Theory of Hidden Variables

David Kershaw
Phys. Rev. 136, B1850 – Published 21 December 1964
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Abstract

It is shown that the stationary states of the nonrelativistic Schrödinger's equation are just the stationary states of a classical-mechanical system which is subject to random submicroscopic fluctuations of position. The proof covers the case (1) of a single particle moving in a potential, and (2) of two particles interacting through a potential V(x1x2). The results can be easily generalized to the case of n interacting particles.

  • Received 1 July 1964

DOI:https://doi.org/10.1103/PhysRev.136.B1850

©1964 American Physical Society

Authors & Affiliations

David Kershaw

  • Harvard College, Cambridge, Massachusetts

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Issue

Vol. 136, Iss. 6B — December 1964

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