Muehllrhner G, Karp J S, Surti S
ADAC UGM, Philadelphia, PA 19104, USA.
Q J Nucl Med. 2002 Mar;46(1):16-23.
In 2-D PET scanners employing septa, scattered radiation is reduced by the septa, placing less importance on good energy resolution. Additionally, the reduced sensitivity in 2-D limits the maximum countrates encountered in clinical FDG studies. In contrast, 3-D PET scanners rely on good energy resolution to reduce the scattered radiation and also must deal with countrates, which are typically 5 times higher than in 2-D mode. To achieve good energy resolution, 3 factors must be considered: 1) choice of a scintillator with good intrinsic energy resolution, 2) choice of a crystal dimension which transmits a uniform amount of light to the PMT in order to avoid light loss along the length of the crystal and 3) choice of a crystal-to-PMT coupling which collects a uniform amount of light from all crystals. As PET scanners are being designed using new, faster scintillators for 3-D imaging, the appropriate trade-off between energy resolution and countrate capability must be found to give the best overall system performance. An example of a fully 3-D PET scanner is the Allegro (ADAC Laboratories), which uses GSO as the detector material. Given the right choice of material and design parameters, good quality, high contrast images can be obtained in 3-D in a relatively short time.
在采用隔板的二维正电子发射断层扫描仪中,隔板可减少散射辐射,因此对良好的能量分辨率要求较低。此外,二维模式下灵敏度的降低限制了临床氟代脱氧葡萄糖(FDG)研究中遇到的最大计数率。相比之下,三维正电子发射断层扫描仪依靠良好的能量分辨率来减少散射辐射,并且还必须处理计数率问题,其计数率通常比二维模式高5倍。为了实现良好的能量分辨率,必须考虑三个因素:1)选择具有良好固有能量分辨率的闪烁体;2)选择能将均匀量的光传输到光电倍增管(PMT)的晶体尺寸,以避免沿晶体长度的光损失;3)选择能从所有晶体收集均匀量光的晶体与光电倍增管的耦合方式。由于正电子发射断层扫描仪在设计时采用了新型、更快的闪烁体用于三维成像,因此必须在能量分辨率和计数率能力之间找到合适的权衡,以实现最佳的整体系统性能。全三维正电子发射断层扫描仪的一个例子是Allegro(ADAC实验室),它使用锗酸锶(GSO)作为探测器材料。在正确选择材料和设计参数的情况下,可以在相对较短的时间内以三维方式获得高质量、高对比度的图像。