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双面硅光子计数计算机断层扫描探测器中的时间分辨率

Timing resolution in double-sided silicon photon-counting computed tomography detectors.

作者信息

Sundberg Christel, Persson Mats, Wikner J Jacob, Danielsson Mats

机构信息

KTH Royal Institute of Technology, Department of Physics, Stockholm, Sweden.

Prismatic Sensors, Part of GE Healthcare, AlbaNova University Center, Stockholm, Sweden.

出版信息

J Med Imaging (Bellingham). 2023 Mar;10(2):023502. doi: 10.1117/1.JMI.10.2.023502. Epub 2023 Mar 23.

DOI:10.1117/1.JMI.10.2.023502
PMID:36969328
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10035543/
Abstract

PURPOSE

Our purpose is to investigate the timing resolution in edge-on silicon strip detectors for photon-counting spectral computed tomography. Today, the timing for detection of individual x-rays is not measured, but in the future, timing information can be valuable to accurately reconstruct the interactions caused by each primary photon.

APPROACH

We assume a pixel size of and a detector with double-sided readout with low-noise CMOS electronics for pulse processing for every pixel on each side. Due to the electrode width in relation to the wafer thickness, the induced current signals are largely dominated by charge movement close to the collecting electrodes. By employing double-sided readout electrodes, at least two signals are generated for each interaction. By comparing the timing of the induced current pulses, the time of the interaction can be determined and used to identify interactions that originate from the same incident photon. Using a Monte Carlo simulation of photon interactions in combination with a charge transport model, we evaluate the performance of estimating the time of the interaction for different interaction positions.

RESULTS

Our simulations indicate that a time resolution of 1 ns can be achieved with a noise level of 0.5 keV. In a detector with no electronic noise, the corresponding time resolution is .

CONCLUSIONS

Time resolution in edge-on silicon strip CT detectors can potentially be used to increase the signal-to-noise-ratio and energy resolution by helping in identifying Compton scattered photons in the detector.

摘要

目的

我们的目的是研究用于光子计数光谱计算机断层扫描的边缘入射硅条探测器的时间分辨率。如今,单个X射线的探测时间并未被测量,但在未来,时间信息对于准确重建每个初级光子引起的相互作用可能很有价值。

方法

我们假设像素尺寸为 ,且探测器具有双面读出功能,每一侧的每个像素都配备用于脉冲处理的低噪声互补金属氧化物半导体(CMOS)电子器件。由于电极宽度与晶圆厚度的关系,感应电流信号在很大程度上由靠近收集电极的电荷移动主导。通过采用双面读出电极,每次相互作用至少会产生两个信号。通过比较感应电流脉冲的时间,可以确定相互作用的时间,并用于识别源自同一入射光子的相互作用。结合电荷传输模型,使用光子相互作用的蒙特卡罗模拟,我们评估了不同相互作用位置下相互作用时间估计的性能。

结果

我们的模拟表明,在噪声水平为0.5 keV时,可以实现1 ns的时间分辨率。在无电子噪声的探测器中,相应的时间分辨率为 。

结论

边缘入射硅条CT探测器中的时间分辨率有可能通过帮助识别探测器中的康普顿散射光子来提高信噪比和能量分辨率。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/fbf0d4fffba8/JMI-010-023502-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/62060926c48a/JMI-010-023502-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/45463cd1cda2/JMI-010-023502-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/e9b54c0d1cd8/JMI-010-023502-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/5ab88620a0d9/JMI-010-023502-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/6f5105cd6d40/JMI-010-023502-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/484f527c2c8b/JMI-010-023502-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/0d6d46f21691/JMI-010-023502-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/8f4a228f2dd4/JMI-010-023502-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/a02426e37708/JMI-010-023502-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/671c4fa3b2e7/JMI-010-023502-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/fbf0d4fffba8/JMI-010-023502-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/62060926c48a/JMI-010-023502-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/45463cd1cda2/JMI-010-023502-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/e9b54c0d1cd8/JMI-010-023502-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/5ab88620a0d9/JMI-010-023502-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/6f5105cd6d40/JMI-010-023502-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/484f527c2c8b/JMI-010-023502-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/0d6d46f21691/JMI-010-023502-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/8f4a228f2dd4/JMI-010-023502-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/a02426e37708/JMI-010-023502-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/671c4fa3b2e7/JMI-010-023502-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8255/10035543/fbf0d4fffba8/JMI-010-023502-g011.jpg

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