Skip to main content
Journal of Radiation Research logoLink to Journal of Radiation Research
. 2020 Dec 21;62(2):309–318. doi: 10.1093/jrr/rraa123

Dosimetric comparison between volumetric modulated arc therapy planning techniques for prostate cancer in the presence of intrafractional organ deformation

Maria Varnava 1,, Iori Sumida 2, Michio Oda 3, Keita Kurosu 4, Fumiaki Isohashi 5, Yuji Seo 6, Keisuke Otani 7, Kazuhiko Ogawa 8
PMCID: PMC7948894  PMID: 33341880

Abstract

The purpose of this study was to compare single-arc (SA) and double-arc (DA) treatment plans, which are planning techniques often used in prostate cancer volumetric modulated arc therapy (VMAT), in the presence of intrafractional deformation (ID) to determine which technique is superior in terms of target dose coverage and sparing of the organs at risk (OARs). SA and DA plans were created for 27 patients with localized prostate cancer. ID was introduced to the clinical target volume (CTV), rectum and bladder to obtain blurred dose distributions using an in-house software. ID was based on the motion probability function of each structure voxel and the intrafractional motion of the respective organs. From the resultant blurred dose distributions of SA and DA plans, various parameters, including the tumor control probability, normal tissue complication probability, homogeneity index, conformity index, modulation complexity score for VMAT, dose–volume indices and monitor units (MUs), were evaluated to compare the two techniques. Statistical analysis showed that most CTV and rectum parameters were significantly larger for SA plans than for DA plans (P < 0.05). Furthermore, SA plans had fewer MUs and were less complex (P < 0.05). The significant differences observed had no clinical significance, indicating that both plans are comparable in terms of target and OAR dosimetry when ID is considered. The use of SA plans is recommended for prostate cancer VMAT because they can be delivered in shorter treatment times than DA plans, and therefore benefit the patients.

Keywords: blurred dose distribution, dose–volume histogram, intrafractional organ deformation, prostate cancer, treatment planning, volumetric modulated arc therapy

INTRODUCTION

One of the common techniques for treating prostate cancer is volumetric modulated arc therapy (VMAT). As compared with 3D conformal radiation therapy, VMAT can deliver a highly conformal dose to the target, while minimizing the dose delivered to the organs at risk (OARs) [1, 2]. Furthermore, it can produce equivalent or even better target dose coverage and normal tissue sparing than intensity-modulated radiation therapy (IMRT) [3, 4], while taking advantage of more efficient monitor units (MUs) and reduced treatment time [3–5].

The VMAT technique uses modulated photon beams by simultaneous adjustment of the dose rate, gantry rotation speed and shape of the multileaf collimator aperture [1, 4, 5]. Treatment modalities that modulate fluence, like VMAT, are more prone to dosimetric errors due to patient setup errors and internal organ motion [6–8]. Such errors can have a significant impact on the dose absorbed by the target or the OARs, possibly yielding insufficient irradiation of the target or excess irradiation of the normal tissues due to reduced geometric and dosimetric accuracies. The expected absorbed dose can be calculated from the treatment planning system (TPS), and the resulting dose distributions are used to evaluate the deliverability of the plans. However, the evaluation is based on a single dose distribution, which shows the dose a patient would receive if that patient’s setup and anatomy were the same throughout treatment as those during the planning computed tomography (CT) imaging. Therefore, after the completion of treatment, the real dose distributions may deviate from the expected dose distributions [9].

Errors in the patient setup or interfractional organ motion can be reduced prior to a treatment session using image guidance [7, 10–12]. Various studies have tried to improve target localization accuracy and to account for interfractional setup errors and organ motion [12, 13]. Intrafractional organ deformation is more complex; it can be thought of as the combination of the motion of organ voxels in any direction. Thus, it is more difficult to correct the associated errors with intrafractional deformation (ID) during a treatment session. Real-time monitoring, tracking and adaptation are necessary to correct such errors. Previous studies have examined intrafractional organ motion during prostate cancer radiotherapy by using 4D ultrasound [14] and by investigating the displacement of fiducial markers implanted in the prostate before and after a treatment session using an on-board kilovoltage imaging system (OBI; Varian Medical Systems, Palo Alto, CA, USA) [15]. Other studies have focused on evaluating intrafractional organ motion using cine magnetic resonance imaging (cine-MRI) [16–18] and the Calypso 4D localization system (Calypso Medical Technologies, Seattle, WA, USA) [19, 20] with electromagnetic markers implanted in the target tissue.

One method to account for ID would be to create a model for organ deformation and to incorporate it into the calculation of dose distributions so as to get a more accurate representation of the real distributions. Pommer et al. [21] created a random walk model for simulating the characteristics of the observed intrafractional motion of the prostate when considering only motion from treatment fractions without transient excursions during the first 5 min. Another study calculated blurred dose (Dblurred) distributions of the prostate clinical target volume (CTV), rectum and bladder in IMRT [22] by simulating ID using displacements of these structures, the concepts of a static dose (Dstat) cloud approximation [23] and a probability density function (PDF) [24].

ID should be considered in radiation therapy, especially for VMAT. Any organ changes could degrade the accuracy of the plan because of the high dose conformality and steep dose gradients of VMAT, resulting in non-optimal plans with insufficient target irradiation and increased complications of the OARs. When creating treatment plans, VMAT offers the option of delivering dose to the target in either a single arc (SA) or multiple arcs. For prostate cancer, SA or double-arc (DA) plans are usually generated. There have been various studies comparing plans for prostate cancer created using either an SA or a DA plan [1–3, 5, 25–27], but none of them considered ID. These studies focused on the dosimetric comparison between SA and DA plans based on the dose distributions generated from the TPS. Non-consideration of ID makes unclear which one of these two options would lead to a more accurate delivery of the treatment. Therefore, the aim of this study was to compare SA and DA treatment plans for prostate cancer after the incorporation of ID and determine whether SA or DA plans are superior in terms of target dose coverage and sparing of the OARs.

MATERIALS AND METHODS

CT simulation and contouring

This study was approved by our Institutional Review Board (Osaka University Ethics Committee, approval number 18129) and written consent was obtained from all patients. Data from 27 patients, who were treated for localized prostate cancer using VMAT between June 2017 and March 2018, were retrospectively analyzed. The mean age [standard deviation (SD)] of the patients at the start of the treatment was 71 (7) years.

