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Surface roughness effect on micropillar cavities

机译:表面粗糙度对微柱腔的影响

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Being applied in many fields such as optoelectronics and quantum information processing, micropillar cavities are stepping into smaller and smaller scales. As a pillar is shrinking to sub-micrometer size, the surface roughness induced by imperfect fabrication process will dramatically influence the quality of such cavity, because of the edge-scattering of cavity modes. Here, we investigated this effect by using finite-difference-time-domain methods. For a micropillar cavity consisting of distributed Bragg-reflectors, the surface roughness is modeled by dividing the disk-shaped layer into a few randomly polygonal layers. One example is the investigation on the InGaAsP/InP-air-aperture micropillar cavity, which is a promised candidate for a 1.55-μm quantum-dot single-photon source. For such cavity, our results show that for short wavelength, both the Q factor and the output efficiency decrease with the increase of the surface roughness. Where, we define the surface roughness as a relative value of radius. It is worth noting that with a surface roughness of 0.01, ~1.3 nm for the InP layers and ~4.7 nm for the InGaAsP layers, the Q factor is close to 90% of the one without any roughness, which suggests that the fabrication process should satisfy a control precision at nanometer level, in order to make a micropillar cavity with good quality.
机译:微柱腔已在光电子学和量子信息处理等许多领域中得到应用,并正在逐步缩小规模。当柱子收缩到亚微米尺寸时,由于腔模的边缘散射,不完善的制造工艺所引起的表面粗糙度将极大地影响这种腔的质量。在这里,我们使用时域有限差分法研究了这种影响。对于由分布式布拉格反射器组成的微柱腔,通过将圆盘形层划分为几个随机的多边形层来模拟表面粗糙度。一个示例是对InGaAsP / InP气孔微柱腔的研究,该腔有望用作1.55μm量子点单光子源。对于这种腔,我们的结果表明,对于短波长,Q因子和输出效率都随表面粗糙度的增加而降低。其中,我们将表面粗糙度定义为半径的相对值。值得注意的是,对于InP层,其表面粗糙度为0.01,〜1.3 nm,对于InGaAsP层,约为〜4.7 nm,Q因子接近没有任何粗糙度的Q因子的90%。为了使微柱腔具有良好的质量,该过程应满足纳米级的控制精度。

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