Bubbling transition

Shankar C. Venkataramani, Brian R. Hunt, and Edward Ott
Phys. Rev. E 54, 1346 – Published 1 August 1996
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Abstract

Recently, physically important examples of dynamical systems that have a chaotic attractor embedded in an invariant submanifold have been pointed out, and the unusual dynamical consequences of this situation have been studied. As a parameter ε of the system is increased, a periodic orbit embedded in the attractor on the invariant manifold can become unstable for perturbations transverse to the invariant manifold. This bifurcation is called the bubbling transition, and it can lead to the occurrence of a recently discovered, new kind of basin of attraction, called a riddled basin. In this paper we study the effects of noise and asymmetry on the bubbling transition. We find that, in the presence of noise or asymmetry, the attractor is replaced either by a chaotic transient or an intermittently bursting time evolution, and we derive scaling relations, valid near the bubbling transition, for the characteristic time (i.e., the average chaotic transient lifetime or the average interburst time interval) as a function of the strength of the asymmetry and the variance of the additive noise. We also present numerical evidence for the predicted scalings. © 1996 The American Physical Society.

  • Received 25 April 1996

DOI:https://doi.org/10.1103/PhysRevE.54.1346

©1996 American Physical Society

Authors & Affiliations

Shankar C. Venkataramani, Brian R. Hunt, and Edward Ott

  • Department of Physics and Institute for Plasma Research, University of Maryland, College Park, Maryland 20742
  • Institute for Physical Science and Technology, University of Maryland, College Park, Maryland 20742
  • Department of Electrical Engineering and Institute for Systems Research, University of Maryland, College Park, Maryland 20742

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Vol. 54, Iss. 2 — August 1996

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