Abstract
Purpose
Transarterial radioembolization (TARE) with yttrium-90 (90Y) microspheres is a liver-directed treatment for primary and secondary hepatic malignancies. Personalized dosimetry aims for maximum treatment effect and reduced toxicity. We aimed to compare pre-treatment voxel-based dosimetry from 99mTc macroaggregated albumin (MAA) SPECT/CT with post-treatment 90Y PET/CT for absorbed dose values, and to evaluate image quality of 90Y SiPM-based PET/CT.
Methods
Forty-two patients (28 men, 14 women, mean age: 67 ± 11 years) with advanced hepatic malignancies were prospectively enrolled. Twenty patients were treated with glass and 22 with resin microspheres. Radiation absorbed doses from planning 99mTc-MAA SPECT/CT and post-therapy 90Y PET/CT were assessed. 90Y PET/CT images were acquired for 20 min and reconstructed to produce 5-, 10-, 15-, and 20-min datasets, then evaluated using the 5-point Likert scale.
Results
The mean administered activity was 3.44 ± 1.5 GBq for glass and 1.62 ± 0.7 GBq for resin microspheres. The mean tumor absorbed doses calculated from 99mTc-MAA SPECT/CT and 90Y PET/CT were 175.69 ± 113.76 Gy and 193.58 ± 111.09 Gy (P = 0.61), respectively for glass microspheres; they were 60.18 ± 42.20 Gy and 70.98 ± 49.65 Gy (P = 0.37), respectively for resin microspheres. The mean normal liver absorbed doses from 99mTc-MAA SPECT/CT and 90Y PET/CT were 32.70 ± 22.25 Gy and 30.62 ± 20.09 Gy (P = 0.77), respectively for glass microspheres; they were 18.33 ± 11.08 Gy and 24.32 ± 15.58 Gy (P = 0.17), respectively for resin microspheres. Image quality of 90Y PET/CT at 5-, 10-, 15-, and 20-min scan time showed a Likert score of 3.6 ± 0.54, 4.57 ± 0.58, 4.84 ± 0.37, and 4.9 ± 0.3, respectively.
Conclusions
99mTc-MAA SPECT/CT demonstrated great accuracy for treatment planning dosimetry. SiPM-based PET/CT scanner showed good image quality at 10-min scan time, acquired in one bed position. A PET/CT scan time of 5 min showed acceptable image quality and suffices for dosimetry and treatment verification. This allows for inclusion of 90Y PET/CT in busy routine clinical workflows. Studies with larger patient cohorts are needed to confirm these findings.
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Introduction
Transarterial radioembolization (TARE) is now an established minimally invasive liver-directed treatment modality. It is used to treat unresectable primary liver cancer, like hepatocellular carcinoma (HCC) and intrahepatic cholangiocarcinoma (ICC), or hepatic metastases from other tumors [1]. Currently, two types of microspheres are available for clinical use: glass (TheraSphere®; Boston Scientific, Marlborough, MA, USA) and resin (SIR-Spheres®; Sirtex, Boston, MA, USA). Several studies have shown that TARE extends progression-free and overall survival [2,3,4,5]. However, treatment efficacy is correlated to tumor absorbed dose and toxicity is determined by the dose to the surrounding, healthy liver tissue [6, 7]. Personalized dosimetry is therefore paramount to keep toxicity at a minimum while aiming for maximal treatment effect. Depending on glass or resin microspheres, different activity calculation models apply. However, the radiation absorbed doses in the tumor(s) vs. the normal liver tissue are not determined [8, 9].
