After yttrium-90 (90Y) microsphere radioembolization (RE), evaluation of extrahepatic activity and liver dosimetry is typically performed on 90Y Bremsstrahlung SPECT images. Since these images demonstrate a low quantitative accuracy, 90Y PET has been suggested as an alternative. The aim of this study is to quantitatively compare SPECT and state-of-the-art PET on the ability to detect small accumulations of 90Y and on the accuracy of liver dosimetry.
SPECT/CT and PET/CT phantom data were acquired using several acquisition and reconstruction protocols, including resolution recovery and Time-Of-Flight (TOF) PET. Image contrast and noise were compared using a torso-shaped phantom containing six hot spheres of various sizes. The ability to detect extra- and intrahepatic accumulations of activity was tested by quantitative evaluation of the visibility and unique detectability of the phantom hot spheres. Image-based dose estimates of the phantom were compared to the true dose. For clinical illustration, the SPECT and PET-based estimated liver dose distributions of five RE patients were compared. At equal noise level, PET showed higher contrast recovery coefficients than SPECT. The highest contrast recovery coefficients were obtained with TOF PET reconstruction including resolution recovery. All six spheres were consistently visible on SPECT and PET images, but PET was able to uniquely detect smaller spheres than SPECT. TOF PET-based estimates of the dose in the phantom spheres were more accurate than SPECT-based dose estimates, with underestimations ranging from 45% (10-mm sphere) to 11% (37-mm sphere) for PET, and 75% to 58% for SPECT, respectively. The differences between TOF PET and SPECT dose-estimates were supported by the patient data.
Citation: Elschot M, Vermolen BJ, Lam MGEH, de Keizer B, van den Bosch MAAJ, de Jong HWAM (2013) Quantitative Comparison of PET and Bremsstrahlung SPECT for Imaging the In Vivo Yttrium-90 Microsphere Distribution after Liver Radioembolization. PLoS ONE 8(2): e55742. doi:10.1371/journal.pone.0055742
Editor: Erica Villa, University of Modena & Reggio Emilia, Italy
Received: August 16, 2012; Accepted: December 30, 2012; Published: February 6, 2013
Copyright: © 2013 Elschot et al. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
Funding: This work was funded by the University Medical Center Utrecht. The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.
Competing interests: The authors have declared that no competing interests exist.
Intra-arterial radioembolization (RE) using microspheres labeled with the high-energy beta-emitter yttrium-90 (90Y), is used in clinical practice for treatment of unresectable liver tumours , . Prior to RE, prophylactic coil-embolization of arteries communicating with the gastrointestinal (GI) tract is performed, followed by administration of technetium-99m macroaggregated-albumin (99mTc-MAA) particles. Subsequent gamma camera imaging is used to assess any extrahepatic particle deposition, which is a contra-indication for RE. Also, the percentage of particles that shunts to the lungs is measured, which may lead to adjustment of the 90Y dose . After administration of the 90Y microspheres, a post-therapy 90Y Bremsstrahlung SPECT scan is performed for two reasons. First, 90Y may unexpectedly be present outside the liver, despite a favorable distribution on the 99mTc-MAA scan. Accumulation of 90Y microspheres in organs other than the liver will likely cause serious complications, like ulceration and bleedings in the GI tract , . Therefore, severe pain after treatment should be aggressively managed to prevent development of more serious complications , which may be facilitated by early detection of possible extrahepatic activity . Second, the intrahepatic microsphere distribution over tumourous and non-tumourous liver tissue is expected to be an important predictor of treatment efficacy . Post-therapy imaging facilitates estimation of the tumour and non-tumour absorbed radiation dose on the image-based microsphere distribution.
Unfortunately, the low photon yield and continuous nature of the Bremsstrahlung X-ray spectrum limit the quantitative accuracy of 90Y Bremsstrahlung SPECT. Per MBq, approximately 23000 Bremsstrahlung photons with energy higher than 50 keV are produced by interaction of the beta particle with tissue , therefore acquisition in a wide energy window is required to maximize sensitivity. The absence of a photopeak prohibits the use of simple window-based scatter rejection, scatter correction, and attenuation correction techniques, and penetration of high-energy photons through the collimator septa leads to further loss of image contrast . Recent efforts to optimize reconstruction algorithms, e.g. by compensation for scatter and collimator blurring with pre-calculated 90Y point-spread functions (PSF) , , have improved the quantitative accuracy of 90Y Bremsstrahlung SPECT, but are not widely available in the clinic to date.
