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CT衰减校正方法对定量呼吸相关(4D)PET/CT成像的影响。

Impact of CT attenuation correction method on quantitative respiratory-correlated (4D) PET/CT imaging.

作者信息

Nyflot Matthew J, Lee Tzu-Cheng, Alessio Adam M, Wollenweber Scott D, Stearns Charles W, Bowen Stephen R, Kinahan Paul E

机构信息

Department of Radiation Oncology, University of Washington, Seattle, Washington 98195-6043.

Department of Bioengineering, University of Washington, Seattle, Washington 98195-6043.

出版信息

Med Phys. 2015 Jan;42(1):110-20. doi: 10.1118/1.4903282.

DOI:10.1118/1.4903282
PMID:25563252
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5148139/
Abstract

PURPOSE

Respiratory-correlated positron emission tomography (PET/CT) 4D PET/CT is used to mitigate errors from respiratory motion; however, the optimal CT attenuation correction (CTAC) method for 4D PET/CT is unknown. The authors performed a phantom study to evaluate the quantitative performance of CTAC methods for 4D PET/CT in the ground truth setting.

METHODS

A programmable respiratory motion phantom with a custom movable insert designed to emulate a lung lesion and lung tissue was used for this study. The insert was driven by one of five waveforms: two sinusoidal waveforms or three patient-specific respiratory waveforms. 3DPET and 4DPET images of the phantom under motion were acquired and reconstructed with six CTAC methods: helical breath-hold (3DHEL), helical free-breathing (3DMOT), 4D phase-averaged (4DAVG), 4D maximum intensity projection (4DMIP), 4D phase-matched (4DMATCH), and 4D end-exhale (4DEXH) CTAC. Recovery of SUV(max), SUV(mean), SUV(peak), and segmented tumor volume was evaluated as RC(max), RC(mean), RC(peak), and RC(vol), representing percent difference relative to the static ground truth case. Paired Wilcoxon tests and Kruskal-Wallis ANOVA were used to test for significant differences.

RESULTS

For 4DPET imaging, the maximum intensity projection CTAC produced significantly more accurate recovery coefficients than all other CTAC methods (p < 0.0001 over all metrics). Over all motion waveforms, ratios of 4DMIP CTAC recovery were 0.2 ± 5.4, -1.8 ± 6.5, -3.2 ± 5.0, and 3.0 ± 5.9 for RC(max), RC(peak), RC(mean), and RC(vol). In comparison, recovery coefficients for phase-matched CTAC were -8.4 ± 5.3, -10.5 ± 6.2, -7.6 ± 5.0, and -13.0 ± 7.7 for RC(max), RC(peak), RC(mean), and RC(vol). When testing differences between phases over all CTAC methods and waveforms, end-exhale phases were significantly more accurate (p = 0.005). However, these differences were driven by the patient-specific respiratory waveforms; when testing patient and sinusoidal waveforms separately, patient waveforms were significantly different between phases (p < 0.0001) while the sinusoidal waveforms were not significantly different (p = 0.98). When considering only the subset of 4DMATCH images that corresponded to the end-exhale image phase, 4DEXH, mean and interquartile range were similar to 4DMATCH but variability was considerably reduced.

CONCLUSIONS

Comparative advantages in accuracy and precision of SUV metrics and segmented volumes were demonstrated with the use of the maximum intensity projection and end-exhale CT attenuation correction. While respiratory phase-matched CTAC should in theory provide optimal corrections, image artifacts and differences in implementation of 4DCT and 4DPET sorting can degrade the benefit of this approach. These results may be useful to guide the implementation, analysis, and development of respiratory-correlated thoracic PET/CT in the radiation oncology and diagnostic settings.

摘要

目的

呼吸相关正电子发射断层扫描(PET/CT)4D PET/CT用于减少呼吸运动产生的误差;然而,4D PET/CT的最佳CT衰减校正(CTAC)方法尚不清楚。作者进行了一项体模研究,以评估在真实情况下4D PET/CT的CTAC方法的定量性能。

方法

本研究使用了一个可编程呼吸运动体模,其带有一个定制的可移动插入物,设计用于模拟肺部病变和肺组织。插入物由五种波形之一驱动:两种正弦波形或三种特定患者的呼吸波形。使用六种CTAC方法对运动状态下的体模进行3DPET和4DPET图像采集及重建:螺旋屏气(3DHEL)、螺旋自由呼吸(3DMOT)、4D相位平均(4DAVG)、4D最大强度投影(4DMIP)、4D相位匹配(4DMATCH)和4D呼气末(4DEXH)CTAC。评估SUV(最大值)、SUV(平均值)、SUV(峰值)和分割肿瘤体积的恢复情况,分别记为RC(最大值)、RC(平均值)、RC(峰值)和RC(体积),表示相对于静态真实情况的差异百分比。采用配对Wilcoxon检验和Kruskal-Wallis方差分析来检验显著差异。

结果

对于4DPET成像,最大强度投影CTAC产生的恢复系数比所有其他CTAC方法都更准确(所有指标p < 0.0001)。在所有运动波形中,4DMIP CTAC的恢复率在RC(最大值)、RC(峰值)、RC(平均值)和RC(体积)方面分别为0.2±5.4、-1.8±6.5、-3.2±5.0和3.0±5.9。相比之下,相位匹配CTAC在RC(最大值)、RC(峰值)、RC(平均值)和RC(体积)方面的恢复系数分别为-8.4±5.3、-10.5±6.2、-7.6±5.0和-13.0±7.7。在测试所有CTAC方法和波形的不同相位之间的差异时,呼气末相位明显更准确(p = 0.005)。然而,这些差异是由特定患者的呼吸波形驱动的;当分别测试患者和正弦波形时,患者波形在不同相位之间有显著差异(p < 0.0001),而正弦波形没有显著差异(p = 0.98)。当仅考虑与呼气末图像相位对应的4DMATCH图像子集时,4DEXH的平均值和四分位间距与4DMATCH相似,但变异性显著降低。

结论

使用最大强度投影和呼气末CT衰减校正证明了在SUV指标和分割体积的准确性和精密度方面具有比较优势。虽然呼吸相位匹配CTAC理论上应提供最佳校正,但图像伪影以及4DCT和4DPET排序实施中的差异可能会降低这种方法的优势。这些结果可能有助于指导放射肿瘤学和诊断环境中呼吸相关胸部PET/CT的实施、分析和开发。