Treatment planning consists of a TARE simulation with an injection of Technetium-99 m (99mTc)-labeled macroaggregated albumin (MAA) in the location(s) of planned 90Y-microsphere delivery, and planar and single-photon emission computed tomography/computed tomography (SPECT/CT) imaging to quantify the lung-shunt fraction (LSF) and to evaluate for collateral extrahepatic tracer deposition. MAA mimics 90Y-microsphere distribution but due to differences in size, shape, and number of particles, it can only give an estimate for radiation absorbed doses for dosimetry [10,11,12,13,14]. Imaging for treatment verification can be performed with 90Y bremsstrahlung SPECT/CT [15]. However, acquisition time is long, and image quality is low [16]. The decay of 90Y produces a positron and electron pair every 32 in 1 million decays allowing for imaging with PET [17]. Despite the higher resolution, image acquisition time is still long, and image quality is suboptimal [18]. Recent technical advances in PET/CT scanners resulted in the development of detectors which combine lutetium-based scintillator crystal arrays with a silicon photomultiplier (SiPM) bloc design leading to higher spatial resolution and with improved reconstruction algorithms, enhance image quality. Not only did hardware advance, currently there are different types of software available to facilitate dosimetry. Several studies indicate that the 3-dimensional voxel-based dosimetry is most accurate in prediction of activity distribution [19,20,21]. However, clinical studies assessing concordance of 3-dimensional voxel-based dosimetry comparing 99mTc-MAA SPECT/CT and post-treatment 90Y PET/CT are lacking.
In this study, we performed personalized, voxel-based dosimetry for radiation absorbed doses based on planning 99mTc-MAA SPECT/CT and post-treatment 90Y PET/CT and evaluated the image quality of SiPM-based PET/CT after 90Y radioembolization.
Material and methods
Participants
We prospectively enrolled consecutive patients with unresectable primary or secondary hepatic malignancies who were scheduled for TARE at our institution. All patients had a diagnostic CT or MRI prior to TARE planning. The administered activity was calculated using the respective vendor’s recommendation: the body surface area (BSA) method was used for resin microspheres and the partition model for glass microspheres. Written informed consent was obtained from all included patients. This study has been approved by the local institutional review board and was registered on clinicaltrials.gov(NCT03109262).
Pre-treatment 99mTc-MAA SPECT/CT protocol
Patients had 99mTc-MAA imaging as part of the standard TARE planning protocol. The intraarterial administration of 148 MBq 99mTc-MAA in the Interventional Radiology suite was followed by anterior and posterior whole-body planar imaging in Nuclear Medicine to quantify LSF. Then a SPECT/CT of the upper abdomen was performed using a dual detector gamma-camera (Infinia Hawkeye 4, Discovery 670 DR or Discovery 870 CZT, GE Healthcare, Waukesha, WI, USA). Images were reconstructed using ordered subset expectation maximization (OSEM).
Post-treatment 90Y SiPM PET/CT protocol
Images were acquired within 24 h after TARE using a SiPM-based PET/CT (Discovery MI, GE Healthcare). A diagnostic contrast-enhanced CT of the upper abdomen was obtained after the administration of 50 mL iodinated contrast media using 120 kV, “smart” modulating mA and a 512 × 512 matrix size. Thereafter, a PET scan was acquired in 3D mode using a single bed position located over the liver, with a total acquisition time of 20 min. The DMI scanner at our institution has an axial field of view of 20 cm. Each field of view contains 71 slices (2.79 mm). The PET emission scan was corrected using the segmented attenuation data of the CT scan and reconstructed both with a standard iterative algorithm (OSEM, 2 iterations, 28 subsets), as well as the vendor recommended reconstruction method, the block sequential regularized expectation maximization (BSREM) (Q.Clear; GE Healthcare). 90Y PET/CT scans were reconstructed as 5-, 10-, 15-, and 20-min datasets to determine image quality at these scan times.
Catheter position of 99mTc-MAA and 90Y-microsphere injection was documented and intended treatment approach, e.g., whole liver vs. lobar vs. segmental.
Image analysis
All images were reformatted into axial, coronal, and sagittal views.
99mTc-MAA planning SPECT/CT was compared to 90Y PET/CT to assess the accuracy of tracer/microsphere distribution. Three-dimensional voxel-based dosimetry was performed using the MIM SurePlan™ software (MIM Software version 6.9.2., Cleveland, OH, USA). This software converts counts per voxel to radiation absorbed dose measured in Gray (Gy). Whole liver and tumor(s) were edge-contoured on the diagnostic CT or MRI obtained prior to TARE planning. These contours were then transferred to 99mTc-MAA SPECT/CT and 90Y PET/CT images using deformable registration to calculate estimated normal liver tissue and tumor radiation absorbed dose, and to assess post-treatment absorbed doses, respectively.
