Quantum and classical Liouville dynamics of the anharmonic oscillator

G. J. Milburn
Phys. Rev. A 33, 674 – Published 1 January 1986
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Abstract

We consider the dynamics of a quantum joint phase-space probability density in an exactly solvable model. The density is defined to be a true (i.e., positive) probability distribution for approximate (and thus simultaneously measurable) position and momentum variables. The dynamics of the quantum density is governed by a second-order partial-differential equation with non-positive-definite second-order coefficients. The quantum dynamics is contrasted with the dynamics of a similar joint density in a classical description. The non-positive-definite second-order terms in the quantum evolution equation, not present in the classical case, are responsible for quantum recurrences and prevent the appearance of fine-scale-structure ‘‘whorls’’ predicted in a classical description. The generation of ‘‘squeezing’’ in the model is also discussed.

  • Received 29 April 1985

DOI:https://doi.org/10.1103/PhysRevA.33.674

©1986 American Physical Society

Authors & Affiliations

G. J. Milburn

  • Blackett Laboratory, Imperial College, London SW7 2BZ, England

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Issue

Vol. 33, Iss. 1 — January 1986

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