dorsal/arxiv
View SchemaQuantum key distribution using polarized coherent states
| Authors | A. Vidiella-Barranco, L. F. M. Borelli |
|---|---|
| Categories | |
| ArXiv ID | quant-ph/0403076 |
| URL | https://arxiv.org/abs/quant-ph/0403076 |
| DOI | 10.1142/S0217979206033929 |
| Journal | Int. J. Mod. Phys. B., 20, 1287 (2006) |
Abstract
We discuss a continuous variables method of quantum key distribution employing strongly polarized coherent states of light. The key encoding is performed using the variables known as Stokes parameters, rather than the field quadratures. Their quantum counterpart, the Stokes operators $\hat{S}_i$ (i=1,2,3), constitute a set of non-commuting operators, being the precision of simultaneous measurements of a pair of them limited by an uncertainty-like relation. Alice transmits a conveniently modulated two-mode coherent state, and Bob randomly measures one of the Stokes parameters of the incoming beam. After performing reconciliation and privacy amplification procedures, it is possible to distill a secret common key. We also consider a non-ideal situation, in which coherent states with thermal noise, instead of pure coherent states, are used for encoding.
{
"annotation_id": "86457ad6-a2f8-4e42-9320-7c6704324bad",
"date_created": "2026-03-02T18:02:06.503000Z",
"date_modified": "2026-03-02T18:02:06.503000Z",
"file_hash": "cf80c64db2a9e1c9b9c5095a67b69bb07d767eacb2ad75066c6437b01e46c79c",
"private": false,
"record": {
"abstract": "We discuss a continuous variables method of quantum key distribution\nemploying strongly polarized coherent states of light. The key encoding is\nperformed using the variables known as Stokes parameters, rather than the field\nquadratures. Their quantum counterpart, the Stokes operators $\\hat{S}_i$\n(i=1,2,3), constitute a set of non-commuting operators, being the precision of\nsimultaneous measurements of a pair of them limited by an uncertainty-like\nrelation. Alice transmits a conveniently modulated two-mode coherent state, and\nBob randomly measures one of the Stokes parameters of the incoming beam. After\nperforming reconciliation and privacy amplification procedures, it is possible\nto distill a secret common key. We also consider a non-ideal situation, in\nwhich coherent states with thermal noise, instead of pure coherent states, are\nused for encoding.",
"arxiv_id": "quant-ph/0403076",
"authors": [
"A. Vidiella-Barranco",
"L. F. M. Borelli"
],
"categories": [
"quant-ph",
"cs.CR",
"physics.optics"
],
"doi": "10.1142/S0217979206033929",
"journal_ref": "Int. J. Mod. Phys. B., 20, 1287 (2006)",
"title": "Quantum key distribution using polarized coherent states",
"url": "https://arxiv.org/abs/quant-ph/0403076"
},
"schema_id": "dorsal/arxiv",
"source": {
"execution_id": "1ba2bd4a-5ff4-4aaa-89ab-26fa4e51d52a",
"id": "arXiv Dataset IDs",
"type": "Model",
"variant": "snapshot-2026-03-01",
"version": "0.1.0"
},
"user_id": 1000002
}