{
  "annotation_id": "2f2d27ea-248f-4fe7-a2db-7404995d8b8b",
  "date_created": "2026-03-02T18:00:11.602000Z",
  "date_modified": "2026-03-02T18:00:11.602000Z",
  "file_hash": "ba4bc1deac6c7f498105b9bb8ee973d143c2dae0a31694c2c5eb2e7c125c4c11",
  "private": false,
  "record": {
    "abstract": "The potentials $V (v)$ in the nonrelativistic (relativistic) nucleon-nucleon\n(NN) Schroedingerequation are related by a quadratic equation. That equation is\nnumerically solved, thus providing phase equivalent v- potentials related for\ninstance to the high precision NN potentials, which are adjusted to NN phase\nshift and mixing parameters in a nonrelativistic Schroedinger equation. The\nrelativistic NN potentials embedded in a three-nucleon (3N)system for total NN\nmomenta different from zero are also constructed in a numerically precise\nmanner. They enter into the relativistic interacting 3N mass operator, which is\nneeded for relativistic 3N calculations for bound and scattering states.",
    "arxiv_id": "nucl-th/0703010",
    "authors": [
      "H. Kamada",
      "W. Gloeckle"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/j.physletb.2007.07.071",
    "journal_ref": "Phys.Lett.B655:119-125,2007",
    "title": "Realistic two-nucleon potentials for the relativistic two-nucleon   Schroedinger equation",
    "url": "https://arxiv.org/abs/nucl-th/0703010"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "f92edc5d-409c-4527-9d08-ada6f9e71bf3",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}