Authors
Jeffrey Barrett
University of California, Irvine
Abstract
argued that there are two options for what he called a realistic solution to the quantum measurement problem: (1) select a preferred set of observables for which definite values are assumed to exist, or (2) attempt to assign definite values to all observables simultaneously (1810–1). While conventional wisdom has it that the second option is ruled out by the Kochen-Specker theorem, Vink nevertheless advocated it. Making every physical quantity determinate in quantum mechanics carries with it significant conceptual costs, but it also provides a way of addressing the preferred basis problem that arises if one chooses to pursue the first option. The potential costs and benefits of a formulation of quantum mechanics where every physical quantity is determinate are herein examined. The preferred-basis problem How to solve the preferred-basis problem Relativistic constraints Conclusion.
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DOI 10.1093/bjps/axi114
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References found in this work BETA

The Scientific Image.William Demopoulos & Bas C. van Fraassen - 1982 - Philosophical Review 91 (4):603.
The Scientific Image.Michael Friedman - 1982 - Journal of Philosophy 79 (5):274-283.
The Problem of Hidden Variables in Quantum Mechanics.Simon Kochen & E. P. Specker - 1967 - Journal of Mathematics and Mechanics 17:59--87.

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Citations of this work BETA

The Measurement Problem Revisited.Shan Gao - 2019 - Synthese 196 (1):299-311.
Entanglement and Disentanglement in Relativistic Quantum Mechanics.Jeffrey A. Barrett - 2014 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 48 (2):168-174.

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