Literature DB >> 35167403

Performance Evaluation of Deformable Image Registration Algorithms Using Computed Tomography of Multiple Lung Metastases.

Min Cheol Han1, Jihun Kim1, Chae-Seon Hong1, Kyung Hwan Chang2, Su Chul Han1, Kwangwoo Park1, Dong Wook Kim1, Hojin Kim1, Jee Suk Chang1, Jina Kim1, Sunsuk Kye3, Ryeong Hwang Park3, Yoonsun Chung4, Jin Sung Kim1.   

Abstract

Purpose: Various deformable image registration (DIR) methods have been used to evaluate organ deformations in 4-dimensional computed tomography (4D CT) images scanned during the respiratory motions of a patient. This study assesses the performance of 10 DIR algorithms using 4D CT images of 5 patients with fiducial markers (FMs) implanted during the postoperative radiosurgery of multiple lung metastases.
Methods: To evaluate DIR algorithms, 4D CT images of 5 patients were used, and ground-truths of FMs and tumors were generated by physicians based on their medical expertise. The positions of FMs and tumors in each 4D CT phase image were determined using 10 DIR algorithms, and the deformed results were compared with ground-truth data.
Results: The target registration errors (TREs) between the FM positions estimated by optical flow algorithms and the ground-truth ranged from 1.82 ± 1.05 to 1.98 ± 1.17 mm, which is within the uncertainty of the ground-truth position. Two algorithm groups, namely, optical flow and demons, were used to estimate tumor positions with TREs ranging from 1.29 ± 1.21 to 1.78 ± 1.75 mm. With respect to the deformed position for tumors, for the 2 DIR algorithm groups, the maximum differences of the deformed positions for gross tumor volume tracking were approximately 4.55 to 7.55 times higher than the mean differences. Errors caused by the aforementioned difference in the Hounsfield unit values were also observed. Conclusions: We quantitatively evaluated 10 DIR algorithms using 4D CT images of 5 patients and compared the results with ground-truth data. The optical flow algorithms showed reasonable FM-tracking results in patient 4D CT images. The iterative optical flow method delivered the best performance in this study. With respect to the tumor volume, the optical flow and demons algorithms delivered the best performance.

Entities:  

Keywords:  deformable image registration; fiducial marker tracking; lung deformation; multiple lung metastases; tumor tracking

Mesh:

Year:  2022        PMID: 35167403      PMCID: PMC9099354          DOI: 10.1177/15330338221078464

Source DB:  PubMed          Journal:  Technol Cancer Res Treat        ISSN: 1533-0338


