{
  "annotation_id": "a6b93856-03eb-469b-b430-b76d8286ae2e",
  "date_created": "2026-02-17T05:53:24.164000Z",
  "date_modified": "2026-02-17T05:53:24.164000Z",
  "file_hash": "f0675e8d0e94d89aa99056b5d0604b5345b0b3080225def84aca52f70d3019fe",
  "private": false,
  "record": {
    "abstract": "Topological field theories (TFTs) play an important role in characterizing the deep infrared (IR) of many quantum systems with a mass gap, as well as the global symmetries of quantum field theories (QFTs) decoupled from gravity. In gravitational asymptotically AdS spacetimes, TFT sectors which are putatively decoupled from local metric data are nevertheless non-perturbatively sensitive to Newton\u0027s constant via a sum over topologically distinct saddle point configurations. Tracking the fate of this non-decoupling in the boundary dual, we argue that in spite of appearances, this dependence on Newton\u0027s constant extends to local metric fluctuations. Said differently, TFTs are in the Swampland. In tandem with earlier results on the absence of global symmetries in theories with subregion-subregion duality, this also establishes that topological operators of boundary systems with a gravity dual are always non-topological in the bulk.",
    "arxiv_id": "2601.09781",
    "authors": [
      "Charlie Cummings",
      "Jonathan J. Heckman"
    ],
    "categories": [
      "hep-th",
      "gr-qc"
    ],
    "license": "http://creativecommons.org/licenses/by/4.0/",
    "title": "The Topological Equivalence Principle: On Decoupling TFTs from Gravity",
    "url": "https://arxiv.org/abs/2601.09781",
    "version": "v1"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "e2e061ce-af2d-4424-83ab-ffd81b188fe4",
    "id": "arXiv Dataset",
    "type": "Model",
    "variant": "snapshot-2026-01-17",
    "version": "0.1.0"
  },
  "user_id": 1000002
}