{
  "annotation_id": "a96a07d3-95c6-41a0-9e3f-45dcc709e000",
  "date_created": "2026-03-02T18:02:06.650000Z",
  "date_modified": "2026-03-02T18:02:06.650000Z",
  "file_hash": "788618f499576fe93acfaab26228f73a2daf2801c72cca678790fe0a00323369",
  "private": false,
  "record": {
    "abstract": "Dequantization is a set of rules which turn quantum mechanics (QM) into\nclassical mechanics (CM). It is not the WKB limit of QM. In this paper we show\nthat, by extending time to a 3-dimensional \"supertime\", we can dequantize the\nsystem in the sense of turning the Feynman path integral version of QM into the\nfunctional counterpart of the Koopman-von Neumann operatorial approach to CM.\nSomehow this procedure is the inverse of geometric quantization and we present\nit in three different polarizations: the Schroedinger, the momentum and the\ncoherent states ones.",
    "arxiv_id": "quant-ph/0406028",
    "authors": [
      "A. A. Abrikosov Jr",
      "E. Gozzi",
      "D. Mauro"
    ],
    "categories": [
      "quant-ph",
      "hep-th"
    ],
    "doi": "10.1016/j.aop.2004.12.001",
    "journal_ref": "Annals Phys. 317 (2005) 24-71",
    "title": "Geometric Dequantization",
    "url": "https://arxiv.org/abs/quant-ph/0406028"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "501f7c4d-d3a9-41e1-9d13-2dcb837cd8f1",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}