TRANSVERSE INSTABILITY AND RIDDLED BASINS IN A SYSTEM OF TWO COUPLED LOGISTIC MAPS

Riddled basins denote a characteristic type of fractal domain of attraction that can arise when a chaotic motion is restricted to an invariant subspace of total phase space. An example is the synchronized motion of two identical chaotic oscillators. The paper examines the conditions for the appearance of such basins for a system of two symmetrically coupled logistic maps. We determine the regions in parameter plane where the transverse Lyapunov exponent is negative. The bifurcation curves for the transverse destabilization of lowperiodic orbits embedded in the chaotic attractor are obtained, and we follow the changes in the attractor and its basin of attraction when scanning across the riddling and blowout bifurcations. It is shown that the appearance of transversely unstable orbits does not necessarily lead to an observable basin riddling, and that the loss of weak stability~when the transverse Lyapunov exponent becomes positive ! does not necessarily destroy the basin of attraction. Instead, the symmetry of the synchronized state may break, and the attractor may spread into two-dimensional phase space. @S1063-651X~98!05303-3#

[1]  M. Jakobson Absolutely continuous invariant measures for one-parameter families of one-dimensional maps , 1981 .

[2]  J. Yorke,et al.  CHAOTIC ATTRACTORS IN CRISIS , 1982 .

[3]  H. Fujisaka,et al.  Stability Theory of Synchronized Motion in Coupled-Oscillator Systems , 1983 .

[4]  Arkady Pikovsky,et al.  On the interaction of strange attractors , 1984 .

[5]  J. Milnor On the concept of attractor , 1985 .

[6]  Hirokazu Fujisaka,et al.  Stability Theory of Synchronized Motion in Coupled-Oscillator Systems. IV ---Instability of Synchronized Chaos and New Intermittency--- , 1986 .

[7]  Celso Grebogi,et al.  Basin boundary metamorphoses: changes in accessible boundary orbits , 1987 .

[8]  Carroll,et al.  Synchronization in chaotic systems. , 1990, Physical review letters.

[9]  P. Grassberger,et al.  Symmetry breaking bifurcation for coupled chaotic attractors , 1991 .

[10]  James A. Yorke,et al.  Analysis of a procedure for finding numerical trajectories close to chaotic saddle hyperbolic sets , 1991, Ergodic Theory and Dynamical Systems.

[11]  Edward Ott,et al.  Fractal distribution of floaters on a fluid surface and the transition to chaos for random maps , 1991 .

[12]  D. Frail,et al.  Identification of PSR1758 – 23 as a runaway pulsar from the supernova remnant W28 , 1993, Nature.

[13]  Spiegel,et al.  On-off intermittency: A mechanism for bursting. , 1993, Physical review letters.

[14]  Ott,et al.  Scaling behavior of chaotic systems with riddled basins. , 1993, Physical review letters.

[15]  Laura Gardini,et al.  A DOUBLE LOGISTIC MAP , 1994 .

[16]  I. Stewart,et al.  Bubbling of attractors and synchronisation of chaotic oscillators , 1994 .

[17]  L. Chua,et al.  A UNIFIED FRAMEWORK FOR SYNCHRONIZATION AND CONTROL OF DYNAMICAL SYSTEMS , 1994 .

[18]  E. Ott,et al.  Blowout bifurcations: the occurrence of riddled basins and on-off intermittency , 1994 .

[19]  Carroll,et al.  Desynchronization by periodic orbits. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[20]  Ott,et al.  Optimal periodic orbits of chaotic systems. , 1996, Physical review letters.

[21]  Nikolai F. Rulkov,et al.  Images of synchronized chaos: Experiments with circuits. , 1996, Chaos.

[22]  Intermingled basins for the triangle map , 1996, Ergodic Theory and Dynamical Systems.

[23]  Kapitaniak,et al.  Different types of chaos synchronization in two coupled piecewise linear maps. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[24]  I. Stewart,et al.  From attractor to chaotic saddle: a tale of transverse instability , 1996 .

[25]  Grebogi,et al.  Riddling Bifurcation in Chaotic Dynamical Systems. , 1996, Physical review letters.