6bc1bc04541cd04ddd93ec1fcdd778a7ec1272890c1c52f1",
  "private": false,
  "record": {
    "abstract": "We address the problem of extracting single-nucleon momentum distributions\n$n(p)$ from inclusice scattering data. A model for these relates nuclear and\nnucleon structure functions (SF) through an intermediate SF $f^{PN}$ for a\nnucleus of point-particles. In addition to the asymptotic limit (AL) which\ndepends on $n(p), f^{PN}$ contains, generally $q$-dependent Final State\nInteractions (FSI) parts. In the inverse problem one wishes to separate\n$q$-dependent FSI from the AL. In general it suffices to know the structure of\nthe theory, but not numerical results. It appears, that in the $q$-range of the\nanalyzed electron scattering data, FSI are only weakly $q$-dependent, making it\nvirtually impossible to obtain parameters in a free fit of the parametrized\ncomponents of $f$. Imposing a restriction, we obtain $n(p)$ for Fe and $^4$Fe.",
    "arxiv_id": "nucl-th/9904027",
    "authors": [
      "A. S. Rinat",
      "M. F. Taragins"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0370-2693(99)00669-3",
    "journal_ref": "Phys.Lett. B459 (1999) 431-436",
    "title": "Extraction of nucleon momentum distributions from inclusive electron   scattering on nuclei",
    "url": "https://arxiv.org/abs/nucl-th/9904027"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "10a8e79d-acb4-4420-bc14-c4e26b4c5072",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}