{
  "annotation_id": "d67994d4-bca1-4ef1-bfcd-45c53ba2b812",
  "date_created": "2026-03-02T18:01:55.797000Z",
  "date_modified": "2026-03-02T18:01:55.797000Z",
  "file_hash": "3eb02e004d371dccbf3a5f7c9062c734e3b939b90150b89ee9cf2c657bbc4b2d",
  "private": false,
  "record": {
    "abstract": "A cavity QED system is analyzed which duplicates the dynamics of a two-level\natom in free space interacting exclusively with broadband squeezed light. We\nconsider atoms in a three or four-level Lambda-configuration coupled to a\nhigh-finesse optical cavity which is driven by a squeezed light field. Raman\ntransitions are induced between a pair of stable atomic ground states via the\nsqueezed cavity mode and coherent driving fields. An analysis of the reduced\nmaster equation for the atomic ground states shows that a three-level atomic\nsystem has insufficient parameter flexibility to act as an effective two-level\natom interacting exclusively with a squeezed reservoir. However, the inclusion\nof a fourth atomic level, coupled dispersively to one of the two ground states\nby an auxiliary laser field, introduces an extra degree of freedom and enables\nthe desired interaction to be realised. As a means of detecting the reduced\nquadrature decay rate of the effective two-level system, we examine the\ntransmission spectrum of a weak coherent probe field incident upon the cavity.",
    "arxiv_id": "quant-ph/0212022",
    "authors": [
      "Stephen Clark",
      "Scott Parkins"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1088/1464-4266/5/2/305",
    "title": "Coupling of effective one-dimensional two-level atoms to squeezed light",
    "url": "https://arxiv.org/abs/quant-ph/0212022"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ea9d25b0-dc1a-4706-ab40-2df35b3788aa",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}