{
  "annotation_id": "599d4f57-7792-4fd0-8c2b-e1cc504f186f",
  "date_created": "2026-03-02T18:00:00.944000Z",
  "date_modified": "2026-03-02T18:00:00.944000Z",
  "file_hash": "700900e5bc3d17f3f4231936b4a1a847e4d459da5b109a2880618e775d18af2a",
  "private": false,
  "record": {
    "abstract": "Using two approaches: dispersion relations and isobar model, we have analyzed\nrecent high precision CLAS data on cross sections of \\pi^0, \\pi^+, and \\eta\nelectroproduction on protons, and the longitudinally polarized electron beam\nasymmetry for p(\\vec{e},e\u0027p)\\pi^0 and p(\\vec{e},e\u0027n)\\pi^+. The contributions of\nthe resonances P33(1232), P11(1440), D13(1520), S11(1535) to \\pi\nelectroproduction and S11(1535) to \\eta electroproduction are found. The\nresults obtained in the two approaches are in good agreement with each other.\nThere is also good agreement between amplitudes of the \\gamma^* N \\to S11(1535)\ntransition found in \\pi and \\eta electroproduction. For the first time accurate\nresults are obtained for the longitudinal amplitudes of the P11(1440),\nD13(1520) and S11(1535) electroexcitation on protons.",
    "arxiv_id": "nucl-th/0407021",
    "authors": [
      "I. G. Aznauryan",
      "V. D. Burkert",
      "H. Egiyan",
      "K. Joo",
      "R. Minehart",
      "L. C. Smith"
    ],
    "categories": [
      "nucl-th",
      "hep-ph",
      "nucl-ex"
    ],
    "doi": "10.1103/PhysRevC.71.015201",
    "journal_ref": "Phys.Rev.C71:015201,2005",
    "title": "Electroexcitation of the P33(1232), P11(1440), D13(1520), S11(1535) at   Q^2=0.4 and 0.65(GeV/c)^2",
    "url": "https://arxiv.org/abs/nucl-th/0407021"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c75ebaf2-84ba-4927-8ab3-d21fe6d9a452",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}