{
  "annotation_id": "128413b5-f1bf-4e62-844c-2b5347113395",
  "date_created": "2026-03-02T18:00:01.136000Z",
  "date_modified": "2026-03-02T18:00:01.136000Z",
  "file_hash": "2c8d9f3b26565bdeeaf023ccfa55265094cd4be9a98396df6697047a49474984",
  "private": false,
  "record": {
    "abstract": "The complex energies of the three-body resonances for one infinitely heavy\nparticle and two non-interacting light particles are the sum of the two\ncontributing two-body complex resonance energies. The bound state of a\nBorromean system originates from a resonance when the third interaction is\nintroduced, a finite mass is allowed and proper angular momentum coupling is\nincluded. The relative importance of these contributions are investigated and\nthe resulting structure of Borromean systems are traced back to the two-body\ncontinuum properties. The $0^+$ and $2^+$ states in $^{6}$He result from\nneutron-core p-states and the ground and first excited state of $^{11}$Li\noriginate from neutron-core $s^2$ and $sp$-states.",
    "arxiv_id": "nucl-th/0406037",
    "authors": [
      "E. Garrido",
      "D. V. Fedorov",
      "A. S. Jensen"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/j.physletb.2004.06.112",
    "journal_ref": "Phys.Lett. B600 (2004) 208-214",
    "title": "Origin of Borromean systems",
    "url": "https://arxiv.org/abs/nucl-th/0406037"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "797608b9-07a4-438f-a190-d7f81b61a58f",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}