{
  "annotation_id": "4fd3f5ed-cfd3-4465-bcc1-5f629aec3d55",
  "date_created": "2026-03-02T18:02:13.220000Z",
  "date_modified": "2026-03-02T18:02:13.220000Z",
  "file_hash": "0483c4bab2cbd849b00df451c5f74f86ab72b586cab027e6be5135bd566cb24f",
  "private": false,
  "record": {
    "abstract": "In relativity there is space-time out there. In quantum mechanics there is\nentanglement. Entanglement manifests itself by producing correlations between\nclassical events (e.g. the firing of some detectors) at any two space-time\nlocations. If the locations are time-like separated, i.e. one is in the future\nof the other, then there is no specific difficulty to understand the\ncorrelations. But if the two locations are space-like separated, the problem is\ndifferent. How can the two space-time locations out there know about what\nhappens in each other without any sort of communication? If space-time really\nexists, the locations must do something like communicating. Or it was all set\nup at the Beginning. But the correlations depend also on the free choice of the\nexperimentalists, one in each space-time location. This allowed John Bell to\nderive his inequality and the experimentalists to violate it, thus refuting the\nassumption that it was all set up at the beginning: the Correlations can\u0027t be\nexplained by common causes.",
    "arxiv_id": "quant-ph/0503007",
    "authors": [
      "Nicolas Gisin"
    ],
    "categories": [
      "quant-ph"
    ],
    "title": "How come the Correlations?",
    "url": "https://arxiv.org/abs/quant-ph/0503007"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "eb811bf4-1b4c-45bb-bebf-800d6991fc98",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}