Yoshida Eiji, Kinouchi Shoko, Tashima Hideaki, Nishikido Fumihiko, Inadama Naoko, Murayama Hideo, Yamaya Taiga
National Institute of Radiological Sciences, Chiba 263-8555, Japan.
Radiol Phys Technol. 2012 Jan;5(1):92-7. doi: 10.1007/s12194-011-0142-1. Epub 2011 Nov 29.
We have proposed an OpenPET geometry which consists of two axially separated detector rings. The open gap is suitable for in-beam PET. We have developed the small prototype of the OpenPET especially for a proof of concept of in-beam imaging. This paper presents an overview of the main features implemented in this prototype. We also evaluated the detector performance. This prototype was designed with 2 detector rings having 8 depth-of-interaction detectors. Each detector consisted of 784 Lu(2x)Gd(2(1-x))SiO₅:Ce (LGSO) which were arranged in a 4-layer design, coupled to a position-sensitive photomultiplier tube (PS-PMT). The size of the LGSO array was smaller than the sensitive area of the PS-PMT, so that we could obtain sufficient LGSO identification. Peripheral LGSOs near the open gap directly detect the gamma rays on the side face in the OpenPET geometry. Output signals of two detectors stacked axially were projected onto one 2-dimensional position histogram for reduction of the scale of a coincidence processor. Front-end circuits were separated from the detector head by 1.2-m coaxial cables for the protection of electronic circuits from radiation damage. The detectors had sufficient crystal identification capability. Cross talk between the combined two detectors could be ignored. The timing and energy resolutions were 3.0 ns and 14%, respectively. The coincidence window was set 20 ns, because the timing histogram showed that not only the main peak, but also two small shifted peaks were caused by the coaxial cable. However, the detector offers the promise of sufficient performance, because random coincidences are at a nearly undetectable level for in-beam PET experiments.
我们提出了一种开放式正电子发射断层扫描仪(OpenPET)的几何结构,它由两个轴向分离的探测器环组成。开放间隙适用于束内正电子发射断层扫描(in-beam PET)。我们开发了OpenPET的小型原型,特别是用于束内成像概念验证。本文概述了该原型中实现的主要特性。我们还评估了探测器性能。该原型设计有2个探测器环,每个环有8个相互作用深度探测器。每个探测器由784个Lu(2x)Gd(2(1 - x))SiO₅:Ce(LGSO)组成,采用4层设计,与一个位置灵敏光电倍增管(PS-PMT)耦合。LGSO阵列的尺寸小于PS-PMT的灵敏面积,这样我们就能获得足够的LGSO识别能力。开放间隙附近的周边LGSO在OpenPET几何结构中直接从侧面探测伽马射线。轴向堆叠的两个探测器的输出信号被投影到一个二维位置直方图上,以减小符合处理器的规模。前端电路通过1.2米长的同轴电缆与探测器头分离,以保护电子电路免受辐射损伤。探测器具有足够的晶体识别能力。两个组合探测器之间的串扰可以忽略不计。定时分辨率和能量分辨率分别为3.0纳秒和14%。符合窗口设置为20纳秒,因为定时直方图显示,不仅主峰,而且两个小的偏移峰都是由同轴电缆引起的。然而,该探测器具有足够性能的前景,因为对于束内PET实验,随机符合处于几乎不可检测的水平。