{
  "annotation_id": "c35e6577-3a9e-467c-9f67-fe4b70939d84",
  "date_created": "2026-03-02T18:00:04.284000Z",
  "date_modified": "2026-03-02T18:00:04.284000Z",
  "file_hash": "c1c3062931c88733a01832bb965bb09f66fb6f610650c53c2abce81cd515339b",
  "private": false,
  "record": {
    "abstract": "Various sum rules for multiple giant dipole resonance states are derived. For\nthe triple giant dipole resonance states, the energy-weighted sum of the\ntransition strengths requires a model to be related to those of the single and\ndouble giant dipole resonance states. It is also shown that the non-diagonal\nmatrix elements of the double commutator between the dipole operator and the\nnuclear Hamiltonian give useful identities for the excitation energy and\ntransition strength of each excited state. Using those identities, the\nrelationship between width of the single dipole state and those of the multiple\nones is qualitatively discussed.",
    "arxiv_id": "nucl-th/0504038",
    "authors": [
      "H. Kurasawa",
      "T. Suzuki",
      "P. F. Bortignon"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1143/PTP.114.805",
    "journal_ref": "Prog.Theor.Phys. 114 (2005) 805-812",
    "title": "Sum Rules of the Multiple Giant Dipole States",
    "url": "https://arxiv.org/abs/nucl-th/0504038"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "07afa4c9-e427-4a5e-aee8-0fe31319d7bd",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}