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Bifurcation to chaos and extreme event in a laser diode with phase-conjugate feedback

机译:具有相位共轭反馈的激光二极管中的分叉到混沌和极端事件

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Phase-conjugate optical feedback (PCF) has been largely used as a way to stabilize and reduce the linewidth of laser emission but is also known to generate complex dynamics including self-pulsation and chaos. In contrast to the large number of theoretical works, there have been only few experiments reporting on nonlinear dynamics from PCF. Most importantly, experiments so far have not addressed the peculiarities of the PCF dynamics in comparison with dynamics observed from conventional optical feedback (COF). We report here experimentally and theoretically on two chaotic dynamics that relate to the peculiar dynamical properties of a laser diode with PCF. First, we find a chaotic dynamics that resembles the so-called low-frequency fluctuations (LFF) of a laser diode with COF, i.e. the output power shows abrupt dropouts at randomly distributed time-intervals followed by a slower recovery. Although the LFF in PCF shows similar statistical properties to those observed in the LFF in COF, they originate from a distinctively different bifurcation scenario. Increasing the PCF strength the laser diode shows successive bifurcations to time-periodic solutions at the frequency of the external cavity and multiples - also called 'external-cavity modes' (ECMs). In contrast to COF the PCF laser system shows no steady state for large enough feedback strength. Following the destabilization of several such ECMs to chaotic attractors, the dynamics shows a transition to a global attractor connecting the chaotic ECMs and that explains the sequence of power dropouts and recoveries. In addition we show how the bifurcations on these self-pulsing ECMs generate dynamics with extreme events, i.e. pulses with peak intensities well above the average value of the peaks in the output power and that show properties similar to the rogue waves in hydrodynamics. This is the first demonstration of temporal extreme events in a time-delayed optical system.
机译:相位共轭光反馈(PCF)已被广泛用作稳定和减小激光发射的线宽的方法,但众所周知,它会产生复杂的动力学,包括自脉冲和混沌。与大量的理论著作相比,仅有很少的实验报道了PCF的非线性动力学。最重要的是,与从常规光学反馈(COF)观察到的动力学相比,到目前为止,实验还没有解决PCF动力学的特殊性。我们在这里从实验和理论上报告与PCF激光二极管的特殊动力学特性有关的两个混沌动力学。首先,我们发现一种混沌动力学,类似于具有COF的激光二极管的低频波动(LFF),即输出功率在随机分布的时间间隔处突然消失,随后恢复较慢。尽管PCF中的LFF与COF中的LFF表现出相似的统计特性,但它们起源于截然不同的分叉场景。增加PCF强度,激光二极管会在外腔和倍数的频率(也称为“外腔模式”(ECM))上显示出连续的分叉,形成时间周期解。与COF相比,PCF激光系统没有显示出足够大的反馈强度的稳定状态。在几个这样的ECM变成混沌吸引子的不稳定因素之后,动力学表明过渡到连接混沌ECM的全局吸引子,这解释了功率下降和恢复的顺序。此外,我们展示了这些自脉冲ECM的分叉如何产生具有极端事件的动力学,即峰值强度远高于输出功率峰值平均值的脉冲,并且显示出类似于流体动力学中无赖波的特性。这是延时光学系统中时间极端事件的首次演示。

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