{
  "annotation_id": "a28818fb-f153-47fe-a1fd-96caf15c6adf",
  "date_created": "2026-03-02T18:02:27.113000Z",
  "date_modified": "2026-03-02T18:02:27.113000Z",
  "file_hash": "e76d1cec33557de36ec018f50c20540a578ab5e23569261d2387162903ad419e",
  "private": false,
  "record": {
    "abstract": "We report on an intrinsic relationship between the maximum-likelihood\nquantum-state estimation and the representation of the signal. A quantum\nanalogy of the transfer function determines the space where the reconstruction\nshould be done without the need for any ad hoc truncations of the Hilbert\nspace. An illustration of this method is provided by a simple yet practically\nimportant tomography of an optical signal registered by realistic binary\ndetectors.",
    "arxiv_id": "quant-ph/0606042",
    "authors": [
      "Z. Hradil",
      "D. Mogilevtsev",
      "J. Rehacek"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevLett.96.230401",
    "title": "Biased tomography schemes: an objective approach",
    "url": "https://arxiv.org/abs/quant-ph/0606042"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "fa02df5a-5258-4297-900e-40a0157d6b08",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}