Introduction
Breast cancer is currently the most frequently diagnosed cancer among women worldwide and remains one of the leading causes of cancer-related mortality. According to the most recent estimates from the International Agency for Research on Cancer, approximately 2.3 million new cases were diagnosed in 2020, accounting for 11.7% of all cancers, with nearly 685,000 deaths worldwide. 1 In Morocco, the situation is particularly concerning, with an annual incidence exceeding 12,000 cases and an estimated 4,000 deaths. 2
The therapeutic management of breast cancer relies on a multimodal approach combining surgery, chemotherapy, hormone therapy, targeted therapies and radiotherapy. Reference Cardoso, Kyriakides and Ohno3 Among these modalities, external beam radiotherapy remains a cornerstone, particularly after breast-conserving surgery. Numerous studies have demonstrated that whole-breast irradiation significantly reduces the risk of loco-regional recurrence in patients with early-stage invasive breast cancer. Reference Darby, McGale and Correa4,Reference Zhang, Zhang, Yang, Liang, Liu and Zhou5 However, this treatment approach also exposes patients to potential side effects, including pulmonary toxicity, cardiotoxicity and an increased risk of secondary malignancies. Reference Taylor, Wang, Macaulay, Jagsi, Duane and Darby6
The evolution of radiotherapy techniques has led to a shift from conventional two-dimensional approaches to more sophisticated modalities, including three-dimensional conformal radiotherapy (3D-CRT), intensity-modulated radiation therapy (IMRT) and volumetric-modulated arc therapy (VMAT). These advanced techniques enable spatial modulation of the dose, improved dose homogeneity within the target volume and better sparing of OARs. Reference Narudom, Pornsriniyom, Somsin, Chitapanarux, Tippanya and Pukanhaphan7,Reference Jin, Li and Wang8
3D-CRT, in particular, has remained a well-established technique for breast cancer treatment due to its use of tangential beams that effectively limit low-dose exposure to surrounding healthy tissues. It continues to be widely used in many centres because of its balance between simplicity, effectiveness and normal tissue preservation. Reference Attallah, Moubachir and Elharrouss9
However, the introduction of new-generation linear accelerators such as the Halcyon system (Varian Medical Systems) has significantly changed clinical practice. This platform, designed for speed, precision and integrated image guidance, does not allow for 3D-CRT planning. It is exclusively based on inverse planning techniques such as IMRT and VMAT, thus obligating clinicians to choose between these two modalities. Reference Patil, Sharma and Mishra10,Reference Zhang, Zhang, Yang, Liang, Liu and Zhou11
This constraint raises an important clinical question: between IMRT and VMAT, which technique provides the best balance between dosimetric efficiency, target coverage and normal tissue sparing for breast cancer treatment delivered with Halcyon? The answer to this question is of particular relevance for institutions equipped exclusively with this type of accelerator.
In this context, the present study was designed to compare the dosimetric and radiobiological performance of two advanced conformal radiotherapy techniques—IMRT and VMAT—for conventionally fractionated breast cancer treatment using the Halcyon platform.
Materials and Methods
Patients and specific characteristics
The study included 25 female patients with non-metastatic breast cancer who underwent adjuvant radiotherapy.
The mean age at treatment was 47 years (range: 35–62 years). Sixteen patients were classified as premenopausal and nine as postmenopausal according to available clinical records. Perimenopausal status was not specifically documented, and therefore, patients were categorized based on recorded menopausal status. The tumour was located in the right breast in 15 patients and in the left breast in 10 patients.
Regarding tumour stage, 19 patients presented with stage T1 disease and 6 patients with stage T2; all patients were node-negative (N0). The predominant histological subtype was invasive breast carcinoma, which accounted for 22 cases. Additionally, there was one case of ductal carcinoma in situ and two cases of mucinous adenocarcinoma.
On a molecular level, most tumours were positive for hormone receptors (ER and PR) and negative for HER. The Ki-67 proliferation index ranged from 1% to 59%. Molecular subtype distribution included 14 Luminal A, 5 Luminal B, 3 HER2-positive, and 3 triple-negative breast cancer cases.
Finally, 10 patients received adjuvant chemotherapy, whereas the remaining 15 patients were treated with radiotherapy alone. The molecular and clinical characteristics of the patients are summarized in Table 1.
Clinical, tumour, and molecular characteristics of the 25 patients included in the study

