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  1. Fixed past and uncertain future: A single-time covariant quantum particle mechanics. [REVIEW]H. Pierre Noyes - 1975 - Foundations of Physics 5 (1):37-43.
    A covariant quantum mechanics for systems of finite-mass particles at finite energy follows from interpreting as Wick-Yukawa fluctuations in particle number the quantum fluctuations which are needed by Phipps to understand measurement theory and by Gyftopoulos to understand the second law of thermodynamics. The dynamical one-variable equations require as input the (N − 1)-particle transition matrices and an N-N vertex or coupling constants at three-particle vertices.
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  • The Logic of Modern Physics.Percy Williams Bridgman - 1927 - New York, NY, USA: Arno Press.
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  • (1 other version)The Relativity of Physical Size.T. E. Phipps - 1969 - Dialectica 23 (3‐4):189-215.
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  • Time asymmetry and quantum equations of motion.T. E. Phipps - 1973 - Foundations of Physics 3 (4):435-455.
    Accepted quantum description is stochastic, yet history is nonstochastic, i.e., not representable by a probability distribution. Therefore ordinary quantum mechanics is unsuited to describe history. This is a limitation of the accepted quantum theory, rather than a failing of mechanics in general. To remove the limitation, it would be desirable to find a form of quantum mechanics that describes the future stochastically and the past nonstochastically. For this purpose it proves sufficient to introduce into quantum mechanics, by means of a (...)
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