{
  "annotation_id": "cf9706fc-d1e2-400f-b137-c2ddc06d7249",
  "date_created": "2026-02-17T05:53:04.940000Z",
  "date_modified": "2026-02-17T05:53:04.940000Z",
  "file_hash": "13068478c2c198449e67586339d5c053453df50fbce3d5a009b1a755324fca7c",
  "private": false,
  "record": {
    "abstract": "The relativistic momentum equation of a collisionless plasma is reformulated to describe the time evolution of canonical vorticity. Compared to the non-relativistic counterpart, an additional source term for canonical vorticity is identified, which embodies the misalignment between the fluid momentum and fluid velocity gradients. This kineclinic term breaks the frozen-in condition of canonical vorticity, thereby enabling generation or dissipation of magnetic fields and vorticity. We verify the role of this effect through particle-in-cell simulations of a modified Beltrami flow. Kineclinicity should be finite for all relativistic plasma systems due to the general lack of a functional relationship between fluid momentum and fluid velocity.",
    "arxiv_id": "2601.05718",
    "authors": [
      "Modhuchandra Laishram",
      "Suresh Basnet",
      "Young Dae Yoon"
    ],
    "categories": [
      "physics.plasm-ph"
    ],
    "license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
    "title": "Kineclinic magnetogenesis in relativistic collisionless plasmas",
    "url": "https://arxiv.org/abs/2601.05718",
    "version": "v1"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "f6f62994-e7f6-45f1-8665-5c5e4f0da937",
    "id": "arXiv Dataset",
    "type": "Model",
    "variant": "snapshot-2026-01-17",
    "version": "0.1.0"
  },
  "user_id": 1000002
}