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Article

How the Rigid and Deformable Image Registration Approaches Affect the Absorbed Dose Estimation Using Images Collected before and after Transarterial Radioembolization with 90Y Resin Microspheres in a Clinical Setting

1
Department of Medical Physics, IRCCS Azienda Ospedaliero-Universitaria di Bologna, 40138 Bologna, Italy
2
Medical Physics Specialization School, Alma Mater Studiorum, University of Bologna, 40138 Bologna, Italy
3
Department of Radiology, IRCCS Azienda Ospedaliero-Universitaria di Bologna, 40138 Bologna, Italy
4
Radiation Oncology, IRCCS Azienda Ospedaliero-Universitaria di Bologna, 40138 Bologna, Italy
*
Authors to whom correspondence should be addressed.
These authors contributed equally to work.
Appl. Sci. 2022, 12(24), 12767; https://doi.org/10.3390/app122412767
Submission received: 12 September 2022 / Revised: 16 November 2022 / Accepted: 1 December 2022 / Published: 12 December 2022
(This article belongs to the Special Issue Developments of Diagnostic Imaging Applied in Radiotherapy)

Abstract

:
Background: Transarterial radioembolization (TARE) relies on directly injected 90Y- or 166Ho-loaded microspheres in the hepatic arteries. The activity to be injected is generally based on pre-TARE 99mTc-macro-aggregated-albumin (MAA) imaging, while the actual dose distribution is based on post-treatment images. The volume of interest (VOIs) propagation methods (i.e., rigid and deformable) from pre- to post-TARE imaging might affect the estimation of the mean absorbed dose in the tumor and non-tumoral liver (NTL), i.e., DT and DNTL, respectively. Methods: In 101 consecutive patients, liver and tumor were delineated on pre-TARE images and semi-automatically transferred on 90Y-PET/CT images with a rigid or deformable registration approach. Pre- and post-TARE volumes and DT/DNTL/DL were compared using correlation coefficient (CC) indexes, such as intra-class (ICC), Pearson’s (PCC), concordance (CCCo) and Bland–Altman analyses. The Kaplan–Meier curves of overall survival (OS) were calculated according to DT. Results: All computed CCs indicated very good (>0.92) agreement for volume comparison, while they suggested good (ICC ≥ 0.869, PCC ≥ 0.876 and CCCo ≥ 0.790) and moderate agreement in the intra- and inter-modality DT/DNTL/DL comparisons, respectively. Bland–Altman analyses showed percentage differences between the manual and deformable approaches of up to about −31%, 9% and 62% for tumoral volumes, DT and DNTL, respectively. The overall survival analysis showed statistically significant differences using DT cutoffs of 110, 90 and 85 Gy for the manual, rigid and deformable approaches, respectively. Conclusions: The semi-automatic transfer of VOIs from pre- and post-TARE imaging is feasible, but the selected method might affect prognostic DT/DNTL constraints.

1. Introduction

Transarterial radioembolization (TARE) is one the most effective treatments for unresectable primary and secondary hepatic lesions. In TARE, 90Y-loaded resin (SIR-Spheres®, Sirtex Medical Ltd., Woburn, MA, USA) or glass (TheraSphere, Boston Scientific, Marlborough, MA, USA) microspheres or 166Ho-loaded PLLA microspheres (Quiremspheres®, Quirem Medical B.V. subsidiary of Terumo Corporation, Tokyo, Japan)) are selectively injected in the hepatic arteries. The injection leads to a preferential deposition in the tumoral tissues, hence sparing the healthy liver lobes.
The use of 99mTc-macro aggregated albumin (99mTc-MAA) SPECT/CT for treatment planning to assess the target coverage is largely established and recommended in the operating instructions of these devices as well as in the international recommendations [1,2,3]. Moreover, the 99mTc-MAA SPECT/CT images are mandatory to evaluate the possible extrahepatic shunts [4] or to identify patients with a Lung Shunt Fraction (LSF) > 20%, both representing exclusion criteria for TARE patients. More recently, exclusively for 166Ho-based TARE treatment, 99mTc-MAA images have been replaced by 166Ho-Scout dose (using an activity up to 250 MBq) to accurately predict the activity distribution of the therapeutic injection of 166Ho-loaded microspheres [5]. Nevertheless, 99mTc-MAA imaging remains the state-of-the-art approach for predicting the therapeutic 90Y-loaded TARE activity distribution.
Specifically, pre-treatment 99mTc-MAA SPECT/CT 3D voxel-based dosimetry allows the calculation of the absorbed dose distribution expected in patients after the TARE procedure, which can be used to identify the 90Y activity to be administered in order to increase the tumor control while reducing the possible risk of toxicity. In addition, the post-treatment 90Y PET/CT-image-based dosimetry allows the verification of the planned absorbed dose distribution.
Pre-treatment voxel-based dosimetry requires the importing of DICOM images, delineation of volumes of interest (VOIs), calculation of the absorbed dose distribution and computing and evaluation of the dose volume histograms (DVHs). These operations can be performed using CE or FDA marked treatment planning systems (TPSs) [6]. In particular, regarding the operation of VOI contouring, nuclear medicine or interventional radiologist physicians can manually or semi-automatically delineate the tumor, lungs, whole liver and non-tumoral liver (NTL) on SPECT/CT images.
Moreover, the available images for TARE generally also include contrast-enhanced computed tomography (CECT) and 90Y PET/CT images. In each of these modalities, all the VOIs might be manually delineated to obtain target volumes or to perform post-treatment dosimetry. Alternatively, deformable or rigid image registration algorithms are implemented in commercial TPSs to transfer VOIs from any reference modality (e.g., 99mTc-MAA SPECT/CT) to another (e.g., 90Y PET/CT) [6].
Unfortunately, the manual delineation of VOIs is time-consuming and might affect the accuracy of the volume, shape and position of the target and organs at risk (OARs), due to the inter-operator delineation variability on a given image [7]. This has been previously shown in TARE, where the variability between different readers led to tumor-absorbed doses with a low intra-class correlation coefficient (ICC), while showing higher ICC values for liver-absorbed doses [8]. In addition, other sources of VOI delineation discrepancies among image modalities are due to respiratory motion and liver deformation [9].
Several authors investigated the impact of the dose calculation method (e.g., dose kernel convolution vs. local deposition) on absorbed dose distributions [10,11,12,13] and the agreement between pre- and post-treatment image-based dosimetry [14,15,16,17,18]. However, the impact of different VOI propagation modalities demands additional investigations.
In this study, the impact of deformable or rigid registration algorithms implemented in a commercial TPS was assessed in terms of the agreement of volumes and mean absorbed doses on post-treatment dosimetry images and compared to ones calculated using pre-treatment images.
In addition, the correlation between overall survival and tumor mean absorbed doses extracted from pre- and post-treatment dosimetry based on deformable or rigid registration was assessed on a large cohort of TARE patients.

