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首页> 外文期刊>Korean journal of radiology : >Accuracy of Model-Based Iterative Reconstruction for CT Volumetry of Part-Solid Nodules and Solid Nodules in Comparison with Filtered Back Projection and Hybrid Iterative Reconstruction at Various Dose Settings: An Anthropomorphic Chest Phantom Study
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Accuracy of Model-Based Iterative Reconstruction for CT Volumetry of Part-Solid Nodules and Solid Nodules in Comparison with Filtered Back Projection and Hybrid Iterative Reconstruction at Various Dose Settings: An Anthropomorphic Chest Phantom Study

机译:在不同剂量设置下,基于模型的迭代重建部分实性结节和实性结节的CT容积与过滤后向投影和混合迭代重建的准确性:拟人化的胸部幻影研究

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Objective To investigate the accuracy of model-based iterative reconstruction (MIR) for volume measurement of part-solid nodules (PSNs) and solid nodules (SNs) in comparison with filtered back projection (FBP) or hybrid iterative reconstruction (HIR) at various radiation dose settings. Materials and Methods CT scanning was performed for eight different diameters of PSNs and SNs placed in the phantom at five radiation dose levels (120 kVp/100 mAs, 120 kVp/50 mAs, 120 kVp/20 mAs, 120 kVp/10 mAs, and 80 kVp/10 mAs). Each CT scan was reconstructed using FBP, HIR, or MIR with three different image definitions (body routine level 1 [IMR-R1], body soft tissue level 1 [IMR-ST1], and sharp plus level 1 [IMR-SP1]; Philips Healthcare). The SN and PSN volumes including each solid/ground-glass opacity portion were measured semi-automatically, after which absolute percentage measurement errors (APEs) of the measured volumes were calculated. Image noise was calculated to assess the image quality. Results Across all nodules and dose settings, the APEs were significantly lower in MIR than in FBP and HIR (all p 0.01). The APEs of the smallest inner solid portion of the PSNs (3 mm) and SNs (3 mm) were the lowest when MIR (IMR-R1 and IMR-ST1) was used for reconstruction for all radiation dose settings. (IMR-R1 and IMR-ST1 at 120 kVp/100 mAs, 1.06 ± 1.36 and 8.75 ± 3.96, p 0.001; at 120 kVp/50 mAs, 1.95 ± 1.56 and 5.61 ± 0.85, p = 0.002; at 120 kVp/20 mAs, 2.88 ± 3.68 and 5.75 ± 1.95, p = 0.001; at 120 kVp/10 mAs, 5.57 ± 6.26 and 6.32 ± 2.91, p = 0.091; at 80 kVp/10 mAs, 5.84 ± 1.96 and 6.90 ± 3.31, p = 0.632). Image noise was significantly lower in MIR than in FBP and HIR for all radiation dose settings (120 kVp/100 mAs, 3.22 ± 0.66; 120 kVp/50 mAs, 4.19 ± 1.37; 120 kVp/20 mAs, 5.49 ± 1.16; 120 kVp/10 mAs, 6.88 ± 1.91; 80 kVp/10 mAs, 12.49 ± 6.14; all p 0.001). Conclusion MIR was the most accurate algorithm for volume measurements of both PSNs and SNs in comparison with FBP and HIR at low-dose as well as standard-dose settings. Specifically, MIR was effective in the volume measurement of the smallest PSNs and SNs.
机译:目的探讨在各种辐射下与基于滤波的反投影(FBP)或混合迭代重建(HIR)相比,基于模型的迭代重建(MIR)进行部分固体结节(PSNs)和固体结节(SNs)体积测量的准确性剂量设定。材料和方法以五个辐射剂量级别(120 kVp / 100 mAs,120 kVp / 50 mAs,120 kVp / 20 mAs,120 kVp / 10 mAs和80 kVp / 10 mAs)。每次CT扫描都是使用FBP,HIR或MIR重建的,具有三种不同的图像定义(身体常规水平1 [IMR-R1],身体软组织水平1 [IMR-ST1]和锐利加水平1 [IMR-SP1];飞利浦医疗保健)。半自动测量包括每个固体/毛玻璃不透明部分的SN和PSN体积,然后计算所测量体积的绝对百分比测量误差(APE)。计算图像噪声以评估图像质量。结果在所有结节和剂量设置中,MIR的APE显着低于FBP和HIR(所有p <0.01)。当将MIR(IMR-R1和IMR-ST1)用于所有辐射剂量设置的重建时,PSN(3mm)和SN(3mm)的最小内部固体部分的APE最低。 (IMR-R1和IMR-ST1在120 kVp / 100 mAs时,1.06±1.36和8.75±3.96,p <0.001;在120 kVp / 50 mAs时,1.95±1.56和5.61±0.85,p = 0.002;在120 kVp / 20 mA,2.88±3.68和5.75±1.95,p = 0.001;在120 kVp / 10 mAs,5.57±6.26和6.32±2.91,p = 0.091;在80 kVp / 10 mAs,5.84±1.96和6.90±3.31,p = 0.632)。在所有辐射剂量设置下(120 kVp / 100 mAs,3.22±0.66; 120 kVp / 50 mAs,4.19±1.37; 120 kVp / 20 mAs,5.49±1.16; 120 kVp),MIR中的图像噪声显着低于FBP和HIR / 10 mAs,6.88±1.91; 80 kVp / 10 mAs,12.49±6.14;所有p <0.001)。结论与低剂量和标准剂量设置下的FBP和HIR相比,MIR是对PSN和SN进行体积测量的最准确算法。具体而言,MIR在最小的PSN和SN的体积测量中很有效。

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