Yttrium-90 PET was recently shown to be feasible in phantoms and patients and may be an interesting alternative to Bremsstrahlung SPECT . Per MBq, 90Y emits 32 positrons per second with a maximum energy of 758 keV , . Consequently, annihilation photon pairs are produced approximately 700 times less often than Bremsstrahlung photons (E >50 keV). Nevertheless, 90Y PET may allow for the detection of extrahepatic activity and accurate tumour and liver dose estimation, since the spatial resolution is expected to be comparable to that of 18F PET, which has a maximum positron energy of 633 keV . Additionally, advanced correction techniques for scatter, random, and attenuation effects that are clinically available for 18F PET, can be directly applied to 90Y PET . Several groups have successfully assessed the post-therapy 90Y microsphere distribution in RE patients , –.
To date, no systematic studies have quantitatively compared clinically available 90Y PET with Bremsstrahlung SPECT. The potential for accurately assessing the intra- and extrahepatic microsphere distribution is determined by fundamental limitations of the imaging modality. The first objective of this study was to quantitatively evaluate and compare the contrast and noise characteristics of 90Y PET and SPECT images, which are relevant parameters for activity detection and liver dosimetry in clinical practice. Image contrast depends on spatial resolution and on other effects that distort quantification of local 90Y content, like photon attenuation, photon scatter, collimator penetration and random coincidences. Image noise is dependent on sensitivity and on the stochastic nature of attenuation, scatter and collimation. The second objective was to quantitatively compare 90Y PET and SPECT on the ability to detect small accumulations of 90Y inside and outside the liver, and on the accuracy of liver dose estimates, based on the recorded 90Y distribution. All quantitative results were obtained in phantom experiments. Additionally, Bremsstrahlung SPECT and PET scans of five 90Y RE patients were evaluated to support the results of the phantom study.
Materials and Methods
Dual post-treatment imaging using both SPECT/CT and PET/CT techniques was part of the quality control protocol for implementation of 90Y-PET imaging as the standard post-radioembolization procedure. All data were retrospectively analyzed, written patient informed consent was therefore not sought nor documented. The institutional review board (IRB) of the University Medical Center Utrecht approves this type of retrospective study and waives the requirements for patient informed consent. The image data were handled anonymously, in accordance with the Declaration of Helsinki and the regulations of the IRB.
Scanners, Acquisition and Reconstruction
PET/CT data were acquired on a state-of-the-art Siemens mCT Time-Of-Flight (TOF) PET/CT scanner (Siemens Medical Solutions USA, Inc.). The mCT combines a whole body LSO PET scanner with a 40-slice CT scanner. The PET component is equipped with a large axial field-of-view (FOV) of 21.8 cm and wide acceptance angle of 13.2° to maximize sensitivity. In whole body mode, consecutive bed positions overlap approximately 43%. A detailed characterization of the physical and clinical performance of the mCT was performed by Jakoby et al . PET data were acquired with a lower- and upper-level discriminator of 435 keV and 650 keV, respectively. Three reconstruction algorithms were compared, all including correction for random coincidences, scatter and attenuation . The first algorithm was fully 3D iterative attenuation weighted ordinary Poisson ordered subset expectation maximization (OP-OSEM) reconstruction  (‘iterative’), the second algorithm was iterative reconstruction extended with a PSF model of the detector response  (‘iterative+PSF’), and the third was iterative reconstruction including PSF and TOF information (‘iterative+PSF+TOF’). Images were reconstructed using 3 iterations with 24 or 21 (iterative+PSF+TOF) subsets and a 5 mm full-width at half-maximum (FWHM) Gaussian post-reconstruction filter. The reconstructed voxel size was 2×2×2 mm3.
