Erkenntnis 41 (2):233 - 252 (1994)

Authors
Jeffrey Barrett
University of California, Irvine
Abstract
Everett proposed resolving the quantum measurement problem by dropping the nonlinear collapse dynamics from quantum mechanics and taking what is left as a complete physical theory. If one takes such a proposal seriously, then the question becomes how much of the predictive and explanatory power of the standard theory can one recover without the collapse postulate and without adding anything else. Quantum mechanics without the collapse postulate has several suggestive properties, which we will consider in some detail. While these properties are not enough to make it acceptable given the usual standards for a satisfactory physical theory, one might want to exploit these properties to cook up a satisfactory no-collapse formulation of quantum mechanics. In considering how this might work, we will see why any no-collapse theory must generally fail to satisfy at least one of two plausible-sounding conditions.
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DOI 10.1007/BF01128831
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References found in this work BETA

The Measurement of Relative Frequency.Neill Graham - 1973 - In B. DeWitt & N. Graham (eds.), The Many-Worlds Interpretation of Quantum Mechanics. Princeton Up. pp. 1--229.
'Relative State' Formulation of Quantum Mechanics.Hugh Everett - 1957 - Reviews of Modern Physics 29 (3):454-462.

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Citations of this work BETA

The Bare Theory Has No Clothes.Jeffrey Bub, Rob Clifton & Bradley Monton - 1998 - In Richard Healey & Geoffrey Hellman (eds.), Quantum Measurement: Beyond Paradox. Minneapolis, USA: University of Minnesota Press. pp. 32-51.
Introduction.Jeffrey A. Barrett - 1995 - Topoi 14 (1):1-6.

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