Introduction

Intensity-modulated radiation therapy (IMRT) has become the standard technique in radiation therapy as an accurate and reliable dose delivery method for treating tumors, while sparing normal tissues from being affected by radiation.[1-4] While implementing IMRT, it is desirable to define the tumor volume as small as possible, but tumor movements due to respiratory motions disturb the clear delineation of the tumor volume.[5,6] In this case, 4-dimensional computed tomography (4D CT) images are an effective option to provide information on the trajectories of tumors during respiratory motion, and the real-time tumor tracking method based on a 4D CT-based plan is one of the most effective ways to deliver a high dose to a focal area while accounting for the respiratory motion. Tumor tracking techniques mostly require the implant of fiducial markers (FMs) around the tumor as surrogates for the tumor position. However, in patients with small lung cancers (eg, oligometastases ), the implant of FMs before radiation treatment is clinically unacceptable due to the risk of pneumothorax up to 50%. Pop et al suggested a new method, that is, peri-operative fiducial implant, for postoperative CyberKnife® (CyberKnife SRS, Accuray, Inc.) radiosurgery for the tumor-tracking treatment of lung tumor patients. For potential risks and local recurrences, they implanted preventive FMs near tumors during surgery, and the FMs were utilized for complementary radiation treatments. However, these methods can increase tumor localization errors.[12-14] Therefore, to use the tumor tracking method with a limited number of FMs, uncertainties related to motion discrepancies between FMs and tumors should be quantified to be considered in the treatment planning. In this field, a deformable image registration (DIR) algorithm is one of the feasible solutions for finding a correlation between the tumor positions and FMs in 4D CT images.[15-17] DIR algorithms have evolved over the last few decades and have been utilized to achieve specialized objectives, such as matching of images generated by homogeneous/heterogeneous modalities and dose accumulation, considering different motion/posture phases.[18,19] Moreover, DIR algorithms have been frequently utilized for the assessment of respiratory motion based on 4D CT images.[20-24] Several literature reports have also presented the accuracies of DIR algorithms in different cases, including the occurrence of high- and low-contrast regions[25-36] and multiorgan deformation.[37,38-40] Based on this information, various DIR algorithms have been implemented in commercial oncology software and treatment planning systems (eg, MIM [MIM Software Inc.] and RayStation [RaySearch Laboratories]) and are being used for practical purposes. Yeo et al quantitatively investigated the accuracy of various DIR algorithms in terms of the displacement of FMs and tumors in the low-contrast regions of images. They also evaluated the deformation performance of DIR algorithms using a deformable phantom. Based on the literature, the DIR methods have been already used clinically for lung cases. Unfortunately, these DIR algorithms were not quantitatively evaluated using the CT data of patients who received perioperative FM implant in the lungs to treat multiple lung metastases using postoperative radiosurgery. Accordingly, evaluating the trajectory correlation between FMs and tumors in tumor-tracking radiation therapy is necessary using implanted FMs. Thus, in this study, we evaluated the tracking performance of 10 DIR algorithms for FMs and tumors using 4D CT images of 5 patients with multiple lung metastases.

Materials and Methods

Patients and 4D CT Images

This study was approved by the institutional review board of the Severance Hospital (4-2020-0311), and all methods were performed under relevant guidelines and regulations. The requirement for informed consent waived with the approval of the ethics committee given that patient anonymity was ensured. The 4D CT images of 5 consecutive patients with intraoperative FM implant were retrospectively evaluated in this study. Patient characteristics are summarized in Table 1. The number of multiple metastatic tumor lesions (gross tumor volume) in the lungs varied among the patients (range: 1-10). Four to six FMs were implanted for each patient during the surgery performed prior to radiation therapy. A maximum of 3 FMs were implanted in each of the right and left lobes. In general, one FM was implanted into each of the upper, middle, and lower lobes of the lung. The number of implanted FMs was determined during surgery by the surgeon considering the number and location of the tumor and patient factors. Figure 1 shows a schematic illustration and representative CT image with 6 FMs.
Table 1.

Summary of Patient Characteristics.

No.FMsGTVs
LeftRightTotalLeftRightTotal
Patient #13365510
Patient #2325022
Patient #3235011
Patient #4224213
Patient #5336145
Total13132681321

Abbreviations: FM, fiducial markers; GTV, gross tumor volume.

Figure 1.

(a) Schematic and (b) patient CT images of perioperative fiducial implant for postoperative radiosurgery in the lung.

(a) Schematic and (b) patient CT images of perioperative fiducial implant for postoperative radiosurgery in the lung. Summary of Patient Characteristics. Abbreviations: FM, fiducial markers; GTV, gross tumor volume. Patients were set up in the head-first supine position and immobilized using a vacuum BodyFix® (BodyFix, Elekta AB) and Kneefix™ (CIVCO, Civco Medical Solutions). For respiratory motion control, all 4D CT simulations were scanned with free breathing and continuous positive airway pressure (C-PAP). The C-PAP levels were set to 10 to 15 cmH2O depending on the breathing condition of the patient. Under the consideration of clinical practice, the pixel resolution of CT images was approximately 1.0 × 1.0 mm2, and the slice thickness of each image was fixed at 3.0 mm. All 4D CT images were acquired with a 16-slice scanner (Aquilion LB, Canon Medical Systems) using a respiratory monitoring system (Anzai, Anzai Medical) and retrospectively sorted (reconstructed) into 10-phase bins within the respiratory cycle. Table 1 provides information regarding the number of FMs and the tumors (or gross tumor volumes [GTVs]).

