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  1. Quantum Mechanics: Historical Contingency and the Copenhagen Hegemony.James T. Cushing - 1994 - University of Chicago Press.
    Why does one theory "succeed" while another, possibly clearer interpretation, fails? By exploring two observationally equivalent yet conceptually incompatible views of quantum mechanics, James T. Cushing shows how historical contingency can be crucial to determining a theory's construction and its position among competing views. Since the late 1920s, the theory formulated by Niels Bohr and his colleagues at Copenhagen has been the dominant interpretation of quantum mechanics. Yet an alternative interpretation, rooted in the work of Louis de Broglie in the (...)
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  • Mathematical Rigor in Physics: Putting Exact Results in Their Place.Axel Gelfert - 2005 - Philosophy of Science 72 (5):723-738.
    The present paper examines the role of exact results in the theory of many‐body physics, and specifically the example of the Mermin‐Wagner theorem, a rigorous result concerning the absence of phase transitions in low‐dimensional systems. While the theorem has been shown to hold for a wide range of many‐body models, it is frequently ‘violated’ by results derived from the same models using numerical techniques. This raises the question of how scientists regulate their theoretical commitments in such cases, given that the (...)
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  • The Ehrenfest Classification of Phase Transitions: Introduction and Evolution.Gregg Jaeger - 1998 - Archive for History of Exact Sciences 53 (1):51-81.
    The first classification of general types of transition between phases of matter, introduced by Paul Ehrenfest in 1933, lies at a crossroads in the thermodynamical study of critical phenomena. It arose following the discovery in 1932 of a suprising new phase transition in liquid helium, the “lambda transition,” when W. H. Keesom and coworkers in Leiden, Holland observed a λhaped “jump” discontinuity in the curve giving the temperature dependence of the specific heat of helium at a critical value. This apparent (...)
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  • History of the Lenz-Ising Model 1920–1950: From Ferromagnetic to Cooperative Phenomena.Martin Niss - 2005 - Archive for History of Exact Sciences 59 (3):267-318.
    Abstract.I chart the considerable changes in the status and conception of the Lenz-Ising model from 1920 to 1950 in terms of three phases: In the early 1920s, Lenz and Ising introduced the model in the field of ferromagnetism. Based on an exact derivation, Ising concluded that it is incapable of displaying ferromagnetic behavior, a result he erroneously extended to three dimensions. In the next phase, Lenz and Ising’s contemporaries rejected the model as a representation of ferromagnetic materials because of its (...)
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  • Introduction.Mitchell Green & John N. Williams - 2007 - In Mitchell S. Green & John N. Williams (eds.), Moore’s Paradox: New Essays on Belief, Rationality, and the First Person. New York: Oxford University Press.
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  • The calculation of lattice constants in crystal statistics.C. Domb & M. F. Sykes - 1957 - Philosophical Magazine 2 (18):733-749.
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  • (2 other versions)Quantum Mechanics: Historical Contingency and the Copenhagen Hegemony.James T. Cushing - 1998 - Philosophical Quarterly 48 (191):250-252.
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  • (2 other versions)Quantum Mechanics. Historical Contingency and the Copenhagen Hegemony.James T. Cushing - 1996 - Journal for General Philosophy of Science / Zeitschrift für Allgemeine Wissenschaftstheorie 27 (2):353-358.
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  • Some magnetic properties of the ising model.D. M. Burley - 1960 - Philosophical Magazine 5 (57):909-919.
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