{
  "annotation_id": "4069ec50-b3be-47dd-a4c4-2b53812e2027",
  "date_created": "2026-03-02T18:01:41.643000Z",
  "date_modified": "2026-03-02T18:01:41.643000Z",
  "file_hash": "81a22d8ef2186bffd8d97bf0917f2586c70b4bdc5c735e5ffda8df074a5d9157",
  "private": false,
  "record": {
    "abstract": "In quantum experiments the acquisition and representation of basic\nexperimental information is governed by the multinomial probability\ndistribution. There exist unique random variables, whose standard deviation\nbecomes asymptotically invariant of physical conditions. Representing all\ninformation by means of such random variables gives the quantum mechanical\nprobability amplitude and a real alternative. For predictions, the linear\nevolution law (Schrodinger or Dirac equation) turns out to be the only way to\nextend the invariance property of the standard deviation to the predicted\nquantities. This indicates that quantum theory originates in the structure of\ngaining pure, probabilistic information, without any mechanical underpinning.",
    "arxiv_id": "quant-ph/0102099",
    "authors": [
      "Johann Summhammer"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1142/9789812810809_0025",
    "title": "Structure of Probabilistic Information and Quantum Laws",
    "url": "https://arxiv.org/abs/quant-ph/0102099"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "5a2c4c4b-71c7-4e2d-b283-0d347536c3c6",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}