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Research Article

Radiobiological risk estimates of adverse events and secondary cancer for proton and photon radiation therapy of pediatric medulloblastoma

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Pages 806-816 | Received 15 Mar 2011, Accepted 08 Apr 2011, Published online: 18 Jul 2011

Abstract

Introduction. The aim of this model study was to estimate and compare the risk of radiation-induced adverse late effects in pediatric patients with medulloblastoma (MB) treated with either three-dimensional conformal radiotherapy (3D CRT), inversely-optimized arc therapy (RapidArc® (RA)) or spot-scanned intensity-modulated proton therapy (IMPT). The aim was also to find dose-volume toxicity parameters relevant to children undergoing RT to be used in the inverse planning of RA and IMPT, and to use in the risk estimations. Material and methods. Treatment plans were created for all three techniques on 10 pediatric patients that have been treated with craniospinal irradiation (CSI) at our institution in 2007–2009. Plans were generated for two prescription CSI doses, 23.4 Gy and 36 Gy. Risk estimates were based on childhood cancer survivor data when available and secondary cancer (SC) risks were estimated as a function of age at exposure and attained age according to the organ-equivalent dose (OED) concept. Results. Estimates of SC risk was higher for the RA plans and differentiable from the estimates for 3D CRT at attained ages above 40 years. The risk of developing heart failure, hearing loss, hypothyroidism and xerostomia was highest for the 3D CRT plans. The risks of all adverse effects were estimated as lowest for the IMPT plans, even when including secondary neutron (SN) irradiation with high values of the neutron radiation weighting factors (WRneutron). Conclusions. When comparing RA and 3D CRT treatment for pediatric MB it is a matter of comparing higher SC risk against higher risks of non-cancer adverse events. Considering time until onset of the different complications is necessary to fully assess patient benefit in such a comparison. The IMPT plans, including SN dose contribution, compared favorably to the photon techniques in terms of all radiobiological risk estimates.

Cancers of the central nervous system (CNS) are, second to lymphomas and leukemias, the most common types of childhood cancers corresponding to 20–30% of all pediatric cases [Citation1,Citation2]. The most common malignant CNS tumor in children is medulloblastoma (MB) which is a primitive neuroectodermal tumor located in the posterior cranial fossa. MBs are characterized by a relatively high rate of spinal metastases at the time of diagnosis [Citation3,Citation4]. The overall five-year survival for standard risk MB (patients with primary tumor in the posterior fossa but without confirmed spinal metastases and with negative cerebrospinal fluid cytology) is 75–85% for children treated with modern day multimodality regimens [Citation5,Citation6]. Treatment consists of surgery followed by post-operative multi-agent chemotherapy and craniospinal irradiation (CSI). Survival rates are relatively high but there are substantial long-term side effects related to radio-chemotherapy of pediatric patients; including loss of hearing or vision, neurocognitive deficits, gonadal dysfunction, cardiopulmonary impairment and endocrine effects [Citation7–16]. The concern regarding therapy-induced secondary cancer (SC) has increased in recent years and is especially relevant for childhood cancer survivors. It has been shown that young age at treatment is associated with an increase in risk for development of most SCs [Citation17,Citation18]. Several approaches have been suggested for estimating the risk of SC induction via different models with dose-responses relating to either linear, linear-exponential or linear-quadratic behavior [Citation19–23]. When comparing results of SC risk estimates from different studies it is vital to consider whether it concerns the risk of contracting a SC or the risk of dying from that SC as this endpoint may vary between studies. It is also important to stratify if the estimates concern lifetime risk or the risk up to a certain attained age as these estimates will differ. Estimating the SC risk on an organ-specific basis would provide the option of assessing whether limiting the dose to the organs most responsible for SC induction can lower the total SC risk.

