面向微腔垂直腔激光器:高效低阈值的孔径和腔体设计

E. Hegblom, B. Thibeault, L. Coldren
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引用次数: 2

摘要

我们制造了/spl λ /=980 nm的垂直腔激光器,该激光器具有锥形氧化物外形,通过在第一个p-镜层(230 nm (3/4 /spl λ /)厚的Al/sub 0.9/Ga/sub 0.1/As层内放置10.5 nm的AlAs层而产生。我们绘制了散射损耗(由锥形和突变型孔径器件的效率差决定)与氧化物开口半径的关系图。对四分之一波厚度孔径减小超过/spl μ m/3 /spl μ m/ m的980 nm AlAs/GaAs vcl的模拟表明,它们没有多余的损耗。尽管对于给定的模态尺寸,这种“长”锥形孔径的散射损失远低于突然孔径,但在模态尺寸缩小到l/e/sup / 2/半径为/spl sim/1.5 /spl mu/m以下之前,孔径关闭。在较短的距离(/spl sim/1 /spl mu/m)上逐渐减小四分之一波厚孔径不仅降低了小孔径下的散射损失,而且将模式限制在最小尺寸。最后,由单个孔径限制的最小尺寸模式(通过使用抛物线(理想透镜)剖面获得)受DBR反射镜的角止光带的限制。对于带有AlAs/GaAs反射镜的980 nm vcl,最小模式尺寸的l/e/sup /半径为/spl sim/0.6 /spl mu/m。为了进一步减小这个尺寸,人们需要使用介电镜或使用多个薄孔径,以避免引入额外的损耗。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Towards microcavity vertical cavity lasers: aperture and cavity design for high efficiency and low threshold
We have fabricated /spl lambda/=980 nm vertical cavity lasers with a tapered oxide profile which is produced by placing a 10.5 nm layer of AlAs within the first p-mirror layer which is a 230 nm (3/4 /spl lambda/) thick Al/sub 0.9/Ga/sub 0.1/As layer. We have plotted the scattering loss (as determined from the differential efficiency of tapered and abrupt apertured devices) vs. the radius of the opening in the oxide. Simulations of 980 nm AlAs/GaAs VCLs with quarter-wave thick apertures tapered over more than /spl sim/3 /spl mu/m show they have no excess loss. Although for a given mode size, scattering losses from such a "long" tapered aperture are much lower than for an abrupt aperture, the apertures close off before the mode size can shrink below a l/e/sup 2/ radius of /spl sim/1.5 /spl mu/m. Tapering quarter-wave thick apertures over a shorter distance (/spl sim/1 /spl mu/m) not only lowers scattering losses at the small aperture sizes, but also confines the mode to the smallest sizes. Ultimately, the smallest size mode confined by a single aperture (obtained by using a parabolic (ideal lens) profile) is limited by the angular stop-band of the DBR mirror. For 980 nm VCLs with AlAs/GaAs mirrors the smallest mode size has a l/e/sup 2/ radius of /spl sim/0.6 /spl mu/m. To reduce this size further one would need to turn to dielectric mirrors or use multiple apertures which are thin so as not to introduce additional losses.
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