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Publication details

Title:
Autocorrelation function of eigenstates in chaotic and mixed systems
Authors:
A. Bäcker and R. Schubert
Journal:
J. Phys. A 35 (2002) 539-564
Abstract:
We study the autocorrelation function of different types of eigenfunctions in quantum mechanical systems with either chaotic or mixed classical limits. We obtain an expansion of the autocorrelation function in terms of the correlation length. For localized states, like bouncing ball modes or states living on tori, a simple model using only classical input gives good agreement with the exact result. In particular, a prediction for irregular eigenfunctions in mixed systems is derived and tested. For chaotic systems, the expansion of the autocorrelation function can be used to test quantum ergodicity on different length scales.
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Please refer to the above published version.
(The preprint version of this article can be obtained as BRIMS Report HPL-BRIMS-00-11, April 2001, 30 pp. [.ps.gz] (1.2 MB compressed, 5 MB uncompressed).)

Illustration

For eigenfunctions which localize on an elliptic orbit the expansion of the autocorrelation function gives a prediction in the semiclassical limit:
Autocorrelation function, elliptic state



For irregular states in mixed systems one obtains a prediction for the autocorrelation function which is substantially different from the J0(r) behaviour in ergodic systems. The figure below shows an eigenfunction in the limaçon billiard (ε=0.3, approx 130516th state), the corresponding Poincaré Husimi representation and the classical angular momentum distribution and finally the resulting autocorrelation function.
Autocorrelation function, irregular state


Thus, even for irregular states the autocorrelation function clearly differs from the J0(r) behaviour!

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