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Improvement of the depth of interaction detector for PET on full energy pulse height uniformity

机译:全能脉冲高度均匀性PET相互作用深度检测仪的改进

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摘要

As part of the next generation PET project, uniformity of full energy pulse height for all crystal elements was improved in the depth of interaction (DOI) detector constructed of three-dimensional crystal arrays. In our previous report, we found that the DOI detector constructed of four stages of a 2 /spl times/ 2 Gd/sub 2/SiO/sub 5/:Ce (GSO) crystal array provides good crystal identification performance but poor uniformity of the energy pulse height distribution. The upper stage crystal elements which stay further from the photocathode of a PMT have a tendency to show lower energy pulse height. For example, the ratio of the full energy peak of the top stage crystal to the bottom stage one was about 0.3. We designed a new DOI detector improved in the uniformity. By optimizing crystal surface finishes, reflector configurations, and optical coupling between crystal elements, we got comparable energy pulse height from the upper stage crystals to the bottom stage crystals. Despite this change of detector conditions, good separation between each area corresponding to crystal elements is maintained on two-dimensional histograms obtained by Anger-type position calculation. The uniform full energy pulse height of every stage crystal allows a narrower dynamic range of the electrical circuits, and may give a great advantage in getting an accurate scatter correction. It also improves energy and timing resolution.
机译:作为下一代PET项目的一部分,在由三维晶体阵列构成的相互作用深度(DOI)检测器中,所有晶体元素的全能脉冲高度的均匀性得到了改善。在我们之前的报告中,我们发现由2个/ spl次/ 2 Gd / sub 2 / SiO / sub 5 /:Ce(GSO)晶体阵列的四个阶段构成的DOI检测器提供了良好的晶体识别性能,但均匀性较差。能量脉冲高度分布。与PMT的光电阴极相距较远的上层晶体元素倾向于显示出较低的能量脉冲高度。例如,顶层晶体的全能峰与底层晶体的全能峰之比约为0.3。我们设计了一种改进了均匀性的新型DOI检测器。通过优化晶体的表面光洁度,反射器配置以及晶体元件之间的光学耦合,我们获得了从上级晶体到下级晶体可比的能量脉冲高度。尽管检测器条件发生了这种变化,但在通过Anger型位置计算获得的二维直方图上,与晶体元素相对应的每个区域之间仍保持了良好的分隔。每级晶体的均匀全能量脉冲高度允许电路的动态范围更窄,并且在获得准确的散射校正方面可能具有很大的优势。它还提高了能量和时序分辨率。

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