{
  "annotation_id": "80a5a256-9b13-44ff-b07e-76deb3821c14",
  "date_created": "2026-03-02T18:00:35.579000Z",
  "date_modified": "2026-03-02T18:00:35.579000Z",
  "file_hash": "f6856c319017983ee84e311e89e9003d1745e87d00cf0e87b6352b2f847c6f62",
  "private": false,
  "record": {
    "abstract": "As a light beam is produced by an amplification of modes of the zero point\nfield in its source, this field cannot be distinguished; consequently a\nnonlinear optical effect is a function of the total field. However, we\ngenerally prefer to use a conventional field which excludes the zero point\nfield; for a low conventional field, the total field may be developed to the\nfirst order, so that the effect appears linear.\n  This nearly trivial remark allows a correct computation of the signal of a\nphotocell used for photon counting and shows that the \"impulsive stimulated\nRaman scattering\" (ISRS), a nonlinear, without threshold effect, which shifts\nthe frequencies, becomes linear at low light levels, so that the shifted\nspectra are not distorted.",
    "arxiv_id": "physics/0105055",
    "authors": [
      "Jacques Moret-Bailly"
    ],
    "categories": [
      "physics.optics"
    ],
    "title": "Linearisation of optical effects at low light levels",
    "url": "https://arxiv.org/abs/physics/0105055"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "2b8ef516-d6bd-4496-baa0-90ab2eae7be4",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}