{
  "annotation_id": "1634a857-6675-4304-afae-1b03ca77d0ad",
  "date_created": "2026-03-02T18:00:01.605000Z",
  "date_modified": "2026-03-02T18:00:01.605000Z",
  "file_hash": "d348e69cc04dacbbb981b597491ac15e98afaa848ac14f049a6453f872e0ee0c",
  "private": false,
  "record": {
    "abstract": "We use the hyperspherical adiabatic expansion method to discuss the the two\nmechanisms of sequential and direct three-body decay. Both short-range and\nCoulomb interactions are included. Resonances are assumed initially populated\nby a process independent of the subsequent decay. The lowest adiabatic\npotentials describe the resonances rather accurately at distances smaller than\nthe outer turning point of the confining barrier. We illustrate with realistic\nexamples of nuclei from neutron ($^{6}$He) and proton ($^{17}$Ne) driplines as\nwell as excited states of beta-stable nuclei ($^{12}$C).",
    "arxiv_id": "nucl-th/0411079",
    "authors": [
      "E. Garrido",
      "D. V. Fedorov",
      "A. S. Jensen",
      "H. O. U. Fynbo"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/j.nuclphysa.2004.11.008",
    "journal_ref": "Nucl.Phys. A748 (2005) 39-58",
    "title": "Anatomy of three-body decay II. Decay mechanism and resonance structure",
    "url": "https://arxiv.org/abs/nucl-th/0411079"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "a36f4d47-6480-4da1-8d8d-dea07f0ff6a8",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}