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  1. An interpretation of macroscopic irreversibility within the Newtonian framework.Henry B. Hollinger & Michael J. Zenzen - 1982 - Philosophy of Science 49 (3):309-354.
    Some of the most imaginative analyses in contemporary science have been fostered by the paradox of irreversibility. Rendered as a question the paradox reads: How can the anisotropic macrophysical behavior of a system of molecules be reconciled with the underlying reversible molecular model? Attempts to resolve and dissolve the paradox have appealed to large numbers of particles, jammed correlations, unseen perturbations, hidden variables or constraints, uncertainty principles, averaging procedures (e.g., coarse graining and time smoothing), stochastic flaws, cosmological origins, etc. While (...)
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  • De Broglie's wave particle duality in the stochastic interpretation of quantum mechanics: A testable physical assumption. [REVIEW]Ph Gueret & J. -P. Vigier - 1982 - Foundations of Physics 12 (11):1057-1083.
    If one starts from de Broglie's basic relativistic assumptions, i.e., that all particles have an intrinsic real internal vibration in their rest frame, i.e., hv 0 =m 0 c 2 ; that when they are at any one point in space-time the phase of this vibration cannot depend on the choice of the reference frame, then, one can show (following Mackinnon (1) ) that there exists a nondispersive wave packet of de Broglie's waves which can be assimilated to the nonlinear (...)
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  • Some local models for correlation experiments.Arthur Fine - 1982 - Synthese 50 (2):279 - 294.
    This paper constructs two classes of models for the quantum correlation experiments used to test the Bell-type inequalities, synchronization models and prism models. Both classes employ deterministic hidden variables, satisfy the causal requirements of physical locality, and yield precisely the quantum mechanical statistics. In the synchronization models, the joint probabilities, for each emission, do not factor in the manner of stochastic independence, showing that such factorizability is not required for locality. In the prism models the observables are not random variables (...)
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  • The effect of localization on interference. II. Bearing on locality violation and the interpretation of quantum mechanics.Charles E. Engelke - 1986 - Foundations of Physics 16 (9):917-921.
    In a two-channel interference experiment such as that considered in the preceding companion paper, a quantum may be localizable predominantly in one channel by a time-coincident experiment on a correlated quantum. The Copenhagen interpretation of quantum mechanics then requires a coincidence intensity prediction having the same reduced interference between channels as if the probability amplitude in the other channel had been attenuated by a filter. The quantum mechanical treatment of correlated systems originated by von Neumann does predict this reduced interference, (...)
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