{
  "annotation_id": "4d368ae7-464e-42ac-86b9-1ef851bd6528",
  "date_created": "2026-03-02T18:02:13.679000Z",
  "date_modified": "2026-03-02T18:02:13.679000Z",
  "file_hash": "d91b3c774ddc3d7a11d504b746a8f8bfe7f73a57705a6f12a380b223159467e2",
  "private": false,
  "record": {
    "abstract": "Bell\u0027s theorem states that, to simulate the correlations created by\nmeasurement on pure entangled quantum states, shared randomness is not enough:\nsome \"non-local\" resources are required. It has been demonstrated recently that\nall projective measurements on the maximally entangled state of two qubits can\nbe simulated with a single use of a \"non-local machine\". We prove that a\nstrictly larger amount of this non-local resource is required for the\nsimulation of pure non-maximally entangled states of two qubits\n$\\ket{\\psi(\\alpha)}= \\cos\\alpha\\ket{00}+\\sin\\alpha\\ket{11}$ with\n$0\u003c\\alpha\\lesssim\\frac{\\pi}{7.8}$.",
    "arxiv_id": "quant-ph/0412109",
    "authors": [
      "Nicolas Brunner",
      "Nicolas Gisin",
      "Valerio Scarani"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1088/1367-2630/7/1/088",
    "journal_ref": "New J. Phys. 7, 88 (2005)",
    "title": "Entanglement and non-locality are different resources",
    "url": "https://arxiv.org/abs/quant-ph/0412109"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "bf4b05fb-6ff9-4fd1-a445-fe133367e5e1",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}