基于FPGA处理的单片PET探测器三维光子冲击测定

A. Aguilar, M. Galasso, J. Barberá, C. Correcher, A. Fabbri, L. Hernández, Antonio J. González, J. Benlloch
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引用次数: 3

摘要

这项工作展示了在PET系统中精确确定单片闪烁晶体内伽马射线冲击位置的新方法的实现。这些方法已在安装在脑PET插入器MindView数据采集系统(DAQ)的每个ADC板上的FPGA (Kintex 7)上实现,以实时提供511kev光子撞击坐标。比较了两种不同的方法:常用的重心(CoG)方法和一种名为RTP(提高到幂)的替代方法,该方法结合了伽马光子DOI(相互作用深度)的估计。DOI是通过每个光分布的能量与峰值最大强度的比值来估计的。尽管CoG已在dsp上实现,但基于lut的RTP方法提高了性能,将处理时间从1μ ns减少到640 ns。包括当前开发在内,已实现的时间性能约为640 ns,确保以高数据速率处理所有检测到的事件。用FPGA实现得到的结果与直接将全部原始数据传输到PC工作站后脱机处理的数据进行了比较。在这里,我们在空间分辨率和DOI能力方面比较了探测器图像质量,没有观察到任何差异。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
3D photon impact determination in monolithic based PET detectors using FPGA processing
This work shows the implementation of novel methods to accurately determine the gamma ray impact position within monolithic scintillation crystals in PET systems. These methods have been implemented in an FPGA (Kintex 7) installed on each ADC board of the data acquisition system (DAQ) of the brain PET insert named MindView to provide the 511 keV photon impinging coordinates in real time. Two different methods have been compared: the commonly used Center of Gravity (CoG) approach and an alternative method named RTP (Raise To the Power) in combination with an estimation of the gamma photons DOI (depth of interaction). The DOI is estimated through the ratio of the energy to the peak maximum intensity of each light distribution. Despite CoG has been implemented with DSPs, performance has been improved with the RTP approach LUT-based, reducing the processing time from 1μ to 640 ns. The achieved time performance including the current development has been measured to be around 640 ns, ensuring the processing of all detected events at high data rates. The obtained results using the FPGA implementation have been compared to data processed off-line after directly transferred the whole raw data to a PC workstation. Here, we compared detector image quality in terms of spatial resolution and DOI capabilities without observing any difference.
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