{
  "annotation_id": "693d4ece-cedf-4b7d-8ae8-94382722f5d5",
  "date_created": "2026-03-02T18:01:45.506000Z",
  "date_modified": "2026-03-02T18:01:45.506000Z",
  "file_hash": "54f1e5516b9eb5606e679621c398b173590d6efa1fb8e0f8ef9ce625bc7f95ea",
  "private": false,
  "record": {
    "abstract": "Starting from a general relativistic kinetic equation, a self-consistent\nmean-field equation for fermions is derived within a covariant density matrix\napproach of QED plasmas in strong external fields. A Schr\\\"odinger picture\nformulation on space-like hyperplanes is applied. The evolution of the\ndistribution function is described by the one-particle gauge-invariant 4x4\nWigner matrix, which is decomposed in spinor space. A coupled system of\nequations for the corresponding Wigner components is obtained. The polarization\ncurrent is expressed in terms of the Wigner function. Charge conservation is\nobeyed. In the quasi-classical limit for the Wigner components a relativistic\nVlasov equation is obtained, which is presented in an invariant, i.e.\nhyperplane independent, form.",
    "arxiv_id": "quant-ph/0106004",
    "authors": [
      "A. Hoell",
      "V. Morozov",
      "G. Roepke"
    ],
    "categories": [
      "quant-ph",
      "hep-th",
      "physics.plasm-ph"
    ],
    "journal_ref": "Theor.Math.Phys. 132 (2002) 1029-1042; Teor.Mat.Fiz. 132 (2002)\n  161-174",
    "title": "Kinetic theory of QED plasmas in a strong electromagnetic field. II. The   mean-field description",
    "url": "https://arxiv.org/abs/quant-ph/0106004"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "f858f2af-b6fe-4f70-a109-2f5d8127cb43",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}