Next-generation infrared focal plane arrays for high-responsivity low-noise applications

M. Goldflam, S. Hawkins, S. Parameswaran, A. Tauke-Pedretti, L. Warne, D. Peters, S. Campione, W. Coon, G. Keeler, E. Shaner, J. Wendt, E. Kadlec, T. Fortune, J. Klem, P. Davids, J. Kim
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引用次数: 4

Abstract

High-quality infrared focal plane arrays (FPAs) are used in many satellite, astronomical, and terrestrial applications. These applications require highly-sensitive, low-noise FPAs, and therefore do not benefit from advances made in low-cost thermal imagers where reducing cost and enabling high-temperature operation drive device development. Infrared detectors used in FPAs have been made for decades from alloys of mercury cadmium telluride (MCT). These infrared detectors are nearing the believed limit of their performance. This limit, known in the infrared detector community as Rule 07, dictates the dark current floor for MCT detectors, in their traditional architecture, for a given temperature and cutoff wavelength. To overcome the bounds imposed by Rule 07, many groups are working on detector compounds other than MCT. We focus on detectors employing III-V-based gallium-free In As Sb superlattice active regions while also changing the basic architecture of the pixel to improve signal-to-noise. Our architecture relies on a resonant, metallic, subwavelength nanoantenna patterned on the absorber surface, in combination with a Fabry-Perot cavity, to couple the incoming radiation into tightly confined modes near the nanoantenna. This confinement of the incident energy in a thin layer allows us to greatly reduce the volume of the absorbing layer to a fraction of the free-space wavelength, yielding a corresponding reduction in dark current from spontaneously generated electron-hole pairs in the absorber material. This architecture is detector material agnostic and could be applied to MCT detector structures as well, although we focus on using superlattice antimonide-based detector materials. This detector concept has been applied to both mid-wave (3–5 μm) and longwave (8–12 μm) infrared detectors and absorbers. Here we examine long-wave devices, as these detectors currently have a larger gap between desired device performance and that of currently existing detectors. The measured structures show an external quantum efficiency exceeding 50%. We present a comparison of the modeled and measured photoresponse of these detectors and compare these detectors to currently available commercial detectors using relevant metrics such as external quantum efficiency. We also discuss modeling of crosstalk between adjacent pixels and its influence on the potential for a dual-wavelength detector. Finally, we evaluate potential advances in these detectors that may occur in the near future.
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用于高响应性低噪声应用的下一代红外焦平面阵列
高质量的红外焦平面阵列(fpa)用于许多卫星、天文和地面应用。这些应用需要高灵敏度、低噪声的fpa,因此无法从低成本热成像仪的进步中获益,因为低成本热成像仪可以降低成本并实现高温操作,从而驱动设备的开发。几十年来,fpa中使用的红外探测器一直是由碲化汞镉(MCT)合金制成的。这些红外探测器正接近其性能的极限。这个限制,在红外探测器界被称为规则07,规定了MCT探测器的暗电流底限,在他们的传统架构中,对于给定的温度和截止波长。为了克服规则07规定的限制,许多团体正在研究除MCT以外的检测化合物。我们专注于采用iii - v基无镓In As Sb超晶格有源区域的探测器,同时也改变了像素的基本结构以改善信噪比。我们的结构依赖于在吸收器表面设计的谐振金属亚波长纳米天线,结合法布里-珀罗腔,将入射辐射耦合到纳米天线附近的紧密受限模式中。将入射能量限制在薄层中,使我们能够将吸收层的体积大大减小到自由空间波长的一小部分,从而使吸收材料中自发产生的电子-空穴对产生的暗电流相应减少。这种结构与探测器材料无关,也可以应用于MCT探测器结构,尽管我们主要使用超晶格锑基探测器材料。该探测器概念已应用于中波(3-5 μm)和长波(8-12 μm)红外探测器和吸收器。在这里,我们研究长波器件,因为这些探测器目前在期望的设备性能和目前现有的探测器之间有较大的差距。所测结构的外量子效率超过50%。我们将这些探测器的模拟光响应和测量光响应进行了比较,并将这些探测器与目前可用的商用探测器进行了比较,使用相关指标(如外部量子效率)。我们还讨论了相邻像素之间串扰的建模及其对双波长检测器电位的影响。最后,我们评估了这些探测器在不久的将来可能出现的潜在进展。
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