dorsal/arxiv
View SchemaOn the equivalence of the CH and CHSH inequalities for two three-level systems
| Authors | Jose L. Cereceda |
|---|---|
| Categories | |
| ArXiv ID | quant-ph/0212117 |
| URL | https://arxiv.org/abs/quant-ph/0212117 |
| Journal | International Journal of Quantum Information 1, 115-133 (2003) |
Abstract
In this paper we show a Clauser-Horne (CH) inequality for two three-level quantum systems or qutrits, alternative to the CH inequality given by Kaszlikowski et al. [PRA 65, 032118 (2002)]. In contrast to this latter CH inequality, the new one is shown to be equivalent to the Clauser-Horne-Shimony-Holt (CHSH) inequality for two qutrits given by Collins et al. [PRL 88, 040404 (2002)]. Both the CH and CHSH inequalities exhibit the strongest resistance to noise for a nonmaximally entangled state for the case of two von Neumann measurements per site, as first shown by Acin et al. [PRA 65, 052325 (2002)]. This equivalence, however, breaks down when one takes into account the less-than-perfect quantum efficiency of detectors. Indeed, for the noiseless case, the threshold quantum efficiency above which there is no local and realistic description of the experiment for the optimal choice of measurements is found to be 0.814 for the CH inequality, whereas it is equal to 0.828 for the CHSH inequality.
{
"annotation_id": "12923a97-1c3f-47a2-a0f2-6582184a8e5c",
"date_created": "2026-03-02T18:01:56.665000Z",
"date_modified": "2026-03-02T18:01:56.665000Z",
"file_hash": "7cf979e1963b428bad08dd79651aece590663261ba67c1b0d6c8217e24bdd9e4",
"private": false,
"record": {
"abstract": "In this paper we show a Clauser-Horne (CH) inequality for two three-level\nquantum systems or qutrits, alternative to the CH inequality given by\nKaszlikowski et al. [PRA 65, 032118 (2002)]. In contrast to this latter CH\ninequality, the new one is shown to be equivalent to the\nClauser-Horne-Shimony-Holt (CHSH) inequality for two qutrits given by Collins\net al. [PRL 88, 040404 (2002)]. Both the CH and CHSH inequalities exhibit the\nstrongest resistance to noise for a nonmaximally entangled state for the case\nof two von Neumann measurements per site, as first shown by Acin et al. [PRA\n65, 052325 (2002)]. This equivalence, however, breaks down when one takes into\naccount the less-than-perfect quantum efficiency of detectors. Indeed, for the\nnoiseless case, the threshold quantum efficiency above which there is no local\nand realistic description of the experiment for the optimal choice of\nmeasurements is found to be 0.814 for the CH inequality, whereas it is equal to\n0.828 for the CHSH inequality.",
"arxiv_id": "quant-ph/0212117",
"authors": [
"Jose L. Cereceda"
],
"categories": [
"quant-ph"
],
"journal_ref": "International Journal of Quantum Information 1, 115-133 (2003)",
"title": "On the equivalence of the CH and CHSH inequalities for two three-level systems",
"url": "https://arxiv.org/abs/quant-ph/0212117"
},
"schema_id": "dorsal/arxiv",
"source": {
"execution_id": "7a6d50b1-f570-493c-a7ee-38b067850fd0",
"id": "arXiv Dataset IDs",
"type": "Model",
"variant": "snapshot-2026-03-01",
"version": "0.1.0"
},
"user_id": 1000002
}