{
  "annotation_id": "40979432-f44a-4294-a96b-24971c119ebe",
  "date_created": "2026-03-02T18:01:46.029000Z",
  "date_modified": "2026-03-02T18:01:46.029000Z",
  "file_hash": "84ec459332754bca2fe8d0dab9731e0806e4544c0f96f063449e2e3c396fbb94",
  "private": false,
  "record": {
    "abstract": "Wheeler\u0027s delayed choice experiment, a well known manifestation of the\ncomplementarity principle, has proved somewhat difficult to physically\ninterpret. We show that, restated in quantum field theoretic language, the\nexperiment submits to a simple explanation: that wave- or particle-nature is\nimposed not at the slit plane but at the detector system. The intepretational\ndifficulty conventionally encountered is due to the assumption of enforcement\nof complementarity at the former.",
    "arxiv_id": "quant-ph/0106154",
    "authors": [
      "R. Srikanth"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "A quantum field theoretic description of the delayed choice experiment",
    "url": "https://arxiv.org/abs/quant-ph/0106154"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "852a8da9-1a58-48a2-8eb9-653958a87acb",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}