{
  "annotation_id": "9cdbfbe1-e25b-4ca4-be87-e49df1e6b448",
  "date_created": "2026-03-02T18:02:37.835000Z",
  "date_modified": "2026-03-02T18:02:37.835000Z",
  "file_hash": "0158abe8e8ffc11f7cff024fcd7bfbc64337dc2da19260498923a9a14095eb2d",
  "private": false,
  "record": {
    "abstract": "In the extension of the de-Broglie-Bohm causal quantum theory of motion to\nthe relativistic particles, one faces with serious problems, like the problem\nof superluminal motion. This forces many authors to believe that there is not\nany satisfactory causal theory for particles of integer spin. In this paper, it\nis shown that the quantal behaviour is the result of\ndirect-particle-interaction of the particle with all of its possibilities. The\nformulation is, then, extended to the relativistic particles of arbitrary spin.\nThe presented theory has the following advantages. (1) It leads to a deeper\nunderstanding of the quantal behaviour. (2) It has no superluminal motion. (3)\nIt is applicable to any spin. (4) It provides a framework for understanding the\nproblem of creation and annihilation of particles. (5) It provides a framework\nfor understanding the spin-statistics relationship. (6) It does not need the\ntwo fundamental assumptions of the de-Broglie-Bohm quantum theory of motion,\ni.e., the guiding-formula postulate and the statistical postulate.",
    "arxiv_id": "quant-ph/9612023",
    "authors": [
      "Ali Shojai",
      "Mehdi Golshani"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "On the Relativistic Quantum Force",
    "url": "https://arxiv.org/abs/quant-ph/9612023"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ec081d14-6d79-4344-a318-99ae3c915a35",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}