Patient positioning and computed tomography acquisition
Patients were positioned in the supine position on an inclined breast board specifically designed for breast cancer treatment. This setup elevates the thorax, thereby optimizing exposure of the breast region. A knee support was used to enhance patient comfort and to minimize involuntary movements, both during computed tomography (CT) image acquisition and throughout the course of radiotherapy. These immobilization devices, integrated into the standardized protocol of the International Oncology Center, ensure optimal reproducibility of patient positioning, which is essential for the accuracy of highly conformal techniques such as IMRT and VMAT.
CT simulation was performed using a multi-slice CT scanner (General Electric, GE), enabling the acquisition of thin axial slices to achieve precise anatomical reconstruction and reliable dose calculation. This scanner is equipped with a wide bore, which facilitates patient positioning in treatment conditions, and a flat carbon fibre couch identical to that of the linear accelerator, thereby ensuring strict reproducibility between the simulation and treatment phases.
The laser positioning system, identical to that of the linear accelerator, includes two lateral transverse lasers (right and left), two frontal lasers and a sagittal laser. This configuration guarantees optimal geometric consistency between simulation and treatment and contributes to the accurate delineation of target volumes and OARs during the planning process. Such precise alignment helps reduce setup uncertainties and ensures reproducibility throughout the treatment course. This consistency is particularly important in advanced techniques such as IMRT and VMAT, where even small deviations may affect dose distribution.
Target volume delineation and dose constraints
A radiation oncologist specialized in breast irradiation performed meticulous delineation of the planning target volume (PTV) and OARs, including the ipsilateral, contralateral and bilateral lungs, the whole heart, the contralateral breast, the spinal cord and the skin. Target and OAR delineation followed standardized international contouring recommendations. The spinal cord was contoured from the cervical to thoracic region according to RTOG contouring guidelines to allow evaluation of dose constraints.
The gross tumour volume (GTV) corresponds to any visible residual tumour, when present. The clinical target volume (CTV) encompasses the operated breast gland, with or without regional lymphatic areas (axillary, supraclavicular, etc.), depending on the clinical characteristics and therapeutic recommendations. The PTV is defined by adding appropriate margins around the CTV to account for uncertainties related to respiratory motion, setup variations between fractions and the inherent limitations of immobilization systems (breast board, knee support, arms raised, etc.). 12,13
Subsequently, the radiation oncologist established specific dosimetric constraints for the OARs detailed in Table 2, to ensure treatment safety while maintaining therapeutic efficacy. This anatomoclinical approach allows precise targeting of the tumour region while optimally sparing surrounding healthy structures and ensuring dose homogeneity. Such accuracy is made possible through the use of highly conformal treatment techniques such as intensity-IMRT and VMAT.
Clinical goals for organs at risk (OARs) Reference Balaji21,Reference Noël, Antoni, Barthelemy and Chauvet22

Treatment planning
In the Eclipse treatment planning system, a virtual bolus is used to optimize the dose distribution in superficial regions such as the chest wall. This structure mimics tissue on the skin surface, compensating for dose loss due to respiratory motion and ensuring a homogeneous target coverage, particularly in cases of tumour or chest wall displacement. Considered as part of the patient’s anatomy, this virtual bolus directly influences dose calculation and plan optimization. Using the Acuros 18.1 algorithm, which provides advanced heterogeneity corrections and highly accurate dose computations in complex geometries, further enhances the precision of dose calculations in the presence of a virtual bolus.
Modern techniques such as IMRT and VMAT allow for precise modulation of the dose.
For each patient, both IMRT and VMAT plans were generated under identical planning objectives and constraints, allowing intra-patient comparison and minimizing anatomical variability.
IMRT is based on the use of four static fields (dynamic MLC modulation) for both left and right breast cases. Gantry and collimator angles are adjusted to optimize dose distribution while minimizing exposure to OARs. For left-sided breast IMRT, gantry angles typically range from 125° to 325°, whereas for right-sided cases they extend from 35° to 235°, with adapted collimator angles (10° or 350°).
VMAT, on the other hand, employs partial arcs with simultaneous modulation of beam intensity, gantry rotation speed and MLC position. Four arcs are used for each breast, with specific configurations: for left-sided cases, arcs range from 300° to 179° and from 179° to 300°, with collimator angles set at 0° and 90°; a similar configuration is applied for the right breast, but with arcs ranging from 181° to 60° and from 60° to 181°. This technique enables fast and homogeneous dose delivery, optimizing both treatment time and organ-at-risk sparing. Figure 1 illustrates the beam arrangements for IMRT and VMAT techniques.
Beam arrangements for IMRT and VMAT treatment techniques.

