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A 1024#x00D7;8 700ps time-gated SPAD line sensor for laser raman spectroscopy and LIBS in space and rover-based planetary exploration

机译:一个1024×8 700ps时间门控SPAD线传感器,用于基于太空和漫游者的行星探测中的激光拉曼光谱和LIBS

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Raman spectroscopy is a nondestructive, label-free optical analysis technique used to obtain structural and compositional information without any advance preparation. However, the Raman signature is often overwhelmed by strong fluorescence background. Due to its generation mechanism, the fluorescence background can be filtered out in the “time domain” even though it contains exactly the same wavelength components as the Raman signature. To realize such functionality, highly sensitive, time-resolved imagers, such as an intensified charge-coupled devices (iCCDs) or streak cameras are the sensors of choice. These delicate instruments are generally costly, bulky, and unsuitable for space flight and planetary landings. Time-gated, single-photon avalanche diode (SPAD) cameras have been studied for time-resolved imaging modalities, such as fluorescence lifetime imaging microscopy [1], taking advantage of SPAD picosecond temporal resolution as well as single-photon detection capability. Recently, a 128×128, time-gated SPAD array has been proposed to tackle fluorescence background reduction from highly fluorescent minerals for laser Raman spectroscopy targeting potential future on-surface planetary instruments [2]. However, due to long gating (∼30ns), the obtained Raman signature was contaminated by background noise, which overcame minor Raman peaks. In addition, due to extensive on-pixel electronics, the fill factor was reduced, resulting in low photon detection efficiency (PDE). A larger SPAD with sub-nanosecond time-gating was proposed and implemented as a single pixel, operated with a mechanical scanning stage to obtain a Raman signature [3]. To avoid any mechanical moving parts or multiple detectors to obtain a complete Raman signature, a 2D array or line sensor format is thus required.
机译:拉曼光谱法是一种无损,无标记的光学分析技术,无需任何事先准备即可用于获得结构和成分信息。然而,拉曼信号常常被强烈的荧光背景所淹没。由于其生成机理,即使荧光背景包含与拉曼信号完全相同的波长成分,也可以在“时域”中滤除荧光背景。为了实现这种功能,高度敏感的时间分辨成像仪(例如增强型电荷耦合器件(iCCD)或条纹相机)是首选传感器。这些精致的仪器通常昂贵,笨重,并且不适合太空飞行和行星着陆。已经研究了时间门控的单光子雪崩二极管(SPAD)相机的时间分辨成像方式,例如利用SPAD皮秒时间分辨率和单光子检测能力的荧光寿命成像显微镜[1]。最近,有人提出了一种128×128的带时间门控的SPAD阵列来解决来自高荧光性矿物的荧光本底的减少,用于激光拉曼光谱法,目标是潜在的未来地面行星仪器[2]。但是,由于长时间的门控(约30ns),获得的拉曼信号被背景噪声污染,克服了较小的拉曼峰。另外,由于广泛的像素上电子设备,填充因子降低,导致光子检测效率(PDE)降低。提出了具有亚纳秒级时间门控的较大SPAD,并将其实现为单个像素,并通过机械扫描台进行操作以获得拉曼信号[3]。为了避免任何机械运动部件或多个检测器获得完整的拉曼信号,因此需要2D阵列或线传感器格式。

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