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Multi-contrast imaging on dual-source photon-counting-detector (PCD) CT

机译:双源光子计数检测器(PCD)CT上的多对比度成像

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Photon-counting-detector (PCD) CT can provide multiple energy bin data sets and allows single-acquisition, multiple-contrast-injection imaging using materials such as iodine, gadolinium and bismuth. However, due to technical limitations, PCDs can suffer from compromised energy-resolving capability, which degrades multicontrast imaging performance. In this work, we investigate the use of a dual-source (DS)-PCD system architecture with additional beam filtration to improve spectral separation among energy bin data sets, and quantify its performance for multi-contrast imaging. Experiments were performed using a CT phantom including various concentrations of iodine (I), gadolinium (Gd) and bismuth (Bi). The DS-PCD architecture was emulated by scanning the same phantom twice on a single-source (SS) PCD-CT with two different tube potentials: 80 kV (energy thresholds = 25/50 keV), and 140 kV (energy thresholds = 25/90 keV) with a 0.4-mm tin filter. We further compared material decomposition performance using the proposed DS-PCD approach with that of the current SS-PCD approach. For the SS-PCD, chess mode with 4 energy bins was used, with energy thresholds of 25/50/75/90 keV to resolve the K-edges of Gd and Bi. The mean energies of the four energy bins in SS-PCD were 72/76/93/109 keV, while those of the four energy bins using DS-PCD were 57/64/88/111 keV, denoting a better spectral separation using DS-PCD. The material quantification root mean square error (RMSE) was reduced from 4.5/3.3/1.2 mg/mL for iodine/Gd/Bi using SS-PCD, to 1.4/1.2/1.1 mg/mL using DS-PCD. These results demonstrate that the DS-PCD can improve multi-contrast imaging performance compared to a SS-PCD acquisition.
机译:光子计数检测器(PCD)CT可以提供多个能量箱数据集,并允许单获取,使用碘,钆和铋等材料进行多重对比注射成像。但是,由于技术限制,PCD可以遭受受损的能量 - 解析能力,这降低了多模量成像性能。在这项工作中,我们调查了双源(DS)-PCD系统架构的使用具有额外的光束过滤,以改善能量箱数据集之间的光谱分离,并量化其对多对比度成像的性能。使用包括各种浓度的碘(I),钆(Gd)和铋(BI)进行实验。通过两个不同的管电位扫描两次在单源(SS)PCD-CT上两次扫描DS-PCD架构:80 kV(能量阈值= 25/50kev)和140 kV(能量阈值= 25 / 90 kev)用0.4mm锡过滤器。我们进一步使用所提出的DS-PCD方法与当前的SS-PCD方法进行比较了材料分解性能。对于SS-PCD,使用具有4个能量箱的国际象棋模式,能量阈值为25/50/75/90 Kev以解决GD和BI的K边缘。 SS-PCD中的四个能量箱的平均能量为72/76/93/109 kev,而使用DS-PCD的四个能量箱的速度为57/64/88/111 keV,表示使用DS的更好的光谱分离-pcd。使用SS-PCD的碘/ GD / BI的材料量化均方误差(RMSE)从4.5 / 3.3 / 1.2mg / ml降低至1.4 / 1.2 / 1.1mg / ml,使用DS-PCD。这些结果表明,与SS-PCD采集相比,DS-PCD可以改善多对比度成像性能。

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