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本文引用的文献

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2
Development of a single detector ring micro crystal element scanner: QuickPET II.单探测器环微晶元扫描仪QuickPET II的研发
Mol Imaging. 2005 Apr-Jun;4(2):117-27. doi: 10.1162/15353500200504154.
3
MicroPET II: design, development and initial performance of an improved microPET scanner for small-animal imaging.微型正电子发射断层扫描仪II:用于小动物成像的改进型微型正电子发射断层扫描仪的设计、开发及初始性能
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A full-field modular gamma camera.一种全场模块化γ相机。
J Nucl Med. 1990 May;31(5):632-9.

提高连续微型晶体元件(cMiCE)探测器的固有空间分辨率性能。

Improving the intrinsic spatial resolution performance of the continuous miniature crystal element (cMiCE) detector.

作者信息

Ling Tao, Lewellen Tom K, Miyaoka Robert S

机构信息

Washington Mutual, Seattle, WA.

出版信息

IEEE Nucl Sci Symp Conf Rec (1997). 2007 Oct 26;2007:4308-4313. doi: 10.1109/NSSMIC.2007.4437069.

DOI:10.1109/NSSMIC.2007.4437069
PMID:21804759
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3145461/
Abstract

We have previously reported performance characteristics of a cMiCE detector composed of a 50 mm by 50 mm by 8 mm thick slab of LYSO, coupled to a 64 channel flat-panel PMT. In that work, all 64 PMT channels were digitized and a statistics-based positioning method was used for event positioning. In characterizing the detector, the intrinsic spatial resolution performance for the corner sections of the crystal was degraded compared to the central section of the crystal, even when using our SBP method. It is our belief that the poorer positioning performance at the corners is because much of the light is lost (i.e., not collected by our PMT). To offset this problem, we propose to place light sensors (i.e., micro-pixel avalanche photo diodes, MAPD) at the corners along the short edge of the crystal. The new design would require an additional 8 MAPD devices. Monte Carlo simulation was used to compare the performance of the original cMiCE design and this new enhanced design. Simulation results using DETECT2000 are presented. In addition to doing light ray tracing, GEANT was used to track gamma interactions (i.e., Compton scatter and photoelectric absorption) in the crystal. Thus the simulations include the effects of Compton scatter in the detector. Results indicate that adding the sensors improves the intrinsic spatial resolution performance from 0.99 mm FWHM to 0.79 mm FWHM for the corner section of the crystal, thereby nearly matching the intrinsic spatial resolution of the center section of the crystal (i.e., 0.73 mm FWHM). These results are based upon using dual-DOI look up tables. Additional results were that energy histograms were better using just the 64 channels from the flat panel PMT than using all 72 signal channels.

摘要

我们之前报道过一种cMiCE探测器的性能特征,该探测器由一块50毫米×50毫米×8毫米厚的LYSO晶体平板与一个64通道平板光电倍增管(PMT)耦合而成。在那项工作中,所有64个PMT通道都进行了数字化处理,并使用了一种基于统计的定位方法进行事件定位。在对探测器进行表征时,即使使用我们的SBP方法,晶体角落部分的固有空间分辨率性能与晶体中心部分相比仍有所下降。我们认为角落处定位性能较差是因为大部分光损失了(即未被我们的PMT收集)。为了抵消这个问题,我们建议在晶体短边的角落处放置光传感器(即微像素雪崩光电二极管,MAPD)。新设计将需要额外的8个MAPD器件。使用蒙特卡罗模拟来比较原始cMiCE设计和这种新的增强设计的性能。展示了使用DETECT2000的模拟结果。除了进行光线追踪外,还使用GEANT来跟踪晶体中的伽马相互作用(即康普顿散射和光电吸收)。因此,模拟包括了探测器中康普顿散射的影响。结果表明,添加传感器后,晶体角落部分的固有空间分辨率性能从半高宽0.99毫米提高到了0.79毫米,从而几乎与晶体中心部分的固有空间分辨率(即半高宽0.73毫米)相匹配。这些结果基于使用双深度-of-interaction查找表。另外的结果是,仅使用平板PMT的64个通道得到的能量直方图比使用所有72个信号通道时更好。