Synthese 107 (1):55 - 82 (1996)
Models of the EPR-Bohm experiment usually consider just two times, an initial time, and the time of measurement. Within such analyses, it has been argued that locality is equivalent to determinism, given the strict correlations of quantum mechanics. However, an analysis based on such models is only a preliminary to an analysis based on a complete dynamical model. The latter analysis is carried out, and it is shown that, given certain definitions of locality and determinism for completely dynamical models, locality implies, but is not implied by, determinism. Further, it is suggested that a local deterministic model has not been ruled out by Bell's theorem. It is suggested that such a model could naturally deny the independence of initial complete states from the settings of the apparatuses (a crucial assumption in the derivation of Bell's inequality).
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References found in this work BETA
Speakable and Unspeakable in Quantum Mechanics: Collected Papers on Quantum Philosophy.J. S. Bell - 2004 - Cambridge University Press.
On the Einstein-Podolsky-Rosen Paradox.J. S. Bell - 2004  - In Speakable and Unspeakable in Quantum Mechanics. Cambridge University Press. pp. 14--21.
Quantum Mechanics: Historical Contingency and the Copenhagen Hegemony.James T. Cushing - 1994 - University of Chicago Press.
On the Physical Significance of the Locality Conditions in the Bell Arguments.Jon P. Jarrett - 1984 - Noûs 18 (4):569-589.
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Citations of this work BETA
Fine's Ways to Fail to Secure Local Realism.Soazig Le Bihan - 2009 - Studies in the History and Philosophy of Modern Physics 40 (2):142-150.
Multiple-Context Event Spaces and Distributions: A New Framework for Bell's Theorems.Brandon Fogel - 2013 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 44 (3):153-161.
Fine Ways to Fail to Secure Local Realism.Soazig Le Bihan - 2009 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 40 (2):142-150.
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