2012
DOI: 10.1103/physreve.85.026216
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Optimal phase description of chaotic oscillators

Abstract: We introduce an optimal phase description of chaotic oscillations by generalizing the concept of isochrones. On chaotic attractors possessing a general phase description, we define the optimal isophases as Poincaré surfaces showing return times as constant as possible. The dynamics of the resultant optimal phase is maximally decoupled of the amplitude dynamics, and provides a proper description of phase resetting of chaotic oscillations. The method is illustrated with the Rössler and Lorenz systems.

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Cited by 28 publications
(24 citation statements)
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“…Nevertheless, methods that allow one to effectively reduce the influence of these and other confounding variables are still missing. It remains to be shown whether recently proposed methods for an improved phase extraction 78,79 or specifically designed surrogate techniques can be of help to better delineate functional from spurious interactions between dynamical systems.…”
Section: Resultsmentioning
confidence: 99%
“…Nevertheless, methods that allow one to effectively reduce the influence of these and other confounding variables are still missing. It remains to be shown whether recently proposed methods for an improved phase extraction 78,79 or specifically designed surrogate techniques can be of help to better delineate functional from spurious interactions between dynamical systems.…”
Section: Resultsmentioning
confidence: 99%
“…Finally, we emphasize that our corresponding considerations are closely related to the problem of finding an optimal phase definition for a chaotic system. [80][81][82][83][84] Achieving a better understanding of the linkage between both geometric and optimal phase approaches will be a subject of future research. …”
Section: -11mentioning
confidence: 99%
“…Many chaotic attractors allow a representation in terms of amplitudes and phases [3,15,16], but because the phase generally performs a chaos-induced diffusion, isophases in the strict sense do not exist. Recently, description of chaotic oscillations in terms of approximate isophases has been suggested [17]. With noise, the return times to a Poincaré surface of a strange attractor can be defined in the averaged sense only, and in this respect there is no difference between chaotic and regular deterministic oscillators.…”
mentioning
confidence: 99%