The prescribed CSI dose has been successfully decreased from 36 Gy to 23.4 Gy in standard-risk MB patients without compromising survival rates [Citation24]. Provided that the disease is properly staged as either standard or high risk, the treatment regimen can be stratified accordingly. Common to both standard- and high-risk patients is that the CSI treatment is followed by a boost to the primary tumor site (posterior cranial fossa) up to 54–55 Gy [Citation5]. Since radiotherapy can be given with varying prescribed CSI doses it is warranted to consider the impact of this variation in estimations of treatment-related long-term complications. There is lack of general consensus on the lateral extent of the spinal part of the target volume. Including the entire vertebral column is a viable option as this prevents asymmetric spinal growth. This is based on the findings that bone growth is inhibited at absorbed doses above approximately 20 Gy [Citation25].

Today the standard technique for CSI is three-dimensional conformal radiotherapy (3D CRT). This technique results in irradiation of a large volume of normal tissue to high doses. Several studies have investigated the feasibility of CSI with intensity-modulated radiotherapy (IMRT) or proton therapy and the estimated effect on SC risk [Citation21,Citation26–28].

This study was aimed at estimating and comparing SC risk and risks of several other non-cancer long-term complications between 3D CRT, rotational IMRT and spot-scanned intensity-modulated proton therapy (IMPT). The aim was also to use the inverse optimization tools in IMRT and IMPT to purposely limit the dose to most organs at risk (OARs), as an attempt at radiobiological treatment optimization for pediatric MB. Using the full potential of the different treatment techniques in this way allows for a realistic comparison of modalities. The treatment plans and risk estimations were performed for varying CSI prescription doses and spinal target volumes in order to gain some perspective into the effect of these variations on long-term complications.

Material and methods

Patient material and treatment planning

Ten pediatric patients, four males and six females, ages 4 to 15 years (mean age 8 years), were included in this study. They had all received CSI for MB at the Copenhagen University Hospital in 2007–2009. The craniospinal clinical target volume (CTV) was defined as comprised of a cranial CTV consisting of the whole brain and a spinal CTV defined as the spinal canal extending caudally to the S2-S3 junction. Target volume definitions were based on computed tomography (CT) scans. The craniospinal planning target volume (PTV) consisted of the cranial CTV with a 5 mm isotropic margin and the spinal CTV with a 7 mm isotropic margin. An alternative PTV was created with the spinal part consisting of the entire vertebral column with 3 mm lateral margins. This alternative PTV was not considered for the main analysis but rather to test how different definitions of spinal target volume would affect the risk estimates. To facilitate treatment planning comparison, prescription doses were set as 23.4 Gy and 36 Gy to the craniospinal PTV. The fractionation scheme was chosen as 1.8 Gy/fraction for all prescription levels and each prescription regimen was followed by boost treatment to a total dose of 54 Gy to the boost PTV comprised of the posterior cranial fossa with a 5 mm isotropic margin.

All treatment plans were generated using the Eclipse treatment planning system version 8.9 (Varian Medical Systems, Palo Alto, CA). The different techniques were normalized to all have the same mean target dose as the 3D CRT plans, in order to facilitate objective plan comparison. The 3D CRT plans were created with two lateral opposed cranial fields. The caudal edge of these fields was positioned just above the cranial edge of the patient's shoulders in order to protect the thyroid gland. The eyes were shielded by MLC-leaves but only to the extent that it did not compromise PTV coverage. Additionally, a spinal posterio-anterior field encompassing the spinal part of the PTV was applied. The junction between the cranial and spinal fields was moved 1.0 cm caudally once in the 23.4 Gy prescription regimen and twice in the 36 Gy regimen to limit over or under dosage due to possible set-up variations in a clinical treatment setting. In order to assess the importance of the lateral extent of the spinal target volume in 3D CRT, multiple plans were created with varying spinal field widths. For the different plans the multi-leaf-collimator (MLC) leaves were fitted to the spinal PTV with 0.5 cm, 0.75 cm, 1.0 cm and 1.5 cm lateral margins, respectively. When reviewing the treatment records of the patients, the 1.0 cm leaf-to-PTV margin corresponded best to the set-up in which most of the patients had been treated. This margin was chosen when comparing the 3D CRT plans to the other techniques. The boost plans were created using four fields, two opposing fields from the right and left sides along with two wedged fields incident from a more posterior direction.

Rotational IMRT plans were created using the RapidArc® (RA) technique (Varian Medical Systems, Palo Alto, CA). RA plans consisted of a cranial arc covering the whole brain and the cranial part of the spinal canal down to the C2 or C3 vertebra. The rest of the spinal canal was covered by a spinal arc delivering radiation from a posterior 140 degree arc only to avoid unnecessary irradiation through the arms and ventral parts of the patient. There was substantial overlap between the cranial and spinal arcs to facilitate an intensity-modulated junction that was less sensitive to set-up error than a sharp junction between field edges. Two spinal arcs were used in the case where the cranio-caudal extent of the spinal canal exceeded the span of a single arc. The boost plans consisted of a 220 degree arc covering the boost PTV without irradiating through the anterior parts of the head.

IMPT plans were generated with machine data corresponding to a PT2 Varian proton therapy system utilizing active spot-scanning. The plans were generated using three fields incident from the posterior direction. A range shifter can be introduced when necessary, in order to reach both shallow and deeply situated structures in the body. The range shifter effectively lowers the span of the achievable nominal energy, which is 70–250 MeV for this machine, and thus decreasing the depth to which the protons reach. The IMPT plans consisted of one field with a range shifter covering most of the spinal canal and two fields, of which one had a range shifter, covering the brain and the cranial part of the spinal canal. The junction between the IMPT fields was set with an overlap and modulated between fields as for the RA technique. The boost plans consisted of a single posterior field with a range shifter to ensure full coverage of the posterior fossa. illustrates the difference in dose distribution relating to the different treatment techniques.

Figure 1. Dose distributions in the sagittal and transversal plane related to treatment with (from left) 3D CRT, RapidAarc and IMPT.

Figure 1. Dose distributions in the sagittal and transversal plane related to treatment with (from left) 3D CRT, RapidAarc and IMPT.

Proton radiotherapy exposes the patient to secondary neutron (SN) irradiation which is not considered in the treatment planning system hence this extra dose contribution was added manually. This was done by using organ-specific neutron doses corresponding to a spot-scanned proton beam taken from the study by Newhauser et al. [Citation26]. In that study the neutron dose contribution was simulated using Monte Carlo methods for a pediatric mathematical phantom receiving craniospinal proton irradiation. A limitation of using this data is that SNs are assumed to be generated within the patient only. This will underestimate the SN contribution, especially when a range shifter is applied as the beam passing through the range shifter will induce SNs. In order to account for possible uncertainty in the relative biological effectiveness (RBE) of SNs, neutron radiation weighting factors (WRneutron) five times higher than the energy-dependent values recommended in ICRP publication 92 were used as a sensitivity analysis [Citation29].

The inverse planning optimization for RA and IMPT was focused on lowering the risk of treatment-induced complications by limiting the dose to as many critical structures as possible. The actual optimization objectives were set with the aim of fulfilling the dose objectives proposed in , when possible. The data shown in are the results of an extensive literature search focused on finding dose tolerance levels relevant for pediatric MB patients. The dose objectives and the inter-organ priority were based on the references given in and the preferences of experienced physicians in pediatric- and general oncology (BL, TBE). The main difference between RA and IMPT optimization was the fact that most of the OARs did not receive any absorbed dose from the protons as the distal edge of a beam is very sharp.

Table I. Organ-specific dose objectives relating to children treated with radiation therapy.

