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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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  • Discrete Excitation Spectrum of a Classical Harmonic Oscillator in Zero-Point Radiation.Wayne Cheng-Wei Huang & Herman Batelaan - 2015 - Foundations of Physics 45 (3):333-353.
    We report that upon excitation by a single pulse, a classical harmonic oscillator immersed in the classical electromagnetic zero-point radiation exhibits a discrete harmonic spectrum in agreement with that of its quantum counterpart. This result is interesting in view of the fact that the vacuum field is needed in the classical calculation to obtain the agreement.
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  • Quantum ontology without speculation.Matthias Egg - 2021 - European Journal for Philosophy of Science 11 (1):1-26.
    Existing proposals concerning the ontology of quantum mechanics either involve speculation that goes beyond the scientific evidence or abandon realism about large parts of QM. This paper proposes a way out of this dilemma, by showing that QM as it is formulated in standard textbooks allows for a much more substantive ontological commitment than is usually acknowledged. For this purpose, I defend a non-fundamentalist approach to ontology, which is then applied to various aspects of QM. In particular, I will defend (...)
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  • Bipartite Entanglement Induced by a Common Background (Zero-Point) Radiation Field.A. Valdés-Hernández, L. de la Peña & A. M. Cetto - 2011 - Foundations of Physics 41 (5):843-862.
    This paper deals with an (otherwise classical) two-(non-interacting) particle system immersed in a common stochastic zero-point radiation field. The treatment is an extension of the one-particle case for which it has been shown that the quantum properties of the particle emerge from its interaction with the background field under stationary and ergodic conditions. In the present case we show that non-classical correlations—describable only in terms of entanglement—arise between the (nearby) particles whenever both of them resonate to a common frequency of (...)
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  • Quantum Mechanics: Historical Contingency and the Copenhagen Hegemony.James T. Cushing - 1998 - Philosophical Quarterly 48 (191):250-252.
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  • 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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  • The physical meaning of quantization.Emilio Santos - 1992 - Foundations of Physics 22 (3):371-379.
    After analyzing the difficulties for a local realistic interpretation of quantum theory, it is argued that such an interpretation might be possible if some new postulates are added to the standard ones. We propose a stochastic interpretation of quantum theory, which involves the need of joint probability distributions for all relevant observables. The well known problems for the existence of joint distributions are solved by assuming that neither all Hermitian operators correspond to observables nor all density matrices represent physical states. (...)
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  • Stochastic theory for classical and quantum mechanical systems.L. de la Peña & A. M. Cetto - 1975 - Foundations of Physics 5 (2):355-370.
    We formulate from first principles a theory of stochastic processes in configuration space. The fundamental equations of the theory are an equation of motion which generalizes Newton's second law and an equation which expresses the condition of conservation of matter. Two types of stochastic motion are possible, both described by the same general equations, but leading in one case to classical Brownian motion behavior and in the other to quantum mechanical behavior. The Schrödinger equation, which is derived here with no (...)
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