Before treatment, planning CT images were acquired using either a 16-slice multi-detector row CT (Bright Speed Elite; GE Healthcare, Waukesha, WI, USA) or a 320-slice multi-detector row CT (Aquilion ONE™; Canon Medical Systems, Otawara, Tochigi, Japan). The CT images were acquired with a slice thickness of 2.5 or 2 mm and with patients in a supine position on a vacuum-formed cushion (Vac-Lok™ cushion; CIVCO Medical Solutions, Kalona, IA, USA).

The CTV, rectum and bladder were delineated on the CT images on the Eclipse TPS (version 13.7.29, Varian Medical Systems, Palo Alto, CA, USA). The CTV was defined as the sum of the prostate and the proximal seminal vesicles, plus 3 or 1 mm in the posterior direction in order to avoid the rectum. The rectum and bladder were delineated by a medical physicist with 5 years of experience, and the CTV was delineated by a radiation oncologist with 8 years of experience.

Treatment planning and optimization

Two sets of VMAT treatment plans, SA and DA plans, were created for each patient using the arc parameters shown in Table 1. A dosage of 78 Gy was applied in 39 fractions to cover 50% of the planning target volume (PTV), which was defined as the CTV plus 5 mm. The treatment plans were inversely optimized. The optimization parameters were kept constant between the SA and DA plans of each patient and were based on the dosimetric planning goals (Table 2). In this study, the optimization parameters used for each plan were the same as the ones used to optimize the plan of the actual treatment of the patient. After optimization, all plans were calculated using the Acuros XB algorithm (version 13.7.14, Varian Medical Systems, Palo Alto, CA, USA) in the Eclipse TPS with a calculation grid size of 1 mm. Optimization was performed separately for each plan. SA and DA plans were optimized only once, and no alterations of the weightings of the optimization parameters were made so as to make fair comparisons between SA and DA plans possible.

Table 1.

Arc parameters used for creating SA and DA plans

Parameter SA plan DA plan (first arc/second arc)
Arc direction Anticlockwise Anticlockwise/clockwise
Gantry angle (start–stop) 179–181° 179–181°/181–179°
Collimator angle 5–30° 330–350°

Table 2.

Dosimetric planning goals used for designing treatment plans

Structure Planning goal
CTV D 95% ≥ 74.1 Gy
Rectum V 40Gy < 35%, V65Gy < 17%
Bladder V 40Gy < 50%, V65Gy < 25%

D xx% = dose incident on xx% structure volume, VxxGy = %volume of structure receiving a dose of xx Gy.

Intrafractional organ deformation

The incorporation of organ deformation into the calculation of dose distributions and the estimation of Dblurred distributions were performed by following the procedure described in Sumida et al. [22]. Dblurred distributions refer to the resulting dose distributions after the completion of treatment. We assumed that the patient setup error was already accounted for by image guidance in each treatment session, so we considered only ID over the treatment course. The DICOM RT files including the treatment plan, structure set and dose were exported from the Eclipse TPS and were imported into an in-house software developed using Delphi2007 (Borland Software Corporation, Austin, TX, USA) to introduce ID to the structures of interest (CTV, rectum and bladder). The dose distribution at this point is referred to as the Dstat distribution because it is the distribution before considering ID, i.e. the dose distribution as calculated from the TPS. The software can create a probability dose distribution to each voxel of each structure based on a motion PDF. It was assumed that the motion PDF has three components, including axes of motion in the left–right (LR), anterior–posterior (AP) and superior–inferior (SI) directions, and that the motion probability was based on random organ deformations. The real motion distribution of the organs is unknown and can be affected by various factors, including respiration. However, according to the central limit theorem, even a non-uniform distribution will converge towards a Gaussian shape after a great number of fractions. Previous studies investigated the motion of the diaphragm under the influence of respiration [28, 29]. George et al. reported that the motion of the diaphragm tends to have a normal distribution when considering the respiration effect over multiple fractions for a single patient or when considering multiple fractions for all patients combined [28]. Rit et al. observed that the variability of the respiratory cycle over 2 min, which is similar to the treatment time of DA plans, is close to a skew normal distribution. Organs that have fewer mobile points than the diaphragm are expected to exhibit less asymmetry because the random baseline variations will dominate the probability density function [29]. Therefore, we assumed that the random deformations of the prostate, rectum and bladder over all 39 treatment fractions follow a normal distribution. Even though the prostate is known to move spontaneously [18, 30], by observing the overall dosimetric effect of ID through the whole treatment course of VMAT, spontaneous prostate movements will have a small dosimetric effect and can thus be neglected. Our proposed method, though, is not suitable for stereotactic or hypofractionated treatments, in which case the dosimetric effect of such prostate movements is great.

Amplitudes of the motion for the prostate, rectum and bladder during treatment in the LR, AP and SI directions have been reported in previous studies [31–33]. Two SDs of the reported motion of each organ were assumed to be the magnitude of ID and were used as inputs in our software to introduce ID to the CTV, rectum and bladder (Table 3).

Table 3.

ID magnitudes for the structures in each direction

Structure ID magnitude (2 SDs, mm) Study reference
LR direction AP direction SI direction
CTV 6 8 6 [31]
Rectum 6 10 0 [32]
Bladder 5 8 6 [33]

In order to consider ID, the number of times each organ (prostate, rectum and bladder) moves in a specific amount of time was necessary. From the results of a previous study, it was determined that the prostate position varied about 76 times in 4 min [16]. Furthermore, SA and DA plans usually have treatment times of 1 and 2 min, respectively. By taking these observations into account, we estimated that the prostate will move about 750 and 1500 times during the whole treatment course (39 fractions) of SA and DA plans, respectively. Since there have been no previous studies reporting data about the number of variations of the rectum and bladder positions in a specific period of time, we assumed that both OARs have the same number of variations as the prostate. Therefore, to calculate the Dblurred distributions for the CTV, rectum and bladder in the presence of ID, motion was introduced independently to each structure voxel. This was achieved by altering the location of the dose grid of each structure in the original dose cloud distribution, which was kept static, to fulfill the normal distribution criterion, as follows [22]:

graphic file with name M1.gif (1)

where Dblurred(x,y,z) is the mean value of the blurred dose at location (x,y,z), with x, y and z corresponding to the LR, AP and SI directions, respectively. The location (x,y,z) is the same as the DICOM RT dose grid. The parameters Inline graphic, Inline graphic and Inline graphic are the probable ith location shifts in the LR, AP and SI directions (Table 3), respectively, with the locations randomly changed N = 750 times for SA plans and N = 1500 times for DA plans, based on the normal distribution. Figure 1 shows an example of the dose distribution before (Dstat) and after introducing ID (Dblurred) to the CTV in an SA plan.

