{
  "annotation_id": "09291baa-fc43-4078-8949-d2518b62458f",
  "date_created": "2026-03-02T18:00:00.891000Z",
  "date_modified": "2026-03-02T18:00:00.891000Z",
  "file_hash": "58abaffc66c83c1c56e75c9da8e55266be5185e7e76271a8693a1f360c536a7a",
  "private": false,
  "record": {
    "abstract": "The generalized Gerasimov-Drell-Hearn sum rule $I^{GDH}_{\\gamma^*d}(Q^2)$ for\ndeuteron electrodisintegration $d(e,e\u0027)np$ as function of the squared\nfour-momentum transfer $Q^2$ is evaluated by explicit integration. The\ncalculation is based on a conventional nonrelativistic framework using a\nrealistic $NN$-potential and including contributions from meson exchange\ncurrents, isobar configurations and leading order relativistic terms. Good\nconvergence is achieved. The prominent feature is a deep negative minimum,\n$I_{\\gamma^* d}^{GDH}=-9.5$ mb, at low $Q^2\\approx 0.2$ fm$^{-2}$ which is\nalmost exclusively driven by the nucleon isovector anomalous magnetic moment\ncontribution to the magnetic dipole transition to the $^1S_0$-state. Above\n$Q^2=20$ fm$^{-2}$ the integral $I^{GDH}_{\\gamma^*}(Q^2)$ approaches zero\nrapidly.",
    "arxiv_id": "nucl-th/0404044",
    "authors": [
      "Hartmuth Arenhoevel"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/j.physletb.2004.05.055",
    "journal_ref": "Phys.Lett. B595 (2004) 223-230",
    "title": "The generalized Gerasimov-Drell-Hearn sum rule for deuteron   electrodisintegration",
    "url": "https://arxiv.org/abs/nucl-th/0404044"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "6104232b-0f44-4737-bdb7-ec3342148e05",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}