Image quality of SiPM-based PET/CT was evaluated using the 5-point Likert scale (1 non-diagnostic, 2 suboptimal image quality, 3 acceptable image quality, 4 good image quality, 5 excellent image quality). Images were reviewed and analyzed independently in random order by two experienced Nuclear Medicine physicians.
Statistical analysis
Statistical analysis was performed with Prism GraphPad v8.3.0 (GraphPad Software, San Diego, CA, USA).
A two-tailed paired student’s t test was performed to determine differences between 99mTc-MAA SPECT/CT and 90Y PET/CT. A P value of < 0.05 was considered statistically significant. Continuous data are presented as mean ± standard deviation (SD), range: minimum (min)–maximum (max) values.
Results
Forty-two patients (28 males, 14 females, mean age 67 ± 11 (range: 40–88) years) with unresectable, advanced hepatic malignant lesions were prospectively enrolled in this study. The patients were divided into two groups according to the type of microspheres used: 20 patients received TARE with glass and 22 with resin microspheres. The mean administered activity for 90Y glass microspheres was 3.44 ± 1.5 (range: 0.93–7.05) GBq and 1.62 ± 0.7 (range: 0.56–3.15) GBq for 90Y resin. Patients’ characteristics are shown in Table 1.
Comparison of dosimetry estimated from 99mTc-MAA SPECT/CT and 90Y PET/CT
The mean tumor absorbed dose estimated from 99mTc-MAA SPECT/CT was 175.69 ± 113.76 (range: 11.91–381.41) Gy vs. 193.58 ± 111.09 (range: 0.68–391.07) Gy from 90Y PET/CT for glass microspheres and 60.18 ± 42.20 (range: 0.71–183.25) Gy vs. 70.98 ± 49.65 (range: 18.32–270.64) Gy respectively for resin microspheres. For normal liver, the mean absorbed dose from 99mTc-MAA, SPECT/CT was 32.70 ± 22.25 (range: 6.93–80.68) Gy, and 30.62 ± 20.09 (range: 5.29–74.43) Gy from 90Y PET/CT for glass microspheres, and 18.33 ± 11.08 (range: 2.21–39.50) Gy and 24.32 ± 15.81 (range: 1.45–57.61) Gy for resin, respectively. Radiation absorbed doses for tumors and normal liver tissue were not significantly different between 99mTc-MAA SPECT/CT and 90Y PET/CT neither for glass (P = 0.61 and P = 0.77) nor resin (P = 0.37 and P = 0.17) microspheres, indicating high concordance of 99mTc-MAA SPECT/CT and 90Y PET/CT and predictive accuracy of 99mTc-MAA SPECT/CT for absorbed doses for tumor and healthy liver tissue. Data are shown in Table 2 and Fig. 1.
In 24 patients (57.1%), 90Y-microspheres were administered in the same location as 99mTc-MAA in the planning angiography and showed great accuracy in distribution (Fig. 2). In 18 patients (42.9%), 90Y-microspheres were injected differently, either more selectively or only to one lobe for a sequential treatment approach. For glass microspheres (n = 8), we observed a non-significant upward trend in tumor absorbed dose with 203.21 ± 105.78 (range: 0.68–344.44) Gy calculated from 90Y PET/CT vs. 155.11 ± 107.83 (range: 11.91–353.10) Gy from 99mTc-MAA SPECT/CT (P = 0.35). This trend was not seen in normal tissue absorbed dose which stayed consistent with 39.23 ± 27.62 (range: 12.28–80.68) Gy from 99mTc-MAA SPECT/CT vs. 30.50 ± 27.95 (range: 5.67–74.43) Gy calculated from 90Y PET/CT (P = 0.57). Figure 3 shows a patient treated with glass microspheres with a sequential treatment approach and selective treatment of liver segment 1. For resin microspheres (n = 10), different catheter position did not make a change in absorbed doses: For tumor, 62.32 ± 44.59 (range: 0.71–160.78) Gy calculated from 99mTc-MAA SPECT/CT vs. 61.97 ± 32.22 (range: 20.75–130.03) Gy from 90Y PET/CT (P = 0.98); and for normal liver tissue, 22.26 ± 10.83 (range: 3.46–33.75) Gy vs. 33.48 ± 17.03 (range: 8.83–57.61) Gy (P = 0.14), respectively. Data are shown in Table 3.
