{
  "annotation_id": "00682cdc-cdac-4dc4-bc6b-6a69127157e5",
  "date_created": "2026-03-02T18:02:48.229000Z",
  "date_modified": "2026-03-02T18:02:48.229000Z",
  "file_hash": "38bf280c72f02152cb53f4797bb03a039a27d5698b6e96e591ec5d11f569a17d",
  "private": false,
  "record": {
    "abstract": "If several interventions performed on a quantum system are localized in\nmutually space-like regions, they will be recorded as a sequence of ``quantum\njumps\u0027\u0027 in one Lorentz frame, and as a different sequence of jumps in another\nLorentz frame. Conditions are specified that must be obeyed by the various\noperators involved in the calculations so that these two different sequences\nlead to the same observable results. These conditions are similar to the\nequal-time commutation relations in quantum field theory. They are sufficient\nto prevent superluminal signaling. (The derivation of these results does not\nrequire most of the contents of the preceding article. What is needed is\nbriefly summarized here, so that the present article is essentially\nself-contained.)",
    "arxiv_id": "quant-ph/9906034",
    "authors": [
      "Asher Peres"
    ],
    "categories": [
      "quant-ph",
      "hep-th"
    ],
    "doi": "10.1103/PhysRevA.61.022117",
    "journal_ref": "Physical Review A 61 (2000) 022117",
    "title": "Classical interventions in quantum systems. II. Relativistic invariance",
    "url": "https://arxiv.org/abs/quant-ph/9906034"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "7a206247-b9f2-4383-91b0-d5a8d1da4ef1",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}