首页> 外国专利> Insensitivity time correction method in quantitative positron emission tomography (PET) reconstruction for various subjects and radioactivity distributions

Insensitivity time correction method in quantitative positron emission tomography (PET) reconstruction for various subjects and radioactivity distributions

机译:各种科目和放射性分布定量正电子发射断层扫描(PET)重建的不敏感时间校正方法

摘要

To perform the image reconstruction method 100, the non-temporary computer-readable medium stores instructions that can be read and executed by the workstation 18 including at least one electronic processor 20. The method is a step of determining the singles rate of the plurality of radiation detectors in the frame of the imaging data detected by the plurality of radiation detectors 17; the energy correction coefficient Nwgt for each radiation detector is acquired in the frame of the imaging data. Steps to determine based on the energy spectrum distribution of gamma rays incident on the radiation detector; the singles effective counting time correction coefficient for each radiation detector is determined for the singles factor and the energy for the radiation detector. Steps to determine from the correction coefficient; Steps to determine the system coincidence effective counting time correction coefficient from the system singles rate; For each LOR of a plurality of simultaneous counting lines (LORs) connecting a pair of radiation detectors, for the LOR The step of determining the effective counting time correction coefficient from the determined singles effective counting time correction coefficient and the determined system coincidence counting effective counting time correction coefficient of the pair of radiation detectors connected by the LOR; and the imaging data. Includes the step of reconstructing the frame of the above using the effective counting time correction coefficient for the determined LOR;
机译:为了执行图像重建方法100,非临时计算机可读介质存储由包括至少一个电子处理器20的工作站18可以读取和执行的指令。该方法是确定多个单个速率的步骤由多个辐射检测器17检测到的成像数据框架中的辐射检测器;在成像数据的帧中获取每个辐射检测器的能量校正系数NWGT。基于辐射探测器入射在辐射探测器上的伽马射线能谱分布的步骤;单打有效计数每个辐射检测器的时间校正系数用于单打因子和用于辐射检测器的能量。从校正系数确定的步骤;从系统单打率确定系统重合计数时间校正系数的步骤;对于连接一对辐射检测器的多个同时计数线(LOR)的每个LOR,对于LOR确定从所确定的单个有效计数时间校正系数和确定的系统巧合计数有效计数的有效计数时间校正系数的步骤由LOR连接的一对辐射检测器的时间校正系数;和成像数据。包括使用所确定的LOR的有效计数时间校正系数来重建上述帧的步骤;

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