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TH‐CD‐207B‐07: Noise Modeling of Single Photon Avalanche Diode (SPAD) for Photon Counting CT Applications

机译:TH-CD-207B-07:光子计数CT应用的单光子雪崩二极管(SPAD)的噪声建模

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Purpose: Silicon photomultiplier (SiPM) has recently emerged as a promising photodetector for biomedical imaging applications. Due to its high multiplication gain (comparable to PMT), fast timing, low cost and compactness, it is considered a good candidate for photon counting CT. Dark noise is a limiting factor which impacts both energy resolution and detection dynamic range. Our goal is to develop a comprehensive model for noise sources for SiPM sensors. Methods: The physical parameters used in this work were based upon a test SPAD fabricated in 130nm CMOS process. The SPAD uses an n+/p‐well junction, which is isolated from the p‐substrate by a deep n‐well junction. Inter‐avalanche time measurement was used to record the time interval between two adjacent avalanche pulses. After collecting 1×106 counts, the histogram was obtained and multiple exponential fitting process was used to extract the lifetime associated with the traps within the bandgap. Results: At room temperature, the breakdown voltage of the SPAD is ~11.4V and shows a temperature coefficient of 7.7mV/°C. The dark noise of SPAD increases with both the excess biasing voltage and temperature. The primary dark counts from the model were validated against the measurement results. A maximum relative error of 8.7% is observed at 20 °C with an excess voltage of 0.5V. The probabilities of after‐pulsing are found to be dependent of both temperature and excess voltage. With 0.5V excess voltage, the after‐pulsing probability is 63.5% at ‐ 30 °C and drops to ~6.6% at 40 °C. Conclusion: A comprehensive noise model for SPAD sensor was proposed. The model takes into account of static, dynamic and statistical behavior of SPADs. We believe that this is the first SPAD circuit simulation model that includes the band‐to‐band tunneling dark noise contribution and temporal dependence of the after‐pulsing probability.
机译:目的:硅光电倍增管(SIPM)最近被出现为用于生物医学成像应用的有前途的光电探测器。由于其高乘法增益(可与PMT相当),快速定时,低成本和紧凑,它被认为是光子计数CT的良好候选者。暗噪声是影响能量分辨率和检测动态范围的限制因素。我们的目标是为SIPM传感器开发噪声源的综合模型。方法:本作工作中使用的物理参数基于130nm CMOS工艺中制造的测试用品。该选饼使用N + / p井连接点,其通过深N阱结从P衬底隔离。雪崩间时间测量用于记录两个相邻雪崩脉冲之间的时间间隔。在收集1×106计数之后,获得直方图,并使用多个指数拟合过程来提取与带隙内的陷阱相关联的寿命。结果:在室温下,SPAD的击穿电压为〜11.4V,显示温度系数为7.7mV /°C。 SWAD的暗噪声随着过度的偏置电压和温度而增加。模型的主要暗计数针对测量结果验证。在20°C下观察到8.7%的最大相对误差,电压超过0.5V。发现后脉冲的概率依赖于温度和过量电压。具有0.5V过量电压,后脉冲概率在-30℃下为63.5%,在40°C下降至〜6.6%。结论:提出了一种用于SPAD传感器的综合噪声模型。该模型考虑了SPAD的静态,动态和统计行为。我们认为这是第一个SPAD电路仿真模型,包括脉冲带隧道的暗噪声贡献和后续脉冲概率的时间依赖性。

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