Transition-Strength Fluctuations and the Onset of Chaotic Motion

Y. Alhassid and R. D. Levine
Phys. Rev. Lett. 57, 2879 – Published 8 December 1986
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Abstract

The maximum-entropy formalism is used to characterize the fluctuations in transition strengths for a bound quantum-mechanical system. In the chaotic limit only one, ever present, sum rule is required as a constraint. The resulting distribution is that of Porter and Thomas, which can also be derived from random-matrix theory. For nonchaotic systems the distribution of transition strengths has a lower entropy. A possible additional constraint, operative during the onset of chaos, is proposed. The distribution of maximal entropy subject to both constraints accords with computed intensities in a system of two degrees of freedom.

  • Received 1 May 1986

DOI:https://doi.org/10.1103/PhysRevLett.57.2879

©1986 American Physical Society

Authors & Affiliations

Y. Alhassid

  • A. W. Wright Nuclear Structure Laboratory, Yale University, New Haven, Connecticut 06511

R. D. Levine

  • The Fritz Haber Research Center for Molecular Dynamics, The Hebrew University, Jerusalem 91904, Israel

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Vol. 57, Iss. 23 — 8 December 1986

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