{
  "annotation_id": "9767a129-a9be-43fd-b863-d56d3ff30ee8",
  "date_created": "2026-03-02T18:00:25.319000Z",
  "date_modified": "2026-03-02T18:00:25.319000Z",
  "file_hash": "92cb00c53967c5b3a05a7c44552f51732f8abcbb86df5a85ddea35a56f26963b",
  "private": false,
  "record": {
    "abstract": "We compare the properties of three-body systems obtained with two-body\npotentials with Pauli forbidden states and with the corresponding phase\nequivalent two-body potentials. In the first case the forbidden states are\nexplicitly excluded in the calculation. Differences arise due to the off-shell\nproperties of these on-shell equivalent potentials. We use the adiabatic\nhyperspherical method to formulate a practical prescription to exclude Pauli\nforbidden states in three-body calculations. Schematic as well as realistic\npotentials are used. Almost indistinguishable results are obtained.",
    "arxiv_id": "nucl-th/9903004",
    "authors": [
      "E. Garrido",
      "D. V. Fedorov",
      "A. S. Jensen"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0375-9474(99)00112-8",
    "journal_ref": "Nucl.Phys. A650 (1999) 247-266",
    "title": "Phase equivalent potentials for three-body halos",
    "url": "https://arxiv.org/abs/nucl-th/9903004"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "0ff277de-5de7-46d7-8e4c-b1c6d7462f37",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}