Fig. 1.

Fig. 1.

Dose distributions of an SA plan. (a) The dose distributions as obtained from the TPS before introducing ID. (b) The Dblurred distributions after introducing ID to the CTV. (c) The subtraction image derived from (b) − (a).

Radiobiological evaluation

In order to compare SA and DA plans, various parameters were evaluated, including the generalized equivalent uniform dose (gEUD), tumor control probability (TCP), normal tissue complication probability (NTCP) and modulation complexity score for VMAT (MCSv).

The gEUD was calculated for each structure according to the Niemierko’s phenomenological equation given by [34, 35]:

graphic file with name M5.gif (2)

where N is the number of voxels of each structure, each voxel receiving dose Di in Gy, and a is a parameter specific to the tumor or normal tissue that describes the dose–volume effect. The TCP was calculated using the Niemierko EUD-based model given by the following equation [34, 36]:

graphic file with name M6.gif (3)

where TCD50 is the dose needed to control 50% of the tumor when the tumor is homogeneously irradiated, and γ50 is a unitless parameter that is specific to the tumor and describes the slope of the dose–response curve. The individual voxel NTCP (P) was calculated using the relative seriality model [37], as follows:

graphic file with name M7.gif (4)

where D50 refers to the tolerance dose that would produce a 50% complication rate at a specific time interval (e.g. 5 years) [38]. By considering the functional architecture of the organs, the NTCP was evaluated using the following equation [37]:

graphic file with name M8.gif (5)

where n is the number of sub-volumes in the organ, and s is the relative seriality parameter, which ranges between 0 for parallel organs and 1 for serial organs. The parameter Δvi is defined as vi/V, where vi is the sub-volume in the differential dose–volume histogram (DVH) and V is the total volume of the organ. Table 4 shows the radiobiological parameters used for evaluating the gEUD, TCP and NTCP of the structures of interest.

Table 4.

Radiobiological parameters used to calculate the gEUD, TCP and NTCP

Structure a TCD50/D50 (Gy) γ50 s Clinical endpoint Study reference
CTV −13 67.5 2.2 - Local control [39, 40]
Rectum 8.33 83.1 1.69 0.49 Grade 2 rectal bleeding [39, 41]
Bladder 2 80 3 0.18 Symptomatic contracture [39, 42]

The MCSv is a parameter that evaluates the complexity of VMAT plans. It was calculated based on the method described by Masi et al. [43], who modified the modulation complexity score for step-and-shoot IMRT proposed by McNiven et al. [44] to make it applicable for VMAT. The MCSv can take values in the range 0–1, with 1 showing no modulation, and thus no complexity. For example, a plan with MCSv = 1 would correspond to an arc with a fixed rectangular aperture with no leaves moving during the arc motion. VMAT plans with increased modulation have decreased MCSv.

Besides the parameters described above, dose–volume indices, the CTV homogeneity index (HI), the CTV conformity index (CI) and MUs were also used for comparing SA and DA plans.

The HI and CI were evaluated based on the definitions given by the International Commission on Radiation Units and Measurements (ICRU) Report 83 [45] and ICRU Report 62 [46], respectively:

graphic file with name M9.gif (6)
graphic file with name M10.gif (7)

The D2%, D98% and D50% indices represent the doses received by 2, 98 and 50% of the CTV, respectively. VTV refers to the treated volume, which is the volume enclosed by the 95% isodose lines, while Vtarget refers to the volume of the target. Based on ICRU Report 62, Vtarget corresponds to the PTV. However, for comparing SA and DA plans, we considered only the CTV and not the PTV. Therefore, in our study, Vtarget corresponds to the CTV, while VTV corresponds to the volume covered by at least 74.1 Gy since the prescription dose was 78 Gy.

Statistical analysis

Statistical analyses were performed using R software (version 3.5.0, Foundation for Statistical Computing, Vienna, Austria). The Shapiro–Wilk test was used to test the normality of the data. To investigate for differences between SA and DA plans, the two-tailed paired t-test or the Wilcoxon signed-rank test was used as appropriate. These tests were also used to investigate the effect ID has on SA and DA plans. A P-value of < 0.05 was considered statistically significant.

RESULTS

Table 5 shows the results after comparing the MUs and MCSv between SA and DA plans. Significant differences were found in both the MUs and MCSv. SA plans had fewer MUs than DA plans, whereas SA plans had larger MCSv, indicating less complexity and modulation than DA plans.

Table 5.

Comparison of MUs and MCSv between SA and DA plans; data are presented as mean ± SD

Parameter SA plans DA plans P-value
MUs 550 ± 53 574 ± 52 <0.001*
MCSv 0.19 ± 0.03 0.18 ± 0.03 <0.001*

* P-values that indicate statistically significant differences.

The plan parameters of SA and DA plans before and after introducing ID, i.e. the plan parameters of the Dstat and Dblurred distributions, are summarized in Supplementary Table S1, see online supplementary material. Statistical analysis of the dose–volume indices and radiobiological parameters of the structures of interest showed that most indices and parameters had statistically significant differences between the Dstat and Dblurred distributions of SA and DA plans (Supplementary Table S1). For both plans, the plan parameters of the Dstat distribution were larger overall than those of the Dblurred distribution. On the other hand, comparisons of the Dblurred distributions of the structures of interest between SA and DA plans revealed that there were no significant differences found in any dose–volume indices and radiobiological parameters for the bladder, while most parameters exhibited significant differences for the CTV and rectum. All CTV indices and parameters except the CTV D98% and CTV CI had significantly larger values for SA plans than for DA plans. Similarly, all rectum indices and parameters except V40Gy also had significantly larger values for SA plans. For the Dstat distributions, there were significant differences between SA and DA plans in the rectum V65Gy, rectum NTCP and all CTV parameters. Out of all the plan parameters, the rectum D2% had the largest significant difference between the Dstat and Dblurred distributions in both SA and DA plans. The rectum D2% also had the largest significant difference in the Dblurred distribution between SA and DA plans, while the rectum V65Gy had the largest significant difference in the Dstat distribution. Figure 2 shows a graphical representation of this result.