2A total of 21 patients (50%) were treated for a single tumor and another 21 patients (50%) for multiple liver tumors. Tumor absorbed doses for single tumor treatment were 126.11 ± 90.24 (range: 29.23–347.64) Gy vs. 144.66 ± 93 (range: 20.75–344.44) Gy from 99mTc-MAA SPECT/CT and 90Y PET/CT respectively (P = 0.52). For multiple tumors, absorbed doses were slightly lower with 99.84 ± 89.23 (range: 0.71–353.1) Gy from 99mTc-MAA SPECT/CT vs. 109.01 ± 91.73 (range: 5.26–326.98) Gy from 90Y PET/CT respectively (P = 0.69). When tumor absorbed doses from 99mTc-MAA SPECT/CT and 90Y PET/CT for single tumor and multiple tumor treatment were compared to each other, no significant difference was seen (P = 0.31 vs. P = 0.18). No statistically significant difference was seen in normal liver tissue as well. Data are shown in Table 4.
Image quality of SiPM-based PET/CT
The best image quality was seen at a scan time of 20 min with a Likert score of 4.9 ± 0.3 (range: 4–5). There was no significant difference between a scan time of 20 min and 15 min (4.84 ± 0.37, range: 4–5, P = 0.3). Image quality improved significantly from 5 min (3.6 ± 0.54, range: 3–4) to 10 min scan time (4.57 ± 0.58, range: 3–5, P = 0.000) as well as from 10 min to 15 min (P = 0.001). Data are shown in Table 5. However, a scan time of 5 min suffices for treatment verification and dosimetry (Fig. 4).
In 3 patients, 90Y PET/CT was obtained 24 h after TARE. Figure 5 shows these images reconstructed with OSEM and BSREM at 10-min and 15-min scan time. Image quality was deemed excellent (Likert scale 4.75 ± 0.5, range: 4–5) with both reconstruction methods; however, BSREM was superior.
Discussion
In this prospective study, we evaluated voxel-based dosimetry data and image quality of 90Y PET/CT after TARE using a new generation scanner based on SiPM which shows a higher spatial resolution and allows for improved reconstruction methods like the BSREM algorithm, all resulting in higher sensitivity and image quality [22, 23].
Post-treatment imaging can either be performed with bremsstrahlung SPECT/CT or low-abundance internal pair production PET/CT. SPECT/CT has poor spatial resolution due to detector efficiency, leading to noisy images and long acquisition times [16]. Standard time of flight (ToF) PET provides higher image quality, but still requires a long scan time of approximately 30 min and multiple bed positions [24,25,26]. To date, no studies evaluating SiPM-based PET/CT for post-treatment 90Y imaging have been published. Kunnen et al. compared the performance of a digital PET/CT to an analog PET/CT based on photomultiplier tubes (PMT) in a phantom study to determine the best reconstruction setting for the digital PET/CT [27]. No clinically significant differences were found between the two scanner systems. Visually, the digital PET/CT showed less noise but on a quantitative level, both scanners were equal. Our data show excellent image quality of SiPM-based PET/CT at a scan time of 20 min in a single bed position. However, a short scan time of 5 min showed acceptable to good image quality and suffices for treatment verification and dosimetry calculation. Early visualization of inadvertently extrahepatic 90Y deposition post-therapy is important as interventions can be made accordingly in a timely manner to confine complications.
