{
  "annotation_id": "8567c8ee-4183-4268-9954-4e7b51b683fd",
  "date_created": "2026-03-02T18:02:27.400000Z",
  "date_modified": "2026-03-02T18:02:27.400000Z",
  "file_hash": "a8ef83ad7c7d9f51f06e46ec32b1ac1ac0666da6bbe47242f8872ab9cd9bb4ef",
  "private": false,
  "record": {
    "abstract": "Light scattered by a regular structure of atoms can exhibit interference\nsignatures, similar to the classical double-slit. These first-order\ninterferences, however, vanish for strong light intensities, restricting\npotential applications. Here, we show how to overcome these limitations to\nquantum interference in strong fields. First, we recover the first-order\ninterference in strong fields via a tailored electromagnetic bath with a\nsuitable frequency dependence. At strong driving, the optical properties for\ndifferent spectral bands are distinct, thus extending the set of observables.\nWe further show that for a two-photon detector as, e.g., in lithography,\nincreasing the field intensity leads to twice the spatial resolution of the\nsecond-order interference pattern compared to the weak-field case.",
    "arxiv_id": "quant-ph/0606151",
    "authors": [
      "M. Macovei",
      "J. Evers",
      "G. -x. Li",
      "C. H. Keitel"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevLett.98.043602",
    "journal_ref": "Phys. Rev. Lett. 98, 043602 (2007)",
    "title": "Strong-field spatial interference in a tailored electromagnetic bath",
    "url": "https://arxiv.org/abs/quant-ph/0606151"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "d7879be2-5868-4999-a38d-e5a5b4479b4c",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}