{
  "id": "0904.2343",
  "version": "v1",
  "published": "2009-04-15T19:03:17.000Z",
  "updated": "2009-04-15T19:03:17.000Z",
  "title": "Purification of multipartite entanglement by local operations",
  "authors": [
    "Ming Yang",
    "Fei Yan",
    "Zhuo-Liang Cao"
  ],
  "comment": "5 pages, 2 figures",
  "categories": [
    "quant-ph"
  ],
  "abstract": "Multipartite entanglement purification is revisited by using the Local operations and classical communications(LOCCs). We demonstrate our idea by considering the tripartite case, i.e. the purification of tripartite entanglement. We express the general tripartite entangled states in a special representation of total spin operators $J_{123}^{2}$ and $% J_{12}^{2}$ of tripartite system with eigenvalues 15/4 and 2 respectively. This basis is a \\textit{genuine basis} because it consists of of all the genuine entangled states of tripartite system. Our protocol is a recurrence one, and only two copies of the initial mixed tripartite entangled states are needed in each round. It is shown that if the initial fidelity is larger than a threshold 0.4, the purification process will succeed.The yield of the current protocol is higher than the previous multipartite entanglement purification protocols. As a by-product, we can get a bipartite pure Bell state when the purification protocol fails for W state. Our protocol also shows that there may be some special kind of tripartite entanglement which belongs to neither W-type entanglement nor GHZ-type entanglement.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2009-04-15T19:03:17.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "local operations",
      "mixed tripartite entangled states",
      "tripartite entanglement",
      "bipartite pure bell state",
      "multipartite entanglement purification protocols"
    ],
    "note": {
      "typesetting": "TeX",
      "pages": 5,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "adsabs": "2009arXiv0904.2343Y"
    }
  }
}