Modeling of secondary cancer risk and non-cancer adverse effects

A concept for phenomenological modeling of SC risks is that of organ equivalent dose (OED) which was developed by Schneider et al. in 2005 [Citation22]. This provides a single measure of an OED in Gy which represents the often heterogeneous dose distribution of a dose-volume histogram (DVH). This value represents the uniform dose that would yield the same SC risk to an organ as the inhomogeneous dose distribution described in the DVH. An alternative way of estimating OED was presented by Schneider et al. in 2008 based on the combined SC data of Hodgkin's disease patients having undergone radiotherapy and that of the atomic bomb survivors extrapolated to higher doses more relevant to radiotherapy [Citation30]. The authors fitted this data to OED models with a linear, linear-exponential (bell-shaped) and plateau dose-response, although the linear model did not provide a good fit to data. There is evidence from large clinical studies of SC that does not support a decrease in risk at high radiotherapy doses [Citation31,Citation32]; the plateau-model thus appears to be a more appropriate selection/model. Even with appropriate models the uncertainties in SC risk estimates are considerable. When faced with clinical decisions one needs to consider the differences, for example between modern treatment and that given several decades ago and the possible variations in genetic cancer susceptibility between the atomic bomb survivors and modern day cancer patients.

The OED for the plateau-model was calculated as

where δorg is the organ-specific dose-response parameter derived from fitting the model to the Hodgkin's cohort data. Di is the dose to bin i in the DVH and N is the total number of dose bins. To test the sensitivity of the SC risk on the choice of model, estimates were also made with the bell shaped and linear models from Schneider et al. [Citation30] as a comparison. The excess absolute risk (EAR) of SC was estimated as a linear function of the OED adjusted for population-specific variables according to Equation 2.

The parameter μ represents the population-specific risk modification and is a function of age at exposure, e, attained age, a and gender, s, and < describes the initial slope of the dose-response curve [Citation30].

The constants γe and γa are related to attained age and age at exposure and were derived from fitting the model to the original data. The cumulative EAR of developing a SC was then estimated to a given attained age by taking into account competing risks of death according to Equation 4.

The ratio S(i)/S(e) represent the gender-specific conditional probability of a person alive at age e to reach age i. The survival functions were taken from Kellerer et al. [Citation33].

A limitation of the model by Schneider et al. is that no organ-specific model parameters were derived in the original publication [Citation30]. The dose-response curve relates to the induction of any solid secondary cancer, thus representing the mean dose-response for all secondary cancers studied. In order to calculate the organ-specific risk contribution, the dose-response was assumed to be valid for all studied organs.

To take the risk contribution from each of the relevant organs into account, a weighted mean OED was calculated for all organs for which incidence of radiation-induced cancers was published in the Life Span Study (LSS) [Citation34]. The weighted mean OED was calculated based on the data provided in according to Equation 5.

Table II. Radiation-related secondary cancer incidence from the lSS [Citation34] and as adopted in this study. the incidence is given as average excess absolute risk due to external low-lEt radiation as per 10 000 person years and Sieverts equivalent dose.

As the ability of organ-specific SC risk estimation is dependent of knowing where a SC might occur, the cancer types where no localized anatomical site relating to radiation exposure could be specified were excluded (shown in italics). An attempt was made at estimating the risk of secondary leukemia but no model could be found that well predicts the risk as a function of radiation dose [Citation35]. We thus estimate the risk of contracting a localized solid SC. Negative values in are interpreted as zero and thus not contributing to the secondary cancer risk.

Modeling of non-cancer normal tissue complication probabilities (NTCP) was done according to the radiation dose-response functions presented in . The basic rationale of NTCP modeling is to use the dose-response relationship of a complication derived from a patient cohort and apply it as a predictor of complication rate in other patients. This is used to define dose limits for OARs that should keep the risk of complications at an acceptable level. Although NTCP modeling can be a powerful tool in treatment planning, the model parameters are associated with considerable uncertainty. Relative comparison of pairs of treatment plans or modalities are however less sensitive to these uncertainties than absolute risk estimates.

Table III. Dose-response functions and corresponding model parameters utilized in the estimation of treatment-induced non-cancer adverse effects.

Results

The estimations in show that the SC risk is highest for the RA treatments but the difference between the photon techniques does not become apparent until attained ages above 40 years, representing a latency period since treatment of about 30 years. The estimate of solid SC risk at an attained age corresponding to the average lifetime of a Danish person (78.5 years) was 45%, 56% and 7% for 3D CRT, RA and IMPT, respectively, for 23.4 Gy prescribed CSI dose. The corresponding risks for the 36 Gy CSI dose were 54%, 71% and 9%. These results were compared with the corresponding EARs estimated with a bell shape and a linear model as shown in . It is shown that the choice of model does affect the absolute risk estimates especially for the RA plans. The absolute estimates depend strongly on the initial slope of the different dose-response curves. The EAR estimate at an attained age of 78.5 years was lower for RA than for 3D CRT according to the linear model, 33% vs. 36% for the 23.4 Gy CSI dose and 50% vs. 54% for the 36 Gy CSI dose. This is attributable to the fact that the mean doses to the SC critical structures were lower with RA and any linear model will thus favor RA over 3D CRT for these patients because of the direct relationship to mean dose.

Figure 2. Mean values for all 10 patients of cumulative solid secondary cancer risk as a function of attained age for the three different treatment modalities studied. Results are given for the two different prescription CSI dose levels that are relevant for this patient group. The results are shown up to an attained age of 100 years, after this the cumulative risk levels out since the probability of surviving to older ages is very low. For IMPT the results are given as including SN dose with values of the WRneutron as proposed in ICRP publication 92, denoted IMPT_SN and values five times higher, denoted IMPT_SNx5.

Figure 2. Mean values for all 10 patients of cumulative solid secondary cancer risk as a function of attained age for the three different treatment modalities studied. Results are given for the two different prescription CSI dose levels that are relevant for this patient group. The results are shown up to an attained age of 100 years, after this the cumulative risk levels out since the probability of surviving to older ages is very low. For IMPT the results are given as including SN dose with values of the WRneutron as proposed in ICRP publication 92, denoted IMPT_SN and values five times higher, denoted IMPT_SNx5.

Figure 3. Mean values of EAR are given for a plateau, bell shape and a linear model, normalized to the EAR of the plateau model. The estimates are given for prescribed CSI doses of a) 23.4 Gy and b) 36 Gy. The relative difference between models depends on the initial slope of the dose-response curves and at what doses the risk plateaus out/turns over. The linear model deviates somewhat from the other two, likely since it did not provide a good fit to the original input data.

Figure 3. Mean values of EAR are given for a plateau, bell shape and a linear model, normalized to the EAR of the plateau model. The estimates are given for prescribed CSI doses of a) 23.4 Gy and b) 36 Gy. The relative difference between models depends on the initial slope of the dose-response curves and at what doses the risk plateaus out/turns over. The linear model deviates somewhat from the other two, likely since it did not provide a good fit to the original input data.

It is shown that the excess absolute SC risk estimated for IMPT is affected by a large variation in the neutron RBE. The risk is however substantially lower with IMPT than for both photon techniques even with high values of WRneutron.

shows the results of the NTCP estimations calculated according to . The risk of inducing heart failure, xerostomia, hypothyroidism and ototoxicity was estimated as substantially higher for 3D CRT than for RA. The risk of pneumonitis was equivalent for the two photon techniques while the risk of inducing blindness was slightly higher for the RA plans. All NTCP estimates were lower with IMPT compared to the photon techniques even though the results in are presented for the IMPT_SNx5 plans. The risk of developing ototoxicity was shown to be higher for the lower CSI prescription dose for the RA plans. This was due to the boost plans with RA yielding a higher dose to the cochlea per prescription Gy than the main craniospinal plans. The estimates of chronic renal failure were not shown since the kidney doses were sufficiently low to not yield any considerable risk of renal failure; the highest estimate for any plan was below 2%. As NTCP estimates are subject to uncertainty, the absolute values should be considered somewhat cautiously with more emphasis on the relative comparison between modalities.