2. Materials and Methods

2.1. Planning and Verification Dosimetry Workflows

In the following sections, the protocol adopted for patient selection, planning and treatment verification is reported and comprehensively summarized in Figure 1. All patients included in the study followed the described protocol.

2.1.1. Patient Eligibility for TARE Treatment

The eligibility of patients was discussed by a multidisciplinary team that included professionals of Interventional Radiology, Radiation Oncology, Nuclear Medicine, Hepatology, Surgery and Medical Physics. Inclusion criteria included: age >18 years, unresectable primary or secondary liver disease. Exclusion criteria included: presence of extrahepatic metastasis; reduced liver functionality; strong impairment of blood tests (bilirubin, albumin); LSF > 20%.

2.1.2. Pre-Treatment Images and Angiographic Procedure

When considered eligible for the treatment, patients underwent a multiphasic CECT to properly identify the intrahepatic tumoral or metastatic areas. The CECT was acquired within one to three weeks from planning the angiographic procedure. The manual contouring of the tumor was jointly performed by the Radiation Oncology and the Interventional Radiology physicians using MIM SurePlan Liver Y90 (MIM Software Inc., Cleveland, OH, USA) by reviewing the arterial or venous phases of the CECT. In a limited number of cases, a magnetic resonance acquisition with contrast media was used for target delineation instead of the CECT.
An angiographic procedure was fully performed to correctly identify the hepatic arteries that primarily supplied the tumor, as described by Gramenzi et al. [19]. During the angiographic procedure, a 150 MBq injection of 99mTc-MAA was performed.

2.1.3. SPECT/CT Imaging

After the angiographic procedure, SPECT/CT and a planar scintigraphy were acquired within one hour.
Planar scintigraphy and SPECT/CT were acquired on a dual-head Discovery 670 NM/CT (GE Healthcare, Chicago, IL, USA; Milwaukee, Brookfield, WI, USA) equipped with low-energy high-resolution collimators, 60 views, 2 projections-per-view and 15 s of acquisition per frame. Ordered subset expectation maximization (OSEM) reconstruction algorithm (2 iterations, 10 subsets, Butterworth post-filtering with order 10 and cutoff frequency 0.48) was used. Attenuation correction based on hybrid CT image, scatter correction (energy window: 120 ± 5 keV) and resolution recovery was applied.
The LSF was assessed on planar scintigraphy. If an LSF > 20% was measured or unwanted/unavoidable shunts to other districts (e.g., gastric shunt) occurred, the patient was excluded from the treatment.

2.1.4. Pre-Treatment Dosimetry and Activity Determination

The phase of the CECT selected for the contouring was rigidly registered to the CT of the SPECT/CT acquisition and the delineated target volume was transferred from the CECT to the SPECT/CT image. Organs at risk (i.e., liver and lungs) were delineated on the CT of the SPECT/CT acquisition using manual contouring or semi-automated tools provided by the TPS. Non-tumoral liver was obtained as a boolean subtraction of the target contour from the whole liver contour.
Activity prescription was performed according to MIRD equations by partitioning the liver and the lungs [20]. The activity was prescribed so that not exceeding 40 Gy to the whole liver. For hepatocellular carcinoma (HCC) patients included in a research trial comparing personalized voxel-based activity prescription with body surface area (BSA) or MIRD activity prescription methods (clinicaltrial.gov ID: NCT05227482), the activity was prescribed based on voxel-based dosimetry obtained on SPECT/CT images to achieve a tumor mean absorbed dose of at least 150 Gy while not exceeding 40 Gy to the normal liver.

