{
  "annotation_id": "47831146-f2ef-4722-8091-7a191fe13655",
  "date_created": "2026-03-02T18:00:01.535000Z",
  "date_modified": "2026-03-02T18:00:01.535000Z",
  "file_hash": "f26af67824675e28fca2b889df7c098ebd96a0c7068a672296bc4575e240bc98",
  "private": false,
  "record": {
    "abstract": "The Faddeev equation for three-body scattering at arbitrary energies is\nformulated in momentum space and directly solved in terms of momentum vectors\nwithout employing a partial wave decomposition. In its simplest form the\nFaddeev equation for identical bosons is a three-dimensional integral equation\nin five variables, magnitudes of relative momenta and angles. The elastic\ndifferential cross section, semi-exclusive d(N,N\u0027) cross sections and total\ncross sections of both elastic and breakup processes in the intermediate energy\nrange up to about 1 GeV are calculated based on a Malfliet-Tjon type potential,\nand the convergence of the multiple scattering series is investigated in every\ncase. In general a truncation in the first or second order in the two-body\nt-matrix is quite insufficient.",
    "arxiv_id": "nucl-th/0409080",
    "authors": [
      "H. Liu",
      "Ch. Elster",
      "W. Gloeckle"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1063/1.1932988",
    "title": "Three-Body Scattering without Partial Waves",
    "url": "https://arxiv.org/abs/nucl-th/0409080"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "bb04b647-7e27-4d3a-a45a-443d7c269527",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}