How quantum paradoxes originate from the non-classical statistics of physical properties related to each other by half-periodic transformations
arXiv:1406.3085 · doi:10.1103/PhysRevA.91.062123
Abstract
Quantum paradoxes show that quantum statistics can exceed the limits of positive joint probabilities for physical properties that cannot be measured jointly. It is therefore impossible to describe the relations between the different physical properties of a quantum system by assigning joint realities to their observable values. Instead, recent experimental results obtained by weak measurements suggest that non-classical correlations could be expressed by complex valued quasi-probabilities, where the phases of the complex probabilities express the action of transformations between the non-commuting properties (H. F. Hofmann, New J. Phys. 13, 103009 (2011)). In these relations, negative probabilities necessarily emerge whenever the physical properties involved are related to each other by half-periodic transformations, since such transformations are characterized by action phases of Pi in their complex probabilities. It is therefore possible to trace the failure of realist assumptions back to a fundamental and universally valid relation between statistics and dynamics that associates half-periodic transformations with negative probabilities.
14 pages, including 2 figures and 1 table, major improvements and updates, e.g. in the explanation of Eq.(5) and in the discussion of contextuality in section VII
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- Characterization of the non-classical relation between measurement outcomes represented by non-orthogonal quantum states
- Advantages of the Kirkwood-Dirac distribution among general quasi-probabilities for finite-state quantum systems
- Sequential propagation of a single photon through five measurement contexts in a three-path interferometer
- Statistical signatures of quantum contextuality
- Separating a particle's mass from its momentum
- Origin of meter fluctuations in weak measurement interactions
- Almost no experiments have classical Kirkwood-Dirac representations