Fig. 2.

Fig. 2.

Boxplots of the plan parameters that had the largest significant difference (a) between the Dstat and Dblurred distributions of SA plans (rectum D2%), (b) between the Dstat and Dblurred distributions of DA plans (rectum D2%), (c) in the Dstat distribution between SA and DA plans (rectum V65Gy), and (d) in the Dblurred distribution between SA and DA plans (rectum D2%) Dxx% = dose incident on xx% structure volume, VxxGy = %volume of structure receiving a dose of xx Gy.

DISCUSSION

This paper aimed to incorporate ID into the calculation of dose distributions and compare SA and DA plans based on the target dose coverage and sparing of the OARs. Significant differences between SA and DA plans were found in almost all the CTV and rectum parameters after ID introduction. From these results, we deduced that SA plans provide better CTV dosimetry and conformity, whereas DA plans provide better rectal dosimetry and CTV homogeneity.

Previous studies have investigated the differences between SA and DA plans for prostate cancer. Similar to our study, some studies detected better rectal dosimetry for DA plans than for SA plans [5, 25, 27]. On the other hand, Sale and Moloney [1] and Wolff et al. [2] found no significant differences in the rectal dosimetry between SA and DA plans, while Kang et al. [3] found no significant differences in the rectum NTCP. Furthermore, a different study reported an increased rectum dose–volume index (V70Gy) in DA plans [26].

With regard to the target, Sze et al. [5], Chow and Jiang [25] and Guckenberger et al. [26] showed that DA plans have better target homogeneity, which agrees with our results, and better target dose conformity and coverage, while Wolff et al. [2] showed no significant differences in the target dosimetry. Moreover, one study reported no significant differences for the TCP [3].

In our study, no statistically significant differences were observed in any bladder parameters. This result is consistent with previous reports that found no significant differences in bladder dose–volume indices and NTCP between SA and DA plans [1, 3, 5]. Other studies, though, found better bladder dosimetry for DA plans [25–27].

Inconsistencies between our findings with previously published research can be mainly attributed to the consideration of ID in our study. Statistically significant dosimetric differences were observed between the plans in our study before and after the incorporation of ID (P < 0.05). Different planning designs, such as planning goals, planning strategies, arc parameters, optimization parameters, target definitions and PTV margins, may also affect the dosimetric results and constitute a reason for the inconsistencies.

Despite the inconsistencies between studies, we found that our significant differences were in general smaller in magnitude than those in the above-mentioned studies. This could be explained from the dose blurring and interplay effect caused by ID [47]. Dose blurring effect is the reduction of the dose delivered to a point in a structure due to the motion of this point. Interplay effect is the dosimetric effect caused by the relative motion of the structures between the leaves and the treatment region. Both the dose blurring and interplay effects yield a non-uniform dose distribution delivered to the moving structures. By considering the mean dose delivered across all fractions, as in our study, the dosimetric differences caused by these two effects become smaller [47] compared with when ID is not considered. This is also the reason most of the plan parameters of the Dstat distributions were larger than those of the Dblurred distributions in both SA and DA plans.

Our results show that the significant differences found in the Dblurred distributions between SA and DA plans were very small, with the largest difference being <0.6 Gy for the rectum D2% (Supplementary Table S1). A previous study found a statistically significant difference in the mean dose of the small bowel between IMRT and VMAT DA plans for prostate cancer [27]. This difference was 1.4 Gy, which is larger than our 0.6 Gy difference, and the indices between the two plans were considered comparable. Furthermore, our CTV D2%, the index with the largest significant difference among the CTV indices, had a difference of 0.2 Gy, with the D2% of SA plans being 0.2% higher than that of DA plans. Dose differences should be interpreted in the context of the total uncertainty in radiation therapy that is clinically accepted. The International Commission on Radiation Protection [48] has reported an estimated standard uncertainty of 5% in a clinical setup when considering the uncertainty in the complete workflow (uncertainty in beam calibration, relative dosimetry, dose calculations and dose delivery). Our CTV D2% difference of 0.2% only makes up for a small fraction of the total uncertainty. Additionally, the bladder NTCP had no significant differences between SA and DA plans, while the significant differences for the TCP and rectum NTCP were <0.1%. Kang et al. [3] reported a 0.2% difference in the rectum NTCP results in radiobiological outcomes that have no difference between the various VMAT plans investigated. Our TCP and rectum NTCP differences were much smaller than 0.2%, meaning that both SA and DA plans result in similar tumor control and OAR complications. In addition, the significant differences observed in the MCSv had a magnitude of 0.01, indicating that even though SA and DA plans have statistically different complexities, their complexities are similar. Therefore, we deduced that SA and DA plans are comparable in terms of target dose coverage, sparing of the OARs and plan complexity.

For the Dstat distributions, significant differences were found in all CTV parameters, the rectum V65% and rectum NTCP between SA and DA plans. Almost all indices had significantly larger values for SA plans than for DA plans. This implies that the Dstat SA plans have better CTV dosimetry than the Dstat DA plans, while Dstat DA plans have better rectal dosimetry [5, 25, 27]. These are consistent with the findings of the Dblurred distributions. Furthermore, the Dstat SA and Dstat DA plans are comparable in terms of the bladder dosimetry, which agrees with previous studies [1, 3, 5]. It can be deduced that Dstat SA and DA plans exhibit the same trend as Dblurred plans.

