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Enhanced modulation bandwidth for strain-compensatedInGaAlAs-InGaAsP MQW lasers

机译:用于应变补偿的InGaAlAs-InGaAsP MQW激光器的增强调制带宽

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Strain-compensated (SC) multiple-quantum-well (MQW) lasers werendesigned using tensile-strained InGaAlAs barrier layers in order tonenhance the modulation bandwidth of MQW lasers at 1.55 Μm. The designnscheme simultaneously ensures the pseudomorphic growth of a large stacknof highly strained wells, a uniform hole injection into large number ofnwells, a large conduction band discontinuity to suppress the carriernoverflow effect, and a large differential gain by suppressing the bandnmixing effect. The SC-MQW structures were processed into a mushroomnstripe laser structure to obtain a low parasitic capacitance. The numbernof wells and the cavity length were optimized to maximize the modulationnbandwidth. Both the relaxation oscillation and RC cutoff frequenciesnincreased with reducing the cavity length, and a maximum 3-dB modulationnbandwidth of 30 GHz was obtained at a short cavity length of 120 Μmnfor 20-well SC-MQW lasers. Moreover, a high internal quantum efficiencynand large differential gain were obtained for the SC-MQW lasers withnwell numbers of up to 20 as a result of the reduced carrier transportnand overflow effects. The differential gain, gain compression factor,nand K factor were evaluated experimentally from the modulationncharacteristics and compared to the theoretical calculation based on thenspectral hole burning theory. The observed experimental results werenwell explained by the model using the identical intraband relaxationntimes typically used for 1.55-Μm bulk lasers
机译:使用拉伸应变的InGaAlAs势垒层设计应变补偿(SC)多量子阱(MQW)激光器,以增强1.55μm处MQW激光器的调制带宽。设计方案同时确保了大叠叠的高应变阱的拟晶生长,向大量nwell中均匀注入空穴,通过抑制带隙混频效应实现了较大的导带不连续性以抑制载流子溢出效应以及大的差分增益。将SC-MQW结构加工成蘑菇形激光结构,以获得低寄生电容。优化孔的数量和腔的长度以最大化调制带宽。对于20孔SC-MQW激光器,在120 Mmn的短腔长下,弛豫振荡和RC截止频率均随腔长度的减小而增加,并且在30μm的短腔内获得了30 GHz的最大3-dB调制带宽。此外,由于减少了载流子传输和溢出效应,具有高达20的阱数的SC-MQW激光器获得了较高的内部量子效率和较大的差分增益。通过调制特性对差分增益,增益压缩因子,n和K因子进行了实验评估,并与基于光谱孔燃烧理论的理论计算结果进行了比较。该模型使用通常用于1.55-μm体激光器的相同带内弛豫时间很好地解释了观察到的实验结果

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