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Electronic structure engineering of the linewidth enhancement factor in mid-infrared semiconductor laser active regions

机译:中红外半导体激光有源区中线宽增强因子的电子结构工程

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The linewidth enhancement factor is a fundamental parameter that characterizes the limit of spectral purity and the tendency for filamentation in a semiconductor laser. For either narrow-line or high-power operation, it is generally desirable that the linewidth enhancement factor be minimized. This parameter depends primarily on the shape of the differential gain spectrum of the active region material. In mid-infrared laser materials, band structure engineering has been used routinely to minimize the effects of nonradiative recombination. This same approach can be used to tailor the differential gain spectrum of these materials to minimize the linewidth enhancement factor. Favorable features of the electronic structure of the material include 1) band-edge dispersion in the conduction band which shifts the peak of the gain away from the band edge and 2) intersubband absorption resonances, which can be designed to lie above the peak gain in energy. Both of these strategies shift the peak of the differential gain closer to the peak gain, and thus reduce the linewidth enhancement factor. These electronic structure design strategies can be used to reduce the linewidth enhancement factor in type-II InAs/GaInSb systems to almost 1.0, which is significantly smaller than typical values of 2.5-5 in type-I strained quantum wells. We note that a linewidth enhancement factor close to 1 is much smaller even than a typical linewidth enhancement factor in visible or near-infrared semiconductor lasers. Furthermore in some materials the peak of the differential gain lies in a region of positive gain, indicating that a grating could be used to select a mode with negligible linewidth enhancement factor.
机译:线宽增强因子是一种基本参数,其表征光谱纯度的极限以及半导体激光器中的细丝趋势。对于窄线或高功率操作,通常希望线宽增强因子最小化。该参数主要取决于有源区材料的差分增益谱的形状。在中红外激光材料中,频带结构工程经常使用,以最大限度地减少非阵列重组的影响。相同的方法可用于根据这些材料的差分增益谱定制以最小化线宽增强因子。材料的电子结构的有利特征包括在传导带中的带边缘色散,其使得远离带边缘的增益的峰值和2)三角机吸收谐振,这可以设计为高于峰值增益活力。这两种策略都将差分增益的峰值偏好于峰值增益,从而减少了线宽增强因子。这些电子结构设计策略可用于将II型INA / GAINTB系统中的线宽增强因子降低至近1.0型,这显着小于I型紧张量子孔中2.5-5的典型值。我们注意到,即使是可见或近红外半导体激光器的典型线宽增强因子,较近1的线宽增强因子要小得多。此外,在一些材料中,差分增益的峰值位于正增益区域,表明光栅可用于选择具有可忽略的线宽增强因子的模式。

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