The rectum V40Gy was the only dose–volume index that increased after applying ID. As can be seen in Fig. 3a, the low-dose isodose lines (≤40 Gy) have steep gradients around the rectum. The rectum moves in the LR and AP direction (Table 3). The shape of the low-dose isodose lines and the shift of the rectal wall causes an excess of the planned dose in the rectal posterior region after the completion of treatment (Fig. 3b), which results in the observed increase in the rectum V40Gy. The remaining dose–volume indices decreased after the introduction of ID probably due to the dose blurring and interplay effects that were previously discussed.

Fig. 3.

Fig. 3.

Effect of ID on the low doses delivered to the rectum (≤40 Gy). (a) Dstat distributions of an SA plan as obtained from the TPS. The bold light-green line represents the 40-Gy isodose line. (b) Dose differences between the Dblurred distributions after introducing ID to the rectum and the Dstat distributions in (a).

Analysis of our data revealed the importance of considering ID during plan quality evaluation. In general, when a dose–volume constraint was met before ID introduction, the constraint was also met after ID introduction since the values of the dose–volume indices decreased. This was not the case for the rectum V40Gy constraint, which was met in 20 Dstat SA and 20 Dstat DA plans, whereas it was met in 14 Dblurred SA plans and 13 Dblurred DA plans. This indicates that the unfulfilled rectum V40Gy constraint would have remained undetected in 6 SA and 7 DA plans without ID consideration. Relying only on the dose distributions created by the TPS may lead to the wrong conclusions about the real dose distributions, and result in accepting treatment plans that do not fulfil all the dose–volume constraints, without being aware of it. Introducing ID to the plans leads to more realistic dose distributions. Therefore, considering ID during plan quality evaluation is important so as to confirm that all dose–volume constraints are met and avoid any unnecessary complications. Furthermore, the fact that the V40Gy constraint was met in a different number of SA and DA plans in both Dstat and Dblurred distributions shows that even though the differences between SA and DA plans are small, they could lead to different fulfilled dose–volume constraints, which would not always be apparent without ID consideration.

In our study, the same dose–volume constraints were used for creating SA and DA plans for each patient. It could be argued that using the same constraints would lead to similar plans. In a previous study, three institutions created IMRT plans for a prostate cancer patient using the same contours [49]. Each institution used different optimization parameters and constraints to create the best possible IMRT plan. Even though the plan parameters were different, the resulting plans were similar with respect to dose–volume constraints, with greater variations in the DVHs of the OARs. This implies that plans created for the same patient will be similar regardless of the constraints used when aiming for a good quality plan. Tang et al. reported that transforming multiple-arc plans to SA plans in intensity-modulated arc therapy for five different sites resulted in similar plans [50]. Also, a different study created IMRT plans for head-and-neck cancer using 3, 5, 7 and 9 beams [51]. The constraints and weight factors were modified during optimization to control the progress of the DVH curves. Increasing the number of beams led to improved dosimetric results, while the plans created using 7 and 9 beams had similar dose distributions. It can be deduced that plans with multiple beams will yield similar dose distributions for the same patient regardless of the choice of dose–volume constraints. This is consistent with our results that SA and DA plans are similar, as these plans can be described as plans with multiple beams.

During the radiobiological evaluation of the plans, dose-rate effects were not considered. It has been reported that considerable differences are apparent for dose rates in the range 0.1–100 cGy/min; some cell systems exhibit more cell sub-lethal damage for lower dose-rates, while other cell systems exhibit more damage repair [52]. However, there is no effect on cells for dose-rates in the range 100–1000 cGy/min [52]. A previous study that investigated the radiobiological effects of total body irradiation on the spinal cord showed that for dose rates >50 cGy/min the effect is negligible for various fractionation schemes [53]. Another study reviewed the dose-rate effect on external beam radiation therapy and reported that for treatments using a dose of 1.8–2 Gy per fraction, the effect of dose rate is relatively small and is mainly influenced by the overall beam-on-time and not by the average linac dose rate nor by the instantaneous dose rate within the individual linac pulses [54]. On the other hand, Bewes et al. showed that besides treatment time, average dose rate also has different effects on the clonogenic cell survival: shorter treatment times and higher dose rates led to reduced cell survival [55]. In this study, the dose rates in the SA and DA plans had minimum/maximum values (mean ± SD) of 425 ± 60/600 ± 0 and 222 ± 26/440 ± 103 MU/min, respectively. By taking into consideration the findings of previous research, it can be deduced that SA plans may possibly have better therapeutic gain than DA plans. The difference in therapeutic effect, though, would be relatively small.

The results of the current study lead to the same conclusion as published research: both SA and DA plans are similar and acceptable options for prostate cancer VMAT [1–3, 5, 25]. SA plans, which have shorter treatment times than DA plans, may be preferred [5], unless the dose–volume criteria are difficult to achieve [1, 25]. Previous studies, though, have only focused on the dose distributions as obtained from the TPS, whereas we introduced ID to the plans in order to obtain more accurate representations of the dose distributions. The fact that the conclusions of our study agree with the conclusions of previous studies strengthens the consensus that SA and DA plans are similar.

A limitation of this study is the fact that residual errors were not considered. After image guidance, residual geometric setup errors remain due to inaccuracies of the imaging system, the repositioning system and the intrafractional motion of the prostate [56]. The system-related setup errors have been reported to be <2 mm [56]. In this study, we focused only on organ deformation. A future study could also incorporate system-related residual errors so as to obtain an even more realistic representation of the dose distributions. Another limitation is the assumption that the magnitude of organ motion is the same as the magnitude of intrafractional organ deformation. During the actual treatment, this might not always be true, as movement of the voxels of an organ could lead to movement of the organ as a whole and not in deformation of the organ. Moreover, it was assumed that, in each direction, all voxels of an organ have the same motion magnitude. A previous study showed that the prostate has different motion magnitudes for different parts of the prostate in a specific direction [57]. From this, it can be deduced that the magnitude of the prostate deformation in one direction is not the same for all prostate voxels. The same thing most likely applies to all organs. Various studies used cine-MRI to investigate intrafractional organ motion for the prostate, bladder and seminal vesicles in terms of time [16–18, 28, 57, 58]. Most of these studies identified dosimetric uncertainties arising from intrafractional organ motion and suggested the consideration of suitable strategies to account for the dosimetric uncertainties, such as control of the rectum and bladder filling [17, 57], the use of a rectal balloon [16] and the use of appropriate intrafractional organ margins [30, 58]. By following a similar method to these studies and their proposed strategies for controlling the rectum and bladder filling, it could be possible to determine ID for the organs (or structures) of interest for each patient during a treatment session and limit any volume variations in the OARs, which could degrade the performance of our model as volume variations were not considered during ID simulation. By using this ID, more accurate dose distributions could be estimated, and the dosimetric effect on SA and DA plans could be reassessed to confirm the reliability of our results. In addition, recent studies have attempted to monitor intrafractional organ motion and deformation using MRI-guided radiation therapy setups [59–61]. Similar to cine-MRI, such setups would enable determination of the ID of the target and OARs in various cancer sites. Based on the way the shape of an organ varies over time, a future study could investigate which arc angles in prostate cancer VMAT are least affected by ID, resulting in treatment plans that are not susceptible to ID and therefore are more accurate than SA and DA plans.