2.1.5. Post-Treatment Residual Activity Assessment

All treatments were performed within one to three weeks from the planning 99mTc-MAA injection. All patients were treated in an angiographic procedure that replicated the arterial access employed during the planning injection. Residual activity in the catheters or in the vial were evaluated after the treatment in an experimental setup by multiple acquisitions at fixed distance with an ionization chamber [21].

2.1.6. PET/CT Imaging

All patients received a 90Y PET/CT acquisition the day after the treatment (typically about 20 h after the 90Y administration).
The PET/CT images were acquired on a Discovery MI (GE Healthcare, Chicago, IL, USA; Milwaukee, Brookfield, WI, USA) 3-rings system with time-of-flight (TOF) corrections. Time-of-flight and attenuation correction based on hybrid CT image was always applied. The acquisition protocol consisted of three beds per patient, 10 min per bed.
The image reconstruction system was equipped with a Bayesian penalized likelihood reconstruction algorithm named Q.Clear [22]. The Q.Clear algorithm had a noise suppression term controlled by a parameter, indicated as β, which was the only user-input variable to the algorithm [23]. In this study, a β-value of 4000 was adopted for PET/CT image reconstruction as reported by Hou et al. [24].

2.2. Voxel-Based Dosimetry Tools

Pre-treatment voxel-based dosimetry was performed on pre-treatment 99mTc-MAA SPECT/CT acquisitions with MIM SurePlan Liver Y90. For dose calculation purposes, all counts of the SPECT acquisition in the field-of-view (FOV) were considered and normalized to an injected activity of 1 GBq (“With known activity” approach). When the pre-treatment dosimetry was used for activity planning, the 1 GBq injected activity was eventually scaled by the user to obtain the desired dose to the target and/or OARs. The dose distributions were obtained with a local deposition method (LDM) [11], which assumed a liver-like density over the entire FOV. After the TARE procedure, the pre-treatment dose distribution was scaled to the actual injected 90Y activity and used for the subsequent comparison.
Post-treatment voxel-based dosimetry was obtained from the post-treatment PET/CT acquisition, with the same LDM, based on the total injected activity in the FOV.
Of note, the CE market workflow implemented in MIM for the post-treatment dosimetry is based on the deformable propagation of VOIs, while the rigid propagation can be implemented by the user. Thus, we decided to focus the study on these two methods.
In more detail, the deformable registration algorithm, which allowed for volume adaptation using the CT images based on Hounsfield units (HU) [25], was applied as default of the workflow named “LDM with known activity”. In addition, the contours of the target and OARs were rigidly transferred from the SPECT/CT to PET/CT images, maintaining the structure volumes, using the “Box-based” image registration MIM tool. This box was manually placed to include the tumor and its surrounding organs or tissues (i.e., structures with different electronic densities or HU), facilitating the relocation of the target when liver modifications occurred from one image modality to the other.

2.3. Patients

The investigated cohort included liver cancer patients who underwent TARE with 90Y resin microspheres at our Institute from April 2017 with a minimum follow up of 3 months, for whom VOIs obtained from both deformable and rigid image registration algorithm were available. The written consensus was obtained for patients enrolled in the prospective clinical trial (clinicaltrial.gov ID: NCT05227482), while for the remaining ones ethics approval and participant consent were not necessary as this study involved the use of retrospective de-identified data according to “Determinazione AIFA-20 Marzo 2008 (G.U. n. 76, 31-03-2008)”.

2.4. Volumes and Mean Absorbed Dose Comparisons and Statistical Analysis

The volumes were separately obtained according to pre- and post-treatment images and the adopted modality for VOI generation (i.e., manual contouring on pre-treatment images, termed as VT,m, VL,m and VNTL,m for tumor, liver and NTL, respectively, and rigid or deformable registration algorithms on post-treatment images, named VT,r, VL,r, VNTL,r and VT,d, VL,d, VNTL,d, respectively). Mean absorbed doses by the tumor, the liver and the NTL were determined from the pre-treatment and the post-treatment absorbed dose distributions accordingly. In particular, on the same post-treatment absorbed dose distribution, mean absorbed doses were separately extracted for the rigid and deformable recontouring workflow. These will be referred to as DT,m, DT,r and DT,d for tumor, DNTL,m, DNTL,r and DNTL,d for NTL and DL,m, DL,r and DL,d for liver.
For all volumes and absorbed mean doses, the comparisons between the pre-treatment and post-treatment data (separately for rigid and deformable recontouring approach) and between rigid and deformable recontouring method on the same post-treatment absorbed dose distribution were performed following a Bland–Altman analysis. In this analysis, the average difference between the two measurements represented the bias, while the 95% limits of agreement (LOA), obtained by the bias ± the standard deviation multiplied by 1.96, represented the precision. Agreement was also assessed by the ICC, the Pearson’s correlation coefficient and the concordance correlation coefficient (CCCo); a value ≥ 0.8 indicated excellent correlation. Statistical significance was defined by a p-value < 0.05.

2.5. Survival Analysis

The Kaplan–Meier (K–M) curves of overall survival (OS) were determined from the date of the TARE procedure to the last available follow up. The K–M curves were stratified according to tumor type and tumor mean absorbed doses, determined using VT,m, VT,r and VT,d.
For each dose dataset (i.e., manual and rigid or manual and deformable) of HCC, CCC and mixed HCC/CCC patients, a tumor mean absorbed dose cutoff was obtained to split survival curve. These dosimetric cutoffs were calculated by iterating the calculation of K–M curves among a range of possible dose cutoff values and keeping the highest dose cutoff resulting in p-value < 0.05 between balanced populations (i.e., assuming a splitting between 40% and 60% of the study population).
The confusion matrixes were calculated reporting the number of doses higher or lower than the cutoff estimated for each VOI delineation/propagation approach.
All the analyses were performed using the statistical language R v.4.0.2 (https://www.r-project.org/ (accessed on 30 November 2022)) and the software RStudio v.1.2.1335 (R Core Team, Vienna, Austria).

