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Phys. Rev. 136, B1850–B1856 (1964)

Theory of Hidden Variables

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David Kershaw
Harvard College, Cambridge, Massachusetts

Received 1 July 1964; published in the issue dated December 1964

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(x1-x2). The results can be easily generalized to the case of n interacting particles.

© 1964 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRev.136.B1850
DOI:
10.1103/PhysRev.136.B1850
PACS: