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Signal Characteristics of Individual Crystals in a High Resolution BGO Detector Design Using PMT-Quadrant Sharing

机译:高分辨率BGO探测器设计中各个晶体的信号特性使用PMT - 象限分享

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The PMT-quadrant sharing (PQS) detector design allows very high resolution detectors to be achieved with 70% fewer PMT and cost. A common concern for the design is that there is a big gap (photo-insensitive area) between 4 circular PMT, and the photoelectron signal (pulse height) may be much lower for the central crystals. The pulse heights and energy resolution for each crystal in 3 different types of PQS blocks for 19 mm PMT have been measured. For a regular square 7×7 block (2.66 ×2.66 ×18 mm BGO): the maximum photopeak signals occurred at the corner crystal of the block. The signals for the worst central-5 crystals (sitting on space with no PMT connection) was found to have pulse heights of 0.87 that of the corner crystals. The 12 crystals (outside the central-5) coupling only to the glass wall but not photocathode had a relative pulse height of 0.92. The 8 crystals with partial exposure to photocathodes had 0.94. The energy resolution for individual crystal was found to be 22-30% with an average of 26%. Asymmetric photopeaks, especially for the corner crystals, were observed, which was found to be from the depth-of-interaction effect. In the latest PQS design, extended blocks with asymmetric light distributions were used on the 4 edges and 4 corners of a large detector module so that the previously unused (wasted) half-row of peripheral PMT are now covered by crystals. An asymmetric blocks, single-extended (7x8 blocks) was also tested. The pulse-height ratio between the worst and best group of crystals in the single-extended block was found to be 0.72 and that of the double extended block was also found to be 0.72. In a more demanding, higher spatial resolution 8×8 array (2.3 × 2.3 × 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, which is better than the typical 4/1 pulse-height ratio in conventional block detectors.
机译:PMT - 象限共享(PQS)检测器设计允许使用70%的PMT和成本实现非常高分辨率的探测器。设计的共同关心是,在4个圆形PMT之间存在大的间隙(光不敏感区域),并且光电子信号(脉冲高度)对于中央晶体可能会低得多。已经测量了3种不同类型PQS块的每个晶体的脉冲高度和能量分辨率。对于常规方形7×7块(2.66×2.66×18 mm BGO):最大PhotoPak信号发生在块的拐角晶体处。发现最糟糕的Central-5晶体的信号(坐在没有PMT连接的空间上)具有0.87的角晶体的脉冲高度。仅12个晶体(中心-5)仅耦合到玻璃壁但非光电阴极的相对脉冲高度为0.92。具有部分暴露于光电阴极的8个晶体有0.94。发现个体晶体的能量分辨率为22-30%,平均为26%。观察到不对称的PhotoPaks,特别是对于角晶体,其被发现来自相互作用的效果。在最新的PQS设计中,在大型检测器模块的4个边缘和4个角上使用具有不对称光分布的扩展块,以便先前未使用(浪费)半行的外围PMT现在被晶体覆盖。还测试了一个不对称块,单扩展(7x8块)。发现单延长块中最差和最佳的晶体之间的脉冲高比率为0.72,并且还发现双延长块的脉冲高比率为0.72。在更苛刻的,具有浅晶体的小鼠PET的较高空间分辨率8×8阵列(2.3×2.3×10mm),脉冲高比例为0.73,平均能量分辨率为20%。本研究表明,使用圆形PMT的PQS设计的脉冲高度均匀性优异,其优于传统块检测器中的典型4/1脉冲高比。

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