{
  "annotation_id": "596fbebe-b7d0-4c3a-aea6-0f01a7e08a3e",
  "date_created": "2026-03-02T18:01:59.339000Z",
  "date_modified": "2026-03-02T18:01:59.339000Z",
  "file_hash": "0f5ecab534eaa96b016d860f1a311e6ed3656ad3ed1950229680128e4ca0b1d0",
  "private": false,
  "record": {
    "abstract": "The Deutsch-Jozsa algorithm distinguishes constant functions from balanced\nfunctions with a single evaluation. In the first part of this work, we present\nsimulations of the nuclear magnetic resonance (NMR) application of the\nDeutsch-Jozsa algorithm to a 3-spin system for all possible balanced functions.\nThree different kinds of initial states are considered: a thermal state, a\npseudopure state, and a pair (difference) of pseudopure states. Then,\nsimulations of several balanced functions and the two constant functions of a\n5-spin system are described. Finally, corresponding experimental spectra\nobtained by using a 16-frequency pulse to create an input equivalent to either\na constant function or a balanced function are presented, and the results are\ncompared with those obtained from computer simulations.",
    "arxiv_id": "quant-ph/0304058",
    "authors": [
      "Vladimir L. Ermakov",
      "B. M. Fung"
    ],
    "categories": [
      "quant-ph"
    ],
    "doi": "10.1063/1.1574802",
    "title": "Nuclear magnetic resonance implementation of the Deutsch-Jozsa algorithm   using different initial states",
    "url": "https://arxiv.org/abs/quant-ph/0304058"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "bb7dfc76-d09a-480a-90c4-82192c198f9d",
    "id": "arXiv Dataset IDs",
    "type": "Model",
    "variant": "snapshot-2026-03-01",
    "version": "0.1.0"
  },
  "user_id": 1000002
}