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Performance of 256ch flat panel PS-PMT with small crystals for a DOI PET detector

机译:带有小晶体的256通道平板PS-PMT在DOI PET探测器中的性能

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A 256ch flat panel position sensitive photomultiplier tube (256ch FP-PMT) was evaluated for application to a depth of interaction (DOI) PET detector composed of small crystal elements. The 256ch FP-PMT has 52 mm/spl times/52 mm opening area with 89% useful area. Its 256 anodes are placed at a 3.04 mm interval. To estimate the FP-PMT performance, light spread functions of anodes at central and peripheral regions of a prototype 256ch FP-PMT were measured with a Gd/sub 2/SiO/sub 5/ (GSO) crystal sized 1.42 mm/spl times/1.42 mm/spl times/4.5 mm, one quarter of the area of the FP-PMT anode area. It was found that light spread functions of peripheral anodes were similar to the functions of central anodes and also the functions measured with a 2.9 mm/spl times/2.9 mm/spl times/7.5 mm GSO crystal, almost the same size as the anode area. Transit time fluctuation among the 256ch FP-PMT anodes was estimated by measuring time resolutions of a LuYSiO/sub 5/ (LYSO) crystal at some central and peripheral positions. The LYSO crystal has the same dimensions as the smaller GSO crystal BaF/sub 2/ was used for a reference detector. The obtained distributions show about the same time resolution between the central and peripheral positions and the full width at half maximum is (366/spl plusmn/15) ps. The transit time fluctuation is /spl plusmn/106 ps. Two-dimensional position histograms of a 32/spl times/32 GSO crystal array and two layers of 9/spl times/9 GSO crystal arrays are obtained by uniform gamma-ray irradiation. The crystal dimensions are 1.42 mm/spl times/1.42 mm/spl times/4.5 mm. The 32/spl times/32 array covers all the useful area. The 9/spl times/9/spl times/2 array is coupled to peripheral region. The resultant histograms confirm that a 256ch FP-PMT has enough capability for identifying crystals of this size even on the periphery.
机译:对256通道平板位置敏感光电倍增管(256通道FP-PMT)进行了评估,以应用于由小晶体元素组成的相互作用深度(DOI)PET检测器。 256通道FP-PMT具有52 mm / spl次/ 52 mm的开口面积,有用面积为89%。它的256个阳极以3.04 mm的间隔放置。为了估算FP-PMT性能,使用尺寸为1.42 mm / spl倍/秒的Gd / sub 2 / SiO / sub 5 /(GSO)晶体测量了256ch FP-PMT原型阳极中心和外围区域的阳极光扩散函数。 1.42 mm / spl倍/4.5 mm,是FP-PMT阳极面积的四分之一。发现外围阳极的光扩散函数与中央阳极的函数相似,并且还使用2.9 mm / spl次/2.9 mm / spl次/7.5 mm GSO晶体测量的函数,其尺寸几乎与阳极面积相同。通过测量LuYSiO / sub 5 /(LYSO)晶体在某些中心和外围位置的时间分辨率,可以估算256ch FP-PMT阳极之间的过渡时间波动。 LYSO晶体与用于参考检测器的较小的GSO晶体BaF / sub 2 /具有相同的尺寸。所获得的分布显示出中心位置和外围位置之间大约相同的时间分辨率,半高处的全宽为(366 / spl plusmn / 15)ps。渡越时间波动为/ spl plusmn / 106 ps。通过均匀的γ射线辐照获得32 / spl×3/32 GSO晶体阵列和两层9 / spl×3/9 GSO晶体阵列的二维位置直方图。晶体尺寸为1.42mm / spl倍/1.42mm/spl倍/4.5mm。 32 / spl times / 32数组覆盖了所有有用的区域。 9 / spl times / 9 / spl times / 2阵列耦合到外围区域。所得直方图证实,即使在外围,256ch FP-PMT也具有足够的能力来识别这种尺寸的晶体。

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