{
  "annotation_id": "858630fe-90a3-4419-8e7a-cc38bd2b5bce",
  "date_created": "2026-03-02T18:01:21.477000Z",
  "date_modified": "2026-03-02T18:01:21.477000Z",
  "file_hash": "b66d59842c73cd213708c78a66d122d4e9962764c1dbdf3f5ae79a9e15d60388",
  "private": false,
  "record": {
    "abstract": "When time reversal is broken the viscosity tensor can have a non vanishing\nodd part. In two dimensions, and only then, such odd viscosity is compatible\nwith isotropy. Elementary and basic features of odd viscosity are examined by\nconsidering solutions of the wave and Navier-Stokes equations for hypothetical\nfluids where the stress is dominated by odd viscosity.",
    "arxiv_id": "physics/9712050",
    "authors": [
      "J. E. Avron"
    ],
    "categories": [
      "physics.flu-dyn"
    ],
    "journal_ref": "J. Stat. Phys. 92, 543-557, (1998)",
    "title": "Odd Viscosity",
    "url": "https://arxiv.org/abs/physics/9712050"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b99aa221-805b-4169-8342-1c3f789beaab",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}