Abstract
A common approach to quantum physics is enshrouded in a jargon which treats state vectors as attributes of physical systems and the concept of state preparation as a filtration scheme wherein a process involving measurement selects from a primordial assembly of systems those bearing some prescribed vector of interest. By contrast, the empirical experiences with which quantum theory is actually concerned relate measurement and preparation in quite an opposite manner. Reproducible preparation schemes are logically and temporally anterior to measurement acts. Measurement extracts numbers from systems prepared in a specified manner; these data are then regularized by the theory by means of a state concept which is in turn used to characterize succinctly the given mode of preparation. The present paper offers, in a simple spin model, a method for determining the quantum state that represents any reproducible preparation.
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J. L. Park,Phil. Sci. 35, 205 (1968);35, 389 (1968).
J. L. Park,Am. J. Phys. 36, 211 (1968).
H. Margenau,Phil. Sci. 4, 352 (1937).
J. L. Park,Scientia CIII, 569 (1968).
E. Feenberg, Thesis, Harvard University (1933); E. C. Kemble,Fundamental Principles of Quantum Mechanics (McGraw-Hill, New York, 1937), p. 71.
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This investigation was supported in part by funds provided by the Graduate School Research Fund.
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Band, W., Park, J.L. The empirical determination of quantum states. Found Phys 1, 133–144 (1970). https://doi.org/10.1007/BF00708723
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DOI: https://doi.org/10.1007/BF00708723