3. Results

3.1. Patient Cohort

A total of 101 patients (58 males, 43 females) were analyzed. Median age at treatment was 68.5 years (min: 38.1 y, max: 96.7 y). Among them, 75 patients had a diagnosis of HCC, 14 cholangiocarcinoma (CCC) or mixed HCC/CCC and 12 liver metastases of various primary tumors. Portal vein thrombosis was reported in 60 out of 101 patients.
Treated tumor and whole liver volumes are reported in Table 1. Median (range) prescribed activity was 1.2 GBq (0.4; 3.5).
The median (range) follow up was 424 days (90; 1863).

3.2. Impact of Rigid and Deformable Image Registration Algorithms on VOI Volumes

Figure 2 shows the Bland–Altman analyses between Vm, Vr and Vd for liver, tumor and NTL. The largest absolute bias was observed between VL,m and V L,d (−103.4 mL), while the largest relative bias was found between VT,m and VT,d (−30.8%). All absolute and relative biases and LOAs are reported in Supplementary Materials (Tables S1 and S2, respectively).
The correlation coefficient (CC) indexes, such as intra-class (ICC), Pearson’s (PCC), concordance (CCCo) of volumes for target, liver and NTL are reported in Table 2. All CC indexes were >0.995 for volume comparison between Vm and Vr. The deformable registration approach always presented CC indexes > 0.92. All the investigated datasets were statistically significant (p < 0.001).

3.3. Impact of Rigid and Deformable Image Registration Algorithms on Mean Absorbed Doses

In Figure 3, panels (a,c,e), respectively, the Bland–Altman analyses between DT,m and DT,r, between DT,m and DT,d and between DT,r and DT,d are reported. The largest absolute bias was observed between DT,m and DT,d (−41.7 Gy). For this comparison, the 95% LOA was −70.1 and +153.5 Gy. Bias and positive (LOA+) and negative (LOA−) LOAs are reported in Supplementary Materials (Table S1 for absolute values and Table S2 for percentage values) for all the investigated dose comparisons.
The CC indexes of mean absorbed doses for target, liver and NTL are reported in Table 2. All these indexes were statistically significant (p < 0.001).
A good correlation was found for the intra-modality comparisons of the mean absorbed doses (i.e., Dr and Dd) for all the investigated VOIs (i.e., ICC ≥ 0.869, PCC ≥ 0.876 and CCCo ≥ 0.790). Moderate correlation was found for inter-modality comparisons (i.e., Dm and Dr or Dm and Dd), as reported in Table 2.
The CCCo among tumor mean absorbed doses (i.e., DT,m vs. DT,r, DT,m vs. DT,d and DT,r vs. DT,d) were 0.602 (0.479; 0.701), 0.493 (0.368; 0.601) and 0.904 (0.856; 0.936) for HCC/CCC patients, while they were 0.579 (0.101; 0.840), 0.512 (0.065; 0.788) and 0.967 (0.913; 0.988) for metastatic patients.
In Figure 2, panels (b,d,f), respectively, the Bland–Altman analyses between DNTL,m and DNTL,r, between DNTL,m and DNTL,d and between DNTL,r and DNTL,d are reported. The largest absolute bias was observed between DNTL,m and DNTL,d (−2.3 Gy).
The difference between the predicted and the observed doses of NTL was lower than 12 Gy, suggested in Jadoul et al. [17], in 96 out of 101 patients (deformable contouring approach) and 97 out of 101 patients (rigid contouring approach). In the remaining five of the deformable contouring group, the pre-treatment NTL mean absorbed dose always overestimated the post-treatment value, while in one out of four patients of the rigid contouring group the post-treatment NTL mean absorbed dose was higher than the pre-treatment one, probably due to a misalignment of the rigid image registration of a target with a volume of 2 mL. For this patient, nevertheless, no liver toxicity was reported after TARE treatment.
The CCCo among NTL mean absorbed doses (i.e., DNTL,m vs. DNTL,r, DNTL,m vs.DNTL,d and DNTL,r vs. DNTL,d) was 0.798 (0.710; 0.862), 0.755 (0.649; 0.832) and 0.926 (0.886; 0.953) for HCC/CCC patients and 0.913 (0.805; 0.962), 0.846 (0.632; 0.940) and 0.965 (0.889; 0.989) for metastatic patients.

