{
  "annotation_id": "40e29a34-d433-4c7d-bbca-133a794efa55",
  "date_created": "2026-03-02T18:02:27.708000Z",
  "date_modified": "2026-03-02T18:02:27.708000Z",
  "file_hash": "858ebc5fca94710730e75b5560806bfc3d801517708d54f84420a743219b3b02",
  "private": false,
  "record": {
    "abstract": "The interaction of a quantized field with three-level atoms in $\\Lambda$\nconfiguration inside a two mode cavity is analyzed. We calculate the stationary\nquadrature noise spectrum of the field outside the cavity in the case where the\ninput probe field is in a squeezed state and the atoms show electromagnetically\ninduced transparency (EIT). If the Rabi frequencies of both dipole transitions\nof the atoms are different from zero, we show that the output probe field have\nfour maxima of squeezing absorption. We show that in some cases two of these\nfrequencies can be very close to the transition frequency of the atom, in a\nregion where the mean value of the field entering the cavity is hardly altered.\nFurthermore, part of the absorbed squeezing of the probe field is transfered to\nthe pump field. For some conditions this transfer of squeezing can be complete.",
    "arxiv_id": "quant-ph/0605168",
    "authors": [
      "P. Barberis-Blostein"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevA.74.013803",
    "journal_ref": "Phys. Rev. A 74, 013803 (2006)",
    "title": "Field autocorrelations in electromagnetically induced transparency:   Effects of a squeezed probe field",
    "url": "https://arxiv.org/abs/quant-ph/0605168"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "92afae7f-5f1c-49ef-8d7b-2b675c675e86",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}