Volume 46 Issue 1
Feb.  2017
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Zhao Jiaheng, Zhao Yiqiang, Ye Mao, Xia Xianzhao, Zhou Guoqing. High precision pixel readout circuit design for GM-APD array[J]. Infrared and Laser Engineering, 2017, 46(1): 106007-0106007(8). doi: 10.3788/IRLA201746.0106007
Citation: Zhao Jiaheng, Zhao Yiqiang, Ye Mao, Xia Xianzhao, Zhou Guoqing. High precision pixel readout circuit design for GM-APD array[J]. Infrared and Laser Engineering, 2017, 46(1): 106007-0106007(8). doi: 10.3788/IRLA201746.0106007

High precision pixel readout circuit design for GM-APD array

doi: 10.3788/IRLA201746.0106007
  • Received Date: 2016-05-01
  • Rev Recd Date: 2016-06-12
  • Publish Date: 2017-01-25
  • A pixel readout circuit was presented and designed for Geiger-mode avalanche photodiode (GM-APD) array applying to laser 3D imaging. Based on the principle of time-of-flight (TOF), the pixel readout circuit consisted of two main parts:active quenching circuit (AQC) and time-to-digital converter (TDC). The adopted TDC was a two-segment coarse-fine architecture to manage a trade-off between clock frequency and temporal resolution. Based on interpolation technique, the LFSR used for coarse counting and the delay-line type TDC used for fine counting achieved a wide dynamic range up to 18-bit together. Meanwhile the clock frequency used in those two parts were reduced to 250 MHz and 50 MHz, which are 1/20 and 1/10 of the conventional design frequency, respectively. Thus, the difficulties of design and applications were reduced significantly. The circuit was designed with SMIC 0.18 m process. The post-simulation results reveal a high precise temporal resolution of 200 ps and a responding range resolution of 3 cm, satisfying the ranging requirements of 3 km laser 3D imaging. Furthermore, the pixel circuit layout area is less than 5095 m2, and the total power consumption is 0.89 mW, having the advantages of small area and low power consumption.
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    [2] Zheng Lixia, Yang Junhao, Liu Zhao, et al. Design and implementation of Gm-APD array readout integrated circuit for infrared 3D imaging[C]//Proceedings of SPIE, 2013, 8907:1-10.
    [3] Li Qi, Chi Xin, Wang Qi. Principle and technology of 3D ladar on a single pulse using geiger-mode APD arrays[J]. Laser Infrared, 2006, 12(3):1116-1119.(in Chinese)李琦, 迟欣, 王骐. 基于盖革模式APD阵列的单脉冲3D激光雷达原理和技术[J]. 激光与红外, 2006, 12(3):1116-1119.
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High precision pixel readout circuit design for GM-APD array

doi: 10.3788/IRLA201746.0106007
  • 1. Tianjin Key Laboratory of Imaging and Sensing Microelectronic Technology(Tianjin University),Tianjin 300072,China;
  • 2. Guangxi Key Laboratory for Spatial Information and Geomatics,Guilin University of Technology,Guilin 541004,China

Abstract: A pixel readout circuit was presented and designed for Geiger-mode avalanche photodiode (GM-APD) array applying to laser 3D imaging. Based on the principle of time-of-flight (TOF), the pixel readout circuit consisted of two main parts:active quenching circuit (AQC) and time-to-digital converter (TDC). The adopted TDC was a two-segment coarse-fine architecture to manage a trade-off between clock frequency and temporal resolution. Based on interpolation technique, the LFSR used for coarse counting and the delay-line type TDC used for fine counting achieved a wide dynamic range up to 18-bit together. Meanwhile the clock frequency used in those two parts were reduced to 250 MHz and 50 MHz, which are 1/20 and 1/10 of the conventional design frequency, respectively. Thus, the difficulties of design and applications were reduced significantly. The circuit was designed with SMIC 0.18 m process. The post-simulation results reveal a high precise temporal resolution of 200 ps and a responding range resolution of 3 cm, satisfying the ranging requirements of 3 km laser 3D imaging. Furthermore, the pixel circuit layout area is less than 5095 m2, and the total power consumption is 0.89 mW, having the advantages of small area and low power consumption.

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