3.4. Overall Survival and Mean Absorbed Doses

The Kaplan–Meier curves of overall survival according to the tumor type for the entire cohort of patients are reported in Figure 4a. The HCC, CCC or mixed HCC/CCC showed similar OS while metastases (i.e., “mets” in Figure 4a) were statistically significantly different; thus, they were excluded for the subsequent analysis. The remaining patients were grouped together and will be referred to as HCC/CCC patients. The Kaplan–Meier curves for the HCC/CCC patients are reported in Figure 4b–d according to the pre-TARE tumor mean absorbed dose for (a) manual, and post-TARE tumor mean absorbed dose with (b) rigid and (c) deformable registration approaches. Higher mean absorbed doses were statistically significantly associated to good prognosis irrespective of tumor type except for metastatic patients.
The best cutoffs of DT,m, DT,r and DT,d were 110, 90 and 85 Gy, respectively. Confusion matrices (Figure 5) for HCC/CCC patients (having a similar survival) revealed that the mislabeled rates were 13%, 16% and 7% using each specific cutoff for the following comparison groups: DT,m vs. DT,r, DT,m vs. DT,d, DT,r vs. DT,d, respectively. Accordingly, for the same comparison groups, the concordance of values above/below the specific group cutoff was 87%, 84% and 93%, respectively. This means that a pre-treatment dose higher than 110 Gy is a good predictor of a post-treatment dose higher than 90 Gy and 85 Gy for the rigid and deformable registration, respectively; thus, a pre-treatment dose higher than 110 Gy can be used to predict higher survival.

4. Discussion

In this study, we focused on the delineation of VOIs in primary and metastatic cancer patients undergoing cone beam CT-guided TARE treatment. In more detail, the impact of transferring manual VOIs to post-treatment images was investigated. Although a high correlation was suggested using each single modality, the pre-treatment and post-treatment volumes and mean absorbed doses in the tumor, liver and NTL showed several discrepancies as highlighted in the following discussion.

4.1. Bland–Altman Plots

The Bland–Altman analyses revealed that the deformable registration approach increased the volumes with regards to the manual one for all the delineated VOIs with a bias (LOA-; LOA+) of −25.6 mL (−115.3; 64.2), −103.4 mL (−403.4; 196.5), −76.5 mL (−349.1; 196.1) for tumor, liver and NTL, respectively. These differences might be due to the dependence of the deformable registration algorithms on liver shape and tumor displacement, which could be strongly affected by the differences in the respiratory phase during the CT acquisition. On the contrary, as expected, the rigid registration kept the volumes almost the same. The slight differences in volume values could be due to the rounding effect in the rototranslation of the VOIs and to the different slice thickness between the CT images of our SPECT/CT and PET/CT systems (i.e., 3.75 mm and 2.78 mm, respectively). Accordingly, the average increase in VT,d and VNTL,d with respect to VT,m and VNTL,m (i.e., a negative bias in Figure 2b) is mirrored by a decrease in the absorbed mean doses of these VOIs. On the contrary, although the volumes are maintained by the rigid registration, a reduction of the DT,r and DNTL,r (i.e., a positive bias in Figure 3a,e) is observed. This is likely to be ascribed to the mispositioning of the VOIs when shape and volume are constrained by the rigid algorithm.
For all the possible combinations in NTL mean absorbed dose (i.e., DNTL,m vs. DNTL,r, DNTL,m vs. DNTL,d and DNTL,r vs. DNTL,d), the Bland–Altman analyses resulted in a maximum bias of 2.3 Gy [−8.8;13.5]. These results were similar to the ones reported in Richetta et al. [15] for 10 HCC patients (i.e., 0.9 Gy (−7.4; 9.1)) using a manually adjusted delineation in both pre- and post-treatment images. On the contrary, tumor mean absorbed dose showed larger biases and LOAs for all the possible combinations (i.e., DT,m vs. DT,r, DT,m vs.DT,d and DT,r vs.DT,d were 31.2 Gy (−80.6; 143.0), 41.7 Gy (−70.1; 153.5) and 10.5 Gy (−37.1; 58.1), respectively) when compared to the same study (i.e., −5.8 (−79.7; 68.2)). These discrepancies are likely due to the different range of evaluated tumor volumes between the two investigated populations and to the VOI delineation/propagation methods. In particular, in our study tumor volumes ranged from 1.3 to 1702.9 mL, while in Richetta et al. they went from 20 to 647 mL, and the VOIs delineated on SPECT/CT images were copied on PET/CT images and adjusted by applying a threshold method to reproduce the same volume values.
Moreover, Brosch et al. [26], using a rigid registration approach, reported that the mean difference for the NTL mean absorbed dose using 99mTc-MAA SPECT/CT and 90Y PET/CT was 2.1 Gy (−1.2; 5.5), while the mean difference for the tumor was 7.2 Gy (−32.9; 47.3) in nine HCC patients (with volumes ranging from 16 to 1760 mL).
These results showed a concordance between pre-treatment and post-treatment dosimetry better than the one reported in our study. The larger absorbed dose discrepancies experienced in our results could be due to the higher number of patients and tumor/liver shape and size variability.
The Bland–Altman plots reported by Jadoul et al. [17] showed that the variations between predicted and effective doses were markedly higher in the tumors than in the NTL, especially in lesions with major uptake. The mean differences in tumors were −11.4 Gy (−68.4; 45.7) for HCC and −8.23 Gy (−68.9; 52.5) for metastatic patients, while in NTL they were 0.22 Gy (−6.02; 6.47) for HCC and −1.41 Gy (−11.9; 9.06) for metastatic patients. Again, these results were obtained in a smaller patient cohort (19 HCC and 20 liver metastases), with tumor volumes delineated on the three-phase injected CT and subsequently transposed on the 99mTc-MAA SPECT/CT and 90Y PET/CT studies with a slight visual adaptation to compensate for the small imperfections of co-registration and volume variations. However, this readjustment operation might have positively affected the results reported in [17] when compared to ours. In addition, the volume of the injected liver was determined on functional images using thresholding of 1% of the maximum activity, while our propagation was based on the morphological images (i.e., CT images). Of note, the search of the actual liver volume through a threshold operation on functional images could be distorted by blurring artifacts related to respiratory motion in both PET and SPECT images [9] and by different image resolutions.
The Bland–Altman plots in d’Abadie et al. [18] also demonstrated that in 95% of cases, NTL doses calculated with 90Y imaging were 21.2% below and 20.6% above whole normal liver doses calculated with MAA imaging (0.788–1.206; 95% LOA of logarithmic differences), while tumor-absorbed doses calculated with 90Y imaging were 74.6% below and up to 4.5 times above tumor-absorbed doses evaluated with MAA imaging (0.254–4.485; 95% LOA of logarithmic differences).