Generation of the Ground-Truth From 4D CT

For the quantitative evaluation of the DIR algorithms, we compared the deformed position and its ground-truth position. First, in this study, the end exhalation (T50) phase was set to the reference phase of 4D CT, and the ground-truth positions for tracking FMs and GTVs in 4D CT were generated from the reference phase to others (ie, T60, …, T0, …, T30, T40). Regarding the ground-truth, the trajectory of an FM was generated by following the position of the voxel that had the maximum Hounsfield unit (HU) value near the FM position of the previous phase, considering the smaller size of the FM as compared to the voxel resolution. A contour of GTVs was defined on each phase of the 4D CT by physicians based on their medical expertise, and subsequently, the trajectory of each GTV was estimated according to the center of mass of the tumor volumes (average volume of GTV <0.5 mL). The final contours used in the analysis were reviewed by the same experienced physician to avoid inter-physician bias. The uncertainty of the ground-truth position was within 1.00 × 1.00 × 3.00 mm3, which is as much as the voxel resolution used in this study.

Assessment of DIR Algorithms

This study aims to evaluate whether the previous phantom-based research could be applied to a real patient image in clinical practice. For this, a total of 10 DIR algorithms were investigated, selected by considering the results obtained by Yeo et al : 4 optical flow algorithms, 3 demon algorithms, 2 level-set motion algorithms, and 1 free-form deformation algorithm. Based on the results reported in the literature, an algorithm in which FMs would not be identifiable (ie, b-spline) and the worst demons algorithm producing significantly incorrect deformation results (ie, double force demons) were excluded in this study. Table 2 lists the DIR algorithms investigated in this study.
Table 2.

List of the Deformable Image Registration (DIR) Algorithms Investigated in This Study.

IndexDIR Algorithm
AOriginal Horn and Schunck 45
BCombined Lucas Kanade and Horn and Schunck 46
CInverse consistent Horn and Schunck 47
DIterative optical flow method 43
EFast demons 34
FModified demons 48
GOriginal demons 44
HOriginal level set motion 49
IAffine approximation of level set motion 49
JFree-form deformation method 50
List of the Deformable Image Registration (DIR) Algorithms Investigated in This Study. All DIR algorithms listed in Table 2 were implemented by the Deformable Image Registration and Adaptive Radiotherapy (DIRART) software. Four multigrid stages were used (n = 1 to 4) with 10n iterations per pass to establish the optimum DIR performance. The DIRART software has been widely used in research and clinical areas with respect to image registration study to this day.[36,52-54] The DIRs were calculated without any postprocessing methods, such as smoothing, and the results were extracted as an array type, including deformation vector fields (DVFs) generated by DIR for the calculation of voxel movements. For performing DIR, the reference phase (ie, T50) and other phases (T60, T70, …, T30, and T40) were selected as a moving image and fixed images, respectively. The entire field of view of the CT image was selected as a region of interest of DIR. Each deformed position of the FMs and GTVs was collected by direction vectors extracted from the DVF corresponding to the index of the maximum HU value and the center of mass of the GTV in the reference phase, respectively. Subsequently, for the evaluation of the DIR performance, the results obtained by the 10 DIR algorithms were compared, in terms of the target registration error (TRE), with the ground-truth generated, as detailed in the section “Generation of the Ground-Truth From 4D CT”.

Results

Assessment of the Deformed Images According to the DIR Algorithms

Figure 2 presents an example of deformed images according to each of the 10 DIR algorithms (top) and their difference maps compared with the original fixed image (bottom). Qualitatively, our results indicate that the images deformed by optical flow algorithms (Algorithms A–D) and demons algorithms (Algorithms E–G) were reasonably well deformed. The images deformed by other algorithms were slightly (Algorithms H) or fairly (Algorithms I–J) different from the original fixed image (Figure 2).
Figure 2.

