{
  "annotation_id": "30cf191c-b12e-4c29-b68b-f172d7f0a82c",
  "date_created": "2026-03-02T18:01:25.354000Z",
  "date_modified": "2026-03-02T18:01:25.354000Z",
  "file_hash": "cc0aebd399166fc744ebd7cd163f3a8aa3bfb6d8beef0188d4efa8589b622860",
  "private": false,
  "record": {
    "abstract": "We examine some issues that arise in the q-deformation of a gauge theory. If\nthe deformation is carried out by replacing the equal time commutators of free\nfields by the corresponding q-commutators, the resulting propagators are not\nvery much different from those of the undeformed theory as long as one is\ndealing with weak fields; but the theory still violates causality. If one\npostulates a q-deformed S matrix, the corresponding q-causal commutator has 2\npoles of different strength and the result again amounts to a deformation of\nthe Lorentz group.",
    "arxiv_id": "q-alg/9506014",
    "authors": [
      "Robert J. Finkelstein"
    ],
    "categories": [
      "q-alg",
      "math.QA"
    ],
    "doi": "10.1142/S0217751X9600033X",
    "journal_ref": "Int.J.Mod.Phys. A11 (1996) 733-746",
    "title": "q-Gauge Theory",
    "url": "https://arxiv.org/abs/q-alg/9506014"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "fa949afa-3b79-4088-913e-72123525e383",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}