{
  "annotation_id": "9980c5f8-b6be-4d7f-90d0-f0e4935d6d74",
  "date_created": "2026-03-02T18:02:17.142000Z",
  "date_modified": "2026-03-02T18:02:17.142000Z",
  "file_hash": "2909d719af12ad9ad25467855b3392e3eb80674178e2c4d984f053a4f57f60ba",
  "private": false,
  "record": {
    "abstract": "Diracs hole theory (HT) and quantum field theory (QFT) are generally\nconsidered to be equivalent to each other. However, it has been recently shown\nby several researchers that this is not necessarily the case. When the change\nin the vacuum energy was calculated for a time independent perturbation HT and\nQFT yielded different results. In this paper we extend this discussion to\ninclude a time dependent perturbation for which the exact solution to the Dirac\nequation is known. It will be shown that for this case, also, HT and QFT yield\ndifferent results. In addition, there will be some discussion of the problem of\nanomalies in QFT.",
    "arxiv_id": "quant-ph/0506271",
    "authors": [
      "Dan Solomon"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1139/p04-086",
    "journal_ref": "Can. J. Phys. 83: 257-271 (2005)",
    "title": "Some differences between Dirac\u0027s hole theory and quantum field theory",
    "url": "https://arxiv.org/abs/quant-ph/0506271"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "e7d8c81b-911a-4e38-9e95-48038378040f",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}