SPECT/CT data were acquired on a Siemens Symbia T16 system (Siemens Medical Solutions USA, Inc.). The Symbia T16 combines a dual detector SPECT scanner with a 16-slice CT scanner. The SPECT detectors are equipped with 3/8 inch thick crystals. All our experiments were performed with the high-energy collimators mounted, which proved to be the best option for 90Y imaging with maximum resolution and contrast , . SPECT data were acquired in a 105–195 keV energy window , , using 120 projections over 360° and a 256×256 matrix with a pixel size of 2.4×2.4 mm2. Images were reconstructed with two different reconstruction algorithms. The first algorithm was 2D OSEM reconstruction including correction for attenuation with an effective broad beam linear attenuation coefficient (‘iterative’), and the second algorithm was iterative reconstruction including a Gaussian PSF model of the geometric collimator-detector response of the camera  (‘iterative+PSF’). In both cases 8 iterations with 8 subsets were used without post-reconstruction filtering. The reconstructed voxel size was 2.4×2.4×2.4 mm3.
Phantom Set Up
The NEMA 2007/IEC 2008 PET Image Quality (IQ) Phantom, which is designed for evaluation of reconstructed image quality and activity recovery, was used for all phantom experiments to allow for direct comparison between the two modalities . The phantom consists of a fillable torso-shaped compartment (volume = 9700 ml) containing six fillable coplanar spheres (inner diameter = 10, 13, 17, 22, 28, and 37 mm) and a cylindrical lung insert.
Table 1 lists the separately performed phantom experiments. PET data were acquired in one bed position centered on the spheres. Since the PET FOV covering a whole liver requires two bed positions (30 cm in axial direction) and for SPECT one FOV (40 cm) is sufficient, all PET scan times were set to half the SPECT scan times. The initial 90Y activity concentration in the spheres ([A]sph) and background compartment ([A]bkg) was 2.40 and 0 MBq ml−1, respectively. All six spheres were filled with activity, which slightly deviates from the NEMA recommendations. After performing experiments 1, 90Y was added to the background for experiments 2–4, resulting in [A]bkg = 0.27 MBq ml−1. The total activity in the phantom was 119 and 2600 MBq, for experiments 1, and 2–4, respectively. Instead of adjusting the activity in the phantom, the scan times were prolonged ×2 and ×4 times in experiments 2–4 to obtain the simulated activity concentrations given in Table 1. This approach was deemed valid, because both the measured total activity and the maximum simulated total activity, which corresponded to approximately 2600 MBq for a 2000 ml liver, were within the linear range (i.e. no dead time effects) of 90Y PET and Bremsstrahlung SPECT , .
Image Contrast and Noise
Image contrast and noise measurements were obtained from phantom experiments 4 (Table 1), representing a clinically realistic liver background activity concentration of 1.09 MBq ml−1. For comparison: using the body surface area (BSA) method (see ‘Patients’ section), the mean activity concentration in a 1.5 kg liver with 10% tumour involvement of an ‘average’ patient (1.70 m, 70 kg) would be 1.14 MBq ml−1. Six circular hot sphere regions of interest (ROIs) were automatically delineated on the CT slice through the center of the spheres, covering the inner compartment voxels of each of the six phantom spheres. A background ROI was delineated on the same slice consisting of all voxels that fell within the physical phantom boundaries, excluding the voxels belonging to the hot sphere ROIs and the lung insert. For each reconstructed SPECT and PET volume, contrast recovery coefficients (QH) were calculated with equation 1.(1)Here, CH is the mean intensity in the hot sphere ROIs, CB is the mean intensity in the background ROI and R is the true sphere-to-background activity concentration ratio. As a measure of image noise, the coefficient of variation (CV) was calculated with equation 2.(2)Here, STDVB is the standard deviation in the background ROI.
The ability to detect small accumulations of activity (detectability) in a region without background activity is important for evaluation of extrahepatic microsphere deposition. Additionally, the detectability of activity in a region with background activity is important when intrahepatic tumour identification is based on the contrast in the SPECT and PET scans, e.g. using isocontours when the target volume cannot be derived from a CT or MRI scan.
A hot spot of activity can only be accurately identified, if it can be reliably distinguished from the background, i.e. if it is visible. The visibility (υH) of the six hot spheres was tested by quantitative evaluation of the hot sphere and background signal; for each hot sphere the effective contrast-to-noise ratio (CNR) was calculated according to equation 3.(3)with CH, CB, and STDVB as defined in the previous section and Nvoxels the number of voxels in the hot sphere ROI. Subsequently, a hot sphere was scored ‘visible’ when υH was larger than 4, in accordance with the Rose criterion , .
In addition to the visibility criterion, which is an established method for detection of false negatives, a new method is presented to evaluate the presence of false positive hot spots. Since accumulations of activity are not ‘uniquely detectable’ if false positives are present, we will refer to this criterion as ‘unique detectability’ in the remainder of this work. The unique detectability of the six hot spheres was evaluated in five consecutive background slices, placed five cm away from the slice through the center of the spheres. Circular ROIs to test for false positives (ROITEST-FP) with the same diameter as the hot sphere ROIs were centered on all phantom voxels in the five slices. The visibility (υTEST-FP) of each ROITEST-FP was calculated with equation 4.(4)Here, CTEST-FP is the mean intensity in ROITEST-FP, CB the mean intensity in the background ROI of the same slice (consisting of all voxels falling within the phantom boundaries, excluding the lung insert), STDVB the standard deviation in the background ROI and Nvoxels the number of voxels in ROITEST-FP. We investigated two different criteria to score a sphere ‘uniquely detectable’. According to the first criterion, a visible hot sphere was scored ‘uniquely detectable’, if υTEST-FP was smaller than 4 for all ROITEST-FP of the same size, i.e. if none of the corresponding ROITEST-FP were visible according to the Rose criterion. Translated to clinical practice, this criterion measures whether any visible hot spot of a certain diameter can be reliably characterized as ‘true positive’. According to the second criterion, a visible hot sphere was scored ‘uniquely detectable’ if υTEST-FP was smaller than υH for all ROITEST-FP of the same size, i.e. if the hot sphere was better visible than all corresponding ROITEST-FP. This criterion is less strict and measures whether the visible hot spot with the highest CNR can be reliably characterized as ‘true positive’.
When using CNR with the relaxation term √Nvoxels for evaluation of the visibility of hot spots, a uniform count density in the hot spot ROI is assumed. However, the mean intensities of the relatively small hot sphere and false positive ROIs are susceptible to outliers and may therefore not accurately represent human perception. Median values, on the other hand, are less sensitive to outliers and may be a better measure for this purpose. Consequently, equations 3 and 4 were also evaluated using median intensities for CH and CTEST-FP, respectively. The ‘median-based’ hot sphere visibility and unique detectability results were presented next to their ‘mean-based’ equivalents. Data from experiments 1 (Table 1) were used to analyze the extrahepatic detectability and experiments 2–4 were used to mimic the intrahepatic situation, for three different activity concentrations.
Radioembolization with 90Y-labelled resin microspheres (SIR-Spheres, Sirtex Medical, Sydney, Australia) was performed in 5 consecutive patients (2 women, 3 men; mean age +/− SD, 56.8+/−13.0 y; age range 43–76 y) according to the international consensus report from the Radioembolization Brachytherapy Oncology Consortium . The BSA method was used to calculate the activities (A) administered to the patients, according to the equation A (GBq) = BSA−0.2+ VT/VL, with BSA (m2) = 0.20247 * height0.725 * weight0.725, and VT and VL the tumour and whole liver volume derived from CT or MRI, respectively. Dose adjustments were not required, since the percentage 99mTc-MAA lung shunting was below 10% for all patients. Four patients were diagnosed with liver metastases (2 colorectal carcinomas, 1 nasopharyngeal carcinoma, and 1 mammary carcinoma) and one patient was diagnosed with hepatocellular carcinoma. Four patients received whole liver treatment and one patient received left lobar treatment. PET data were acquired in two bed positions (total scan length 30 cm) centered on the liver, whereas the SPECT axial FOV was 40 cm. SPECT and PET data were both acquired in 30 minutes, which was considered the maximum desirable scan time for a RE patient. All patient and treatment characteristics are summarized in Table 2.
Absorbed Dose Estimation
The iterative+PSF+TOF PET and iterative+PSF SPECT images of experiments 4 (Table 1) were used to evaluate the accuracy of dosimetry. Calibration factors to convert the PET and SPECT images into units of activity were determined by dividing the total reconstructed counts in the phantom by the known activity in the phantom. A digital phantom representing the ‘true activity distribution’ (TRUE) was constructed from a segmented high-resolution CT dataset (voxel size 0.6×0.6×0.6 mm3). Activity concentrations of 1.09 MBq ml−1 and 9.6 MBq ml−1 were applied to the segmented 3D background ROI and 3D hot sphere ROIs, respectively. Dose maps were calculated from the PET, SPECT, and TRUE activity images by convolution with the appropriate 90Y 3D dose-point kernel (DPK), in accordance with MIRD Pamphlet No. 17 . For this purpose, DPKs with the same voxel sizes as the high-resolution CT, SPECT and PET images were calculated using the Monte Carlo engine MCNPX 2.5.0 .
Three-dimensional ROIs of the fillable spheres and a 2000 ml background region were delineated on the CT scans, altogether representing a liver with tumours. Cumulative dose-volume histograms (CDVH) and mean absorbed doses were calculated for all ROIs. Additionally, the mean absorbed doses in the hot sphere ROIs were corrected for incomplete activity recovery due to partial volume effects (PVE), by multiplication with the corresponding correction factors calculated as R * CB/CH. Errors in the uncorrected and corrected SPECT and PET-based dose estimates were calculated in comparison to the TRUE dose.
Patient data were reconstructed with the same settings as the phantom data. Three-dimensional liver ROIs were manually delineated on the CT scans. To be able to mutually compare the SPECT and PET-based dose distributions, the liver ROI of each patient was segmented into a low-dose ROI and a high-dose ROI. The high-dose ROI included all voxels that had on one or both modalities an activity concentration of at least two times the mean liver concentration. The low-dose ROI consisted of the other liver voxels, i.e. the liver ROI excluding the high-dose ROI. The resulting ‘integrated’ SPECT/PET ROIs allowed for an unbiased, direct comparison of the dose distribution between the modalities. Following conversion of PET and SPECT activity images into dose maps, CDVH and mean absorbed doses were calculated for all ROIs.
Image Contrast and Noise
Figure 1 shows that iterative+PSF+TOF reconstruction resulted in PET images with the highest contrast recovery. Iterative+PSF reconstruction resulted in the highest contrast recovery for SPECT. PET contrast recovery coefficients were substantially higher than those of SPECT in all spheres. In comparison, both image contrast and image noise were higher in PET than in SPECT (Figure 2A), which is also evident from the transversal slices through the phantom in Figure 2B and 2C. The noise level in the PET images was substantially reduced when reconstructed with 1 iteration and a 15 mm FWHM post-reconstruction filter (equal noise (EQN) PET), approximately to the noise level of the SPECT images (approximately 18% CV, Figure 2A and 2D). This set-up allows for a fair comparison of image contrast. At equal noise level, all PET images still showed higher contrast than SPECT, although contrast was lost in comparison with PET images reconstructed with optimal settings.
Contrast recovery and image noise in the 22-mm sphere for all reconstruction methods (A), the slice through the center of the SPECT volume (iterative+PSF) (B), the slice through the center of the PET volume (iterative+PSF+TOF) (C), and the slice through the center of the PET volume (iterative+PSF+TOF) reconstructed with SPECT-like noise level (D). All images were linearly window-leveled from 0 to 4 times the mean intensity in the background ROI. The boundaries of the central lung insert, the six hot sphere ROIs, and the background ROI are illustrated by the red lines and the 22-mm sphere is indicated by the arrow.
From Table 3 it can be appreciated that the ‘mean-based’ and ‘median-based’ visibility results were equal for all images but one. The unique detectability results differed between the ‘mean-based’ and ‘median-based’ approach, for both detectability criteria. From Figure 3 it is apparent the ‘mean-based’ approach detected more false positives than the ‘median-based’ approach. Being less affected by outliers, the ‘median-based’ approach only detected the more or less uniform false positives regions and was therefore considered the best approach for false positive detection. Consequently, in the remainder of this section the ‘median-based’ results are reported for hot sphere visibility and unique detectability. Table 3 and Figure 3 show that in the extrahepatic situation, all six spheres were visible on SPECT and PET images according to the Rose criterion. According to the criterion υTEST-FP<4, none of the spheres were uniquely detectable with SPECT, whereas the smallest sphere uniquely detectable with PET was 28 mm in diameter. According to the criterion υTEST-FP< υH, all hot spheres in the cold background were uniquely detectable with PET, whereas the smallest sphere uniquely detectable with SPECT was 13 mm in diameter. For all three activity concentrations of the intrahepatic situation, all six spheres were visible with both SPECT and PET, but none of them was uniquely detectable according to the criterion υTEST-FP<4. According to the criterion υTEST-FP< υH, the smallest sphere uniquely detectable with PET was 13 mm in diameter, whereas this was 22 mm for SPECT, for all activity concentrations.
The activity concentration in the hot spheres was 2.4 MBq ml−1 for both the images without (rows 1–3) and with background activity (rows 4–6). In the 1st and 4th row, the SPECT+PSF (1st and 3rd column) and PET+PSF+TOF (2nd and 4th column) slices are overlaid with the location of the visible phantom spheres (red). In rows 2, 3, 5 and 6 a background slice is overlaid with the location of false positive regions. For illustrative reasons, only the largest false positive ROIs are shown (red: 10 mm; green: 13 mm; blue: 17 mm; yellow: 22 mm; purple: 37 mm). Clustered ROIs with connecting center voxels are represented by the ROI with the highest υTEST-FP value.
Absorbed Dose Estimation
The error of the uncorrected (in brackets: corrected for PVE) PET dose estimates ranged from −11% (+6%) for the largest sphere to −45% (+40%) for the smallest sphere (Table 4). For SPECT the errors were larger, ranging from −58% (+18%) to −75% (+69%). Figure 4 shows that the PET-based CDVH of the hot sphere ROI followed the true CDVH more closely than the SPECT-based CDVH. The higher image noise in TOF PET was reflected by the flattened slope of the CDVH curve.
CDVH of the phantom background ROI and the ROI of the 37-mm diameter sphere. The presented doses were not corrected for PVE.
For all patients, the difference between the estimated dose in the high-dose ROI and the low-dose ROI was larger for PET than for SPECT (Table 5). This effect is also illustrated by the CDVH and fused images of patient 2 in Figure 5. Images of patients 1, 3, 4, and 5 are provided as Figure S1, Figure S2, Figure S3 and Figure S4, respectively.
The CDVH of the whole liver (WL), low-dose (LD) and high-dose (HD) ROIs of patient 2 (A), a transversal slice through the SPECT-based dose map, fused with CT (B), and the same transversal slice through the PET-based dose map (C). The boundary of the high-dose ROI is depicted by the green line.
In this study, we quantitatively compared the accuracy of 90Y Bremsstrahlung SPECT and state-of-the-art PET for the assessment of the intra- and extrahepatic microsphere distribution after radioembolization, using the physical parameters image contrast and image noise, and the clinically relevant parameters detectability and dosimetry. We realize that image contrast and noise not only depend on the fundamental limitations of the imaging modalities, but also on acquisition and reconstruction settings; e.g., a well-known property of iterative reconstruction algorithms is that contrast can be maximized at the cost of noise amplification by varying the number of iterations . Before defining the study setup as published, we evaluated image contrast and noise for various energy windows (wide: 50–250 keV , , , –; medium-wide: 105–195 keV , ; small: 76–105 keV , , SPECT only), various numbers of iterations (1, 3, 5, and 8), and various post-reconstruction filters (0, 5, and 10 mm FWHM). The settings resulting in the highest image contrast were the starting point for this study. The results imply that 90Y Bremsstrahlung SPECT and PET image contrast is improved by inclusion of a PSF model in the reconstruction process. The PET image contrast is further improved by inclusion of TOF information, which also resulted in slightly higher image noise. The latter can be attributed to faster convergence of TOF reconstruction . At similar noise level, all PET algorithms demonstrated higher contrast recovery coefficients than optimal SPECT. Therefore, we conclude that the image quality of 90Y state-of-the-art PET outperforms Bremsstrahlung SPECT.
