Laminar chaotic saddle within a turbulent attractor

Intermittent switchings between weakly chaotic (laminar) and strongly chaotic (bursty) states are often observed in systems with high-dimensional chaotic attractors, such as fluid turbulence. They differ from the intermittency of a low-dimensional system accompanied by the stability change of a fixed point or a periodic orbit in that the intermittency of a high-dimensional system tends to appear in a wide range of parameters. This paper considers a case where the skeleton of a laminar state L exists as a proper chaotic subset S of a chaotic attractor X, that is, S⊊X. We characterize such a laminar state L by a chaotic saddle S, which is densely filled with periodic orbits of different numbers of unstable directions. This study demonstrates the presence of chaotic saddles underlying intermittency in fluid turbulence and phase synchronization. Furthermore, we confirm that chaotic saddles persist for a wide range of parameters. Also, a kind of phase synchronization turns out to occur in the turbulent model.

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Publication Details

Journal
Physical review. E
Published
2024-11-07
DOI
https://doi.org/10.1103/physreve.110.l052202
Primary Topic
Chaos control and synchronization
Type
article
Field-Weighted Citation Impact
0.00

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article

Laminar chaotic saddle within a turbulent attractor

Yoshitaka Saiki, James A. Yorke, Hibiki Kato, Miki U. Kobayashi
Physical review. E
Chaos control and synchronization
article

Laminar chaotic saddle within a turbulent attractor

Yoshitaka Saiki, James A. Yorke, Hibiki Kato, Miki U. Kobayashi
article en

Abstract

Intermittent switchings between weakly chaotic (laminar) and strongly chaotic (bursty) states are often observed in systems with high-dimensional chaotic attractors, such as fluid turbulence. They differ from the intermittency of a low-dimensional system accompanied by the stability change of a fixed point or a periodic orbit in that the intermittency of a high-dimensional system tends to appear in a wide range of parameters. This paper considers a case where the skeleton of a laminar state L exists as a proper chaotic subset S of a chaotic attractor X, that is, S⊊X. We characterize such a laminar state L by a chaotic saddle S, which is densely filled with periodic orbits of different numbers of unstable directions. This study demonstrates the presence of chaotic saddles underlying intermittency in fluid turbulence and phase synchronization. Furthermore, we confirm that chaotic saddles persist for a wide range of parameters. Also, a kind of phase synchronization turns out to occur in the turbulent model.

Physical review. EVol. 110(5)
Hitotsubashi University (JP), Rissho University (JP), University of Maryland, College Park (US)
Japan Society for the Promotion of Science
Openalex Percentile: Top 81%
Chaos control and synchronization
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Laminar chaotic saddle within a turbulent attractor — Yoshitaka Saiki, James A. Yorke, et al. · Physical review. E (2024) | TGRS Research Map | TGRS