In conclusion, the evidence from this study points towards the idea that ID incorporation into the calculation of dose distributions is important for ensuring that all dosimetric planning goals are met. Moreover, our results indicate that SA and DA treatment plans for prostate cancer are comparable in terms of target and OAR dosimetry when ID is considered. SA plans, though, can be delivered in shorter treatment times than DA plans, leading to less patient discomfort and possibly better therapeutic gain. Thus, the use of SA plans, in combination with ID consideration during plan quality evaluation, is recommended so as to benefit patients.

Supplementary Material

Revised_Supplementary_Table_1_Clean_Copy_rraa123

Contributor Information

Maria Varnava, Department of Radiation Oncology, Osaka University Graduate School of Medicine, 2-2 (D10) Yamadaoka, Suita, Osaka, 565-0871, Japan.

Iori Sumida, Department of Radiation Oncology, Osaka University Graduate School of Medicine, 2-2 (D10) Yamadaoka, Suita, Osaka, 565-0871, Japan.

Michio Oda, Department of Medical Technology, Osaka University Hospital, 2-15 Yamadaoka, Suita, Osaka, 565-0871, Japan.

Keita Kurosu, Department of Medical Technology, Osaka University Hospital, 2-15 Yamadaoka, Suita, Osaka, 565-0871, Japan.

Fumiaki Isohashi, Department of Radiation Oncology, Osaka University Graduate School of Medicine, 2-2 (D10) Yamadaoka, Suita, Osaka, 565-0871, Japan.

Yuji Seo, Department of Radiation Oncology, Osaka University Graduate School of Medicine, 2-2 (D10) Yamadaoka, Suita, Osaka, 565-0871, Japan.

Keisuke Otani, Department of Radiation Oncology, Osaka University Graduate School of Medicine, 2-2 (D10) Yamadaoka, Suita, Osaka, 565-0871, Japan.

Kazuhiko Ogawa, Department of Radiation Oncology, Osaka University Graduate School of Medicine, 2-2 (D10) Yamadaoka, Suita, Osaka, 565-0871, Japan.

CONFLICT OF INTEREST

None declared.

