{
  "annotation_id": "b0bb18cc-c531-4414-a29c-2f2690257527",
  "date_created": "2026-03-02T18:02:48.364000Z",
  "date_modified": "2026-03-02T18:02:48.364000Z",
  "file_hash": "24c357314793602e89af71eb29dca32979a990a81ae72f8ae7ce287ffcf688ff",
  "private": false,
  "record": {
    "abstract": "The quantum teleportation process is composed of a joint measurement\nperformed upon two subsystems A and B (uncorrelated), followed by a unitary\ntransformation (parameters of which depend on the outcome of the measurement)\nperformed upon a third subsystem C (EPR correlated with system B). The\ninformation about the outcome of the measurement is transferred by classical\nmeans. The measurement performed upon the systems A and B collapses their joint\nwavefunction into one of the four {\\it entangled} Bell states. It is shown here\nthat this measurement process plus a possible measurement on the third\nsubsystem (with classical channel switched off - no additional unitary\ntransformation performed) cannot be described by a local realistic theory.",
    "arxiv_id": "quant-ph/9912029",
    "authors": [
      "Marek Zukowski"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1103/PhysRevA.62.032101",
    "title": "Bell Theorem for Nonclassical Part of Quantum Teleportation Process",
    "url": "https://arxiv.org/abs/quant-ph/9912029"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ed9cd50d-730b-4202-b609-659d223cd62b",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}