{
  "annotation_id": "cba2a2d1-1be0-4219-a286-1e1226249498",
  "date_created": "2026-03-02T18:01:38.727000Z",
  "date_modified": "2026-03-02T18:01:38.727000Z",
  "file_hash": "07a697cd4824c277b60ba0a838a6b3792f29dc3b8f0ce21801252e9ad251380b",
  "private": false,
  "record": {
    "abstract": "Following the previous paper in which quantum teleportation is rig orously\ndiscussed with coherent entangled states given by beam splittings, we further\ndiscuss two types of models, perfect teleportation model and non-perfect\nteleportation model, in general scheme. Then the difference among several\nmodels, i.e., the perfect models and the non-perfect models, is studied. Our\nteleportation models are constructed by means of coherent states in some Fock\nspace with counting measures, so that our model can be treated in the frame of\nusual optical communication.",
    "arxiv_id": "quant-ph/0005040",
    "authors": [
      "Karl-Heinz Fichtner",
      "Masanori Ohya"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1007/s002201000571",
    "journal_ref": "Commun.Math.Phys.225,67-89(2002)",
    "title": "Quantum Teleportation and Beam Splitting",
    "url": "https://arxiv.org/abs/quant-ph/0005040"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "b520c265-763d-46d5-a501-8ecd8a905f49",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}