Figure 4. Mean values for all 10 patients comparing long-term risks of inducing pneumonitis, heart failure, xerostomia, blindness, hypothyroidism and ototoxicity between the different treatment modalities.

Figure 4. Mean values for all 10 patients comparing long-term risks of inducing pneumonitis, heart failure, xerostomia, blindness, hypothyroidism and ototoxicity between the different treatment modalities.

The risk of inducing heart failure was considerably higher for 3D CRT compared to the other two techniques. The effect on this endpoint of varying the spinal field widths was studied separately and shown in . The risk of heart failure increases with spinal field width since the mean heart dose becomes larger. This shows that depending on the choice of field set-up in 3D CRT the risk of inducing heart failure is 2–2.5 times higher than that of RA.

Figure 5. Mean values of all 10 patients comparing the risk of heart failure for different spinal field widths in 3D CRT treatment.

Figure 5. Mean values of all 10 patients comparing the risk of heart failure for different spinal field widths in 3D CRT treatment.

represents target coverage parameters for the three different treatment techniques normalized to the same mean craniospinal PTV dose. The cranial target coverage was slightly better with 3D CRT compared to RA. The lack of conformity in the 3D CRT plans was shown by the high value of V107% in the spinal CTV and the low scores in conformity index.

Table IV. Mean values for all ten patients of target coverage parameters comparing the 3D CRT, RapidArc and IMPT plans for the 23.4 Gy craniospinal prescription dose.

Discussion

The results of this study show the estimated radiobiological differences between 3D CRT, RA and IMPT in the treatment of pediatric MB. As expected the solid SC risk was higher for intensity-modulated photon treatment compared to 3D CRT. The EAR estimates are relatively high but we believe that this is the case for pediatric MB patients. Estimates are in reasonable accordance with the study by Mu et al., who also focused on pediatric MB. They estimated the lifetime risk of contracting a lethal SC to be 20% for 3D CRT and 30% for IMRT relating to a 23.4 Gy CSI prescription dose [Citation21]. In the study by Miralbell et al. the yearly risk of SC induction was estimated for a 3-year-old MB patient to 0.76%, 0.43% and 0.05% for 3D CRT, IMRT and proton therapy, respectively [Citation36]. This would correspond to respective lifetime risks of 55%, 31% and 4%, their estimates were based on a prescribed dose to the craniospinal axis of 36 Gy. The high risk related to 3D CRT in their study was likely attributed to the very young age of the patient as the treatment field would cover a large proportion of such a small body. A recent study estimated the long-term mortality in childhood cancer survivors based on the current follow-up of the childhood cancer survivor study (CCSS) cohort [Citation37]. The authors showed that compared to other pediatric cases, MB patients were at high risk of SC mortality despite the fact that MB patients were the most prone to die from late recurrences.

Estimates of SC risk are in general subject to considerable uncertainty and often affected by the choice of model as shown in , so the absolute estimates should be treated with caution. However, relative comparisons between treatment modalities can likely be more reliably considered. Treating children with IMRT, whether rotational or fixed-field, should because of the underlying uncertainties still be considered as somewhat controversial.

The time since exposure aspect needs to be considered when trying to estimate actual patient detriment and when the late effects are most likely to occur. As modern, highly conformal, radiotherapy techniques are more commonly used, the definition of target volume becomes increasingly important. If, for example the entire vertebral column is included as PTV to receive at least 20 Gy we found that the SC risk was slightly increased for the RA plans and nearly doubled for the IMPT plans (data not shown). This results in weighting the risk of asymmetrical spinal growth, i.e. scoliosis, against that of an increased risk of SC. For such a comparison it is vital to consider at what ages the different complications are most likely to occur.

