{ "id": "quant-ph/0609076", "version": "v1", "published": "2006-09-11T09:30:54.000Z", "updated": "2006-09-11T09:30:54.000Z", "title": "Maximum observable correlation for a bipartite quantum system", "authors": [ "Michael J. W. Hall", "Erika Andersson", "Thomas Brougham" ], "comment": "Revtex, no figures", "journal": "Phys. Rev. A 74 (2006) 062308", "doi": "10.1103/PhysRevA.74.062308", "categories": [ "quant-ph" ], "abstract": "The maximum observable correlation between the two components of a bipartite quantum system is a property of the joint density operator, and is achieved by making particular measurements on the respective components. For pure states it corresponds to making measurements diagonal in a corresponding Schmidt basis. More generally, it is shown that the maximum correlation may be characterised in terms of a `correlation basis' for the joint density operator, which defines the corresponding (nondegenerate) optimal measurements. The maximum coincidence rate for spin measurements on two-qubit systems is determined to be (1+s)/2, where s is the spectral norm of the spin correlation matrix, and upper bounds are obtained for n-valued measurements on general bipartite systems. It is shown that the maximum coincidence rate is never greater than the computable cross norm measure of entanglement, and a much tighter upper bound is conjectured. Connections with optimal state discrimination and entanglement bounds are briefly discussed.", "revisions": [ { "version": "v1", "updated": "2006-09-11T09:30:54.000Z" } ], "analyses": { "keywords": [ "bipartite quantum system", "maximum observable correlation", "maximum coincidence rate", "joint density operator", "measurements" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. A" }, "note": { "typesetting": "RevTeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }