{
  "annotation_id": "ab788f6b-7645-4c0e-80a0-5794d7206a14",
  "date_created": "2026-03-02T18:02:13.748000Z",
  "date_modified": "2026-03-02T18:02:13.748000Z",
  "file_hash": "219b9fac58ff0e56c42ab94b5369a9e114e40d47d571b54a5ec24324fcb98e83",
  "private": false,
  "record": {
    "abstract": "Both Bohmian mechanics, a version of quantum mechanics with trajectories, and\nFeynman\u0027s path integral formalism have something to do with particle paths in\nspace and time. The question thus arises how the two ideas relate to each\nother. In short, the answer is, path integrals provide a re-formulation of\nSchroedinger\u0027s equation, which is half of the defining equations of Bohmian\nmechanics. I try to give a clear and concise description of the various aspects\nof the situation.",
    "arxiv_id": "quant-ph/0501167",
    "authors": [
      "Roderich Tumulka"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1088/0143-0807/26/3/L01",
    "journal_ref": "Eur. J. Phys. 26 (2005) L11-L13",
    "title": "Feynman\u0027s Path Integrals and Bohm\u0027s Particle Paths",
    "url": "https://arxiv.org/abs/quant-ph/0501167"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "8bef7fa5-4914-4a02-899a-85d37c3e094a",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}