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Active-Reset for the N

机译:N的主动复位

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摘要

A monolithic resistorless circuit has been designed for active reset of the N+P single-ended (common anode) single-photon avalanche diode (SPAD). This type of SPAD has enhanced the photon detection efficiency in the near-infrared (NIR) region relatively to the P+N (two-ended) SPAD. Due to this fact, the N+P SPAD is a better candidate for the light detection and range (LiDAR) working in the NIR region. The circuit is fabricated in a standard 0.18- mu ext{m} CMOS image sensor process. The dead time after each photon detection is adjustable; the minimum measured value is 4 ns. The maximum photon count rate corresponding to this dead time is {2.5}cdot {10}{{8}} photons/s. This circuit guarantees precise repeatable response, short and well-controlled dead time, and after-pulsing effect reduction. All these are essential for many SPAD applications and crucial for increasing the saturation level of the silicon photo multiplier (SiPM)-based LiDAR systems working in strong background light conditions on sunny day.
机译:设计了单片无电阻电路,用于N + P单端(共阳极)单光子雪崩二极管(SPAD)的有源复位。相对于P + N(两端)SPAD,这种类型的SPAD增强了近红外(NIR)区域中的光子检测效率。由于这个事实,N + P SPAD是在NIR区域工作的光检测和测距(LiDAR)的更好候选者。该电路是采用标准的0.18-μm文本CMOS图像传感器工艺制造的。每个光子检测后的死区时间是可调的;最小测量值为4 ns。对应于该死区时间的最大光子计数率为{2.5} cdot {10} {{8}}光子/ s。该电路可确保精确的可重复响应,短而可控的死区时间以及减少后脉冲效应。所有这些对于许多SPAD应用都是必不可少的,对于提高基于硅光电倍增器(SiPM)的LiDAR系统在晴天在强背景光条件下的饱和度至关重要。

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