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首页> 外文期刊>IEEE Transactions on Nuclear Science >Probability Distribution of After Pulsing in Passive-Quenched Single-Photon Avalanche Diodes
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Probability Distribution of After Pulsing in Passive-Quenched Single-Photon Avalanche Diodes

机译:被动淬火单光子雪崩二极管中脉冲后的概率分布

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摘要

The resolution and accuracy of the number of photons detected by a silicon photomultiplier (SiPM) are limited by the excess noise, which consists mainly of after pulsing and optical crosstalk. Since these excess noises are correlated with each other, it is challenging to determine the after pulsing and the optical crosstalk probabilities independently of the output signal of the SiPM. Here we examine the dynamic response of passive-quenched single-photon avalanche diodes to clarify the characteristics of the after pulsing. Optical crosstalk is not present in the output signals of single-photon avalanche diodes; therefore, we can obtain the after-pulsing probability directly from the experimental results. We derive an analytical expression for the probability density function of after-pulse timing and analyze the experimental data based on this expression. We confirm that two types of trap levels with emission lifetimes on the order of 10 and 100 ns are responsible for the after pulsing in our devices. The dependence of the after-pulsing probability on the device recovery time is also well explained by our model.
机译:硅光电倍增管(SiPM)检测到的光子数量的分辨率和精度受到多余噪声的限制,该噪声主要由脉冲和光学串扰组成。由于这些多余的噪声相互关联,因此很难确定后脉冲和光串扰概率,而与SiPM的输出信号无关。在这里,我们检查了无源淬火单光子雪崩二极管的动态响应,以阐明脉冲后的特性。单光子雪崩二极管的输出信号中不存在光串扰;因此,我们可以直接从实验结果获得后脉冲概率。我们推导了脉冲后正时的概率密度函数的解析表达式,并基于该表达式分析了实验数据。我们确认,我们的设备中的后脉冲是两种类型的陷阱能级,它们的发射寿命分别为10 ns和100 ns。后脉冲概率对设备恢复时间的依赖性也由我们的模型很好地解释了。

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