{
  "annotation_id": "152d0161-e272-430a-a87a-38f30f71941a",
  "date_created": "2026-03-02T18:01:42.686000Z",
  "date_modified": "2026-03-02T18:01:42.686000Z",
  "file_hash": "a284e8fa59400f6fccb69c081338a8742868702e15618591fa5e882cd6abe54b",
  "private": false,
  "record": {
    "abstract": "The aim of this paper is twofold: First, to present an examination of the\nprinciples underlying gauge field theories. I shall argue that there are two\nprinciples directly connected to the two well-known theorems of Emmy Noether\nconcerning global and local symmetries of the free matter-field Lagrangian, in\nthe following referred to as \"conservation principle\" and \"gauge principle\".\nSince both these express nothing but certain symmetry features of the free\nfield theory, they are not sufficient to derive a true interaction coupling to\na new gauge field. For this purpose it is necessary to advocate a third, truly\nempirical principle which may be understood as a generalization of the\nequivalence principle. The second task of the paper is to deal with the\nontological question concerning the reality status of gauge potentials in the\nlight of the proposed logical structure of gauge theories. A nonlocal\ninterpretation of topological effects in gauge theories and, thus, the\nnon-reality of gauge potentials in accordance with the generalized equivalence\nprinciple will be favoured.",
    "arxiv_id": "quant-ph/0101047",
    "authors": [
      "Holger Lyre"
    ],
    "categories": [
      "quant-ph",
      "hep-th"
    ],
    "title": "The Principles of Gauging",
    "url": "https://arxiv.org/abs/quant-ph/0101047"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "76ded43a-4765-4245-abe4-4a639bd8c6af",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}