Giant gain in a rare-earth-ion-doped waveguide

D. Geskus, S. Aravazhi, S. García-Blanco, M. Pollnau
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引用次数: 1

Abstract

Nowadays two types of optical amplifiers are widely used: rare-earth (RE) doped fiber amplifiers (RDFAs) and semiconductor optical amplifiers (SOAs). RDFAs are not suitable for micro-scale on-chip integration, partly because their gain per unit length is hampered by the combination of small transition cross-sections in RE ions and the restriction to low doping concentrations. SOAs can deliver high gain over short distances, which makes them suitable for providing on-chip gain on silicon wafers. Despite the extraordinarily high material gain in the nm-sized recombination region of a III–V semiconductor, the usually μm-sized confinement of the signal beam results in a poor overlap factor with the active gain region, reducing accordingly the modal gain to a few hundred dB/cm. On the other hand, the typical gain per unit length reported so far for RE-doped integrated waveguides has hardly exceeded a few dB/cm [1, 2], almost two orders of magnitude less than in SOAs.
稀土离子掺杂波导的巨大增益
目前广泛应用的光放大器有两种:掺稀土光纤放大器(rdfa)和半导体光放大器(soa)。rdfa不适合微尺度的片上集成,部分原因是它们的单位长度增益受到RE离子的小跃迁截面和低掺杂浓度的限制。soa可以在短距离内提供高增益,这使得它们适合在硅片上提供片上增益。尽管III-V半导体纳米级复合区域的材料增益非常高,但通常μm大小的信号束限制导致与有源增益区域的重叠系数很差,相应地将模态增益降低到几百dB/cm。另一方面,迄今为止报道的re掺杂集成波导单位长度的典型增益几乎没有超过几dB/cm[1,2],几乎比soa少了两个数量级。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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