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  1.  51
    Bivariate probability densities with given margins.Peter D. Finch & Roman Groblicki - 1984 - Foundations of Physics 14 (6):549-552.
    We determine the bivariate probability densities with specified margins and show that the Cohen-Zaparovanny class of positive phase-space density functions, with the quantum mechanical marginal distributions of position and momentum, contains all such densities.
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  2.  39
    Classical probability and the quantum mechanical trace formulation for expectations.Peter D. Finch - 1982 - Foundations of Physics 12 (4):327-345.
    The trace formulation of quantum mechanical expectations is derived in a classical deterministic setting by averaging over an assembly of states. Interference of probabilities is discussed and its usual Hilbert space formulation is questioned. Nevertheless, it is shown that the observable predictions of quantum statics remain unchanged in the framework developed here.
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  3.  24
    On the role of description in statistical enquiry.Peter D. Finch - 1981 - British Journal for the Philosophy of Science 32 (2):127-144.
  4.  76
    State assembles and the Bell-Wigner locality argument.Peter D. Finch - 1982 - Foundations of Physics 12 (8):759-764.
    The Bell-Wigner locality argument is shown to be a special case of the nonexistence of certain state assembles with preassigned densities when there are restrictions on the allowable states.
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  5.  69
    The operator formalism of quantum mechanics from the viewpoint of short disturbances in nonrelativistic classical motion.Peter D. Finch - 1984 - Foundations of Physics 14 (4):281-306.
    The effect of short disturbances on nonrelativistic motion is formulated in terms of operators. Analogies with quantum mechanics are developed and some disparities noted. For the one-dimensional particle we obtain analogues of the de Broglie wave commonly associated with particle motion, Heisenberg's commutation relation, Schrödinger's equation, and the statistical interpretation. Whether these results have any bearing on quantum mechanics itself is left an open question.
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