{
  "annotation_id": "ac373eb2-b6ed-4d91-9ff5-1911ae216a3b",
  "date_created": "2026-03-02T18:02:03.486000Z",
  "date_modified": "2026-03-02T18:02:03.486000Z",
  "file_hash": "cd561dea051e73153cb1f328dd988883735aef666356b30ee6d5df632c27a1cb",
  "private": false,
  "record": {
    "abstract": "Dirac\u0027s hole theory (HT) and quantum field theory (QFT) are generally\nconsidered to be equivalent to each other. However, it has been recently shown\nthat for a time independent perturbation different results are obtained when\nthe change in the vacuum energy is calculated. Here we shall extend this\ndiscussion to include a time dependent perturbation. It will be shown that HT\nand QFT yield different results for the change in the vacuum energy due to a\ntime dependent perturbation.",
    "arxiv_id": "quant-ph/0312106",
    "authors": [
      "Dan Solomon"
    ],
    "categories": [
      "quant-ph",
      "hep-th"
    ],
    "title": "Dirac\u0027s hole theory versus field theory for a time dependent   perturbation",
    "url": "https://arxiv.org/abs/quant-ph/0312106"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "99310890-2d7d-4f32-92ca-2748767f5d15",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}