Difference between revisions of "Store:QLMen08"

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 Comm. Math. Phys., 17 (1970), pp. 239-260
-View Record in ScopusGoogle Scholar</ref> Ozawa, 1984<ref name=":0" />) quantum instrument or simply quantum instrument. As we shall see in Section 4, complete positivity is a sufficient condition for an instrument to be physically realizable. On the other hand, necessity is derived as follows (Ozawa, 2004)<ref> Ozawa M.
+View Record in ScopusGoogle Scholar</ref> Ozawa, 1984<ref name=":Ozawa M (1984)">Ozawa M. Quantum measuring processes for continuous observables. J. Math. Phys., 25 (1984), pp. 79-87. Google Scholar</ref> quantum instrument or simply quantum instrument. As we shall see in Section 4, complete positivity is a sufficient condition for an instrument to be physically realizable. On the other hand, necessity is derived as follows (Ozawa, 2004)<ref> Ozawa M.
 Uncertainty relations for noise and disturbance in generalized quantum measurements
 Ann. Phys., NY, 311 (2004), pp. 350-416</ref>