4.2. Concordance Correlation Coefficients

The CCCos among tumor mean absorbed doses for metastatic patients (i.e., 0.58 (0.10–0.84)) were similar to the ones reported by Jadoul et al. [17] (i.e., 0.52 (0.50; 0.53)), while for HCC/CCC patients CCCos (i.e., 0.60 (0.48; 0.70)) were lower (i.e., 0.82 (0.79; 0.84)). For NTL mean absorbed doses, CCCos resulted in 0.91 (0.80; 0.96) vs. 0.80 (0.76; 0.83) in metastatic patients and 0.80 (0.71; 0.86) vs. 0.94 (0.93; 0.95) in HCC/CCC patients.
The difference between the predicted and the observed doses of NTL generally did not exceed 12 Gy, with few exceptions, similarly to Jadoul et al. [17].
Based on these results, the DNTL were accurately predicted with MAA imaging and could be used to optimize the activity planning using the voxel dosimetry. Similar results were obtained by d’Abadie et al. [18] but using the partition model.
In more detail, in a cohort of 66 patients d’Abadie et al. [18] delineated the target using the baseline contrast-enhanced MRI or CT scan: these images were fused with 99mTc-MAA SPECT and 90Y PET using a rigid registration. The correlation between 99mTc-MAA- and 90Y-based dosimetry NTL doses was very strong with a median absolute deviation of only 1.9 Gy, while for tumor-absorbed dose discrepancies were larger.

4.3. Dose–Survival Relationship

The number of studies reporting a relationship between response and tumor dose are increasing over time for patients treated with TARE. Specifically concerning 90Y-loaded resin microspheres, a threshold of 100–120 Gy as a predictor of treatment response or OS has been identified by several studies [27]. In this context, therefore, the cutoff reported in the cohort of patients investigated in this study was in agreement with other authors [7,28,29,30].
In detail, Strigari et al. reported a significantly higher mean target-absorbed dose of 99 Gy in patients with complete or partial tumor response using 90Y-bremsstrahlung SPECT [30]. Allimant et al. [28] reported a TD of 92 Gy for predicting the complete or partial tumor response. In a much smaller series, all patients who showed a response after resin microsphere treatment had received a tumor dose of at least 91 Gy [29].
Moreover, Nodari et al. [7] reported a cutoff in terms of the target mean absorbed dose of 115 and 98 Gy, using 99mTc-MAA SPECT/CT- and 90Y PET/CT-based dosimetry, respectively, for predicting the OS.
Of note, the methodology proposed in this paper for the evaluation of the impact of VOI transfer can also be applied to images from TARE patients treated with 90Y-loaded glass or 166Ho-PLLA microspheres. It should be noted, nevertheless, that the cutoffs of mean absorbed dose used for stratifying survival curves reported in this study are only applicable to 90Y-loaded resin microspheres as the tumor mean absorbed doses that are needed to treat the patients depend on the characteristics of the used device (e.g., the specific activity per microsphere, the dose rate, the heterogeneity of the absorbed dose distribution and the embolization capability) [31,32]. In particular, these characteristics led to reported threshold doses ranging from 205 Gy to 257 Gy for various tumor types treated with 90Y-loaded glass microspheres [27] and 90 Gy for colorectal cancer metastasis treated with 166Ho microspheres [33].
In addition, the role of 99mTc-MAA should be carefully considered when compared to 90Y-loaded resin/glass microspheres, due to the intrinsic differences in terms of shape, size, size variability, density and number of injected particles [20]. Moreover, there are differences in the image-based activity quantification when comparing the 99mTc-MAA SPECT/CT and 90Y PET/CT activity distributions. Both issues could partially explain the disagreement between pre- and post-treatment absorbed dose distributions reported in this study. These limitations could be overcome in 166Ho-loaded microsphere TARE, where a superior predictive value of 166Ho scout dose for intrahepatic distribution with respect to 99mTc-MAA was reported [34]. Nevertheless, the replication of the angiographic procedure simulated with the 99mTc-MAA or 166Ho scout dose during the treatment still plays a critical role for the pre- and post-treatment absorbed dose distribution agreement [35].
A limitation of this study is that the post-treatment dosimetry image is optimized according to 2020 Hou, indicating 4000 as the optimal beta value for dosimetric purposes. Nevertheless, the results of the impact of VOI propagation remain generally applicable to reconstructed images. Of note, in all the patients we used the same 99mTc MAA SPECT/CT acquisition and reconstruction protocol.
Another issue is that the VOI propagation algorithm previously validated in Calusi et al. [25] is only based on the CT images of both SPECT/CT and PET/CT. In particular, we recognize that the hybrid CT has a poor image quality when compared to CECT but it is still able to capture the mechanical deformation of the liver that occurs between SPECT/CT and PET/CT image acquisitions due to patient breathing and positioning. In addition, the CT-based image registration may represent an advantage because it is not dependent on the possible mismatch of the activity distributions between the 99mTc-MAA SPECT and 90Y PET images.
Concerning the possible misalignment from SPECT or PET images and the attenuation correction maps due to respiratory motion during each multimodality image acquisition, this problem was also addressed by our group developing an ad hoc solution for SPECT/CT motion correction [36], while a commercial PET/CT motion correction solution was developed [37] but is not available in our Institute. For this reason, we preferred to not apply any motion correction in this study.
In this work, only the mean absorbed doses on tumors and organs were reported. Nevertheless, the mean absorbed dose approach may not be suitable for all tumors. For example, large tumors with relevant volumes of necrosis are associated to lower mean absorbed doses given the heterogeneity of the activity distributions but may respond to TARE due to high uptake in vital areas. In practice, the mean absorbed dose of vital tumor volumes is generally higher than the one of the entire tumor volumes, leading to a possible change in the absorbed dose thresholds reported from our OS-based analysis. Moreover, since these volumes are typically visible in CECT in terms of contrast media uptake but not in hybrid CT images, necrotic volumes might represent a critical issue in the use of automatic contouring or re-contouring tools. The impact of necrosis in the assessment of mean absorbed dose to the vital areas of the tumors will be addressed in future studies.
As for future improvements, several proposed solutions for compensating the respiratory motion in SPECT/CT [36,38,39] and PET/CT [37] images could improve the image recovery and enable a better agreement among corrected pre- and post-TARE images, thus potentially reducing the dosimetric disagreement among VOIs.

