{
  "annotation_id": "76d930af-36fd-42e9-97b2-0561478185e1",
  "date_created": "2026-03-02T18:00:25.775000Z",
  "date_modified": "2026-03-02T18:00:25.775000Z",
  "file_hash": "554ac7bbc0476f692df17d541045d386970e5a56cc95ab910b8f0c54dd3239a1",
  "private": false,
  "record": {
    "abstract": "We calculate the spin-polarizabilities of the nucleon by means of dispersion\nrelation, where the pion photoproduction amplitude predicted by chiral soliton\nmodel is utilized. We consider the $N\\pi$ and $\\Delta\\pi$ channels in the\npion-photoproduction amplitude, and also evaluate the contribution of the\nanomalous term of the $\\pi^0\\gamma\\gamma$ process. In a narrow decay-width\nlimit of the $\\Delta$ particle the result coincides with that in heavy baryon\nchiral perturbation theory (HBChPT) except for the interference part of the\nelectric and magnetic amplitudes. A comparison with the multipole analysis is\ngiven.",
    "arxiv_id": "nucl-th/9901010",
    "authors": [
      "Y. Tanushi",
      "S. Saito",
      "M. Uehara"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "doi": "10.1103/PhysRevC.60.065213",
    "title": "Spin-Polarizabilities of the Nucleon in Chiral Soliton Model with   Dispersion Relation",
    "url": "https://arxiv.org/abs/nucl-th/9901010"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "16544cf9-4e13-4fb0-a66a-3727587580a3",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}