Evaluation parameters
The treatment plans were evaluated based on dosimetric parameters, including the dose homogeneity index (DHI) and the conformity index (CI) for the PTV. Dosimetric parameters such as monitor units (MUs), minimum dose (D2%) and maximum dose (D98%) delivered to the PTV were recorded and analysed using dose–volume histograms (DVHs). For the OARs, the volumes receiving 5Gy, 20Gy and 30Gy (V5Gy, V20Gy and V30Gy) were extracted and documented for each structure. In addition, the normal tissue complication probability (NTCP) was calculated for the lungs and whole heart, the secondary cancer complication probability (SCCP) was estimated for the contralateral breast and both lungs, and TCP was calculated for the PTV for each treatment plan.
The DHI Reference Sylla14 and CI 15 indices were calculated according to the following equations:
The lower the DHI, the more homogeneous the dose distribution within the target volume. Similarly, the closer the CI is to 1, the more accurately the dose distribution conforms to the shape of the target volume, thus reflecting a high-quality treatment plan. In this context, VRI refers to the volume receiving the prescription dose (typically corresponding to the 95% isodose line), while VPTV represents the total volume of the PTV. The Lyman–Kutcher–Burman (LKB) model Reference Purdy16,Reference Landberg, Chavaudra, Dobbs, Gerard, Hanks, Horiot, Johansson, Möller, Purdy, Suntharalingam and Svensson17 was used to calculate the NTCP for both the ipsilateral and contralateral lungs.
The definitions and parameter values used in this model are presented in Table 3. The equations used are as follow:
$EUD = {\left( {\sum\limits_i {D_i^{{1 \over n}}} \cdot {{{v_i}} \over {{v_{{\rm{tot}}}}}}} \right)^n}$
Definitions and parameter values in the LKB model Reference Alqahtani, Alshammari and Alhussain20

The relative seriality model Reference Aldosary, Alnajjar, Alhussain and Alshammari19 was used to calculate the NTCP for the whole heart. The definitions and parameter values used in this model are summarized in Table 4. The equations applied are as follows:
$NTCP = {\left\{ {1 - \mathop {\mathop \prod \limits_i }\limits^n {{\left( {1 - P{{({D_i})}^s}} \right)}^{{v_i}}}} \right\}^{{1 \over s}}}$
Parameter definitions for NTCP calculation in relative seriality model Reference Alqahtani, Alshammari and Alhussain20

The Schneider model was used to calculate the SCCP for the contralateral breast and both lungs. Reference Landberg, Chavaudra, Dobbs, Gerard, Hanks, Horiot, Johansson, Möller, Purdy, Suntharalingam and Svensson17,18 The definitions and parameter values used in this model are presented in Table 5. The equations applied are as follows:
$OE{D_{{\it{org}}}} = {1 \over {{V_T}}}\sum\limits_i {\left( {{v_i} \cdot {{1 - {e^{ - {\delta _{{\it{org}}}}{D_i}}}} \over {{\delta _{{\it{org}}}}}}} \right)}$
Secondary cancer risk parameter in the relative seriality model framework Reference Alqahtani, Alshammari and Alhussain20

The LQ-Poisson model was used to calculate TCP for the PTV. The definitions and parameter values used in this model are summarized in Table 6. The equation applied is as follows:
Definitions and parameter values in the LQ-Poisson model Reference Alqahtani, Alshammari and Alhussain20

