Chaotic stochastic resonance in Mackey-Glass equations
Eiki Kojima, Yuzuru Sato

TL;DR
This paper introduces chaotic stochastic resonance in nonlinear stochastic systems, showing it as a universal phenomenon characterized by coexistence of resonance and chaos, with positive Lyapunov exponents.
Contribution
It identifies and characterizes chaotic stochastic resonance in the Mackey-Glass equation and demonstrates its universality across various nonlinear systems.
Findings
Chaotic SR occurs with positive Lyapunov exponents.
Chaotic SR observed in Mackey-Glass, Duffing, and FitzHugh-Nagumo equations.
Chaotic SR differs from classical SR by involving chaos and strange attractors.
Abstract
Stochastic resonance (SR) manifests as switching dynamics between two quasi-stationary states in the stochastic Mackey-Glass equation. We identify chaotic SR, arising from the coexistence of resonance and chaos in stochastic dynamics. In contrast to classical SR, which is described by a random point attractor with a negative largest Lyapunov exponent, chaotic SR is described by a random strange attractor with a positive largest Lyapunov exponent. We observe chaotic SR in the Mackey-Glass equation as well as chaotic SR in the Duffing equation and the underdamped FitzHugh-Nagumo equation, demonstrating the universality of this phenomenon across a broad class of strongly nonlinear random dynamical systems.
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Taxonomy
TopicsStochastic processes and statistical mechanics · advanced mathematical theories · Stochastic processes and financial applications
