{
  "annotation_id": "b341684d-798a-4d36-b4a0-4997a86c1eae",
  "date_created": "2026-03-02T18:02:27.230000Z",
  "date_modified": "2026-03-02T18:02:27.230000Z",
  "file_hash": "eb0b1b1a9ae4d418a3d0e2901e9197c6e6a9abf487f2df2fefcd945071c99709",
  "private": false,
  "record": {
    "abstract": "We construct a representation of the coherent state path integral using the\nWeyl symbol of the Hamiltonian operator. This representation is very different\nfrom the usual path integral forms suggested by Klauder and Skagerstan in\n\\cite{Klau85}, which involve the normal or the antinormal ordering of the\nHamiltonian. These different representations, although equivalent quantum\nmechanically, lead to different semiclassical limits. We show that the\nsemiclassical limit of the coherent state propagator in Weyl representation is\ninvolves classical trajectories that are independent on the coherent states\nwidth. This propagator is also free from the phase corrections found in\n\\cite{Bar01} for the two Klauder forms and provides an explicit connection\nbetween the Wigner and the Husimi representations of the evolution operator.",
    "arxiv_id": "quant-ph/0607136",
    "authors": [
      "L. C. dos Santos",
      "M. A. M. de Aguiar"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1088/0305-4470/39/43/006",
    "journal_ref": "J. Phys. A: Math. Gen. 39 (2006) 13465-13482.",
    "title": "Coherent State Path Integrals in the Weyl Representation",
    "url": "https://arxiv.org/abs/quant-ph/0607136"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "874cdbd6-2164-400f-8d49-cabdeeb027b8",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}