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  1. Bohmian mechanics and quantum theory: an appraisal.James T. Cushing, Arthur Fine & Sheldon Goldstein - 1996 - Springer.
    We are often told that quantum phenomena demand radical revisions of our scientific world view and that no physical theory describing well defined objects, such as particles described by their positions, evolving in a well defined way, let alone deterministically, can account for such phenomena. The great majority of physicists continue to subscribe to this view, despite the fact that just such a deterministic theory, accounting for all of the phe nomena of nonrelativistic quantum mechanics, was proposed by David Bohm (...)
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  • The Spin-Echo Experiments and the Second Law of Thermodynamics.T. M. Ridderbos & M. L. G. Redhead - 1998 - Foundations of Physics 28 (8):1237-1270.
    We introduce a simple model for so-called spin-echo experiments. We show that the model is a mincing system. On the basis of this model we study fine-grained entropy and coarse-grained entropy descriptions of these experiments. The coarse-grained description is shown to be unable to provide an explanation of the echo signals, as a result of the way in which it ignores dynamically generated correlations. This conclusion is extended to the general debate on the foundations of statistical mechanics. We emphasize the (...)
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  • The Modal Interpretation of Quantum Mechanics.Dennis Dieks & Pieter Vermaas - 1998 - Kluwer Academic Publishers.
    According to the modal interpretation, the standard mathematical framework of quantum mechanics specifies the physical magnitudes of a system, which have definite values. Probabilities are assigned to the possible values that these magnitudes may adopt. The interpretation is thus concerned with physical properties rather than with measurement results: it is a realistic interpretation. One of the notable achievements of this interpretation is that it dissolves the notorious measurement problem. The papers collected here, together with the introduction and concluding critical appraisal, (...)
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  • The Many-Worlds Interpretation of Quantum Mechanics.B. DeWitt & N. Graham (eds.) - 1973 - Princeton UP.
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  • Unified dynamics for microscopic and macroscopic systems.GianCarlo Ghirardi, Alberto Rimini & Tullio Weber - 1986 - Physical Review D 34 (D):470–491.
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  • The foundations of quantum mechanics and the approach to thermodynamic equilibrium.David Z. Albert - 1994 - British Journal for the Philosophy of Science 45 (2):669-677.
    It is argued that certain recent advances in the construction of a theory of the collapses of Quantum Mechanical wave functions suggest the possibility of new and improved foundations for statistical mechanics, foundations in which epistemic considerations play no role.
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  • Bluff Your Way in the Second Law of Thermodynamics.Jos Uffink - 2001 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 32 (3):305-394.
    The aim of this article is to analyse the relation between the second law of thermodynamics and the so-called arrow of time. For this purpose, a number of different aspects in this arrow of time are distinguished, in particular those of time-reversal (non-)invariance and of (ir)reversibility. Next I review versions of the second law in the work of Carnot, Clausius, Kelvin, Planck, Gibbs, Caratheodory and Lieb and Yngvason, and investigate their connection with these aspects of the arrow of time. It (...)
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  • The Origins of Time-Asymmetry in Thermodynamics: The Minus First Law.Harvey R. Brown & Jos Uffink - 2001 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 32 (4):525-538.
    This paper investigates what the source of time-asymmetry is in thermodynamics, and comments on the question whether a time-symmetric formulation of the Second Law is possible.
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  • Is - kTr( ln ) the entropy in quantum mechanics.Orly Shenker - 1999 - British Journal for the Philosophy of Science 50 (1):33-48.
    In quantum mechanics, the expression for entropy is usually taken to be -kTr(ln), where is the density matrix. The convention first appears in Von Neumann's Mathematical Foundations of Quantum Mechanics. The argument given there to justify this convention is the only one hitherto offered. All the arguments in the field refer to it at one point or another. Here this argument is shown to be invalid. Moreover, it is shown that, if entropy is -kTr(ln), then perpetual motion machines are possible. (...)
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  • The foundations of quantum mechanics and the approach to thermodynamic equilibrium.David Z. Albert - 1994 - Erkenntnis 41 (2):191-206.
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