Introduction
Radiotherapy (RT) is pivotal in the adjuvant treatment of breast cancer, improving both local control and overall survival [
1,
2]. Various radiation concepts and techniques have been established over time. Static three-dimensional radiotherapy (3D-CRT) represents the conventional radiation technique, whereby tangential opposing fields with hard wedge filters (HWF) are used. Modern dynamic irradiation techniques, such as intensity-modulated radiation therapy (IMRT) and volumetric modulated arc therapy (VMAT), attempt to generate more homogeneous and conformal dose distributions for the planning target volume (PTV). Furthermore, better protection of organs at risk (OAR) may be achieved [
3,
4]. Nevertheless, dynamic radiation techniques bear the risk of increased induction of secondary tumors attributed to larger areas of low-dose exposure and increased monitor units (MU) [
5]. To balance the respective advantages of static and dynamic radiation techniques, Mayo et al. [
6] have developed a composite approach combining 3D-CRT and IMRT named hybrid intensity-modulated radiation therapy (H‑IMRT). In our study, we examined the impact of different variations with respect to HWF in the 3D-CRT base plan and beam energies for the application of hybrid volumetric arc therapy (H‑VMAT). Patients were evaluated in terms of PTV dose coverage and OAR exposure. Concerning OAR, dose comparisons were established and differences between left- and right-sided breast therapy were analyzed.
Materials and methods
Patient selection, positioning, and computed tomography
The patients included in this study were selected by defining a volume-based standardized breast size (
n = 200), whereby the PTV sizes were evaluated as a measure of breast size. The computed tomography (CT) scans (Canon Aquilion LB, Canon Medical Systems Europe B.V., Zoetermeer, the Netherlands) were acquired with a slice thickness of 3.0 mm. Patients were positioned in a headfirst supine position. An arm board helped to immobilize the chest and thorax with the arms positioned overhead. To minimize intrafractional movement, the CT scans were carried out in deep-inspiration breath-hold (DIBH). This method bears dosimetric advantages, especially for cardiopulmonary OAR exposure and secondary lung cancer risk [
7‐
10]. Of the 200 patients analyzed, 110 patients met the inclusion criteria of the study regarding PTV size and no exclusion criteria were included, such as funnel chests, pathological enlarged hearts, or anatomic variations. Out of these patients, 40 (20 per breast side) were selected randomly.
Treatment planning and techniques
The Eclipse software (version 15.6, Varian Medical Systems, Palo Alto, CA, USA) was used for treatment planning. Treatment plans were created for a Varian TrueBeam linear accelerator, the calculation model was based on the anisotropic analytical algorithm (AAA, version 15.5.12) and a calculation grid size of 2.5 mm. Each PTV included the whole breast and was cropped 5 mm from the skin surface, resulting in a VMAT optimization where the dose is not forcibly modulated to the surface. The thoracic wall was defined as part of the PTV. Individual treatment plans were created using the H‑VMAT technique and the 3D-CRT technique as reference (Ref). The H‑VMAT plans represented sum plans: each consisted of two treatment plans including 3D-CRT and VMAT. The prescribed dose was 40.05 Gy in 15 fractions (2.67 Gy per fraction) based on the START B trail, which demonstrated the non-inferiority of this hypofractionated regime regarding locoregional control and toxicity in comparison to normofractionated treatment [
11]. The reference treatment plans were planned as tangential opposing fields with mixed beam energies (6 MV and 15 MV) and HWF. All planning parameters such as gantry and wedge filter angles, collimator position, and field weightings were individually optimized. H‑VMAT plans were weighted 80/20 between 3D-CRT and VMAT, which included 3D-CRT as a base plan for VMAT optimization. The supplementary dose consisted of a single VMAT field with an identical isocenter position. Its range of rotation angle corresponded to the tangential angles from the base plan. The collimator rotation angle was set to 5° and the maximum dose rate to 600 MU/min. A standard optimization protocol was used for the inverse planning process of VMAT, which was adapted individually. Flattening-filter beams were used in all treatment plans. Within the hybrid approach, six different H‑VMAT combinations (HV1–HV6, Table
1) were used, varying beam energy and the application or omission of HWF in the 3D-CRT plans. The selection of these combinations was based on a previous evaluation by our group. This previous study was an initial assessment of 32 different combinations, 16 of which were within the weightings 60/40 and 80/20, which were evaluated based on a case number of 5 patients. To assess the optimal hybrid combination, superior combinations of this evaluation with respect to quality indices (PTV coverage, conformity, homogeneity) and OAR doses were analyzed in detail (Table
1).
