Tracking unstable phenomena in chaotic laser experiments: Extending regions of stability in a multimode laser

Z. Gills, Christina Iwata, R. Roy, I. Schwartz, Ioana Triandaf
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Abstract

Recently, experimental systems which exhibit chaos have been controlled using techniques such as OGY [1] and the related occasional proportional feedback, OPF [2]. The methods have been able to stabilize both low dimensional experiments, such as electronic circuits [2] as well as high dimensional multimode chaotic lasers [3]. Controlling a chaotic system consists of stabilizing an unstable steady state or periodic orbit by having the system perform small amplitude fluctuations about some fixed parameter value. The OPF method is implemented by choosing the fluctuations so that the system is brought closer to the unstable orbit of interest. In the OGY method, the fluctuations are chosen so that the iterates fall on the stable manifold of the unstable orbit, thus keeping the dynamics in the neighborhood of the point of interest in phase space. Both methods are clearly related [4].
混沌激光实验中不稳定现象的跟踪:多模激光器稳定区域的扩展
最近,出现混沌的实验系统已经使用诸如OGY b[1]和相关的偶次比例反馈OPF b[2]等技术进行控制。该方法既可以稳定低维实验,如电子电路[2],也可以稳定高维多模混沌激光器[3]。混沌系统的控制包括通过使系统围绕某一固定参数值进行小幅度波动来稳定不稳定的稳态或周期轨道。OPF方法通过选择波动来实现,使系统更接近目标不稳定轨道。在该方法中,选择波动使迭代落在不稳定轨道的稳定流形上,从而使动力学保持在相空间兴趣点附近。这两种方法显然是相关的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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