Abstract
A so called "weak value" of an observable in quantum mechanics (QM) may be obtained in a weak measurement + post-selection procedure on the QM system under study. Applied to number operators, it has been invoked in revisiting some QM paradoxes (e.g., the so called Three-Box Paradox and Hardy's Paradox). This requires the weak value to be interpreted as a bona fide property of the system considered, a par with entities like operator mean values and eigenvalues. I question such an interpretation; it has no support in the basic axioms of quantum mechanics and it leads to unreasonable results in concrete situations.
Original language | English |
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Pages (from-to) | 1193-1205 |
Journal | Foundations of Physics |
Volume | 43 |
Issue number | 10 |
DOIs | |
Publication status | Published - 2013 |
Subject classification (UKÄ)
- Subatomic Physics
Free keywords
- Weak value
- Number operator
- Hardy's paradox
- Interpretation of QM