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Enhancing the fill-factor of CMOS SPAD arrays using microlens integration

机译:使用微透镜集成来提高CMOS SPAD阵列的填充系数

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摘要

Arrays of single-photon avalanche diode (SPAD) detectors were fabricated, using a 0.35 μm CMOS technology process,udfor use in applications such as time-of-flight 3D ranging and microscopy. Each 150 x 150 μm pixel comprises a 30 μmudactive area diameter SPAD and its associated circuitry for counting, timing and quenching, resulting in a fill-factor ofud3.14%. This paper reports how a higher effective fill-factor was achieved as a result of integrating microlens arrays onudtop of the 32 x 32 SPAD arrays. Diffractive and refractive microlens arrays were designed to concentrate the incomingudlight onto the active area of each pixel. A telecentric imaging system was used to measure the improvement factor (IF)udresulting from microlens integration, whilst varying the f-number of incident light from f/2 to f/22 in one-stopudincrements across a spectral range of 500-900 nm. These measurements have demonstrated an increasing IF with fnumber,udand a maximum of ~16 at the peak wavelength, showing a good agreement with theoretical values. An IF of 16udrepresents the highest value reported in the literature for microlenses integrated onto a SPAD detector array. The resultsudfrom statistical analysis indicated the variation of detector efficiency was between 3-10% across the whole f-numberudrange, demonstrating excellent uniformity across the detector plane with and without microlenses.
机译:采用0.35μmCMOS技术工艺制造了单光子雪崩二极管(SPAD)检测器阵列,用于飞行时间3D测距和显微镜等应用。每个150 x 150μm像素包括一个30μm的有效区域直径SPAD及其相关的电路,用于计数,计时和猝灭,因此填充因子为ud3.14%。本文报告了如何在32 x 32 SPAD阵列的 udtop上集成微透镜阵列,从而实现更高的有效填充因子。设计了衍射和折射微透镜阵列,以将入射的 udlight聚光到每个像素的有效区域上。远心成像系统用于测量因微透镜集成而产生的改善因子(IF),同时在500-光谱范围内以一站式 udincrement将入射光的f数从f / 2改变为f / 22。 900纳米这些测量表明,IF随f数增加,在峰值波长处最大为〜16,与理论值显示出良好的一致性。 16的IF代表文献中报道的集成到SPAD检测器阵列上的微透镜的最高值。统计分析的结果表明,在整个f值范围内,检测器效率的变化在3%至10%之间,这表明在有或没有微透镜的情况下,整个检测器平面均具有出色的均匀性。

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