提高连续微型晶元(cMiCE)探测器的固有空间分辨率。

Tao Ling, Tom K Lewellen, Robert S Miyaoka
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引用次数: 6

摘要

我们之前已经报道了由50mm × 50mm × 8mm厚的LYSO板与64通道平板PMT耦合组成的cMiCE探测器的性能特征。在这项工作中,所有64个PMT通道都被数字化,并使用基于统计的定位方法进行事件定位。在表征探测器时,即使使用我们的SBP方法,晶体角段的固有空间分辨率性能也比晶体中心部分下降。我们认为,在弯角定位性能较差是因为大部分光线丢失(即,没有被我们的PMT收集)。为了解决这个问题,我们建议在沿晶体短边缘的角落放置光传感器(即微像素雪崩光电二极管,MAPD)。新设计将需要额外的8个MAPD器件。通过蒙特卡罗仿真比较了原cMiCE设计和新增强设计的性能。给出了利用DETECT2000进行仿真的结果。除了进行光线追踪外,GEANT还用于跟踪晶体中的伽马相互作用(即康普顿散射和光电吸收)。因此,模拟包括康普顿散射在探测器中的影响。结果表明,加入传感器后,晶体边角部分的固有空间分辨率从0.99 mm FWHM提高到0.79 mm FWHM,从而接近晶体中心部分(0.73 mm FWHM)的固有空间分辨率。这些结果是基于使用双doi查找表得出的。额外的结果是,能量直方图仅使用来自平板PMT的64通道比使用所有72个信号通道更好。
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Improving the intrinsic spatial resolution performance of the continuous miniature crystal element (cMiCE) detector.

We have previously reported performance characteristics of a cMiCE detector composed of a 50 mm by 50 mm by 8 mm thick slab of LYSO, coupled to a 64 channel flat-panel PMT. In that work, all 64 PMT channels were digitized and a statistics-based positioning method was used for event positioning. In characterizing the detector, the intrinsic spatial resolution performance for the corner sections of the crystal was degraded compared to the central section of the crystal, even when using our SBP method. It is our belief that the poorer positioning performance at the corners is because much of the light is lost (i.e., not collected by our PMT). To offset this problem, we propose to place light sensors (i.e., micro-pixel avalanche photo diodes, MAPD) at the corners along the short edge of the crystal. The new design would require an additional 8 MAPD devices. Monte Carlo simulation was used to compare the performance of the original cMiCE design and this new enhanced design. Simulation results using DETECT2000 are presented. In addition to doing light ray tracing, GEANT was used to track gamma interactions (i.e., Compton scatter and photoelectric absorption) in the crystal. Thus the simulations include the effects of Compton scatter in the detector. Results indicate that adding the sensors improves the intrinsic spatial resolution performance from 0.99 mm FWHM to 0.79 mm FWHM for the corner section of the crystal, thereby nearly matching the intrinsic spatial resolution of the center section of the crystal (i.e., 0.73 mm FWHM). These results are based upon using dual-DOI look up tables. Additional results were that energy histograms were better using just the 64 channels from the flat panel PMT than using all 72 signal channels.

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