Fractal snapshot components in chaos induced by strong noise.

In systems exhibiting transient chaos in coexistence with periodic attractors, the inclusion of weak noise might give rise to noise-induced chaotic attractors. When the noise amplitude exceeds a critical value, an extended attractor appears along the fractal unstable manifold of the underlying nonattracting chaotic set. A further increase of noise leads to a fuzzy nonfractal pattern. By means of the concept of snapshot attractors and random maps, we point out that the fuzzy pattern can be decomposed into well-defined fractal components, the snapshot attractors belonging to a given realization of the noise and generated by following an ensemble of noisy trajectories. The pattern of the snapshot attractor and its characteristic numbers, such as the finite time Lyapunov exponents and numerically evaluated fractal dimensions, change continuously in time. We find that this temporal fluctuation is a robust property of the system which hardly changes with increasing ensemble size. The validity of the Kaplan-Yorke formula is also investigated. A superposition of about 100 snapshot attractors provides a good approximant to the fuzzy noise-induced attractor at the same noise strength.

[1]  Grebogi,et al.  Scaling behavior of transition to chaos in quasiperiodically driven dynamical systems. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[2]  Edward Ott,et al.  Particles Floating on a Moving Fluid: A Dynamically Comprehensible Physical Fractal , 1993, Science.

[3]  H. B. Wilson,et al.  Chaotic stochasticity: a ubiquitous source of unpredictability in epidemics , 1991, Proceedings of the Royal Society of London. Series B: Biological Sciences.

[4]  Schieve,et al.  Homoclinic chaos in systems perturbed by weak Langevin noise. , 1990, Physical review. A, Atomic, molecular, and optical physics.

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

[6]  Y. Lai,et al.  Experimental characterization of transition to chaos in the presence of noise. , 2003, Physical review letters.

[7]  Tamás Tél,et al.  Dynamics of "leaking" Hamiltonian systems. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[8]  Ira B. Schwartz,et al.  Bi-instability and the global role of unstable resonant orbits in a driven laser , 2000 .

[9]  Michael Ghil,et al.  Stochastic climate dynamics: Random attractors and time-dependent invariant measures , 2011 .

[10]  Ying-Cheng Lai,et al.  Characterization of nonstationary chaotic systems. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[11]  Transient fractal behavior in snapshot attractors of driven chaotic systems. , 1999, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[12]  Hu,et al.  Noise and chaos in a fractal basin boundary regime of a Josephson junction. , 1985, Physical review letters.

[13]  C. Grebogi,et al.  Escape from attracting sets in randomly perturbed systems. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.

[14]  Ira B Schwartz,et al.  Phase-space transport of stochastic chaos in population dynamics of virus spread. , 2002, Physical review letters.

[15]  Eric Forgoston,et al.  Accurate noise projection for reduced stochastic epidemic models , 2009, Chaos.

[16]  Nonuniform Chaotic Dynamics and Effects of Noise in Biochemical Systems , 1987 .

[17]  Ying-Cheng Lai,et al.  Quasipotential approach to critical scaling in noise-induced chaos. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.

[18]  Thomas M. Antonsen,et al.  Modeling fractal entrainment sets of tracers advected by chaotic temporally irregular fluid flows using random maps , 1997 .

[19]  Pikovsky Comment on "Noisy uncoupled chaotic map ensembles violate the law of large numbers" , 1993, Physical review letters.

[20]  A. Vulpiani,et al.  Predictability: a way to characterize complexity , 2001, nlin/0101029.

[21]  Michael Ghil,et al.  Climate dynamics and fluid mechanics: Natural variability and related uncertainties , 2008, 1006.2864.

[22]  Stephen P. Ellner,et al.  When can noise induce chaos and why does it matter: a critique , 2005 .

[23]  E. Altmann,et al.  Noise-enhanced trapping in chaotic scattering. , 2010, Physical review letters.

[24]  J. Yorke,et al.  Fractal basin boundaries , 1985 .

[25]  E. Ott Chaos in Dynamical Systems: Contents , 1993 .

[26]  Celso Grebogi,et al.  Reactive particles in random flows. , 2004, Physical review letters.

[27]  Ying-Cheng Lai,et al.  Noise-induced unstable dimension variability and transition to chaos in random dynamical systems. , 2003, Physical review. E, Statistical, nonlinear, and soft matter physics.

[28]  Michael Brereton,et al.  A Modern Course in Statistical Physics , 1981 .

[29]  Chen,et al.  Transition to chaos for random dynamical systems. , 1990, Physical review letters.

[30]  L Billings,et al.  Exciting chaos with noise: unexpected dynamics in epidemic outbreaks , 2002, Journal of mathematical biology.

[31]  Tamás Tél,et al.  Advection in chaotically time-dependent open flows , 1998 .

[32]  Grebogi,et al.  Multifractal properties of snapshot attractors of random maps. , 1990, Physical review. A, Atomic, molecular, and optical physics.

[33]  Ying-Cheng Lai,et al.  Noise-Induced Chaos: a Consequence of Long Deterministic Transients , 2008, Int. J. Bifurc. Chaos.

[34]  Lai-Sang Young,et al.  Dimension formula for random transformations , 1988 .

[35]  E. Bollt,et al.  A manifold independent approach to understanding transport in stochastic dynamical systems , 2002 .

[36]  W. Marsden I and J , 2012 .