Infrared multispectral imaging with silicon-based multiband pass filter and infrared focal plane array

R. Ueno, K. Ishii, Kazuhiro Suzuki, H. Honda, H. Funaki
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引用次数: 1

Abstract

This paper reports the implementation of a silicon-based infrared (IR) multiband pass filter (BPF) on an uncooled microbolometer IR focal plane array (IR-FPA), both of which are fabricated by the standard CMOS process. IR spectroscopy has been widely used as a sample identification technique, exploiting the fact that each molecule structure has a unique spectral feature. Using IR-BPF and IR-FPA, a low-cost and compact IR-spectral imaging system is realized. The microbolometer IR-FPA exhibits broad spectral response sufficient to cover the IR-region from the mid-infrared (3 μm) to far-infrared (8 μm~), which is broader than the coverage of conventional non-silicon-based photodetectors such as mercury cadmium telluride. Single-band images of invisible gases such as ethanol vapor and CO2 in breath are obtained with the IR-FPA. For multiband imaging, a guided-mode resonance IR filter is fabricated by patterning aluminum (Al) layer of 100 nm thickness on a silicon-on-insulator wafer. Measured peak transmittance wavelengths (λc) of square and hexagonal Al array are compared with results of rigorous coupled-wave analysis, as a function of the Al pattern period. The λc of 3.3, 3.9, and 4.4 μm are obtained at the pattern period of 1.8, 2.4, and 2.8 μm for the square array. In all cases, the λc slightly decreases for the hexagonal array. The full-width at half-maximum (FWHM) of each filter is approximately 200 nm for the λc of 4.4 μm, 400 nm for λc of 3.3 μm.
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基于硅基多带通滤波器和红外焦平面阵列的红外多光谱成像
本文报道了在非制冷微热计红外焦平面阵列(IR- fpa)上实现硅基红外(IR)多带通滤波器(BPF),这两个滤波器都是用标准CMOS工艺制造的。红外光谱已被广泛用作样品鉴定技术,利用了每个分子结构具有独特的光谱特征的事实。采用IR-BPF和IR-FPA实现了低成本、紧凑的红外光谱成像系统。红外- fpa微辐射热计具有较宽的光谱响应,足以覆盖从中红外(3 μm)到远红外(8 μm~)的红外区域,这比传统的非硅基光电探测器(如碲化汞镉)的覆盖范围更广。IR-FPA可获得呼气中乙醇蒸气和二氧化碳等不可见气体的单波段图像。为了实现多波段成像,在绝缘体上硅晶片上制作了100 nm厚度的铝层,制成了导模共振红外滤波器。将方形和六边形Al阵列的透射光谱峰值波长(λc)与严格耦合波分析结果进行了比较,并将其作为Al模式周期的函数。在图形周期为1.8、2.4和2.8 μm时,方形阵列的λc分别为3.3、3.9和4.4 μm。在所有情况下,对于六边形阵列,λc都略有减小。当λc为4.4 μm时,各滤波器的半最大全宽约为200 nm,当λc为3.3 μm时,各滤波器的半最大全宽约为400 nm。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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