{
  "annotation_id": "528d8321-e333-46f8-8082-fc20a92d8744",
  "date_created": "2026-03-02T18:02:13.321000Z",
  "date_modified": "2026-03-02T18:02:13.321000Z",
  "file_hash": "9dafa8bd916a8428d0e0456199d2f2eeac9cd304fea8159eb5ec880a30987f40",
  "private": false,
  "record": {
    "abstract": "The quantum theory of the mazer in the non-resonant case (a detuning between\nthe cavity mode and the atomic transition frequencies is present) is written.\nThe generalization from the resonant case is far from being direct. Interesting\neffects of the mazer physics are pointed out. In particular, it is shown that\nthe cavity may slow down or speed up the atoms according to the sign of the\ndetuning and that the induced emission process may be completely blocked by use\nof a positive detuning. It is also shown that the detuning adds a potential\nstep effect not present at resonance and that the use of positive detunings\ndefines a well-controlled cooling mechanism. In the special case of a mesa\ncavity mode function, generalized expressions for the reflection and\ntransmission coefficients have been obtained. The general properties of the\ninduced emission probability are finally discussed in the hot, intermediate and\ncold atom regimes. Comparison with the resonant case is given.",
    "arxiv_id": "quant-ph/0412043",
    "authors": [
      "Thierry Bastin",
      "John Martin"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevA.67.053804",
    "journal_ref": "Phys. Rev. A 67, 053804 (2003)",
    "title": "Detuning effects in the one-photon mazer",
    "url": "https://arxiv.org/abs/quant-ph/0412043"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "5e5191f8-0ac2-4016-814d-77f96a478749",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}