{
  "annotation_id": "603c59b1-fe96-41a5-bac4-8dd6aca24bd7",
  "date_created": "2026-03-02T18:02:37.425000Z",
  "date_modified": "2026-03-02T18:02:37.425000Z",
  "file_hash": "fc4f7e84f05cbcbcfbb63a78010ffb858f75d351b4f10e4d546dcce26aa05cf6",
  "private": false,
  "record": {
    "abstract": "The Lindblad master equation for an open quantum system with a Hamiltonian\ncontaining an arbitrary potential is written as an equation for the Wigner\ndistribution function in the phase space representation. The time derivative of\nthis function is given by a sum of three parts: the classical one, the quantum\ncorrections and the contribution due to the opening of the system. In the\nparticular case of a harmonic oscillator, quantum corrections do not exist.",
    "arxiv_id": "quant-ph/9605041",
    "authors": [
      "A. Isar",
      "A. Sandulescu",
      "W. Scheid"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1142/S0217979296001240",
    "journal_ref": "Int.J.Mod.Phys.B10:2767,1996",
    "title": "Phase Space Representation for Open Quantum Systems within the Lindblad   Theory",
    "url": "https://arxiv.org/abs/quant-ph/9605041"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "6fcea778-db8d-4c11-b8f8-c4a9c05a361f",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}