Dosimetry uses the pre-treatment planning 99mTc-MAA SPECT/CT to estimate the tumor dose to ensure the delivery of a tumorcidal dose while sparing the surrounding healthy liver tissue. Since MAA is different to 90Y-microspheres, it can only give an estimate of tumor absorbed dose. There are multiple studies comparing estimated doses from 99mTc-MAA SPECT/CT and verified doses from post-treatment imaging with controversial results. Some have shown differences [13, 28] while others found a better correlation in primary liver tumors than metastatic liver disease [28, 29]. Most studies comparing pre-treatment 99mTc-MAA SPECT/CT and post-treatment 90Y bremsstrahlung or PET/CT use manually drawn region of interests or rigid contours over tumor and normal liver tissue to quantify for mean counts per pixel and to evaluate the tumor to background ratio [28, 30, 31]. In this study, we used 3-dimensional, voxel-based dosimetry and converted counts per voxel to radiation absorbed dose measured in Gray by taking tumor volume and total liver volume into account. We used a local deposition model with scaling for a known injected activity for simulation 99mTc-MAA SPECT/CT and post-treatment 90Y PET/CT. Our data show that absorbed doses of the tumor and normal liver tissue from 99mTc-MAA SPECT/CT were not significantly different to post-treatment 90Y PET/CT even when stratified for single vs. multiple tumors treated. 99mTc-MAA SPECT/CT accurately predicted the absorbed dose of the tumor and normal liver tissue. This indicates a high accuracy of 99mTc-MAA based dosimetry.
The catheter tip position at the administration of 99mTc-MAA and 90Y-microspheres might contribute to discrepancies of absorbed doses [10]. Our data show that when the catheter position was changed, it was for selective lobar/segmental treatment approach which resulted in no significant difference in absorbed doses between 99mTc-MAA SPECT/CT and 90Y PET/CT. Only in glass microspheres, a not significant trend to higher tumor absorbed dose was observed in post-treatment 90Y PET/CT, suggesting that a more selective treatment might lead to a higher tumor dose. However, this needs to be confirmed in larger and more homogenous patient cohorts.
Depending on which microspheres are administered, different treatment activity calculation models apply. For resin microspheres, a semiempirical method relying on the BSA is used, and for glass microspheres, a whole liver partition model is used, based on medical internal radiation dose (MIRD) principles. Both do not calculate the radiation absorbed dose in the tumors and normal liver tissue. Using accurate dosimetry methods, individualized tumor dose intensification can be made possible to maximize treatment effect while not exceeding the maximal tolerated dose of healthy liver tissue.
Limitations of this study include the small and heterogenous patient cohort. A variety of primary and metastatic liver tumors were treated with resin microspheres whereas glass microspheres were majorly used for primary hepatic malignancies. In total, more patients (27 vs. 15) received TARE for their primary liver tumor. Since this was a very heterogenous patient population with various types of tumor entities, we did not analyze the impact of treatment in terms of response rate and progression-free survival.
Conclusion
99mTc-MAA SPECT/CT showed great accuracy in predicting the absorbed dose of the tumor and normal liver tissue. Good image quality was seen at a reduced scan time of 10 min with SiPM-based 90Y PET/CT, acquired in a single bed position. A PET/CT scan time of 5 min showed acceptable image quality and suffices for dosimetry and treatment verification. A short scan time allows for the inclusion of 90Y PET/CT in busy routine clinical workflows. Studies with larger patient cohorts are needed to confirm these findings.
Data availability
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HD: content planning, data analyses, and manuscript writing and editing; MHK: data analyses and manuscript editing; VF: statistical analyses and manuscript editing; LB: data analyses and manuscript editing; SMS: concept planning and data manuscript editing; DYS: content planning and manuscript editing; AI content planning and manuscript editing
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Duan, H., Khalaf, M.H., Ferri, V. et al. High quality imaging and dosimetry for yttrium-90 (90Y) liver radioembolization using a SiPM-based PET/CT scanner. Eur J Nucl Med Mol Imaging 48, 2426–2436 (2021). https://doi.org/10.1007/s00259-021-05188-4
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DOI: https://doi.org/10.1007/s00259-021-05188-4