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  1. Consciousness Explained.Daniel Dennett - 1991 - Philosophy and Phenomenological Research 53 (4):905-910.
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  • Consciousness Explained.Daniel C. Dennett - 1991 - Penguin Books.
    Little, Brown, 1992 Review by Glenn Branch on Jul 5th 1999 Volume: 3, Number: 27.
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  • The Bare Theory Has No Clothes.Jeffrey Bub, Rob Clifton & Bradley Monton - 1998 - In Richard Healey & Geoffrey Hellman (eds.), Quantum Measurement: Beyond Paradox. University of Minnesota Press. pp. 32-51.
    We criticize the bare theory of quantum mechanics -- a theory on which the Schrödinger equation is universally valid, and standard way of thinking about superpositions is correct.
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  • Quantum Mechanics and Experience.David Z. Albert - 1992 - Harvard Up.
    Presents a guide to the basics of quantum mechanics and measurement.
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  • The Quantum Mechanics of Minds and Worlds.Jeffrey Alan Barrett - 1999 - Oxford, GB: Oxford University Press.
    Jeffrey Barrett presents the most comprehensive study yet of a problem that has puzzled physicists and philosophers since the 1930s.
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  • The Quantum Mechanics of Minds and Worlds.Simon Saunders - 2001 - Mind 110 (440):1039-1043.
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  • Empirical adequacy and the availability of reliable records in quantum mechanics.Jeffrey A. Barrett - 1996 - Philosophy of Science 63 (1):49-64.
    In order to judge whether a theory is empirically adequate one must have epistemic access to reliable records of past measurement results that can be compared against the predictions of the theory. Some formulations of quantum mechanics fail to satisfy this condition. The standard theory without the collapse postulate is an example. Bell's reading of Everett's relative-state formulation is another. Furthermore, there are formulations of quantum mechanics that only satisfy this condition for a special class of observers, formulations whose empirical (...)
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  • The bare theory and how to fix it.Jeffrey Barrett - unknown
    The bare theory is the standard von Neumann·Dirac formulation of quantum mechanics without the collapse postulate but with the eigenvalueeigenstate link. Albert (1992, 1i6-125) presented the bare theory as one way of understanding EverettRi7;s relative-state interpretation. At first glance, it looks as if the bare theory cannot possibly account for our experience. After all, at the end of a measurement an observer will typically be in a superposition of having recorded mutually incompatible results, which on the standard interpretation of states (...)
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