共查询到19条相似文献,搜索用时 58 毫秒
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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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本文提出了一种新型的3腔结构谐振腔增强型光探测器,并进行了实验研究。此器件的光谱响应线宽由其滤波腔决定。实验测得为小于4nm;它的量子效率由其吸收腔决,器件的整体响应可以在一定程度上补偿其波腔的损耗。 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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A novel resonant cavity enhanced (RCE) photodetector with flat-top and steep-edge response is presented. The response is obtained
by designing a gradient-thickness P area in the absorption cavity. Simulation results show that the maximum and minimum values
of the quantum efficiency in bandpass are 85.242% and 87.564% respectively, the ripple is about 3.6%, and 0.5 dB, 3 dB and
20 dB bandwidths are 0.3 nm, 0.4 nm and 1.2 nm, respectively. The mesa area is 10 μm × 10 μm and the frequency response bandwidth
is 87 GHz. Compared with similar photodetectors, this photodetector has high quantum efficiency, narrow spectral response
linewidth, good flat-top and steep-edge response and ideal high-speed characteristics. 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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The performances of thermal infrared light detector based on a model system of resonant semiconductor microcavities are theoretically investigated. An original transfer matrix formalism of cavity enhanced absorption is presented which makes use of the small thickness of the absorbing layer compared to the light wavelengths. This formalism yields exact expressions which take standing wave effects into account in a built-in way. Approximations lead to tractable expressions which allow deriving asymptotic behaviors and general trends. The tradeoff between large cavity absorption enhancement and reduction of the detector bandwidth is particularly studied, leading to a gain-bandwidth product analysis. Approximated expressions for detectors based on resonant (i.e type I quantum dots) and nonresonant (bulk or type II quantum wells) optical transitions are also derived, which are physically meaningful and may be conveniently used for engineering purposes. It is found that the limitations due to the gain-bandwidth product conservation can be overcome. However, these cavity enhancement effects are only important for very small quantum efficiency for which the finesse of the microcavity is not seriously deteriorated. 相似文献
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新型材料InGaNAs的生长与应用前景 总被引:1,自引:0,他引:1
详细介绍了一种新型半导体材料(InGaNAs)的生长特点及其在制作高特征温度的长波长量子阱激光器、长波长垂直腔面发射激光器、长波长光泵垂直外腔面发射激光器、半导体可饱和吸收镜和长波长谐振腔增强探测器方面的优势。 相似文献
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Organic photodetector with spectral response tunable across the visible spectrum by means of internal optical microcavity 总被引:1,自引:0,他引:1
We demonstrate an organic photodetector (OPD) structure in which the active layers and a thick optical spacer are sandwiched between two metallic electrodes, forming a Fabry–Perot resonant cavity. The second resonant mode of this cavity can be positioned by means of an optical spacer so that its maximum intensity overlaps with the donor–acceptor interface, leading to a peak in the external quantum efficiency (EQE) of the OPD for this resonant wavelength. The photoresponse can thus be tuned across the visible spectrum by adjusting the spacer thickness, while the full width half maximum remains approximately 50 nm. Because the active layers can be thin in this approach, the EQE is not sacrificed, and the device can achieve a relatively high response frequency that does not suffer from the inclusion of the optical spacer. We simulate the photoresponse of OPD structure using transfer matrix optical calculations and an exciton diffusion model; our simulation also explicitly accounts for interface roughness measured by atomic force microscopy. Angular dependence of the OPD’s response is also measured and discussed. 相似文献
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使用共振腔实现受控非门及量子隐形传态的方案 总被引:4,自引:3,他引:1
提出一个使用三能级原子以及通过经典场对单粒子态的操控和两原子与单模腔场的共振作用实现受控非门的方案,并使用该方案完成单粒子态的隐行传态过程.该方案中原子与单模腔场的共振作用时间可以很短,这一特点对量子信息处理过程中的消相干问题的处理是非常有利的,这也是该方案与已有文献报道使用失谐腔的腔QED方案的主要区别之一. 相似文献