What Quantum Measurements Measure
arXiv:1704.08725 · doi:10.1103/PhysRevA.96.032110
Abstract
A solution to the second measurement problem, determining what prior microscopic properties can be inferred from measurement outcomes ("pointer positions"), is worked out for projective and generalized (POVM) measurements, using consistent histories. The result supports the idea that equipment properly designed and calibrated reveals the properties it was designed to measure. Applications include Einstein's hemisphere and Wheeler's delayed choice paradoxes, and a method for analyzing weak measurements without recourse to weak values. Quantum measurements are noncontextual in the original sense employed by Bell and Mermin: if , the outcome of an measurement does not depend on whether it is measured with or with . An application to Bohm's model of the Einstein-Podolsky-Rosen situation suggests that a faulty understanding of quantum measurements is at the root of this paradox.
29 pages, 5 figures. Similar to published version. Only significant change from v1 is the added paragraph at the end of Sec. V E, plus added Refs. [30], [42]
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- On Joint Distributions, Counterfactual Values, and Hidden Variables in Relation to Contextuality
- Quantum postulate vs. quantum nonlocality: Is Devil in h?
- Reply to "Comment on 'Nonlocality claims are inconsistent with Hilbert-space quantum mechanics' '"
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- Quantum Information: What Is It All About?
- Varieties of contextuality based on probability and structural nonembeddability
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- Inconsistency of a realistic interpretation of quantum measurements: A simple example
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- A theory of quantum (statistical) measurement
- Weak continuous measurements require more work than strong ones
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- Logical inconsistencies in quantum mechanics