{
  "annotation_id": "19d88489-04c7-41fc-be2c-4ce55b2baa74",
  "date_created": "2026-03-02T18:00:22.447000Z",
  "date_modified": "2026-03-02T18:00:22.447000Z",
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  "record": {
    "abstract": "The relativistic mean-field theory provides a framework in which the nuclear\nmany-body problem is described as a self-consistent system of nucleons and\nmesons. In the mean-field approximation, the self-consistent time evolution of\nthe nuclear system describes the dynamics of collective motion: nuclear\ncompressibility from monopole resonances, regular and chaotic dynamics of\nisoscalar and isovector collective vibrations.",
    "arxiv_id": "nucl-th/9809036",
    "authors": [
      "D. Vretenar",
      "P. Ring",
      "G. A. Lalazissis",
      "N. Paar"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0375-9474(99)00035-4",
    "journal_ref": "Nucl.Phys. A649 (1999) 29-36",
    "title": "Relativistic mean-field description of the dynamics of giant resonances",
    "url": "https://arxiv.org/abs/nucl-th/9809036"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "bb63f53e-ac47-4859-8922-e00ff93a4195",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}