共查询到17条相似文献,搜索用时 125 毫秒
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对1064nm谐振腔增强型(RCE)光电探测器(PD)的光电响应特性进行了分析研究.利用MBE生长技术得到有源区分别为量子阱和量子点的1064nm RCE探测器的外延片,并对制作的探测器进行了各种光电特性测试.结果表明量子阱结构的RCE探测器量子效率峰值达到57%,谱线半宽6~7nm,峰值波长1059nm;而量子点结构的RCE探测器量子效率峰值达到30%,谱线半宽5nm,峰值波长1056nm.通过分析量子效率和吸收系数之间的关系,对两种结构器件的吸收进行了比较,发现虽然量子点探测器的吸收小,但通过合理设计共振腔等方法也可以达到较高的量子效率.两种结构的器件都有很好的I-V特性. 相似文献
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对1064nm谐振腔增强型(RCE)光电探测器(PD)的光电响应特性进行了分析研究.利用MBE生长技术得到有源区分别为量子阱和量子点的1064nm RCE探测器的外延片,并对制作的探测器进行了各种光电特性测试.结果表明量子阱结构的RCE探测器量子效率峰值达到57%,谱线半宽6~7nm,峰值波长1059nm;而量子点结构的RCE探测器量子效率峰值达到30%,谱线半宽5nm,峰值波长1056nm.通过分析量子效率和吸收系数之间的关系,对两种结构器件的吸收进行了比较,发现虽然量子点探测器的吸收小,但通过合理设计共振腔等方法也可以达到较高的量子效率.两种结构的器件都有很好的I-V特性. 相似文献
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介绍了一种GaAs基的长波长谐振腔增强型(RCE)光探测器.通过两步生长法,在GaAs村底上异质外延生长了InP-InGaAs-InP的p-i-n光吸收结构和GaAs/AlAs的分布布拉格反射镜(DBR).所制备的器件在1 549.4 nm处获得了67.3%的量子效率和17 nm的光谱响应线宽,在1 497.7 nm处获得了53.5%的量子效率和9.6 nm的光谱响应线宽,而InGaAs吸收层厚度仅为200 nm.采用单片集成法,工艺简单、易于产业化,随着缓冲层技术的发展,此种RCE光探测器的性能还将获得进一步提升. 相似文献
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高速长波长光探测器是高速光纤通信系统和网络的关键器件,它要求光探测器具有宽的频率响应带宽和高量子效率。常用的PIN光探测器由于量子效率和高速性能均受到吸收层厚度的牵制,使得二者相互制约,成为一对矛盾。谐振腔增强型(RCE)光探测器为这一矛盾的解决提供了有效的方案。基于谐振腔增强型光探测器的实际设计和制作模型,分析了器件吸收层中的光场分布,并将其运用于载流子的连续方程,从理论上详细地分析了器件的高速响应特性,给出了计算结果。针对研制的高速长波长谐振腔增强型光探测器,进行了理论分析和实际器件测试的结果比较,得到了比较一致的结果。 相似文献
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A systematic optimization procedure for the design of RCE Schottky photodetectors to achieve maximum quantum efficiency and high speed operation at 1.3 and 1.55 μm wavelengths is presented. The quantum efficiency formulation used includes the structural parameters of the photodetector and takes into account the wavelength dependence of the top and bottom mirrors reflectivities. The results have shown that the value of the thickness of the antireflection coating layer has a major influence in selecting the width of the photodetector to simultaneously achieve maximum quantum efficiency and high bandwidth at the two wavelengths. Simulated values of 270 and 40 GHz were obtained, respectively, for the 3-dB carrier-transit time-limited bandwidth and bandwidth-efficiency product for an RCE Schottky photodetector with a 0.02-μm gold layer 相似文献
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Analyses of light field distribution within a lossy resonant-cavity-enhanced (RCE) p-i-n photodetector is performed. A new expression for the field distribution inside the cavity is derived. This expression is used to derive an expression for the quantum efficiency taking into account the standing wave effect. The field distribution expression is also used in the continuity equations to derive and evaluate the frequency response of the RCE photodetector 相似文献
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An expression of quantum efficiency for high-speed resonant-cavity-enhanced (RCE) Schottky photodiodes is derived. This expression includes the structural and the physical parameters of the photodetector and takes into account the parameters of the metallic Schottky mirror and the wavelength dependence of the reflectivities. The metal layer thickness sets the maximum achievable quantum efficiency as it decays exponentially with it. The antireflection coating layer, on the other hand, determines the photodetector selectivity and the optimum absorption layer thickness that maximizes its quantum efficiency. An algorithm for the design and optimization of RCE Schottky photodetectors has been developed. Theoretical values of 647 GHz and 129 GHz were obtained, respectively, for the carrier-transit time limited 3-dB bandwidth and bandwidth-efficiency product for an RCE Schottky photodetector with a 0.02 μm gold layer 相似文献
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Zhou Zhen Han Qin Du Yun Yang Xiaohong Wu Ronghan Huang Yongqing and Ren Xiaomin 《半导体学报》2005,26(6):1087-1093
A GaAs-based micro-opto-electro-mechanical-systems(MOEMS) tunable resonant cavity enhanced(RCE) photodetector with a continuous tuning range of 31nm under a 6V tuning voltage is demonstrated.The single cantilever beam structure is adopted for this MOEMS tunable RCE photodetector.The maximum and minimum peak quantum efficiency during the tuning are 36.9% and 30.8%,respectively.The maximum and minimum full-widthathalf-maximum (FWHM) are 20nm and 14nm,respectively.The dark current density is 7.46A/m2 without bias. 相似文献