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Positioning true coincidences that undergo inter- and intra-crystal scatter for a sub-mm resolution cadmium zinc telluride-based PET system

机译:对于亚毫米分辨率的碲化镉锌基PET系统发生晶体间和晶体内散射的真正巧合的定位

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摘要

The kinematics of Compton scatter can be used to estimate the interaction sequence of inter-crystal scatter interactions in 3-D position-sensitive cadmium zinc telluride (CZT) detectors. However, in the case of intra-crystal scatter in a “cross-strip” CZT detector slab, multiple anode and cathode strips may be triggered, creating position ambiguity due to uncertainty in possible combinations of anode-cathode pairings. As a consequence, methods such as energy-weighted centroid are not applicable to position the interactions. In practice, since the event position is uncertain, these intra-crystal scatters events are discarded. In this work, we studied using Compton kinematics and a “direction difference angle” to provide a method to correctly identify the anode-cathode pair corresponding to the first interaction position in an intra-crystal scatter event. GATE simulation studies of a NEMA NU4 image quality phantom in a small animal positron emission tomography under development composed of 192, 40 mm×40 mm×5 mm CZT crystals shows that 47% of total numbers of multiple-interaction photon events (MIPEs) are intra-crystal scatter with a 100 keV lower energy threshold per interaction. The sensitivity of the system increases from 0.6 to 4.10 (using 10 keV as system lower energy threshold) by including rather than discarding inter- and intra-crystal scatter. The contrast-to-noise ratio (CNR) also increases from 5.81±0.3 to 12.53±0.37. It was shown that a higher energy threshold limits the capability of the system to detect MIPEs and reduces CNR. Results indicate a sensitivity increase (4.1 to 5.88) when raising the lower energy threshold (10 keV to 100 keV) for the case of only two-interaction events. In order to detect MIPEs accurately, a low noise system capable of a low energy threshold (10 keV) per interaction is desired.
机译:康普顿散射的运动学可用于估计3-D位置敏感的碲化​​镉锌(CZT)检测器中晶间散射相互作用的相互作用序列。但是,在“交叉带状” CZT检测器平板中发生晶体内散射的情况下,可能会触发多个阳极条和阴极条,由于阳极-阴极对可能组合的不确定性而造成位置模糊。结果,诸如能量加权质心的方法不适用于定位相互作用。实际上,由于事件位置不确定,因此将丢弃这些晶体内散射事件。在这项工作中,我们使用康普顿运动学和“方向差角”进行了研究,以提供一种正确识别晶体内散射事件中对应于第一相互作用位置的阳极-阴极对的方法。 GATE对由192个40 mm×40 mm×5 mm CZT晶体组成的小型动物正电子发射断层扫描中的NEMA NU4图像质量幻像的GATE模拟研究表明,多相互作用光子事件(MIPE)总数的47%是晶体内散射,每次相互作用的能量阈值低100 keV。通过包括而不是丢弃晶体间和晶体内散射,系统的灵敏度从0.6提高到4.10(使用10 keV作为系统较低的能量阈值)。对比噪声比(CNR)也从5.81±0.3增加到12.53±0.37。结果表明,较高的能量阈值限制了系统检测MIPE的能力并降低了CNR。结果表明,对于仅两次相互作用的事件,提高下限能量阈值(10 keV至100 keV)时,灵敏度会提高(4.1至5.88)。为了准确地检测MIPE,需要每个交互都具有低能量阈值(10 keV)的低噪声系统。

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