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  1. Comment on “Non-representative Quantum Mechanical Weak Values”.Lev Vaidman & Alon Ben-Israel - 2017 - Foundations of Physics 47 (4):467-470.
    Svensson argued that the concept of the weak value of an observable of a pre- and post-selected quantum system cannot be applied when the expectation value of the observable in the initial state vanishes. Svensson’s argument is analyzed and shown to be inconsistent using several examples.
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  • Quantum Weak Values and Logic: An Uneasy Couple.Bengt E. Y. Svensson - 2017 - Foundations of Physics 47 (3):430-452.
    Quantum mechanical weak values of projection operators have been used to answer which-way questions, e.g. to trace which arms in a multiple Mach–Zehnder setup a particle may have traversed from a given initial to a prescribed final state. I show that this procedure might lead to logical inconsistencies in the sense that different methods used to answer composite questions, like “Has the particle traversed the way X or the way Y?”, may result in different answers depending on which methods are (...)
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  • Response to Comment on ‘Non-representative Quantum Mechanical Weak Values’ by Ben-Israel and Vaidman.B. E. Y. Svensson - 2017 - Foundations of Physics 47 (9):1258-1260.
    Ben-Israel and Vaidman have raised objections to my arguments that there are cases where a quantum mechanical weak value can be said not to represent the system to which it pertains. They are correct in pointing out that some of my conclusions were too general. However, for weak values of projection operators my conclusions still stand.
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