InGaAs/GaAs量子阱放大器的非线性极化开关

M. Lin, C. C. Yang, M. Hong, Young-Kai Chen
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引用次数: 0

摘要

非线性自开关是实现激光全光信号处理和无源锁模的重要步骤。在非线性自开关中,两个通道之间的能量依赖于功率的耦合是由两个通道之间的非线性增益/吸收和/或折射率的不平衡引起的。本文报道了InGaAs/GaAs单量子阱(QW) GRINSCH光放大器非线性极化开关的实验结果。放大器也由一个10纳米ingaa组成。在井的两侧,它包括一个40 nm的GaAs势垒,一个约200 nm的AlxGa1-xAs分级指数分离约束层(x从0.4降至0),以及一个Al0.4Ga0.6As p/n型包层。它在974 nm处以120 mA的阈值电流放电,占空比为20%。放大器长约300 μm,脊宽50 μm,用于横向导向。TE (TM)模式下的电致发光集中在975 (940)nm附近,表明了重孔和轻孔子带的相对能量状态。在实验中,我们使用Ti:Sapphire激光器(Mirra 900)处理飞秒和连续波光信号。信号通过放大器后,记录其TE方向和TM方向的极化状态和功率分布,如图1所示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Nonlinear Polarization Switching in an InGaAs/GaAs Quantum Well Amplifier
Nonlinear self-switching is an important step toward all-optical signal processing and passive mode-locking of lasers. In nonlinear self-switching, the power-dependent coupling of energy between two channels is caused by the imbalance of nonlinear gain/absorption and/or refractive-index between the two channels. In this paper, we report the experimental results of nonlinear polarization switching in an InGaAs/GaAs single quantum well(QW) GRINSCH optical amplifier. The amplifier consists of a 10 nm InGaAs well. On either side of the well, it includes a 40 nm GaAs barrier, an about 200 nm graded-index separate confinement layer with AlxGa1-xAs (x drops from 0.4 to 0), and an Al0.4Ga0.6As p/n type cladding. It lased at the threshold current 120 mA with 20 % duty cycle at 974 nm. The amplifier had a length about 300 μm and a ridge 50 μm wide for lateral guiding. The electro-luminescence in the TE (TM) mode was centered near 975 (940) nm, indicating the relative energy state of the heavy and light hole subbands. In the experiment, we used a Ti:Sapphire laser (Mirra 900) for femtosecond and cw optical signals. After the signals passed through the amplifier, their polarization status and power distributions between the TE and TM directions were recorded, as shown in Fig. 1.
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