Maximum observable correlation for a bipartite quantum system

Michael J.W. Hall, Erika Andersson, Thomas Brougham

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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 characterized 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.
Original languageEnglish
Number of pages11
JournalPhysical Review A
Issue number6
Publication statusPublished - 18 Dec 2006


  • bipartite quantum system
  • qubit
  • quantum physics
  • quantum

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