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用于飞行时间正电子发射断层扫描的多阳极微通道板光电倍增管的研究

Investigation of a Multi-Anode Microchannel Plate PMT for Time-of-Flight PET.

作者信息

Choong Woon-Seng

机构信息

W.-S. Choong is with the Lawrence Berkeley National Laboratory, Berkeley, CA 94720 USA (phone: 510-486-6757; fax: 510-486-4768;

出版信息

IEEE Trans Nucl Sci. 2010 Sep 13;57(5):2417-2423. doi: 10.1109/TNS.2010.2060211.

Abstract

We report on an investigation of a mulit-anode microchannel plate PMT for time-of-flight PET detector modules. The primary advantages of an MCP lie in its excellent timing properties (fast rise time and low transit time spread), compact size, and reasonably large active area, thus making it a good candidate for TOF applications. In addition, the anode can be segmented into an array of collection electrodes with fine pitch to attain good position sensitivity. In this paper, we investigate using the Photonis Planacon MCP-PMT with a pore size of 10 µm to construct a PET detector module, specifically for time-of-flight applications. We measure the single electron response by exciting the Planacon with pulsed laser diode. We also measure the performance of the Planacon as a PET detector by coupling a 4 mm × 4 mm × 10 mm LSO crystal to individual pixel to study its gain uniformity, energy resolution, and timing resolution. The rise time of the Planacon is 440 ps with pulse duration of about 1 ns. A transit time spread of 120 ps FWHM is achieved. The gain is fairly uniform across the central region of the Planacon, but drops off by as much as a factor of 2.5 around the edges. The energy resolution is fairly uniform across the Planacon with an average value of 18.6±0.7% FWHM. While the average timing resolution of 252±7 ps FWHM is achieved in the central region of the Planacon, it degrades to 280±9 ps FWHM for edge pixels and 316±15 ps FWHM for corner pixels. We compare the results with measurements performed with a fast timing conventional PMT (Hamamatsu R-9800). We find that the R9800, which has significantly higher PDE, has a better timing resolution than the Planacon. Furthermore, we perform detector simulations to calculate the improvement that can be achieved with a higher PDE Planacon. The calculation shows that the Planacon can achieve significantly better timing resolution if it can attain the same PDE as the R-9800, while only a 30% improvement is needed to yield a similar timing resolution as the R-9800.

摘要

我们报告了一项针对用于飞行时间正电子发射断层扫描(PET)探测器模块的多阳极微通道板光电倍增管(PMT)的研究。微通道板(MCP)的主要优点在于其出色的定时特性(快速上升时间和低渡越时间展宽)、紧凑的尺寸以及相当大的有效面积,因此使其成为飞行时间应用的良好候选者。此外,阳极可以分割成具有精细间距的收集电极阵列,以获得良好的位置灵敏度。在本文中,我们研究使用孔径为10 µm的Photonis Planacon MCP-PMT来构建PET探测器模块,特别是用于飞行时间应用。我们通过用脉冲激光二极管激发Planacon来测量单电子响应。我们还通过将一个4 mm×4 mm×10 mm的LSO晶体耦合到各个像素来研究Planacon作为PET探测器的性能,以研究其增益均匀性、能量分辨率和定时分辨率。Planacon的上升时间为440 ps,脉冲持续时间约为1 ns。实现了120 ps半高宽(FWHM)的渡越时间展宽。在Planacon的中心区域增益相当均匀,但在边缘处下降多达2.5倍。在整个Planacon上能量分辨率相当均匀,平均值为18.6±0.7% FWHM。虽然在Planacon的中心区域实现了平均定时分辨率为252±7 ps FWHM,但对于边缘像素它降至280±9 ps FWHM,对于角落像素降至316±15 ps FWHM。我们将结果与使用快速定时传统PMT(滨松R-9800)进行的测量结果进行比较。我们发现具有显著更高光电探测效率(PDE)的R9800具有比Planacon更好的定时分辨率。此外,我们进行探测器模拟以计算使用具有更高PDE的Planacon可以实现的改进。计算表明,如果Planacon能够达到与R-9800相同的PDE,它可以实现显著更好的定时分辨率,而只需提高30%就能产生与R-9800相似的定时分辨率。

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