{ "id": "0801.1545", "version": "v1", "published": "2008-01-10T05:05:58.000Z", "updated": "2008-01-10T05:05:58.000Z", "title": "Characteristics and benchmarks of entanglement of mixed states -- the two qubit case", "authors": [ "Shanthanu Bhardwaj", "V. Ravishankar" ], "comment": "12 pages, 6 figures. Enlarged version of quant-phy/0703017", "doi": "10.1103/PhysRevA.77.022322", "categories": [ "quant-ph" ], "abstract": "We propose that the entanglement of mixed states is characterised properly in terms of a probability density function $\\mathcal{P}_{\\rho}(\\mathcal{E})$. There is a need for such a measure since the prevalent measures (such as \\textit{concurrence} and \\textit{negativity}) for two qubit systems are rough benchmarks, and not monotones of each other. Focussing on the two qubit states, we provide an explicit construction of $\\mathcal{P}_{\\rho}(\\mathcal{E})$ and show that it is characterised by a set of parameters, of which concurrence is but one particular combination. $\\mathcal{P}_{\\rho}(\\mathcal{E})$ is manifestly invariant under $SU(2) \\times SU(2)$ transformations. It can, in fact, reconstruct the state up to local operations - with the specification of at most four additional parameters. Finally the new measure resolves the controversy regarding the role of entanglement in quantum computation in NMR systems.", "revisions": [ { "version": "v1", "updated": "2008-01-10T05:05:58.000Z" } ], "analyses": { "subjects": [ "03.67.Mn", "03.65.Ud", "03.67.Hk", "76.60.-k" ], "keywords": [ "mixed states", "qubit case", "entanglement", "characteristics", "probability density function" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review A", "year": 2008, "month": "Feb", "volume": 77, "number": 2, "pages": "022322" }, "note": { "typesetting": "TeX", "pages": 12, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2008PhRvA..77b2322B" } } }