{
  "annotation_id": "d9127d4c-6ffa-4e35-8d79-14264ebd44a0",
  "date_created": "2026-03-02T18:00:18.480000Z",
  "date_modified": "2026-03-02T18:00:18.480000Z",
  "file_hash": "b430c912431c1ba705ca1bc98b4030beb80825b33e09e05daa4b41353e68ec73",
  "private": false,
  "record": {
    "abstract": "Using the simple relation between the np scattering and bound state wave\nfunctions, the spin-triplet contributions to the pp -\u003e pi+ (pn) and backward dp\n-\u003e p(pn) reactions are estimated for low np excitation energies. The good\nagreement with the pion production data at 400 and 450 MeV over a range of\nangles shows that spin-singlet final states cannot be more than of the order of\n10%. On the other hand it is seen that the spin-singlet states must provide\nabout 30% of the strength in pion production at 1 GeV as well as\ndeuteron-proton backward scattering at 1.6 GeV.",
    "arxiv_id": "nucl-th/9609032",
    "authors": [
      "A. Boudard",
      "G. Faeldt",
      "C. Wilkin"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0370-2693(96)01325-1",
    "journal_ref": "Phys.Lett. B389 (1996) 440-444",
    "title": "Triplet np Final State Interactions at Large Momentum Transfers",
    "url": "https://arxiv.org/abs/nucl-th/9609032"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "52859ed5-3b0b-4969-9214-70d09fa63214",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}