Table 1
Definition of irradiation techniques using different H‑VMAT constellations and conventional 3D-CRT as a reference treatment plan
Ref | 6/15 (mixed on both sides) | Yes | – |
HV1 | 6/15 (mixed on both sides) | No | 6 |
HV2 | 6 | No | 6 |
HV3 | 6 | No | 15 |
HV4 | 6 | Yes | 6 |
HV5 | 6 | Yes | 15 |
HV6 | 6 (posterior lateral), 15 (anterior medial) | No | 6 |
PTV dose coverage had the first priority in treatment planning. The PTV dose requirements in our study were based on the recommendations of ICRU Report 83 [
12]:
$$\mathrm{PTV} \text{D}_{\text{mean}}=40.05\,\mathrm{Gy}(100 \% )$$
$$38.05\,\mathrm{Gy}(95\mathrm{\% })\leq \text{PTV D}_{95\mathrm{\%}}\leq 38.85\,\mathrm{Gy}(97\mathrm{\% })$$
$$\mathrm{PTV} \text{D}_{2\mathrm{\% }}\leq 42.85\,\mathrm{Gy}(107\mathrm{\% })$$
In order to ensure an appropriate plan comparison with regard to OAR doses, these PTV requirements should be kept as consistent as possible. For this purpose, an upper limit for PTV D95% was set. Minimizing OAR doses was a secondary priority. The protection was implemented so that the PTV dose requirements could be guaranteed. Each of the prepared 520 treatment plans was separately optimized for individual patients.
Dosimetric parameters
Four different indices were used to assess PTV dose conformity and homogeneity:
The Radiation Therapy Oncology Group (RTOG) Report 1005 [
17] served as a guide for dosimetric evaluations of the OAR doses (for detailed OAR constraints, see Table
2). Our previous evaluation showed clinically negligible doses to the contralateral lung and spinal cord, so that these OAR were not considered in this study.
Table 2
Dose constraints of OAR defined in RTOG Report 1005 [
17] for hypofractionated breast radiation therapy
Ipsilateral lung | V16 = 15–20% |
V8 = 35–40% |
V4 = 50–55% |
Heart | Dmean = 320–400 cGy |
Contralateral breast | D5 = 144–240 cGy |
Further evaluation criteria were the planned monitor units (MU) and beam-on time (BOT) that were observed over the total number of patients.
SPSS software (for Windows, version 26, IBM, Armonk, NY, USA) was used for the statistical analysis. A two-sided Wilcoxon rank-sum test for paired samples was used to evaluate dosimetric parameters. A p-value <0.05 was considered statistically significant.
Discussion
To our knowledge, this is the first study to analyze different base plan designs using 3D-CRT, in which the use of HWF and beam energies were varied. Variations in beam energy for the VMAT supplementary dose were also performed. The H‑VMAT combinations HV2 and HV3 (Table
1) uniformly achieved the best values regarding all dosimetric parameters in comparison to the reference treatment plan (Fig.
4; Table
3). Both favored combinations contained a 6-MV photon base plan without the use of HWF, which are conventionally used for shape compensation and dose homogenization. The comparison of different hybrid combinations showed significant disadvantages for quality indices and OAR doses when using HWF in the base plan (Table
4). In a tangential field arrangement using wedge orientation for breast surface compensation, the total body and OAR doses were increased. Advantages of virtual wedges over hard wedge filters are reported in the literature [
18‐
21]. Less scattering effects led to lower average doses outside the irradiation field. Consequently, smaller low-dose areas in the body and lower OAR exposure, e.g., of the contralateral breast in breast radiotherapy, were observed. Furthermore, a reduction in MU was achieved. Nevertheless, virtual wedges were omitted in our study because the collimator would have to be rotated by 90 ° for technical realization (Varian TrueBeam linear accelerator). This would have complicated the exact fitting of the MLC to the PTV contour and would have increased the exposure of the OAR, especially the ipsilateral lung. The use of HWF is not necessary in H‑VMAT for reasons of dynamic supplementary dose and may even be harmful due to the increased MU and beam-on time. Furthermore, higher photon energies in VMAT showed an unfavorable tendency with regard to OAR exposure (Table
3). The maximum of depth dose curves shifts the maximum dose deeper into the tissue and a longer dose extension is created, which also increases the total body and OAR doses.
