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多态跳跃间歇性的控制

Control of multistate hopping intermittency.

作者信息

Goswami B K

机构信息

Laser and Plasma Technology Division, Bhabha Atomic Research Centre, Mumbai 400085, India.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2008 Dec;78(6 Pt 2):066208. doi: 10.1103/PhysRevE.78.066208. Epub 2008 Dec 11.

DOI:10.1103/PhysRevE.78.066208
PMID:19256926
Abstract

In multistable regimes, noise can create "multistate hopping intermittency," i.e., intermittent transitions among coexisting stable attractors. We demonstrate that a small periodic perturbation can significantly control such hopping intermittency. By "control" we imply a qualitative change in the probability distribution of occupation in the phase space around the stable attractors. In other words, if the uncontrolled system exhibits a preference to stay around a given attractor (say " A ") in comparison to another attractor (say " B "), the control perturbation creates a contrasting scenario so that attractor B is most frequently visited and consequently, the occupation probability becomes maximum around B instead of A . The control perturbation works in the following way: It destroys attractor A by boundary crisis while attractor B remains stable. As a result, even if the system is pushed by noise into the erstwhile basin of attractor A , the system does not remain there for long and therefore stays longer around attractor B . Significantly, such a change in the intermittent scenario can be obtained by a small-amplitude and slow-periodic perturbation. The control is theoretically demonstrated with two standard models, namely, Lorenz equations (for autonomous systems), and the periodically driven, damped Toda oscillator (for nonautonomous systems). Recent experiments with a cavity-loss modulated CO2 laser and an analog circuit of Lorenz equations have validated our theoretical demonstrations excellently.

摘要

在多稳态区域,噪声可产生“多态跳跃间歇性”,即共存稳定吸引子之间的间歇性转变。我们证明,一个小的周期性扰动可显著控制这种跳跃间歇性。这里的“控制”是指稳定吸引子周围相空间中占据概率分布的定性变化。换句话说,如果未受控制的系统相较于另一个吸引子(比如“B”)更倾向于停留在给定吸引子(比如“A”)周围,那么控制扰动会创造出一种相反的情形,使得吸引子B被最频繁访问,结果,占据概率在B周围而非A周围达到最大值。控制扰动按以下方式起作用:它通过边界危机破坏吸引子A,而吸引子B保持稳定。因此,即使系统被噪声推到吸引子A的先前吸引域中,系统也不会在那里停留很长时间,所以会在吸引子B周围停留更长时间。值得注意的是,通过小幅度且缓慢的周期性扰动就能实现间歇性情形的这种变化。我们用两个标准模型从理论上证明了这种控制,即洛伦兹方程(用于自治系统)和受周期驱动的阻尼托达振荡器(用于非自治系统)。最近关于腔损耗调制二氧化碳激光器和洛伦兹方程模拟电路的实验出色地验证了我们的理论证明。

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