Karni O, Capua A, Eisenstein G, Franke D, Kreissl J, Kuenzel H, Arsenijević D, Schmeckebier H, Stubenrauch M, Kleinert M, Bimberg D, Gilfert C, Reithmaier J P
Electrical Engineering Dept Technion - Israel Institute of Technology, Haifa 32000, Israel.
Opt Express. 2013 Mar 11;21(5):5715-36. doi: 10.1364/OE.21.005715.
We investigate the nonlinear propagation of an ultra-short, 150 fs, optical pulse along the waveguide of a quantum dot (QD) laser operating above threshold. We demonstrate that among the various nonlinear processes experienced by the propagating pulse, four-wave mixing (FWM) between the pulse and the two oscillating counter-propagating cw fields of the laser is the dominant one. FWM has two important consequences. One is the creation of a spectral hole located in the vicinity of the cw oscillating frequency. The width of the spectral hole is determined by an effective carrier and gain relaxation time. The second is a modification of the shape of the trailing edge of the pulse. The wave mixing involves first and second order processes which result in a complicated interaction among several fields inside the cavity, some of which are cw while the others are time varying, all propagating in both directions. The nonlinear pulse propagation is analyzed using two complementary theoretical approaches. One is a semi-analytical model which considers only the wave mixing interaction between six field components, three of which propagate in each direction (two cw fields and four time-varying signals). This model predicts the deformation of the tail of the output signal by a secondary idler wave, produced in a cascaded FWM process, which co-propagates with the original injected pulse. The second approach is a finite-difference time-domain simulation, which considers also additional nonlinear effects, such as gain saturation and self-phase modulation. The theoretical results are confirmed by a series of experiments in which the time dependent amplitude and phase of the pulse after propagation are measured using the cross-frequency-resolved optical gating technique.
我们研究了一个150飞秒的超短光脉冲在阈值以上工作的量子点(QD)激光器的波导中的非线性传播。我们证明,在传播脉冲所经历的各种非线性过程中,脉冲与激光器的两个反向传播的连续波光场之间的四波混频(FWM)是主导过程。四波混频有两个重要结果。一个是在连续波光振荡频率附近产生一个光谱孔洞。光谱孔洞的宽度由有效载流子和增益弛豫时间决定。另一个是脉冲后沿形状的改变。波混频涉及一阶和二阶过程,这导致腔内几个场之间的复杂相互作用,其中一些是连续波场,而另一些是随时间变化的场,所有这些场都在两个方向上传播。使用两种互补的理论方法分析了非线性脉冲传播。一种是半解析模型,它只考虑六个场分量之间的波混频相互作用,其中三个场分量在每个方向上传播(两个连续波场和四个随时间变化的信号)。该模型预测了在级联四波混频过程中产生的、与原始注入脉冲同向传播的二次闲频波对输出信号尾部的变形。第二种方法是时域有限差分模拟,它还考虑了其他非线性效应,如增益饱和和自相位调制。通过一系列实验证实了理论结果,在这些实验中,使用交叉频率分辨光门技术测量了传播后脉冲的时间相关幅度和相位。