5. Conclusions

Delineation methods might be crucial for assessing dosimetry in patients undergoing TARE. The possibility of VOI transferring between imaging modalities allows sparing time for re-contouring compared to manual delineation especially in large cohorts. In our study, high concordance was found between VOIs manually delineated in 99mTc-MAA SPECT/CT pre-treatment images and semi-automatically transferred on 90Y PET/CT post-treatment images with a rigid or deformable approach. On the contrary, mean absorbed doses obtained by the above-mentioned VOIs showed higher discrepancies.
Survival analyses highlighted different thresholds of mean absorbed doses for OS in HCC/CCC patients obtained when considering the manual delineation approach for pre-treatment and the rigid or deformable approaches for post-treatment images.
Finally, the application of semiautomatic strategies for VOI transfer should be applied carefully especially for small tumors, representing the most critical subgroup.

Supplementary Materials

The following supporting information can be downloaded at: https://www.mdpi.com/article/10.3390/app122412767/s1.

Author Contributions

Conceptualization, L.S.; methodology, G.D.G.; formal analysis, M.S.; investigation, L.S., M.S. and G.D.G.; data curation, G.P, A.C., C.M. and E.L.R.; writing—original draft preparation, L.S., G.D.G. and G.P.; writing—review and editing, M.S. and S.S.; supervision, L.S.; funding acquisition, L.S. All authors have read and agreed to the published version of the manuscript.

Funding

This study was partially supported by Associazione Italiana di Ricerca sul Cancro (AIRC) IG 20809 (2017) PI: L. Strigari.

Institutional Review Board Statement

The study was based on two populations. The first was included in a study approved by the Ethics Committee of IRCCS Azienda Ospedaliero-Universitaria di Bologna (Project identification code: 742/2019/disp/AoUBo and clinicaltrial.gov ID: NCT05227482), while the second comprised retrospective liver cancer and metastatic patients who underwent TARE treatment.

Informed Consent Statement

The study was conducted in accordance with the Declaration of Helsinki. All the subjects enrolled in the prospective clinical trial funded by AIRC and approved by the Ethics Committee of IRCCS Azienda Ospedaliero-Universitaria di Bologna (Project identification code: 742/2019/disp/AoUBo and clinicaltrial.gov ID: NCT05227482) gave their informed consent for inclusion before they participated in the study. For the remaining patients, ethics approval was not necessary as this study involved the use of retrospective de-identified data according to “Determinazione AIFA-20 Marzo 2008 (G.U. n. 76, 31-03-2008)”.

Data Availability Statement

Data are available based on a reasonable request to the corresponding author.