Example of deformed images according to 10 deformable image registration (DIR) algorithms (top) and their difference maps compared with the original fixed image (bottom). The DIR algorithms are listed in Table 2.

Example of deformed images according to 10 deformable image registration (DIR) algorithms (top) and their difference maps compared with the original fixed image (bottom). The DIR algorithms are listed in Table 2.

Assessment of the Deformed Position for FMs

Figure 3 details the TREs of the X, Y, Z, and 3D displacements between the ground-truth and estimated positions obtained using the DIR algorithms for FM movements. In the figure, the optical flow methods (Algorithms A–D) delivered better tendency regardless of the position of FMs, and the mean and standard deviations of TREs were in the range of 1.82 ± 1.05 mm (best performance, Algorithm D) to 1.98 ± 1.17 mm (worst performance, Algorithm B). These errors were within the uncertainty of the ground-truth. With respect to the demons algorithms (Algorithms E–G), the TREs were slightly higher (2.23 ± 2.78 [Algorithm F] to 3.41 ± 4.42 mm [Algorithm G]) than those of the optical flow algorithms. In other DIR algorithms (Algorithms H–J), considerable differences were observed between the ground-truth and deformed positions, varying from 5.43 ± 7.82 mm (Algorithm I) to 7.11 ± 9.76 mm (Algorithm J).
Figure 3.

Comparison of the target registration errors (TREs) between the ground-truth and the DIR results for fiducial marker (FM) movements: (a) X-axis, (b) Y-axis, (c) Z-axis, and (d) distance in the 3D coordinate space. The DIR results were obtained from 9 images deformed from the reference phases (ie, T50) of 5 patients, and outliers over the 14 mm range were not visualized.

Comparison of the target registration errors (TREs) between the ground-truth and the DIR results for fiducial marker (FM) movements: (a) X-axis, (b) Y-axis, (c) Z-axis, and (d) distance in the 3D coordinate space. The DIR results were obtained from 9 images deformed from the reference phases (ie, T50) of 5 patients, and outliers over the 14 mm range were not visualized.

Assessment of the Deformed Position for Tumors

Figure 4 presents the TREs of the X, Y, Z, and 3D displacements between the ground-truth and estimated positions obtained using the DIR algorithms for GTV movements. Figure 4 indicates the reasonable results obtained by the optical flow methods (Algorithms A–D). These results are comparable to the previous FM results, where the mean and standard deviations of TREs ranged from 1.29 ± 1.21 mm (best performance, Algorithm D) to 1.64 ± 1.22 mm (worst performance, Algorithm B). These deformation errors were within the uncertainty of the ground-truth. With respect to the demons algorithms (Algorithms E–G), the TREs showed better tendency than before, ranging from 1.32 ± 1.22 mm (Algorithm E) to 1.78 ± 1.75 mm (Algorithm G)), which has a similar level of error to that in the case of the optical flow methods. In other cases (ie, Algorithms H–J), the TREs were slightly lower than those of the previous FM results but still higher than those of the optical flow and demons algorithms, varying from 3.07 ± 2.16 mm (Algorithm I) to 5.07 ± 9.33 mm (Algorithm J).
Figure 4.

Comparison of the target registration errors (TREs) between the ground-truth and the DIR results for GTV movements: (a) X-axis, (b) Y-axis, (c) Z-axis, and (d) distance in the 3D coordinate space. The DIR results were obtained from 9 images deformed from the reference phases (ie, T50) of 5 patients, and outliers over the 14 mm range were not visualized.

Comparison of the target registration errors (TREs) between the ground-truth and the DIR results for GTV movements: (a) X-axis, (b) Y-axis, (c) Z-axis, and (d) distance in the 3D coordinate space. The DIR results were obtained from 9 images deformed from the reference phases (ie, T50) of 5 patients, and outliers over the 14 mm range were not visualized.

