{
  "annotation_id": "8690988a-f3f2-4afc-bc94-c7d1955aa264",
  "date_created": "2026-03-02T18:00:22.454000Z",
  "date_modified": "2026-03-02T18:00:22.454000Z",
  "file_hash": "cf86468e8219ee42bcad9b72ad36bf228b6b5b4183ab71afc7ccddad39ea3667",
  "private": false,
  "record": {
    "abstract": "The general spin structure of the relativistic nucleon wave function in the\n$3q$-model is found. It contains 16 spin components, in contrast to 8 ones\nknown previously, since in a many-body system the parity conservation does not\nreduce the number of the components. The explicitly covariant form of the wave\nfunction automatically takes into account the relativistic spin rotations,\nwithout introducing any Melosh rotation matrices. It also reduces the\ncalculations to the standard routine of the Dirac matrices and of the trace\ntechniques. In examples of the proton magnetic moment and of the axial nucleon\nform factor, with a particular wave function, we reproduce the results of the\nstandard approach. Calculations beyond the standard assumptions give different\nresults.",
    "arxiv_id": "nucl-th/9802053",
    "authors": [
      "V. A. Karmanov"
    ],
    "categories": [
      "nucl-th"
    ],
    "doi": "10.1016/S0375-9474(98)00579-X",
    "journal_ref": "Nucl.Phys. A644 (1998) 165-200",
    "title": "The nucleon wave function in light-front dynamics",
    "url": "https://arxiv.org/abs/nucl-th/9802053"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "63a7e718-a45b-4f64-80d6-00b1d8aa1bfe",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}