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全局耦合噪声动力学元件的集体相位还原

Collective phase reduction of globally coupled noisy dynamical elements.

作者信息

Kawamura Yoji

机构信息

Department of Mathematical Science and Advanced Technology, Japan Agency for Marine-Earth Science and Technology, Yokohama 236-0001, Japan and Research and Development Center for Marine Biosciences, Japan Agency for Marine-Earth Science and Technology, Yokosuka 237-0061, Japan.

出版信息

Phys Rev E. 2017 Mar;95(3-1):032225. doi: 10.1103/PhysRevE.95.032225. Epub 2017 Mar 31.

Abstract

We formulate a theory for the collective phase reduction of globally coupled noisy dynamical elements exhibiting macroscopic rhythms. We first transform the Langevin-type equation that represents a group of globally coupled noisy dynamical elements into the corresponding nonlinear Fokker-Planck equation and then develop the phase reduction method for limit-cycle solutions to the nonlinear Fokker-Planck equation. The theory enables us to describe the collective dynamics of a group of globally coupled noisy dynamical elements by a single degree of freedom called the collective phase. As long as the group collectively exhibits macroscopic rhythms, the theory is applicable even when the coupling and noise are strong; it is also independent of the assumption that each element of the group is a self-sustained oscillator. We also provide a simple and accurate numerical algorithm for the collective phase description method and numerically illustrate the theory using a group of globally coupled noisy FitzHugh-Nagumo elements.

摘要

我们为呈现宏观节律的全局耦合噪声动力学元件的集体相位约化制定了一种理论。我们首先将表示一组全局耦合噪声动力学元件的朗之万型方程转化为相应的非线性福克 - 普朗克方程,然后针对非线性福克 - 普朗克方程的极限环解开发相位约化方法。该理论使我们能够通过一个称为集体相位的单自由度来描述一组全局耦合噪声动力学元件的集体动力学。只要该组集体呈现宏观节律,即使耦合和噪声很强,该理论也适用;它也独立于该组中每个元件都是自维持振荡器的假设。我们还为集体相位描述方法提供了一种简单而准确的数值算法,并使用一组全局耦合噪声菲茨休 - 纳古莫元件对该理论进行了数值说明。

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