{
  "annotation_id": "562f4287-7a50-404f-97a6-f8109f1dcae0",
  "date_created": "2026-03-02T18:00:18.663000Z",
  "date_modified": "2026-03-02T18:00:18.663000Z",
  "file_hash": "d196257360c3b0c3a6895d3c511106d5fc2fc4bec98886858b3d90668983ddf9",
  "private": false,
  "record": {
    "abstract": "Momentum distributions of particles from nuclear break-up of fast three-body\nhalos are calculated incorporating effects of final state interactions. The\nsame two-body interactions between the particles are used to calculate both the\nground state structure and the final state of the reaction processes. The\nground state wave function reproduces size and energy of the halo nucleus.\nFirst we give a general and detailed description of the method. Then we\ninvestigate the effect of final state interactions in neutron removal and core\nbreak-up reactions for one- and two-dimensional momentum distributions. We\ncompute specifically core and neutron momentum distributions from 11Li\nfragmentation and compare those with available experimental data. We conclude\nthat 11Li must have a neutron-core relative state containing a p-state\nadmixture of 20\\%-30\\%. The fragmentation data also strongly suggest that 10Li\nhas an s-state at about 50 keV and a p-state around 500 keV.",
    "arxiv_id": "nucl-th/9608032",
    "authors": [
      "E. Garrido",
      "D. V. Fedorov",
      "A. S. Jensen"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1103/PhysRevC.55.1327",
    "journal_ref": "Phys.Rev.C55:1327-1343,1997",
    "title": "Three-body Halos. IV. Momentum Distributions after Fragmentation",
    "url": "https://arxiv.org/abs/nucl-th/9608032"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "c52f3a87-9272-4b7d-8093-ec00fbcb1a9d",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}