The DVHs were converted from their cumulative form to differential histograms in order to enable a more detailed analysis of the local dose distribution within the target structures and OARs.
Although NTCP, TCP and SCCP models provide useful estimations, they remain predictive mathematical models and may not fully represent clinical outcomes. Long-term clinical follow-up would be necessary to validate these predictions.
Statistical analysis
Dose differences between the IMRT and VMAT techniques were analysed using Microsoft Excel and MATLAB, taking into account the paired nature of the data. The normality of the differences was assessed using the Shapiro–Wilk test, which indicated a non-normal distribution (p < 0.05). Consequently, the non-parametric Wilcoxon signed-rank test was applied. A p-value of less than 0.05 was considered statistically significant.
Ethics statement
This retrospective planning study was conducted in accordance with institutional ethical standards and approved by the local ethics committee. Patient data were anonymized.
Results
Dose to the PTV
The comparative analysis of IMRT and VMAT techniques (Table 7) highlights statistically significant differences in terms of homogeneity index (HI), conformity (CI), target coverage (D2%, D98%) and irradiation time. The VMAT technique demonstrates superior homogeneity (HI: 0.273 ± 0.045 vs 0.443 ± 0.137; p < 0.001) and a CI closer to the ideal value (CI: 1.021 ± 0.081 vs. 1.068 ± 0.158; p = 0.001), indicating a more uniform dose distribution better adapted to the target volume. It also achieves a significant reduction in treatment delivery time (46.46 s vs. 81.69 s; p = 0.001).
Comparison of dosimetric and technical parameters between IMRT and VMAT

However, the D2% value was higher with VMAT (40.49 Gy vs. 33.07 Gy; p < 0.001), suggesting an increased risk of localized overdosing, whereas IMRT provided a better minimum dose to the PTV (D98%: 55.61 Gy vs 54.38 Gy; p < 0.001). The isodose distributions illustrated in Figure 1 confirm these correlations. VMAT planning shows better peripheral coverage of the PTV, with a reduction in underdosed regions (< 95%), in contrast to IMRT, which presents partially irradiated areas. This is reflected by the higher V95% achieved with VMAT (98.88%) compared to IMRT (90.48%).
Finally, the analysis of low-dose regions (blue areas on the images) demonstrates better healthy tissue sparing with IMRT, which limits low-dose spread outside the PTV. Conversely, the rotational beam delivery of VMAT exposes a larger volume to low doses, as confirmed by the DVH curve (Figure 2), where the steeper slope with VMAT indicates a tighter dose conformity around the prescription dose.
Comparison of low-dose PTV coverage between VMAT (a) and IMRT (b) plans for patient P10.

Dose to OARs
The sparing of OARs is essential to ensure an effective treatment by maximizing the dose to the target volume while minimizing adverse effects on healthy tissues. The analysis (Table 8) shows that the IMRT technique provides better protection for the heart, contralateral lung, contralateral breast and spinal cord, with statistically significant p-values (< 0.001).
Comparison of OAR dosimetric parameters between IMRT and VMAT

Heart : The DVHs (Figure 3) show that the IMRT technique tends to better limit cardiac exposure, particularly in patients treated for left-sided breast cancer, where the heart is closer to the treatment field. The curves indicate a reduction in low cardiac doses with IMRT compared to VMAT, which, due to its rotational nature, results in a broader spread of dose. This observation is confirmed by the dosimetric data (Table 8): the mean heart dose is significantly lower with IMRT (2.67 ± 2.04 Gy) than with VMAT (3.67 ± 1.57 Gy), with a highly significant difference (p < 0.001). Similarly, the heart volume receiving at least 5 Gy (V5Gy) is reduced with IMRT (9.51%) compared to VMAT (17.31%), also with a marked level of significance (p < 0.001). Conversely, V20Gy remains low and comparable between the two techniques (p = 0.470), suggesting similar control of intermediate to high doses. These results indicate better relative cardiac sparing with IMRT, while maintaining good target coverage with both techniques.
The DVHs for both techniques IMRT (▲) and VMAT(■).

