{
  "annotation_id": "2bb9e418-1a88-412d-8c3a-db627683d5bf",
  "date_created": "2026-03-02T18:02:38.177000Z",
  "date_modified": "2026-03-02T18:02:38.177000Z",
  "file_hash": "4556a50b3ac21fbd1eb53498185b0a3ac364f8694aa2b40186ae2848ac44b1ee",
  "private": false,
  "record": {
    "abstract": "We discuss the problem of finding a Lorentz invariant extension of Bohmian\nmechanics. Due to the nonlocality of the theory there is (for systems of more\nthan one particle) no obvious way to achieve such an extension. We present a\nmodel invariant under a certain limit of Lorentz transformations, a limit\nretaining the characteristic feature of relativity, the non-existence of\nabsolute time resp. simultaneity. The analysis of this model exemplifies an\nimportant property of any Bohmian quantum theory: the quantum equilibrium\ndistribution $\\rho = |\\psi |^2$ cannot simultaneously be realized in all\nLorentz frames of reference.",
    "arxiv_id": "quant-ph/9510027",
    "authors": [
      "K. Berndl",
      "D. Duerr",
      "S. Goldstein",
      "N. Zanghi"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevA.53.2062",
    "journal_ref": "Phys.Rev.A53:2062-2073,1996",
    "title": "EPR-Bell Nonlocality, Lorentz Invariance, and Bohmian Quantum Theory",
    "url": "https://arxiv.org/abs/quant-ph/9510027"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ddb46147-86f0-4103-b66b-a73b2ca9d7c9",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}