Discussion

The deformed images obtained by the 10 DIR algorithms exhibited the same trends in all patient images, and our results show that the deformed positions obtained using Algorithms A–F were well estimated within the uncertainty of the tested CT resolution. Here, Algorithm D showed the best performance. Our results were similar to those observed in a prior study on phantom images conducted by Yeo et al. Nevertheless, a few outliers were detected in real patient cases. With respect to the deformed position of FMs, in the 2 DIR algorithm groups, that is, optical flow and demons, the maximum TREs were observed owing to the large discrepancy between the HU values in fixed and moving images. Figure 5 presents an example of outlier results deformed by the original Horn and Schunck optical flow algorithm (Algorithm A). As illustrated in Figure 5a and b, the HU values of the FM included in the fixed image (ie, T30) were relatively lower than those of the moving image (ie, T50), and this HU discrepancy caused the DIR error. In this case, the voxels had to move somewhere, not the ground-truth position, and consequently, TREs would be higher than those in general situations. In Figure 5, the maximum TREs were 2.79 to 4.05 times higher than the mean TREs for all optical flow algorithms. Particularly, when outlier cases that had unclear FMs in 4D CT images were excluded in these samples, the mean, standard deviation, and maximum TREs of the results deformed by the iterative optical flow method were extremely better than before, with values of 1.07, 0.60, and 2.92 mm, respectively. In the clinical approach, FMs may not appear (or appear faintly) in 4D CT images, depending on the status of the 4D CT machine and its configuration (eg, slice thickness and slice increment). This condition would be overcome using an interpolation method between 2 well-deformed results.
Figure 5.

Sample outlier results deformed by the original Horn and Schunck optical flow method (Algorithm A). (a) T50, (b) T30, (c) deformed T50, and (d) the difference between (c) and (b). The red contour in (a) shows a fiducial marker (FM), but the FM is unclear in (b).

Sample outlier results deformed by the original Horn and Schunck optical flow method (Algorithm A). (a) T50, (b) T30, (c) deformed T50, and (d) the difference between (c) and (b). The red contour in (a) shows a fiducial marker (FM), but the FM is unclear in (b). Figure 6 presents an example of another outlier result deformed by the fast demons (Algorithm E) algorithm. Even if FMs were well and clearly defined in moving (Figure 6a) and fixed (Figure 6b) images, under the demons algorithms, the deformation of the FM positions included in the deformed T50 (Figure 6c) was superior to that of the fixed image.
Figure 6.

Sample outlier results deformed by the fast demons algorithm (Algorithm E). (a) T50, (b) T90, (c) deformed T50, and (d) the difference between (c) and (b). The red contours in (a)–(c) show the different positions of an identical fiducial marker (FM) inserted in the patient.

Sample outlier results deformed by the fast demons algorithm (Algorithm E). (a) T50, (b) T90, (c) deformed T50, and (d) the difference between (c) and (b). The red contours in (a)–(c) show the different positions of an identical fiducial marker (FM) inserted in the patient. This trend in the deformation errors did not exhibit any significant difference, in comparison with the results obtained via DIR in phantoms reported by Yeo et al. Hence, the limitations of the demons algorithms described in the literature apply not only to phantom images but also to patient CT images. Considering the deformed positions for tumors, in the 2 DIR algorithm groups, that is, optical flow and demons, the maximum differences of the deformed positions for GTV tracking were approximately 4.55 to 7.55 times higher than the mean differences. Here, errors caused by the aforementioned difference in the HU values were also observed. As shown in Figure 7, when GTV was located at the diaphragm level, it was not clearly distinguished from adjacent normal tissues (ie, liver, stomach, bowel, and spleen), resulting in an error in GTV tracking. Consequently, even if the GTV position could be estimated by the DIR algorithms, the physician should carefully and manually check the position of the GTV in each phase.
Figure 7.

Sample case of DIR errors with similar Hounsfield unit (HU) values between the gross tumor volume (GTV) and nearby normal tissues. In this figure, slices of 4-dimensional computed tomography (4D CT) images for (a) T50 and (b) T0 show an indistinguishable GTV. Hence, DIR could not clearly define the GTV deformation in the (c) deformed T50; (d) shows the difference between (c) and (b) images. Contour lines in (a) and (b) represent the GTV region, and red and green lines in (c) represent the deformed GTV and GTV at T0, respectively.