References

  • 1. Sale  C, Moloney  P. Dose comparisons for conformal, IMRT and VMAT prostate plans. J Med Imaging Radiat Oncol  2011;55:611–21. [DOI] [PubMed] [Google Scholar]
  • 2. Wolff  D, Stieler  F, Welzel  G  et al.  Volumetric modulated arc therapy (VMAT) vs. serial tomotherapy, step-and-shoot IMRT and 3D-conformal RT for treatment of prostate cancer. Radiother Oncol  2009;93:226–33. [DOI] [PubMed] [Google Scholar]
  • 3. Kang  SW, Chung  JB, Kim  JS  et al.  Optimal planning strategy among various arc arrangements for prostate stereotactic body radiotherapy with volumetric modulated arc therapy technique. Radiol Oncol  2017;51:112–20. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 4. Otto  K. Volumetric modulated arc therapy: IMRT in a single gantry arc. Med Phys  2008;35:310–7. [DOI] [PubMed] [Google Scholar]
  • 5. Sze  HC, Lee  MC, Hung  WM  et al.  RapidArc radiotherapy planning for prostate cancer: Single-arc and double-arc techniques vs. intensity-modulated radiotherapy. Med Dosim  2012;37:87–91. [DOI] [PubMed] [Google Scholar]
  • 6. Azcona  JD, Xing  L, Chen  X  et al.  Assessing the dosimetric impact of real-time prostate motion during volumetric modulated arc therapy. Int J Radiat Oncol Biol Phys  2014;88:1167–74. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 7. Palombarini  M, Mengoli  S, Fantazzini  P  et al.  Analysis of inter-fraction setup errors and organ motion by daily kilovoltage cone beam computed tomography in intensity modulated radiotherapy of prostate cancer. Radiat Oncol  2012;7:56. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 8. Trofimov  A, Rietzel  E, Lu  HM  et al.  Temporo-spatial IMRT optimization: Concepts, implementation and initial results. Phys Med Biol  2005;50:2779–98. [DOI] [PubMed] [Google Scholar]
  • 9. Langen  KM, Jones  DT. Organ motion and its management. Int J Radiat Oncol Biol Phys  2001;50:265–78. [DOI] [PubMed] [Google Scholar]
  • 10. Mc Parland  NA. kV-cone beam CT as an IGRT tool in the treatment of early stage prostate cancer: A literature review. J Med Imaging Radiat Sci  2009;40:9–14. [DOI] [PubMed] [Google Scholar]
  • 11. McBain  CA, Henry  AM, Sykes  J  et al.  X-ray volumetric imaging in image-guided radiotherapy: The new standard in on-treatment imaging. Int J Radiat Oncol Biol Phys  2006;64:625–34. [DOI] [PubMed] [Google Scholar]
  • 12. Willoughby  TR, Kupelian  PA, Pouliot  J  et al.  Target localization and real-time tracking using the calypso 4D localization system in patients with localized prostate cancer. Int J Radiat Oncol Biol Phys  2006;65:528–34. [DOI] [PubMed] [Google Scholar]
  • 13. Boda-Heggemann  J, Köhler  FM, Küpper  B  et al.  Accuracy of ultrasound-based (BAT) prostate-repositioning: A three-dimensional on-line fiducial-based assessment with cone-beam computed tomography. Int J Radiat Oncol Biol Phys  2008;70:1247–55. [DOI] [PubMed] [Google Scholar]
  • 14. Baker  M, Behrens  CF. Determining intrafractional prostate motion using four dimensional ultrasound system. BMC Cancer  2016;16:484. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 15. Kron  T, Thomas  J, Fox  C  et al.  Intra-fraction prostate displacement in radiotherapy estimated from pre- and post-treatment imaging of patients with implanted fiducial markers. Radiother Oncol  2010;95:191–7. [DOI] [PubMed] [Google Scholar]
  • 16. Vargas  C, Saito  AI, Hsi  WC  et al.  Cine-magnetic resonance imaging assessment of intrafraction motion for prostate cancer patients supine or prone with and without a rectal balloon. Am J Clin Oncol  2010;33:11–6. [DOI] [PubMed] [Google Scholar]
  • 17. McBain  CA, Khoo  VS, Buckley  DL  et al.  Assessment of bladder motion for clinical radiotherapy practice using cine-magnetic resonance imaging. Int J Radiat Oncol Biol Phys  2009;75:664–71. [DOI] [PubMed] [Google Scholar]
  • 18. Mah  D, Freedman  G, Milestone  B  et al.  Measurement of intrafractional prostate motion using magnetic resonance imaging. Int J Radiat Oncol Biol Phys  2002;54:568–75. [DOI] [PubMed] [Google Scholar]
  • 19. Tong  X, Chen  X, Li  J  et al.  Intrafractional prostate motion during external beam radiotherapy monitored by a real-time target localization system. J Appl Clin Med Phys  2015;16:51–61. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 20. Langen  KM, Willoughby  TR, Meeks  SL  et al.  Observations on real-time prostate gland motion using electromagnetic tracking. Int J Radiat Oncol Biol Phys  2008;71:1084–90. [DOI] [PubMed] [Google Scholar]
  • 21. Pommer  T, Oh  JH, Munck Af Rosenschöld  P  et al.  Simulating intrafraction prostate motion with a random walk model. Adv Radiat Oncol  2017;2:429–36. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 22. Sumida  I, Yamaguchi  H, Das  IJ  et al.  Robust plan optimization using edge-enhanced intensity for intrafraction organ deformation in prostate intensity-modulated radiation therapy. PLoS One  2017;12:e0173643. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 23. Craig  T, Battista  J, Van Dyk  J. Limitations of a convolution method for modeling geometric uncertainties in radiation therapy. I. the effect of shift invariance. Med Phys  2003;30:2001–11. [DOI] [PubMed] [Google Scholar]
  • 24. Bortfeld  T, Jokivarsi  K, Goitein  M  et al.  Effects of intra-fraction motion on IMRT dose delivery: Statistical analysis and simulation. Phys Med Biol  2002;47:2203–20. [DOI] [PubMed] [Google Scholar]
  • 25. Chow  JC, Jiang  R. Prostate volumetric-modulated arc therapy: Dosimetry and radiobiological model variation between the single-arc and double-arc technique. J Appl Clin Med Phys  2013;14:3–12. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 26. Guckenberger  M, Richter  A, Krieger  T  et al.  Is a single arc sufficient in volumetric-modulated arc therapy (VMAT) for complex-shaped target volumes?  Radiother Oncol  2009;93:259–65. [DOI] [PubMed] [Google Scholar]
  • 27. Yoo  S, Wu  QJ, Lee  WR  et al.  Radiotherapy treatment plans with RapidArc for prostate cancer involving seminal vesicles and lymph nodes. Int J Radiat Oncol Biol Phys  2010;76:935–42. [DOI] [PubMed] [Google Scholar]
  • 28. George  R, Keall  PJ, Kini  VR  et al.  Is the diaphragm motion probability density function normally distributed?  Med Phys  2005;32:396–404. [DOI] [PubMed] [Google Scholar]
  • 29. Rit  S, van  Herk  M, Zijp  L  et al.  Quantification of the variability of diaphragm motion and implications for treatment margin construction. Int J Radiat Oncol Biol Phys  2012;82:e399–407. [DOI] [PubMed] [Google Scholar]
  • 30. Ghilezan  MJ, Jaffray  DA, Siewerdsen  JH  et al.  Prostate gland motion assessed with cine-magnetic resonance imaging (cine-MRI). Int J Radiat Oncol Biol Phys  2005;62:406–17. [DOI] [PubMed] [Google Scholar]
  • 31. Maleike  D, Unkelbach  J, Oelfke  U. Simulation and visualization of dose uncertainties due to interfractional organ motion. Phys Med Biol  2006;51:2237–52. [DOI] [PubMed] [Google Scholar]