In the present study, the weighting between the radiation techniques 3D-CRT and VMAT was uniform for all combinations (80/20). Other studies confirmed the benefit of this ratio when using the H‑VMAT technique. Balaji et al. [
22,
23] analyzed different ratios of chest wall radiation and identified 80/20 and 70/30 as optimal weighting concerning dose coverage of the PTV and OAR exposure. Nevertheless, the choice of weighting should be adapted individually, depending on the clinical scenario. Patient age plays an important role, as late side effects are negligible in older patients, but both acute and late effects should be considered in younger patients. With the increase of the VMAT component weighting, the low-dose area expands. In younger patients, these areas can be minimized by choosing 80/20.
The study of Lin et al. [
24] showed benefits of the H‑VMAT technique over pure-VMAT and a fixed-field IMRT technique in radiotherapy of left breast cancer. They used a base plan consisting of tangential IMRT fields (T-IMRT). In our study, 3D-CRT was used in the base plan, which enables a reduction in MU and delivery time compared to dynamic techniques like IMRT. Less MLC radiation leakage and internal body scattering can be the benefit of decreased MU, which leads to a reduction in the total body dose [
25]. With a reduction of the delivery time, patients have to complete fewer breathing cycles per fraction, which makes the treatment more feasible when using DIBH.
For the supplementary dose, various concepts may be used. Balaji et al. [
26] reported clinically similar results of H‑IMRT and H‑VMAT using 6‑MV flattening filter-free (FFF) photon beams. The researchers recommend H‑VMAT for hypofractionated breast RT in DIBH due to reduced MU and treatment delivery time. Another study by Chen et al. [
27] consistently reported advantages of H‑VMAT over H‑IMRT with regard to dose conformity, heart dose, and delivery time. They compared H‑VMAT with two different H‑IMRT designs in the treatment of early-stage left-sided breast cancer. Two tangential beams were used as a base plan and two coplanar 90-degree arcs (H-VMAT) or four IMRT fields (H-IMRT) for the supplementary dose. Ramasubramanian et al. [
28] analyzed the influence of different arc designs for left breast therapy, comparing two partial arcs (2A), four partial arcs (4A), and four tangential arcs (TA). The dosimetric superiority of PTV and OAR doses could be analyzed in 2A and 4A, with the 2A method additionally allowing a reduction of MU and beam-on time. We only used flattening-filter beams and a single VMAT field over the entire tangential angular range for the supplementary dose, such that our approach resembles the 2A method. This approach may realize a further shortening of treatment time due to the uninterrupted continuous arc.
The basis for proper dose application with H‑VMAT to the patient is the existence of good reproducibility of the patient positioning. Dynamic techniques like H‑VMAT may be prone to intra- and interfractional positioning uncertainties, which demand reproducibility of patient positioning both in treatment planning and execution [
27,
29‐
31]. In order to minimize positioning uncertainties and deviations between planned and delivered dose distributions, CT acquisition and radiotherapy should be carried out in DIBH. Besides, studies have shown benefits of DIBH concerning irradiated cardiac volume and secondary lung cancer risk in left-sided breast radiotherapy [
7‐
10,
32]. Efficient therapy in DIBH, however, requires special measures and skills. Employee training, patient selection criteria, patient coaching, and protocols for verifying the treatment are essential requirements for efficient therapy [
33].
Another key limitation of our study is the restricted patient selection. We evaluated and analyzed standardized breasts or PTV sizes only. Anatomical deviations in size or non-conventional shapes may change the findings.
Conclusion
Our study showed the advantages of the H‑VMAT technique with a weighting of 80% 3D-CRT/20% VMAT compared to the conventional static tangential radiation technique. The combination of static and dynamic radiation techniques improved PTV dose coverage, conformity, and homogeneity. The doses of the OAR ipsilateral lung, heart, and contralateral breast were significantly reduced (p < 0.05) by a suitable choice of the plan combination of H‑VMAT. In treatment planning, a photon energy of 6 MV should be preferred for both the tangential radiation fields of the base plan and the VMAT supplementary dose. The use of radiation wedges in the base plan was found to be disadvantageous for PTV dose coverage and conformity, OAR doses, MU number, and delivery time.