Acknowledgments

The authors acknowledge the Associazione Italiana di Ricerca sul Cancro (AIRC) partially supporting the study.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. TARE pre-treatment planning dosimetry (panel (a)) and post-treatment verification dosimetry (panel (b)) workflows.
Figure 1. TARE pre-treatment planning dosimetry (panel (a)) and post-treatment verification dosimetry (panel (b)) workflows.
Applsci 12 12767 g001
Figure 2. Bland–Altman plots for tumor (i.e., panels (a,b)), whole liver (i.e., panels (c,d)) and NTL (i.e., panels (e,f)) volumes according to the contouring approach.
Figure 2. Bland–Altman plots for tumor (i.e., panels (a,b)), whole liver (i.e., panels (c,d)) and NTL (i.e., panels (e,f)) volumes according to the contouring approach.
Applsci 12 12767 g002
Figure 3. Bland–Altman plots for tumor (i.e., panels (a,b)), whole liver (i.e., panels (c,d)) and NTL (i.e., panels (e,f)) mean absorbed doses according to the contouring approach.
Figure 3. Bland–Altman plots for tumor (i.e., panels (a,b)), whole liver (i.e., panels (c,d)) and NTL (i.e., panels (e,f)) mean absorbed doses according to the contouring approach.
Applsci 12 12767 g003
Figure 4. Kaplan–Meier curves of OS according to the (a) tumor type; K–M curves of OS for all HCC, CCC and mixed HCC/CCC patients according to the pre-TARE tumor mean absorbed dose for (b) manual, and post-TARE tumor mean absorbed dose with (c) rigid and (d) deformable registration approaches. Time is expressed in days.
Figure 4. Kaplan–Meier curves of OS according to the (a) tumor type; K–M curves of OS for all HCC, CCC and mixed HCC/CCC patients according to the pre-TARE tumor mean absorbed dose for (b) manual, and post-TARE tumor mean absorbed dose with (c) rigid and (d) deformable registration approaches. Time is expressed in days.
Applsci 12 12767 g004
Figure 5. Confusion matrices for HCC/CCC patients for all the possible contouring comparisons: (a) manual and rigid; (b) manual and deformable; (c) rigid and deformable.
Figure 5. Confusion matrices for HCC/CCC patients for all the possible contouring comparisons: (a) manual and rigid; (b) manual and deformable; (c) rigid and deformable.
Applsci 12 12767 g005
Table 1. Volumes of treated tumor and whole liver in mL.
Table 1. Volumes of treated tumor and whole liver in mL.
VOIMin Volume (mL)Median Volume (mL)Max Volume (mL)
Treated tumor1.3118.51702.9
Whole liver816.81580.23393.3
NTL764.21379.32964.1
Table 2. ICC of volumes and mean absorbed doses vs. the methods of VOI delineation and propagation. Ninety-five percent confidence intervals (CI) of CCCo are reported. § All values were statistically significant (p < 0.001).
Table 2. ICC of volumes and mean absorbed doses vs. the methods of VOI delineation and propagation. Ninety-five percent confidence intervals (CI) of CCCo are reported. § All values were statistically significant (p < 0.001).
Var.1Var.2ICC §Pearson §CCCo (95% CI)
DT,rDT,d.0.8750.9080.875 (0.826; 0.911)
DT,mDT,r0.5900.7070.605 (0.491; 0.699)
DT,mDT,d0.4860.7210.524 (0.418; 0.617)
VT,rVT,d0.9900.9950.990 (0.986; 0.993)
VT,mVT,r1.0001.0001.000 (1.000; 1.000)
VT,mVT,d0.9900.9950.990 (0.986; 0.992)
DNTL,rDNTL,d.0.8690.8760.790 (0.713; 0.846)
DNTL,mDNTL,r0.8200.8430.821 (0.748; 0.873)
DNTL,mDNTL,d0.7870.8420.789 (0.713; 0.846)
VNTL,rVNTL,d0.9270.9400.927 (0.894; 0.950)
VNTL,mVNTL,r0.9960.9960.996 (0.994; 0.997)
VNTL,mVNTL,d0.9290.9440.929 (0.897; 0.951)
DL,rDL,d.0.9300.9310.929 (0.897; 0.952)
DL,mDL,r0.8600.9070.862 (0.807; 0.903)
DL,mDL,d0.8590.9250.863 (0.810; 0.902)
VL,rVL,d0.9590.9710.959 (0.941; 0.972)
VL,mVL,r0.9980.9980.998 (0.997; 0.999)
VL,mVL,d0.9570.9710.957 (0.938–0.971)
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Della Gala, G.; Santoro, M.; Paolani, G.; Strolin, S.; Cappelli, A.; Mosconi, C.; Lodi Rizzini, E.; Strigari, L. How the Rigid and Deformable Image Registration Approaches Affect the Absorbed Dose Estimation Using Images Collected before and after Transarterial Radioembolization with 90Y Resin Microspheres in a Clinical Setting. Appl. Sci. 2022, 12, 12767. https://doi.org/10.3390/app122412767

AMA Style

Della Gala G, Santoro M, Paolani G, Strolin S, Cappelli A, Mosconi C, Lodi Rizzini E, Strigari L. How the Rigid and Deformable Image Registration Approaches Affect the Absorbed Dose Estimation Using Images Collected before and after Transarterial Radioembolization with 90Y Resin Microspheres in a Clinical Setting. Applied Sciences. 2022; 12(24):12767. https://doi.org/10.3390/app122412767

Chicago/Turabian Style

Della Gala, Giuseppe, Miriam Santoro, Giulia Paolani, Silvia Strolin, Alberta Cappelli, Cristina Mosconi, Elisa Lodi Rizzini, and Lidia Strigari. 2022. "How the Rigid and Deformable Image Registration Approaches Affect the Absorbed Dose Estimation Using Images Collected before and after Transarterial Radioembolization with 90Y Resin Microspheres in a Clinical Setting" Applied Sciences 12, no. 24: 12767. https://doi.org/10.3390/app122412767

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