Sample case of DIR errors with similar Hounsfield unit (HU) values between the gross tumor volume (GTV) and nearby normal tissues. In this figure, slices of 4-dimensional computed tomography (4D CT) images for (a) T50 and (b) T0 show an indistinguishable GTV. Hence, DIR could not clearly define the GTV deformation in the (c) deformed T50; (d) shows the difference between (c) and (b) images. Contour lines in (a) and (b) represent the GTV region, and red and green lines in (c) represent the deformed GTV and GTV at T0, respectively. The limitation of this study is that the DIR algorithms were evaluated only by using a limited number of patients’ 4D CT images (ie, 5 4D-CT datasets). Nevertheless, the trend of the deformed results of more than 20 FMs and GTVs by the DIR algorithms was virtually similar to those of the previous phantom-based study. Another limitation is that the DIR algorithm used in this study was not evaluated at different operational parameters. The parameters used in the detailed options of the DIR process were similar with those suggested by Yeo et al. Hence, the limitations due to the parameters may be the same as those in the previous literature. Properly establishing the best parameters can improve the performance of the algorithm. Other parameters might have a possibility to bring better results than our results.

Conclusions

In this study, we quantitatively evaluated 10 common DIR algorithms in real 4D CT images of patients. The results for 2 categories, namely, FM and GTV, were compared with the ground-truth positions. Based on our results, the optical flow algorithms yielded reasonable results for FMs and GTVs, and the iterative optical flow algorithm yielded the best performance. The mean and standard deviations of TREs were 1.82 ± 1.05 mm for the FM position and 1.29 ± 1.21 mm for the GTV position. The estimations all the GTV positions had some limitations. The demons algorithms exhibited large discrepancies between the deformed and fixed images with respect to FMs, and the other 2 algorithms (level-set motion and free-form deformation) had the worst results. Accordingly, we conclude that FM positions could be estimated using the best DIR algorithms, such as the iterative optical flow method, within the uncertainties of the CT resolution, with respect to the tumor position. However, the DIR algorithms could not be used to estimate several tumor positions tested in this study. Hence, deformed positions for a tumor might need to be manually checked by physicians. We expect that this limitation would be overcome in the near future with the use of advanced methods, such as AI-based techniques.
  47 in total

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5.  4D-CT motion estimation using deformable image registration and 5D respiratory motion modeling.

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Journal:  Med Phys       Date:  2013-10       Impact factor: 4.071

7.  The management of respiratory motion in radiation oncology report of AAPM Task Group 76.

Authors:  Paul J Keall; Gig S Mageras; James M Balter; Richard S Emery; Kenneth M Forster; Steve B Jiang; Jeffrey M Kapatoes; Daniel A Low; Martin J Murphy; Brad R Murray; Chester R Ramsey; Marcel B Van Herk; S Sastry Vedam; John W Wong; Ellen Yorke
Journal:  Med Phys       Date:  2006-10       Impact factor: 4.071

8.  Spherical demons: fast diffeomorphic landmark-free surface registration.

Authors:  B T Thomas Yeo; Mert R Sabuncu; Tom Vercauteren; Nicholas Ayache; Bruce Fischl; Polina Golland
Journal:  IEEE Trans Med Imaging       Date:  2009-08-25       Impact factor: 10.048

9.  Systematic errors in respiratory gating due to intrafraction deformations of the liver.

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Journal:  Med Phys       Date:  2007-09       Impact factor: 4.071

10.  Effect of Deformation Methods on the Accuracy of Deformable Image Registration From Kilovoltage CT to Tomotherapy Megavoltage CT.

Authors:  Wannapha Nobnop; Imjai Chitapanarux; Somsak Wanwilairat; Ekkasit Tharavichitkul; Vicharn Lorvidhaya; Patumrat Sripan
Journal:  Technol Cancer Res Treat       Date:  2019-01-01
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