{
  "annotation_id": "e375ec65-3d2b-45cd-8d6e-6583b283981e",
  "date_created": "2026-03-02T18:00:11.084000Z",
  "date_modified": "2026-03-02T18:00:11.084000Z",
  "file_hash": "c2a257ef7c60928314dbf16a64fa044f7399df4a5aa755e1485e4a635439d470",
  "private": false,
  "record": {
    "abstract": "I calculate the dispersion relation for quarks of mass $m$ and momentum $k$\nin a quark gluon plasma at temperature $T$, in the limit $m^2+k^2 \\gg (gT)^2$,\nwhere $g$ is the strong coupling constant. I find three contributions to the\ndispersion relation: one that depends on $T$ but not $m$ or $k$, one that\ndepends on $m$ and $T$ but not $k$, and third contribution that depends on all\nthree (and is opposite in sign to the other two).",
    "arxiv_id": "nucl-th/9310008",
    "authors": [
      "David Seibert"
    ],
    "categories": [
      "nucl-th",
      "hep-ph"
    ],
    "title": "The high-frequency finite-temperature quark dispersion relation",
    "url": "https://arxiv.org/abs/nucl-th/9310008"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ebddf91e-4dd7-4755-afbd-4827e8bff9f2",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}