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首页> 外文期刊>Physics in medicine and biology. >Towards monolithic scintillator based TOF-PET systems: practical methods for detector calibration and operation
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Towards monolithic scintillator based TOF-PET systems: practical methods for detector calibration and operation

机译:走向单片闪烁体的TOF-PET系统:探测器校准和操作的实用方法

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Gamma-ray detectors based on thick monolithic scintillator crystals can achieve spatial resolutions < 2 mm full-width-at-half-maximum (FWHM) and coincidence resolving times (CRTs) better than 200 ps FWHM. Moreover, they provide high sensitivity and depth-of-interaction (DOI) information. While these are excellent characteristics for clinical time-of-flight (TOF) positron emission tomography (PET), the application of monolithic scintillators has so far been hampered by the lengthy and complex procedures needed for position-and time-of-interaction estimation. Here, the algorithms previously developed in our group are revised to make the calibration and operation of a large number of monolithic scintillator detectors in a TOF-PET system practical. In particular, the k-nearest neighbor (k-NN) classification method for x, y-position estimation is accelerated with an algorithm that quickly preselects only the most useful reference events, reducing the computation time for position estimation by a factor of similar to 200 compared to the previously published k-NN 1D method. Also, the procedures for estimating the DOI and time of interaction are revised to enable full detector calibration by means of fan-beam or flood irradiations only. Moreover, a new technique is presented to allow the use of events in which some of the photosensor pixel values and/or timestamps are missing (e.g. due to dead time), so as to further increase system sensitivity. The accelerated methods were tested on a monolithic scintillator detector specifically developed for clinical PET applications, consisting of a 32 mm x 32 mm x 22 mm LYSO : Ce crystal coupled to a digital photon counter (DPC) array. This resulted in a spatial resolution of 1.7 mm FWHM, an average DOI resolution of 3.7 mm FWHM, and a CRT of 214 ps. Moreover, the possibility of using events missing the information of up to 16 out of 64 photosensor pixels is shown. This results in only a small deterioration of the detector performance.
机译:基于厚整体闪烁体晶体的伽马射线探测器可以实现空间分辨率<2mm全宽半最大(FWHM),并优于200 PS FWHM的巧合分辨率(CRT)。此外,它们提供了高灵敏度和相互作用(DOI)信息。虽然这些是临床飞行时间(TOF)正电子发射断层扫描(PET)的优异特性,但到目前为止,通过相互作用估计所需的漫长和复杂的程序,迄今为止,整体闪烁体的应用已经阻碍了。在这里,预先在我们的组中开发的算法被修改为在TOF-PET系统中的大量单片闪烁体探测器进行校准和操作。特别地,用于X,Y位置估计的k最近邻居(K-NN)分类方法通过算法加速,该算法仅快速预先选择最有用的参考事件,从而减少了相似的定位估计的计算时间200与先前公布的K-NN 1D方法相比。此外,修订了用于估计DOI和交互时间的程序,仅通过扇形梁或洪水照射来实现全检测器校准。此外,提出了一种新技术,以允许使用一些光电传感器像素值和/或时间戳的事件(例如由于死区时间),从而进一步提高系统灵敏度。在专门为临床PET应用的单片闪烁体检测器上测试加速方法,由32mm×32mm×22mmLyso组成:Ce晶体耦合到数字光子计数器(DPC)阵列。这导致空间分辨率为1.7mm FWHM,平均DOI分辨率为3.7mm FWHM,以及214ps的CRT。此外,示出了使用缺少64个光电导像素中最多16个信息的事件的可能性。这导致探测器性能的小恶化。

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