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Use of a central positron emitting reference source to improve the timing alignment of a singles list-mode small animal PET scanner

机译:使用中央正电子发射参考源改善单打列表模式小动物PET扫描仪的时序对准

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To minimize the system-wide timing resolution of a PET scanner, and hence the applied coincidence window, a delay must be added to the signals from each crystal to compensate for inherent time differences between detectors. Without an absolute time reference, this must be been done iteratively. We propose using a new timing probe, consisting of a Ge-68 source imbedded in a plastic scintillator coupled to a fast PMT, to time-calibrate the MADPET-II small animal PET scanner. The probe provides a precise trigger signal with each positron decay and emission of 511 keV photons and, when placed in the center of the scanner, allows all crystals to be aligned to a common reference. MADPET-II is based on the one-to-one coupling of LSO crystals to APD detectors, each of which is read out by a dedicated electronic channel. Time stamps for each singles event are stored in list-mode format, allowing time offsets to be assigned directly to each detector. Signals from the probe were fed into an Ortec 934 CFD, and the trigger signals were digitised using the MADPET-II data acquisition system. Histograms generated by the time difference between the detection of 511 keV photons in the detectors and the corresponding positron decay in the probe give the time offsets for each crystal. After applying the offsets to the singles data, the system-wide timing resolution of the 256 channel MADPET-II prototype improved from 16.5 ns FWHM to 10.2 ns FWHM (450 keV threshold, F-18 flood source).
机译:为了使PET扫描仪的系统范围内的定时分辨率最小化,并因此使应用的重合窗口最小化,必须将延迟添加到每个晶体的信号中,以补偿检测器之间的固有时间差。如果没有绝对的时间参考,则必须迭代完成。我们建议使用一种新的定时探头,该探头由嵌入在与快速PMT耦合的塑料闪烁体中的Ge-68光源组成,以对MADPET-II小动物PET扫描仪进行时间校准。该探头可为每个正电子衰减并发射511 keV光子提供精确的触发信号,当放置在扫描仪中心时,它可使所有晶体对准同一参考。 MADPET-II基于LSO晶体与APD检测器的一对一耦合,每个检测器均通过专用电子通道读取。每个单打事件的时间戳以列表模式格式存储,从而可以将时间偏移量直接分配给每个检测器。来自探头的信号被馈送到Ortec 934 CFD中,并使用MADPET-II数据采集系统将触发信号数字化。由检测器中511 keV光子的检测与探针中相应的正电子衰减之间的时间差产生的直方图给出了每个晶体的时间偏移。将偏移量应用于单声道数据后,256通道MADPET-II原型的系统级时序分辨率从16.5 ns FWHM提高到10.2 ns FWHM(450 keV阈值,F-18泛光源)。

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