Design of a "3.5th generation" photon counting detector CT architecture for higher spatial resolution and decreased ring artifact.

Scott S Hsieh
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Abstract

Fourth generation CT was originally conceived to reduce ring artifacts from inhomogeneities in early energy integrating detector (EID) modules. These inhomogeneities are well controlled in modern EID modules but have reappeared in photon counting detector (PCD) modules, where fabrication techniques are not yet mature. Fourth generation CT was abandoned decades ago because of its high cost and scatter. We propose grafting its central insight into 3rd generation CT using a compact, modified X-ray source that operates with a high-speed flying focal spot over a limited range of travel (e.g., 1 cm). The PCD must be modified so that measured data is rebinned on-the-fly, so that data bandwidth requirements across the slip ring are unchanged. In this geometry, data from each PCD pixel is distributed to a several contiguous radial indices. This reduces ring artifacts that stem from pixel inhomogeneities and also allows recovery of missing data that is due to dead pixels or occlusion by the anti-scatter grid. Finally, if the dwell time at each focal spot location is very short (sub-microsecond), the maximum instantaneous surface temperature at the anode is reduced. This could be used to reduce focal spot size while maintaining the thermal limit of the focal track.

“3.5代”光子计数检测器CT结构设计,提高空间分辨率,减少环形伪影。
第四代CT最初的设想是为了减少早期能量积分检测器(EID)模块中不均匀性造成的环形伪影。这些不均匀性在现代EID模块中得到了很好的控制,但在光子计数检测器(PCD)模块中再次出现,其中制造技术尚未成熟。第四代CT由于成本高且分散,在几十年前就被废弃了。我们建议将其核心洞察力嫁接到第三代CT中,使用紧凑的改良x射线源,该x射线源在有限的旅行范围内(例如,1厘米)使用高速飞行焦斑。必须修改PCD,以便实时调整测量数据,从而保持整个滑环的数据带宽需求不变。在这种几何结构中,来自每个PCD像素的数据被分布到几个连续的径向指数中。这减少了由像素不均匀引起的环形伪影,也允许恢复由于死像素或反散射网格遮挡而丢失的数据。最后,如果每个焦点位置的停留时间非常短(亚微秒),则阳极的最高瞬时表面温度会降低。这可用于减小焦斑尺寸,同时保持焦迹的热极限。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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