Contralateral lung : The contralateral lung benefits from markedly greater sparing with the IMRT technique compared to VMAT, effectively limiting low-dose irradiation. Dosimetric data confirm this results : the mean dose is significantly lower with IMRT (0.35 ± 0.25 Gy) than with VMAT (2.96 ± 1.13 Gy; p < 0.001), as is the volume receiving at least 5 Gy (V5Gy), which is considerably reduced (0.3% vs. 15.57%; p < 0.001). This difference reflects superior protection of the opposite healthy lung, which is crucial for reducing the risk of long-term radiation-induced pulmonary toxicity.
Ipsilateral lung: The DVHs of the ipsilateral lung reveal an overall comparable exposure between IMRT and VMAT, although the latter shows a slight reduction in the volumes exposed to high doses. Specifically, the volume receiving at least 30 Gy (V30Gy) is significantly lower with VMAT (10.19 ± 4.52%) than with IMRT (12.57 ± 5.8%; p < 0.001). Conversely, no significant difference was observed for the mean dose (Dmean; p = 0.168) or for V20Gy (p = 0.43), suggesting equivalent dosimetric performance between the two techniques in this regard.
Contralateral breast: The DVHs of the contralateral breast indicate that the IMRT technique provides better sparing at low doses than VMAT, particularly for doses below 10 Gy. This dosimetric advantage results in a significantly lower mean dose with IMRT (0.93 ± 0.86 Gy) compared to VMAT (3.24 ± 1.29 Gy; p < 0.001). This marked reduction in irradiation may help decrease the risk of late toxicity and radiation-induced secondary cancer in the opposite breast.
Spinal cord: The DVHs show a markedly lower exposure of the spinal cord with the IMRT technique compared to VMAT. The distribution curve drops more steeply with IMRT, reflecting better spinal cord sparing. The maximum dose (Dmax) is significantly reduced with IMRT (0.83 ± 0.36 Gy) compared to 5.11 ± 3.71 Gy with VMAT (p < 0.001), representing a major advantage in reducing the risk of neurological toxicity.
Evaluation of NTCP, SCCP, and TCP
In this study, three radiobiological parameters were calculated for each patient and for each technique (IMRT and VMAT): tumour control probability (TCP), NTCP and the risk of radiation-induced secondary cancer (SCCP). These parameters were derived from validated radiobiological models reported in the literature, namely the Poisson model for TCP, the LKB model for NTCP and the Schneider model for SCCP. The required data were extracted from cumulative dose–DVHs exported from the treatment planning system for each patient and each plan. Calculations were performed using scripts developed in MATLAB (R2015b, The MathWorks, Inc.), implementing the mathematical equations specific to each model. These programmes allow automated reading of DVH files, and the complete set of codes is provided in the appendix.
Analysis of the radiobiological indices shows that NTCP was generally higher with the VMAT contralateral lungs, but without statistically significant differences (p > 0.05). In contrast, SCCP was significantly higher with VMAT for both lungs (2.758% vs. 1.701%; p < 0.001), suggesting a greater spread of low-dose irradiation with this technique. Regarding TCP, both techniques achieved excellent tumour control, with a slight numerical advantage for VMAT (99.839% vs. 99.078%), but without statistical significance (p = 0.400), reflecting comparable efficacy in terms of target volume control (Table 9).
Comparison of biological indices (NTCP, SSCP, and TCP) between IMRT and VMAT techniques