In comparison with 18F PET and 99mTc SPECT, the QH of 90Y were consistently lower (e.g. 66% (90Y) vs 71% (18F) and 11% (90Y) vs 57% (99mTc) for the 22-mm sphere, data not shown). The large difference in SPECT QH can probably be attributed to the low spatial resolution and the large amount of photon scatter and septal penetration with 90Y , all of which increase the PVE. Recent work on 90Y SPECT reconstruction demonstrated that image contrast may be substantially improved by including accurate models of the scattered and penetrated photons, but these algorithms are not available in the clinic to date , . To the contrary, PET reconstruction algorithms include advanced techniques to correct for random coincidences, photon scatter, and attenuation effects. Nevertheless, a slight difference in QH between 90Y and 18F was observed, which was probably not caused by resolution effects; the difference in spatial resolution was estimated to be within 1%, using the analytical resolution model of Lubberink and Herzog . Instead, the intensity in the low-count background region may have been overestimated, possibly due to sparsity of the (smoothed) delayed coincidences sinogram that is used for random correction in the OP-OSEM algorithm . This effect has also been observed in dynamic studies with short frame rates . Further research is required to fully understand the clinical impact of these effects.
Inadvertent extrahepatic deposition of activity may be detected directly post-treatment on 90Y SPECT or PET images. Ahmadzadehfar et al showed that detection of extrahepatic activity on Bremsstrahlung SPECT/CT scans predicted GI ulcers with a sensitivity of 87% and a specificity of 100%, despite low image quality . In this study, we investigated the detectability of accumulations of activity of different sizes with the well-known Rose criterion for detection of false negatives and with a new method for detection of false positives. The ‘median-based’ unique detectability approach was deemed better than its ‘mean-based’ equivalent, since the latter tended to erroneously classify non-uniform regions as ‘false positive’. We demonstrated that the visibility of intra- and extrahepatic accumulations of activity was equal between SPECT and PET, for the investigated sphere sizes and activity concentration ratios. Unique detectability with the υTEST-FP< υH criterion demonstrated larger differences between PET and SPECT than the υTEST-FP<4 criterion, but will depend on the activity concentration in the hot spheres. Nevertheless, according to both criteria, PET was able to uniquely detect smaller accumulations of activity than SPECT, endorsing the use of (TOF) PET/CT instead of SPECT/CT. Given the relative simplicity of the detectability models used, we should emphasize that the results of our phantom study should not be interpreted as the lower limits of (lesion) detection performance by a human observer, but merely as a comparison between 90Y SPECT and PET. The results are likely to be dependent on acquisition and reconstruction settings, which were optimized for image contrast in this study. Optimization of the imaging protocols for noise, e.g. by increasing the FWHM of the post-reconstruction filter, may improve the unique detectability of hot spots.
