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Robustness of optimal energy thresholds in photon-counting spectral CT

机译:光子计数光谱CT中最佳能量阈值的鲁棒性

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摘要

An important question when developing photon-counting detectors for computed tomography is how to select energy thresholds. In this work thresholds are optimized by maximizing signal-difference-to-noise ratio squared (SDNR2) in an optimally weighted image and signal-to-noise ratio squared (SNR2) in a gadolinium basis image in a silicon-strip detector and a cadmium zinc telluride (CZT) detector, factoring in pileup and imperfect energy response based on real-world detector systems. To investigate to what extent one single set of thresholds could be applied in various imaging tasks, the robustness of optimal thresholds with 2 to 8 bins is examined with the variation of phantom thicknesses, target materials and detector configurations. In contrast to previous studies, the optimal threshold locations do not always increase with increasing attenuation if pileup is included. With respect to the tradeoff between higher SDNR~2 or SNR~2 and less data, setting optimal thresholds for a 30 cm phantom yields robust SDNR~2 and setting optimal thresholds for a 50 cm phantom yields robust SNR2 with 6 to 8 bins in the silicon-strip detector. Furthermore, setting optimal thresholds for a 30 cm phantom yields robust SDNR~2 or SNR~2 with 6 to 8 bins and a pixel size less than or equal to 0.5 × 0.5 mm~2 in the CZT detector.
机译:在为计算机断层扫描开发光子计数检测器时的一个重要问题是如何选择能量阈值。在该工作中,通过在硅条检测器中的钆基图像中最佳地加权图像和信噪比(SNR2)中的信号差异对噪声比(SDNR2)在硅条检测器和镉中进行正方形(SNR2)来优化阈值。锌碲化物(CZT)探测器,基于现实世界探测器系统的堆积,堆积和不完美的能源响应。为了调查在各种成像任务中可以应用一组单个阈值的程度,通过体模厚度,目标材料和检测器配置的变化来检查具有2到8个箱的最佳阈值的鲁棒性。与先前的研究相比,如果包括堆叠,则最佳阈值位置并不总是随着衰减而增加。关于更高SDNR〜2或SNR〜2之间的折衷和数据较少,为30cm虚线设定最佳阈值稳健的SDNR〜2,并且为50cm的PHANTOM设定最佳阈值产生强大的SNR2,其中6到8个箱硅条探测器。此外,在CZT检测器中设定具有6至8个箱的鲁棒SDNR〜2或SNR〜2的鲁棒SDNR〜2或SNR〜2的最佳阈值。

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  • 作者单位

    Department of Physics Royal Institute of Technology AVaanova University Center SE-106 91 Stockholm Sweden Key Laboratory of Particle and Radiation Imaging (Ministry of Education) and Department of Engineering Physics Tsinghua University Beijing 100084 China;

    Prismatic Sensors AB Roslagstullsbacken 21 Stockholm 106 91 Sweden;

    Department of Physics Royal Institute of Technology AVaanova University Center SE-106 91 Stockholm Sweden;

    Department of Physics Royal Institute of Technology AVaanova University Center SE-106 91 Stockholm Sweden Prismatic Sensors AB Roslagstullsbacken 21 Stockholm 106 91 Sweden;

    Key Laboratory of Particle and Radiation Imaging (Ministry of Education) and Department of Engineering Physics Tsinghua University Beijing 100084 China;

    Department of Physics Royal Institute of Technology AVaanova University Center SE-106 91 Stockholm Sweden Prismatic Sensors AB Roslagstullsbacken 21 Stockholm 106 91 Sweden;

    Department of Physics Royal Institute of Technology AVaanova University Center SE-106 91 Stockholm Sweden Departments of Bioengmeering and Radiology Stanford University Stanford 94305 CA USA;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Photon counting; Spectral CT; Threshold optimization; Silicon-strip detector; CZT detector;

    机译:光子计数;光谱CT;阈值优化;硅条探测器;CZT探测器;

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