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  1. Towards a separable “empirical reality”?Bernard D'Espagnat - 1990 - Foundations of Physics 20 (10):1147-1172.
    “To be” or “to be found”? Some contributions relative to this modern variant of Hamlet's question are presented here. They aim at better apprehending the differences between the points of view of the physicists who consider that present-day quantum measurement theories do reach their objective and those who deny they do. It is pointed out that these two groups have different interpretations of the verbs “to be” and “to have” and of the criterion for truth. These differences are made explicit. (...)
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  • Why the Laws of Physics Are Just So.Ulrich Mohrhoff - 2002 - Foundations of Physics 32 (8):1313-1324.
    Does a world that contains chemistry entail the validity of both the standard model of elementary particle physics and general relativity, at least as effective theories? This article shows that the answer may very well be affirmative. It further suggests that the very existence of stable, spatially extended material objects, if not the very existence of the physical world, may require the validity of these theories.
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  • A philosopher's understanding of quantum mechanics: possibilities and impossibilities of a modal interpretation.Pieter E. Vermaas - 1999 - New York: Cambridge University Press.
    This book is about how to understand quantum mechanics by means of a modal interpretation. Modal interpretations provide a general framework within which quantum mechanics can be considered as a theory that describes reality in terms of physical systems possessing definite properties. Quantum mechanics is standardly understood to be a theory about probabilities with which measurements have outcomes. Modal interpretations are relatively new attempts to present quantum mechanics as a theory which, like other physical theories, describes an observer-independent reality. In (...)
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  • Beyond the cookie Cutter paradigm.Ulrich Mohrhoff - 2001 - Consciousness and its Transformation: Papers Presented at the Second International Conference on Integral Psychology.
    What makes it so hard to make sense of quantum mechanics (the theory at the heart of contemporary physics) is the cookie cutter paradigm (a fallacy that is both rooted in our neurophysiological make-up and inherent in the nature of mental consciousness) according to which the world's synchronic multiplicity derives from surfaces that carve up space in the manner of three-dimensional cookie cutters. When liberated from this fallacy, quantum mechanics not only describes the physical world as a manifestation of something (...)
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  • Variations on the Theme of the Greenberger-Horne-Zeilinger Proof.Lev Vaidman - 1999 - Foundations of Physics 29 (4):615-630.
    Three arguments based on the Greenberger-Horne-Zeilinger (GHZ) proof of the nonexistence of local hidden variables are presented. The first is a description of a simple game which a team that uses the GHZ method will always win. The second uses counterfactuals in an attempt to show that quantum theory is nonlocal in a stronger sense than is implied by the nonexistence of local hidden variables and the third describes peculiar features of time-symmetrized counterfactuals in quantum theory.
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  • Making Sense of a World of Clicks.Ulrich Mohrhoff - 2002 - Foundations of Physics 32 (8):1295-1311.
    In a recent article, O. Ulfbeck and A. Bohr [Found. Phys. 31, 757 (2001)] have stressed the genuine fortuitousness of detector clicks, which has also been pointed out, in different terms, by the present author [Am. J. Phys. 68, 728 (2000)]. In spite of this basic agreement, the present article raises objections to the presuppositions and conclusions of Ulfbeck and Bohr, in particular their rejection of the terminology of indefinite variables, their identification of reality with “the world of experience,” their (...)
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  • “Haunted” measurements in quantum theory.Daniel M. Greenberger & Alaine YaSin - 1989 - Foundations of Physics 19 (6):679-704.
    Sometimes it is possible in quantum theory for a system to interact with another system in such a way that the information contained in the wave function becomes very scrambled and apparently incoherent. We produce an example which is exactly calculable, in which a macroscopic change is induced in the environment, and all phase information for the system is apparently lost, so that a measurement has seemingly been made. But actually, although the wave function has been badly scrambled, all the (...)
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