{
  "annotation_id": "61abb240-61b7-49c9-9763-820c131700de",
  "date_created": "2026-03-02T18:01:56.061000Z",
  "date_modified": "2026-03-02T18:01:56.061000Z",
  "file_hash": "25a527b703b2fa5d323c01fabadcc9deabb30f5f19da65169a1b357a9a6fc761",
  "private": false,
  "record": {
    "abstract": "Efforts to give an improved mathematical meaning to Feynman\u0027s path integral\nformulation of quantum mechanics started soon after its introduction and\ncontinue to this day. In the present paper, one common thread of development is\nfollowed over many years, with contributions made by various authors. The\npresent version of this line of development involves a continuous-time\nregularization for a general phase space path integral and provides, in the\nauthor\u0027s opinion at least, perhaps the optimal formulation of the path\nintegral.",
    "arxiv_id": "quant-ph/0303034",
    "authors": [
      "John R. Klauder"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1142/9789812795106_0005",
    "title": "The Feynman Path Integral: An Historical Slice",
    "url": "https://arxiv.org/abs/quant-ph/0303034"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "1d293f9d-7313-4b68-83d6-02425794610e",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}