  • 32. Scaife  J, Harrison  K, Romanchikova  M  et al.  Random variation in rectal position during radiotherapy for prostate cancer is two to three times greater than that predicted from prostate motion. Br J Radiol  2014;87:20140343. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 33. Tuomikoski  L, Korhonen  J, Collan  J  et al.  Implementation of adaptive radiation therapy for urinary bladder carcinoma: Imaging, planning and image guidance. Acta Oncol  2013;52:1451–7. [DOI] [PubMed] [Google Scholar]
  • 34. Gay  HA, Niemierko  A. A free program for calculating EUD-based NTCP and TCP in external beam radiotherapy. Phys Med  2007;23:115–25. [DOI] [PubMed] [Google Scholar]
  • 35. Wu  Q, Mohan  R, Niemierko  A  et al.  Optimization of intensity-modulated radiotherapy plans based on the equivalent uniform dose. Int J Radiat Oncol Biol Phys  2002;52:224–35. [DOI] [PubMed] [Google Scholar]
  • 36. Anbumani  S, Arunai Nambi Raj  N, Prabhakar  GS  et al.  Quantification of uncertainties in conventional plan evaluation methods in intensity modulated radiation therapy. J BUON  2014;19:297–303. [PubMed] [Google Scholar]
  • 37. Källman  P, Agren  A, Brahme  A. Tumour and normal tissue responses to fractionated non-uniform dose delivery. Int J Radiat Biol  1992;62:249–62. [DOI] [PubMed] [Google Scholar]
  • 38. Emami  B, Lyman  J, Brown  A  et al.  Tolerance of normal tissue to therapeutic irradiation. Int J Radiat Oncol Biol Phys  1991;21:109–22. [DOI] [PubMed] [Google Scholar]
  • 39. Sumida  I, Yamaguchi  H, Kizaki  H  et al.  Novel radiobiological gamma index for evaluation of 3-dimensional predicted dose distribution. Int J Radiat Oncol Biol Phys  2015;92:779–86. [DOI] [PubMed] [Google Scholar]
  • 40. Cheung  R, Tucker  SL, Lee  AK  et al.  Dose-response characteristics of low- and intermediate-risk prostate cancer treated with external beam radiotherapy. Int J Radiat Oncol Biol Phys  2005;61:993–1002. [DOI] [PubMed] [Google Scholar]
  • 41. Rancati  T, Fiorino  C, Gagliardi  G  et al.  Fitting late rectal bleeding data using different NTCP models: Results from an Italian multi-centric study (AIROPROS0101). Radiother Oncol  2004;73:21–32. [DOI] [PubMed] [Google Scholar]
  • 42. Mavroidis  P, Giantsoudis  D, Awan  MJ  et al.  Consequences of anorectal cancer atlas implementation in the cooperative group setting: Radiobiologic analysis of a prospective randomized in silico target delineation study. Radiother Oncol  2014;112:418–24. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 43. Masi  L, Doro  R, Favuzza  V  et al.  Impact of plan parameters on the dosimetric accuracy of volumetric modulated arc therapy. Med Phys  2013;40:071718-1–071718-11. [DOI] [PubMed] [Google Scholar]
  • 44. McNiven  AL, Sharpe  MB, Purdie  TG. A new metric for assessing IMRT modulation complexity and plan deliverability. Med Phys  2010;37:505–15. [DOI] [PubMed] [Google Scholar]
  • 45. Prescribing  ICRU. Recording, and reporting photon-beam intensity-modulated radiation therapy (IMRT). Special considerations regarding absorbed-dose and dose-volume prescribing and reporting in IMRT. ICRU report 83. J ICRU  2010;10:27–40. [DOI] [PubMed] [Google Scholar]
  • 46. ICRU . Prescribing, recording, and reporting photon beam therapy (Supplement to ICRU Report 50). ICRU Report 62. Bethesda, MD: ICRU, 1999. [Google Scholar]
  • 47. Seco  J, Sharp  GC, Turcotte  J  et al.  Effects of organ motion on IMRT treatments with segments of few monitor units. Med Phys  2007;34:923–34. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 48. ICRP . Prevention of accidents to patients undergoing radiation therapy. ICRP publication 86. Ann ICRP  2000;30:7–70. [DOI] [PubMed] [Google Scholar]
  • 49. Skala  M, Holloway  L, Bailey  M  et al.  Australia-wide comparison of intensity modulated radiation therapy prostate plans. Australas Radiol  2005;49:222–9. [DOI] [PubMed] [Google Scholar]
  • 50. Tang  C, Earl  MA, Luan  S  et al.  Converting multiple-arc intensity modulated arc therapy into a single arc for efficient delivery. Int J Radiat Oncol Biol Phys  2007;69:S673. [Google Scholar]
  • 51. Samuelsson  A, Johansson  KA. Intensity modulated radiotherapy treatment planning for dynamic multileaf collimator delivery: Influence of different parameters on dose distributions. Radiother Oncol  2003;66:19–28. [DOI] [PubMed] [Google Scholar]
  • 52. Hall  EJ, Brenner  DJ. The dose-rate effect revisited: Radiobiological considerations of importance in radiotherapy. Int J Radiat Oncol Biol Phys  1991;21:1403–14. [DOI] [PubMed] [Google Scholar]
  • 53. Nevelsky  A, Bar-Deroma  R, Kuten  A. Radiobiological effects of total body irradiation on the spinal cord. Radiat Environ Biophys  2009;48:385–9. [DOI] [PubMed] [Google Scholar]
  • 54. Ling  CC, Gerweck  LE, Zaider  M  et al.  Dose-rate effects in external beam radiotherapy redux. Radiother Oncol  2010;95:261–8. [DOI] [PubMed] [Google Scholar]
  • 55. Bewes  JM, Suchowerska  N, Jackson  M  et al.  The radiobiological effect of intra-fraction dose-rate modulation in intensity modulated radiation therapy (IMRT). Phys Med Biol  2008;53:3567–78. [DOI] [PubMed] [Google Scholar]
  • 56. Poulsen  PR, Muren  LP, Høyer  M. Residual set-up errors and margins in on-line image-guided prostate localization in radiotherapy. Radiother Oncol  2007;85:201–6. [DOI] [PubMed] [Google Scholar]
  • 57. Ogino  I, Kaneko  T, Suzuki  R  et al.  Rectal content and intrafractional prostate gland motion assessed by magnetic resonance imaging. J Radiat Res  2011;52:199–207. [DOI] [PubMed] [Google Scholar]
  • 58. Gill  S, Dang  K, Fox  C  et al.  Seminal vesicle intrafraction motion analysed with cinematic magnetic resonance imaging. Radiat Oncol  2014;9:174. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 59. Gurney-Champion  OJ, McQuaid  D, Dunlop  A  et al.  MRI-based assessment of 3D Intrafractional motion of head and neck cancer for radiation therapy. Int J Radiat Oncol Biol Phys  2018;100:306–16. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 60. Tetar  SU, Bruynzeel  AME, Lagerwaard  FJ  et al.  Clinical implementation of magnetic resonance imaging guided adaptive radiotherapy for localized prostate cancer. Phys Imag Radiat Oncol  2019;9:69–76. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 61. Bruijnen  T, Stemkens  B, Terhaard  CHJ  et al.  Intrafraction motion quantification and planning target volume margin determination of head-and-neck tumors using cine magnetic resonance imaging. Radiother Oncol  2019;130:82–8. [DOI] [PubMed] [Google Scholar]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Revised_Supplementary_Table_1_Clean_Copy_rraa123

Articles from Journal of Radiation Research are provided here courtesy of Oxford University Press

RESOURCES