{
  "annotation_id": "52f11463-359e-4a98-8300-751e494a090f",
  "date_created": "2026-03-02T18:02:37.578000Z",
  "date_modified": "2026-03-02T18:02:37.578000Z",
  "file_hash": "c167def691aca77b63cc066339ba7875d709b6149e32d535432a22ddaf4d68ba",
  "private": false,
  "record": {
    "abstract": "In order to arrive at Bohmian mechanics from standard nonrelativistic quantum\nmechanics one need do almost nothing! One need only complete the usual quantum\ndescription in what is really the most obvious way: by simply including the\npositions of the particles of a quantum system as part of the state description\nof that system, allowing these positions to evolve in the most natural way. The\nentire quantum formalism, including the uncertainty principle and quantum\nrandomness, emerges from an analysis of this evolution. This can be expressed\nsuccinctly---though in fact not succinctly enough---by declaring that the\nessential innovation of Bohmian mechanics is the insight that {\\it particles\nmove }!",
    "arxiv_id": "quant-ph/9511016",
    "authors": [
      "D. D\u00fcrr",
      "S. Goldstein",
      "N. Zanghi"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "Bohmian Mechanics as the Foundation of Quantum Mechanics",
    "url": "https://arxiv.org/abs/quant-ph/9511016"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "424767f6-06aa-493a-b0cb-99b95295366d",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}