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  1. Why Gibbs Phase Averages Work—The Role of Ergodic Theory.David B. Malament & Sandy L. Zabell - 1980 - Philosophy of Science 47 (3):339-349.
    We propose an "explanation scheme" for why the Gibbs phase average technique in classical equilibrium statistical mechanics works. Our account emphasizes the importance of the Khinchin-Lanford dispersion theorems. We suggest that ergodicity does play a role, but not the one usually assigned to it.
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  • Exorcist XIV: The Wrath of Maxwell’s Demon. Part I. From Maxwell to Szilard.John Earman & John D. Norton - 1998 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 29 (4):435-471.
    In this first part of a two-part paper, we describe efforts in the early decades of this century to restrict the extent of violations of the Second Law of thermodynamics that were brought to light by the rise of the kinetic theory and the identification of fluctuation phenomena. We show how these efforts mutated into Szilard’s proposal that Maxwell’s Demon is exorcised by proper attention to the entropy costs associated with the Demon’s memory and information acquisition. In the second part (...)
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  • Maxwell’s Demon and Baron Munchausen: Free Will as a Perpetuum Mobile.Orly R. Shenker - 1998 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 30 (3):347-372.
    This paper argues that the idea of a Maxwellian Demon presupposes a notion of non-physical free will. The author has changed her mind in this point later on and now thinks that Mawellian Demons are compatible with mechanics; see her paper on this from 2010 and book from 2012.
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  • Locality, factorizability, and the Maxwell Boltzmann distribution.Itamar Pitowsky & Noam Shoresh - 1996 - Foundations of Physics 26 (9):1231-1242.
    A classical gas at equilibrium satisfies the locality conditionif the correlations between local fluctuations at a pair of remote small regions diminish in the thermodynamic limit. The gas satisfies a strong locality conditionif the local fluctuations at any number of remote locations have no (pair, triple, quadruple....) correlations among them in the thermodynamic limit. We prove that locality is equivalent to a certain factorizability condition on the distribution function. The analogous quantum condition fails in the case of a freeBose gas. (...)
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