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Nonequilibrium laser dynamics of quantum-dot lasers with optical feedback and injection

机译:具有光反馈和注入的量子点激光器的非平衡激光动力学

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Quantum-dot (QD) laser devices offer a variety of advantages over conventional quantum-well (QW) lasers due to their low threshold currents and their high temperature stability. In general, QD lasers show strongly damped relaxation oscillations, due to the charge carrier scattering between the QD and off-resonant reservoir states in the device, which leads to less complicated dynamics under optical feedback and optical injection when compared to QW or bulk lasers [1-3]. The charge carriers influence both the gain and the refractive index of the active region, which leads to the amplitude-phase coupling, commonly characterized by the linewidth enhancement factor α. This coupling is widely assumed to be small for QD lasers, leading to α-factors on the order of ∼1. However, the use of an α-factor in QD lasers has been controversially discussed [4], and it was shown that the QD laser dynamics can not be accurately described by using an α-factor [5].
机译:量子点(QD)激光器设备具有低阈值电流和高温稳定性,因此与常规量子阱(QW)激光器相比,具有多种优势。通常,由于QD激光器和器件中非谐振储能器状态之间的载流子散射,QD激光器显示出强烈衰减的弛豫振荡,与QW或体激光器相比,在光反馈和光注入下,动态动力学的复杂度降低了[ 1-3]。电荷载流子影响有源区的增益和折射率,这导致振幅-相位耦合,通常以线宽增强因子α为特征。对于QD激光器,普遍认为这种耦合很小,从而导致α因子约为1。但是,在QD激光器中使用α因子引起了争议[4],这表明使用α因子无法准确描述QD激光器的动力学[5]。

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