{
  "annotation_id": "762ecd40-d43a-4513-b34e-ae82526263e4",
  "date_created": "2026-03-02T18:02:23.667000Z",
  "date_modified": "2026-03-02T18:02:23.667000Z",
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  "record": {
    "abstract": "Bohmian mechanics and the Ghirardi-Rimini-Weber theory provide opposite\nresolutions of the quantum measurement problem: the former postulates\nadditional variables (the particle positions) besides the wave function,\nwhereas the latter implements spontaneous collapses of the wave function by a\nnonlinear and stochastic modification of Schr\\\"odinger\u0027s equation. Still, both\ntheories, when understood appropriately, share the following structure: They\nare ultimately not about wave functions but about ``matter\u0027\u0027 moving in space,\nrepresented by either particle trajectories, fields on space-time, or a\ndiscrete set of space-time points. The role of the wave function then is to\ngovern the motion of the matter.",
    "arxiv_id": "quant-ph/0603027",
    "authors": [
      "Valia Allori",
      "Sheldon Goldstein",
      "Roderich Tumulka",
      "Nino Zanghi"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1093/bjps/axn012",
    "journal_ref": "Brit.J.Phil.Sci.59:353-389,2008",
    "title": "On the Common Structure of Bohmian Mechanics and the   Ghirardi-Rimini-Weber Theory",
    "url": "https://arxiv.org/abs/quant-ph/0603027"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1e167253-650d-410b-a220-df94b7378b63",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}