Impact of CT attenuation correction method on quantitative respiratory‐correlated (4D) PET/CT imaging. Issue 1 (17th December 2014)

• Record Type: Journal Article
• Authors: Nyflot, Matthew J.; Lee, Tzu‐Cheng; Alessio, Adam M.; Wollenweber, Scott D.; Stearns, Charles W.; Bowen, Stephen R.; Kinahan, Paul E.
• Is Part Of: Medical physics. Volume 42:Issue 1(2015)
• Page Start: 110
• Page End: 120
• Publication Date: 2014-12-17
• Subjects: biological tissues -- image motion analysis -- image reconstruction -- image segmentation -- lung -- medical image processing -- phantoms -- pneumodynamics -- positron emission tomography -- statistical testing -- tumours; Positron emission tomography (PET) -- Computed tomography -- Segmentation -- Reconstruction -- Artifacts and distortion -- Pneumodyamics, respiration; Biological material, e.g. blood, urine; Haemocytometers -- Digital computing or data processing equipment or methods, specially adapted for specific applications -- Image data processing or generation, in general -- Analysis of motion -- Scintigraphy -- Measuring half‐life of a radioactive substance; respiratory‐correlated PET/CT -- CT attenuation correction -- 4DPET -- 4DCT -- quantification; Computed tomography -- Positron emission tomography -- Medical image reconstruction -- Optical phase matching -- Cancer -- Wave attenuation -- Lungs -- Medical image artifacts; Medical physics -- Periodicals; Medical physics; Geneeskunde; Natuurkunde; Toepassingen; Biophysics; Periodicals; Periodicals; Electronic journals; 610.153
• DOI: 10.1118/1.4903282
• Languages: English
• ISSNs: 0094-2405

Abstract

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 SUVmax, SUVmean, SUVpeak, and segmented tumor volume was evaluated as RCmax, RCmean, RCpeak, and RCvol, 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 RCmax, RCpeak, RCmean, and RCvol . 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 RCmax, RCpeak, RCmean, and RCvol . 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.