{
  "annotation_id": "2a6f63b5-352f-4b90-9cdb-163d2e9fd8d5",
  "date_created": "2026-03-02T18:01:00.408000Z",
  "date_modified": "2026-03-02T18:01:00.408000Z",
  "file_hash": "b01fbbe3d8b323af3ca279d472c74bb4f1d8b49a8edb0fca989bcfd001721401",
  "private": false,
  "record": {
    "abstract": "A rigorous and most general covariant kinetic formalism is developed to study\nthe nonlinear waves interaction in relativistic Vlasov plasmas. The typical\nnonlinear plasma reaction is a nonlinear current measured by the nonlinear\nplasma conductivity, and these quantities are derived here on the basis of\nrelativistic Vlasov-Maxwell equations. Knowing the nonlinear plasma\nconductivity allows us to determine all plasma modes nonlinearly excited in\nplasma. The general covariant form of nonlinear conductivity is provided first\nfor any value of plasma temperature and for the whole complex frequency plane\nby a correct analytical continuation. The further analysis is restricted to a\ncorrect relativistic particle distribution which is vanishing for particle\nspeeds greater than speed of light. In the limit of nonrelativistic plasma\ntemperatures the covariant nonlinear conductivity is significantly different\nfrom the standard noncovariant nonrelativistic results which are reached only\nin the formal limit of an infinitely large speed of light $c \\to \\infty$.",
    "arxiv_id": "physics/0509238",
    "authors": [
      "M. Lazar",
      "R. Schlickeiser"
    ],
    "categories": [
      "physics.plasm-ph"
    ],
    "doi": "10.1017/S0022377805004253",
    "title": "Covariant kinetic theory of nonlinear plasma waves interaction",
    "url": "https://arxiv.org/abs/physics/0509238"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "d772d0d0-1371-4edb-aaed-dac63cf51ddc",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}