{
  "annotation_id": "661f6475-0fe8-4faa-b7c3-69f96cbb74b1",
  "date_created": "2026-03-02T18:02:37.782000Z",
  "date_modified": "2026-03-02T18:02:37.782000Z",
  "file_hash": "7ee6dc794b28b77c2cbd1732eccf86cc92d1a8e36491c68ececc16838b90f52b",
  "private": false,
  "record": {
    "abstract": "An ordinary unambiguous integral representation for the finite propagator of\na quantum system is found by starting of a privileged skeletonization of the\nfunctional action in phase space, provided by the complete solution of the\nHamilton-Jacobi equation. This representation allows to regard the propagator\nas the sum of the contributions coming from paths where the momenta generated\nby the complete solution of the Hamilton-Jacobi equation are conserved -as it\ndoes happen on the classical trajectory-, but are not restricted to having the\nclassical values associated with the boundary conditions for the original\ncoordinates.",
    "arxiv_id": "quant-ph/9607013",
    "authors": [
      "Rafael Ferraro"
    ],
    "categories": [
      "quant-ph",
      "gr-qc",
      "hep-th"
    ],
    "title": "The complete solution of the Hamilton-Jacobi equation in Quantum   Mechanics",
    "url": "https://arxiv.org/abs/quant-ph/9607013"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "14535ef3-2ccf-44c4-a6da-7f858062f2ff",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}