Discussion
The purpose of this study was to compare the dosimetric and radiobiological performance of IMRT and VMAT techniques for breast cancer treatment using the Halcyon linear accelerator.
Our findings indicate that the VMAT technique provides superior dose homogeneity and conformity within the target volume. This implies that the dose is more evenly distributed, with a closer match between the target geometry and the dose distribution. These results are in agreement with those of Yin et al., Reference Alqahtani, Alshammari and Alhussain20 who reported a significantly higher CI for VMAT (0.923 ± 0.024) compared to IMRT (0.855 ± 0.032).
However, an interesting observation from our analysis is that IMRT achieves a higher minimum dose (D98%) within the target volume. In other words, IMRT better ensures that almost the entire PTV receives at least the prescribed dose.
This finding is consistent with the results of Wang et al. (2022), Reference Wang, Bi, Wu and Xu23 who highlighted that IMRT can sometimes be more reliable in guaranteeing uniform minimum coverage, which is clinically relevant in certain situations.
We also observed that D2% was significantly higher with VMAT. This means that although the dose distribution is more homogeneous overall, VMAT is associated with higher local hot spots, which may be related to the continuous rotational beam delivery characteristic of this technique. This observation is in line with Wang et al. Reference Wang, Bi, Wu and Xu23 who also reported an increase in D2% with VMAT and emphasized the potential risk of localized overdosing within the PTV.
Our results show that IMRT significantly reduces heart irradiation compared with VMAT, resulting in a lower mean heart dose and a lower NTCP for cardiac complications. This finding is particularly important in left-sided breast cancers, where the heart is more exposed. These results are consistent with those of Zhang and Yin, Reference Alqahtani, Alshammari and Alhussain20 who also emphasized the superior cardiac sparing achieved with IMRT.
Similarly, the lungs benefit from better protection with IMRT, particularly in terms of low-dose exposure (V5Gy), which is often associated with a higher risk of late pulmonary toxicity. This advantage is explained by the use of fixed beam angles in IMRT, which limit lateral dose spread. In contrast, VMAT tends to distribute low doses across a larger lung volume, which slightly increases the SCCP. This behaviour has also been described by Yin et al. Reference Alqahtani, Alshammari and Alhussain20
The contralateral breast also receives lower doses with IMRT, resulting in a significantly lower SCCP compared with VMAT. This result is in line with the findings of Zhang et al. Reference Alqahtani, Alshammari and Alhussain20 who reported greater exposure of the contralateral breast in VMAT plans due to the rotational arc delivery. Although the contralateral breast represents one of the principal sites for radiation-induced secondary malignancies in breast radiotherapy, other organs may also contribute to long-term risk, including the lungs, thyroid gland and haematologic system. Low-dose exposure to these structures has been associated with secondary lung cancers and radiation-related haematologic malignancies. Therefore, evaluation of dose distribution beyond the contralateral breast remains important when comparing IMRT and VMAT techniques. For the spinal cord, both techniques complied with the clinical dose constraints. However, IMRT occasionally achieved a slightly lower Dmax, but the difference remained marginal and without any clinically significant impact.
The evaluation of radiobiological models added an additional dimension to our analysis.
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• The TCP, which reflects the probability of tumour control, was slightly higher with VMAT. These findings may be attributed to the improved dose homogeneity within the PTV, as also reported by Zhang. Reference Alqahtani, Alshammari and Alhussain20
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• Conversely, the NTCP values for the heart and lungs remained lower with IMRT, highlighting its better tolerance profile for OARs.
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• Finally, with respect to SCCP, VMAT exhibited higher values, particularly for the contralateral breast and both lungs. This finding confirms that the wider spread of low-dose radiation generated by VMAT arcs results in greater exposure of distant healthy tissues.
The faster delivery observed with VMAT is related to continuous gantry rotation and dynamic modulation, resulting in shorter treatment times compared with step-and-shoot IMRT. Reduced delivery time may decrease intrafraction motion and improve patient comfort and setup stability.
Overall, our results confirm that VMAT performs better in terms of PTV coverage, providing a more homogeneous dose distribution and shorter treatment times. However, IMRT remains more effective for the protection of critical organs, particularly the heart and lungs.
Conclusion
This study objectively compared the dosimetric and radiobiological performance of IMRT and VMAT techniques for breast cancer treatment using the Halcyon linear accelerator. Based on the analysis of data from a cohort of patients, several key parameters were evaluated, including DHI, CI, doses to OARs, as well as radiobiological probabilities for tumour control (TCP) and NTCP and SCCP.
The results demonstrated that the VMAT technique provides better dose homogeneity and higher conformity to the target volume, while also reducing treatment time. Conversely, IMRT proved to be more effective in reducing doses to OARs in certain cases, particularly for the contralateral lung and the heart.
From a biological standpoint, TCP values were comparable between the two techniques, reflecting equivalent tumour control efficacy. However, NTCP and SCCP were slightly higher with VMAT, suggesting a broader exposure of healthy tissues to low-dose radiation.
In conclusion, the choice between IMRT and VMAT should be guided by the specific clinical priorities of each case: maximizing target coverage, minimizing doses to OARs or reducing treatment time. These findings emphasize the importance of individualized treatment planning and confirm the value of the Halcyon platform for optimizing breast cancer radiotherapy in modern clinical practice.








