具有调制损耗的激光器:其周期和非周期行为的完整描述。

A. Poggi, G. Puccioni, W. Gadomski, F. Arecchi, J. Tredicce
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引用次数: 0

摘要

我们报告了具有调制损耗的CO2激光系统的新的和详细的研究。先前的实验和理论都表明,当参数被调制时,这种均匀加宽的激光器[1](以及其他类似的系统[2])会表现出不稳定性并最终出现混沌行为。我们改进了之前系统的稳定性,并使用快速瞬态记录仪,我们能够表征到混沌的倍周期过渡,包括稳定的f/8次谐波。我们发现混沌区域内的周期窗口不遵循众所周知的逻辑映射的预测序列。我们提出了时间行为,庞加莱剖面,相空间肖像和功率谱,允许明确识别过渡到混沌。我们提出了动力学行为的其他度量,如显示广义多稳定性的分岔图和在参数空间中定位不稳定区域的相图。数字化时间序列的维数测试表明,随着参数的变化,奇异吸引子的形成和演化。可以测量费根鲍姆级联积聚点之前和积聚点处的维数,然后测量进入混沌区域的维数。结果与非线性动力学的一般理论相吻合[3]。我们首次从实验系统中获得了返回图,它们揭示了当我们进入混沌区域时,具有二次极大值的图与Feigenbaum模型的类比被打破。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Laser with modulated loss: A complete description of its periodic and aperiodic behaviour.
We report new and detailed studies of a CO2 laser system with modulated losses. It has been shown previously both experimentally and theoretically that such a homogeneously broadened laser [1] (and other similar systems [2]) can display instabilities and eventually chaotic behaviour when a parameter is modulated. We have improved the stability of our previous system and using a fast transient recorder we were able to characterize the period-doubling transition to chaos, including a stable f/8 subharmonic. We find periodic windows inside the chaotic region which do not follow the predicted sequence of the well-known logistic map. We present the time behavior, Poincare sections, phase-space portraits and power spectra that permit unequivocal Identification of a transition to chaos. We present other measures of the dynamical behaviour such as bifurcation diagrams showing generalized multistability and phase diagrams in the parameter space which localize the unstable regions. Dimensionality tests on digitized time series show the formation and evolution of a strange attractor as parameters are varied. It was possible to measure the dimension before and at the accumulation point of a Feigenbaum cascade and then into the chaotic region. The results are in good agreement with general theory on nonlinear dynamics [3]. For the first time return maps have been obtained from an experimental system and they reveal the breakdown of an analogy with the Feigenbaum model for a map with a quadratic maximum when we enter into the chaotic region.
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