Accurate tumour and liver dosimetry can improve RE patient care, e.g. by facilitating (selective) re-treatment of tumourous tissue that did not receive a sufficient dose during the first treatment. The relationship between the 99mTc-MAA SPECT-based tumour absorbed dose and tumour response is reported in numerous publications investigating the possibilities of treatment optimization by individualized 99mTc-MAA SPECT-based dose planning (e.g. , , ). To the contrary, publications on the 90Y SPECT or PET-based dose-response relation are relatively sparse , . The latter approach has the advantage of imaging the real 90Y microsphere distribution, which avoids the question of accurate prediction of the microsphere distribution with 99mTc-MAA, but it is not used for individualized treatment planning. Using phantom experiments, we demonstrated that 90Y TOF PET-based dose estimates were more accurate than Bremsstrahlung SPECT-based dose estimates. Based on the incomplete contrast recovery observed in the image quality phantom, dose underestimations with both PET and SPECT were to be expected. SPECT-based absorbed dose estimates in the high-dose regions of the phantom were lower than those of PET, which was supported by the results of our patient study. When correcting the hot sphere mean dose estimates for PVE, the absolute dose errors were reduced, but dose overestimations up to 69% were still observed. The use of PVE correction factors is restricted to correction of mean ROI values, and PVE correction was therefore applied to the mean absorbed dose values of the hot sphere ROIs. Due to the range of the beta-particles, however, the mean absorbed dose in the hot sphere ROIs not only depends on the locally absorbed energy as a result of activity in the ROIs itself, but also on the energy absorbed as a result of activity in adjacent background voxels. With hot spheres in a warm background, PVE result in an underestimation of the first contribution to the mean absorbed dose, whereas the latter contribution is overestimated. Consequently, application of the activity-based PVE correction factors leads to erroneous up-scaling of the adjacent background voxels’ contribution to the mean absorbed dose in the hot sphere ROIs. This effect is stronger for smaller spheres, due to the relatively large amount of adjacent background voxels, and stronger for SPECT than for PET, due to the higher correction factors of the first. For dosimetry purposes, a better approach may be to determine correction factors on dose images, which not only include PVE but also DPK effects. However, these dose correction factors will strongly depend on the activity concentration ratio between ROIs and adjacent background voxels, which undesirably complicates PVE correction in clinical practice. For this reason, we chose not to correct the mean dose estimates in the patient study for PVE effects. The results of the patient study indicate that the use of high-resolution PET can potentially improve dose-response relationships on the level of the tumour for 90Y RE. The evaluation of the estimated absorbed liver dose in low-dose and high-dose regions, which did not necessarily coincide with healthy liver and tumour regions, did not harm the conclusions presented in this study, since the primary aim was a quantitative comparison of the 90Y SPECT and PET-based dose distribution, and not clinical liver dosimetry. Evaluation of the absorbed dose to tumourous and healthy liver tissue should be performed in a larger (prospective) patient study and is beyond the scope of this study.
This study demonstrates that the 90Y image quality of state-of-the-art PET is superior over Bremsstrahlung SPECT for the assessment of the microsphere distribution after radioembolization. Intra- and extrahepatic hot spots of 10 mm in diameter or larger are visible on SPECT and PET images, but PET is able to uniquely detect smaller accumulations of activity than SPECT. Additionally, TOF PET-based dose estimates are more accurate than SPECT-based dose estimates, which give large underestimations in high-dose regions.
Patient 1 dosimetry. The CDVH of the whole liver (WL), low-dose (LD) and high-dose (HD) ROIs of patient 1 (A), a transversal slice through the SPECT-based dose map, fused with CT (B), and the same transversal slice through the PET-based dose map (C). The boundary of the high-dose ROI is depicted by the green line.
Patient 3 dosimetry. The CDVH of the whole liver (WL), low-dose (LD) and high-dose (HD) ROIs of patient 3 (A), a transversal slice through the SPECT-based dose map, fused with CT (B), and the same transversal slice through the PET-based dose map (C). The boundary of the high-dose ROI is depicted by the green line.
Patient 4 dosimetry. The CDVH of the whole liver (WL), low-dose (LD) and high-dose (HD) ROIs of patient 4 (A), a transversal slice through the SPECT-based dose map, fused with CT (B), and the same transversal slice through the PET-based dose map (C). The boundary of the high-dose ROI is depicted by the green line.
Patient 5 dosimetry. The CDVH of the whole liver (WL), low-dose (LD) and high-dose (HD) ROIs of patient 5 (A), a transversal slice through the SPECT-based dose map, fused with CT (B), and the same transversal slice through the PET-based dose map (C). The boundary of the high-dose ROI is depicted by the green line.
Conceived and designed the experiments: ME BJV MGEHL HJ. Performed the experiments: ME BJV BdK MAAJvdB. Analyzed the data: ME BJV HWAMdJ. Contributed reagents/materials/analysis tools: ME BJV. Wrote the paper: ME BJV MGEHL BdK MAAJvdB HWAMdJ.
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