J-PET断层扫描仪的散射分数

P. Kowalski, W. Wi'slicki, L. Raczy'nski, D. Alfs, T. Bednarski, P. Bialas, E. Czerwi'nski, A. Gajos, B. Glowacz, J. Jasi'nska, D. Kami'nska, G. Korcyl, T. Kozik, W. Krzemie'n, E. Kubicz, M. Mohammad, S. Nied'zwiecki, M. Palka, M. Pawlik-Nied'zwiecka, Z. Rudy, M. Silarski, J. Smyrski, A. Strzelecki, A. Wieczorek, B. Zgardzi'nska, M. Zieli'nski, P. Moskal
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引用次数: 20

摘要

一种基于塑料闪烁体的新型正电子发射层析成像系统正在由J-PET合作开发。在本文中,我们给出了散射分数的模拟结果,它代表了NEMA-NU-2-2012规范中定义的背景研究的关键参数之一。我们详细阐述了一种事件选择方法,可以抑制伽马量子在幻体中散射或在探测器中经历多次散射的事件。单层J-PET扫描仪的估计散射分数根据应用的能量阈值在37%到53%之间变化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Scatter fraction of the J-PET tomography scanner
A novel Positron Emission Tomography system, based on plastic scintillators, is being developed by the J-PET collaboration. In this article we present the simulation results of the scatter fraction, representing one of the parameters crucial for background studies defined in the NEMA-NU-2-2012 norm. We elaborate an event selection methods allowing to suppress events in which gamma quanta were scattered in the phantom or underwent the multiple scattering in the detector. The estimated scatter fraction for the single-layer J-PET scanner varies from 37% to 53% depending on the applied energy threshold.
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