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首页> 外文期刊>IEEE Transactions on Nuclear Science >Signal characteristics of individual crystals in high resolution BGO detector designs using PMT-quadrant sharing
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Signal characteristics of individual crystals in high resolution BGO detector designs using PMT-quadrant sharing

机译:使用PMT-象限共享的高分辨率BGO检测器设计中单个晶体的信号特性

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The PMT-quadrant sharing (PQS) detector design allows very high resolution detectors to be built with 70% fewer PMTs and lower cost. A common concern for the design is that there is a big gap (photo-insensitive area) between four circular PMTs and the photoelectron signal (pulse height) may be much lower for the central crystals. The concern increases with the use of smaller PMTs for high-resolution designs because small PMTs have relatively thicker walls and relatively larger tolerance spaces between them. The authors measured the pulse heights and energy resolution for each crystal in three different types of PQS blocks for 19 mm PMT. For a square 7 /spl times/ 7 block detector (2.66 mm /spl times/ 2.66 mm /spl times/ 18 mm BGO needles), the maximum photopeak signals occurred at the corner crystal of the block. The signals for the worst central five crystals (sitting on space with no PMT connection) had pulse heights 0.87 as high as that of the corner crystals. The 12 crystals (outside the central five) with coupling only to the glass wall but not to the photocathode had a relative pulse height of 0.92. The eight crystals with partial exposure to photocathodes had a 0.94 relative pulse height. The energy resolution for individual crystals was 22% - 30% with an average of 26%. Asymmetric photopeaks, especially for the corner crystals, were observed, and these were found to be the result of the depth-of-interaction effect. In the latest PQS design, extended blocks with asymmetric light distributions were used on the four edges and four corners of a large detector module so that the previously unused (wasted) half-row of peripheral PMT could be covered by crystals. An asymmetric block, single-extended (7 /spl times/ 8 crystals) was also tested. The pulse-height ratio between the worst and best group of crystals in the single-extended block was 0.72 and that of the double-extended block was also 0.72. In a more demanding, higher spatial resolution 8 /spl times/ 8 array (2.3 mm /spl times/ 2.3 mm /spl times/ 10 mm BGO) for mouse PET with shallower crystals, the pulse-height ratio was 0.73 with an average energy resolution of 20%. This study demonstrated that pulse height uniformity for the PQS design using circular PMT was excellent, better than the typical 3/1 pulse-height ratio in conventional block detectors.
机译:PMT-象限共享(PQS)检测器设计允许以70%的PMT减少和成本降低来构建高分辨率的检测器。该设计的一个常见问题是,四个圆形PMT之间存在很大的间隙(光不敏感区域),并且中心晶体的光电子信号(脉冲高度)可能要低得多。对于高分辨率设计,使用较小的PMT会增加关注,因为小型PMT的壁相对较厚,并且它们之间的公差空间相对较大。作者在19 mm PMT的三种不同类型的PQS模块中测量了每种晶体的脉冲高度和能量分辨率。对于方形7 / spl次/ 7块检测器(2.66 mm / spl次/ 2.66 mm / spl次/ 18 mm BGO针),最大光峰信号出现在块的角晶上。最差的中央五个晶体的信号(坐在没有PMT连接的空间上)的脉冲高度与角晶体的脉冲高度一样高,为0.87。仅耦合至玻璃壁但不耦合至光电阴极的12个晶体(在中心5个晶体之外)具有0.92的相对脉冲高度。部分暴露于光电阴极的八个晶体的相对脉冲高度为0.94。单个晶体的能量分辨率为22%-30%,平均为26%。观察到不对称的光峰,尤其是对角晶体而言,是相互作用深度效应的结果。在最新的PQS设计中,在大型检测器模块的四个边缘和四个角上使用了具有不对称光分布的扩展块,从而使以前未使用(浪费)的外围PMT半行可以被晶体覆盖。还测试了不对称块,单延伸(7次/ spl次/ 8个晶体)。单延伸块中最差和最佳晶体组之间的脉冲高度比为0.72,而双延伸块中的脉冲高度比也为0.72。对于具有较浅晶体的小鼠PET,在要求更高的空间分辨率8 / spl次/ 8阵列(2.3 mm / spl次/ 2.3 mm / spl次/ 10 mm BGO)中,脉冲高度比为0.73,具有平均能量分辨率为20%。这项研究表明,使用圆形PMT的PQS设计的脉冲高度均匀性极好,优于常规块探测器中典型的3/1脉冲高度比。

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