As for the risk estimations for non-cancer adverse effects, the results suggest that patients treated with 3D CRT are subject to substantially higher risks of serious complications such as heart failure and severe hearing loss compared to those treated with intensity-modulated therapy. The choice between the two photon techniques thus appears to be a choice between higher SC risk or higher risk of non-cancer adverse events. The basis for these risk comparisons lies in mathematical modeling and the inherit uncertainties need to be considered if the estimates are to guide clinical decision making. There is also the consideration of which technique provides the most robust treatment. A problem in 3D CRT treatment of MB is that it uses junctions between fields, risking over/under dosage due to uncertainties in treatment set-up. Intensity-modulated treatment would not suffer from the same problem since the field junctions can be modulated with intentional overlap between different fields. An error in treatment set-up would in this situation lead to only a small dose variation compared to the sharp junctions in 3D CRT.

The estimates of heart failure are based on patients that were treated with radiation therapy and anthracyclin chemotherapy, which also contributes to the risk of heart failure [Citation38]. The radiotherapy related heart failure risk was about five times higher (data not shown) for 3D CRT compared to RA attributable to a large difference in mean heart dose (18.9 Gy vs. 7.3 Gy for the 36 Gy CSI dose). It is difficult to assess which risks are of greatest importance for the future of these patients. It might, for example be worse to have a 10% risk of developing heart failure before the age of 40 years than a 30% risk of contracting a SC before turning 60. Early results of comparing the effect of different long-term complications on a common scale have recently been shown and appear promising [Citation39]. Estimating risks at old ages for people having survived a cancer in childhood is particularly difficult. This is primarily due to that cohorts in large studies like the CCSS [Citation18] have not yet reached the ages where the general population incidence of cancer and heart complications becomes large. Increasing follow-up in, for example the CCSS will hopefully reveal whether the relative risks at older ages continue to be elevated, or whether they will decrease as the general population incidence increases.

In this work the optimization priority of normal tissue toxicity prevention was based solely on the severity of the different endpoints. The best treatment plans with respect to these risks would likely also include consideration of the incidence of the different complications. This would prevent the optimizer from trying to reduce a risk which is already negligible. We also attempted to optimize the RA plans with respect to SC risk by lowering the dose to the organs suggested as responsible for SC induction presented in . This resulted in lower estimates of solid SC risk but unfortunately also in some deterioration of spinal target coverage. Such an optimization approach should thus preferably be accompanied by assessment of tumor control probability.

The risks of all long-term complications, cancer and non-cancer alike, were shown to be considerably lower for IMPT than for the photon techniques. Pediatric MB thus seems to be an obvious candidate to recommend for proton therapy if available. The risk estimation for the IMPT plans is made difficult by uncertainty in the RBE of SN produced by the proton beam. The conclusions for IMPT as favorable over photon therapy were however shown in this study to hold even for high values of neutron RBE. This suggests that SN irradiation does not warrant the choice of photon therapy over proton therapy for MB. At least if proton therapy is given with IMPT with neutron contamination intensity as that used in the presented work, although the estimates are likely somewhat underestimated for the fields with range shifters. Passively scattered proton beams tend to yield more SN and needs to be investigated separately.

This study provided estimates and comparisons of solid secondary cancer risk and risks of non-cancer late complications for three different radiotherapy techniques for treatment of pediatric MB. The uncertainties involved in the estimates should be considered, especially when interpreting the absolute risk estimates. The results of this study have shown that treating pediatric MB patients with 3D CRT would subject them to higher risks of several severe late complications compared to RA treatment. This shows the potential of intensity-modulated therapy in limiting the dose to important risk organs for these patients. The risk of SC induction was however estimated as higher if treated with RA compared to 3D CRT. This study also provided SC risk estimates as a function of attained age, highlighting the importance of considering at what ages different risks are most likely to occur.

Acknowledgements

This work was supported by funding from the Danish Childhood Cancer Foundation. The authors would like to thank chief physicians Catherine Rechnitzer and Karsten Nysom at the Department of Paediatric Oncology at Rigshospitalet, Copenhagen, for their support of this project. The authors would also like to thank everyone in the research group at the Radiation Oncology Department at Rigshospitalet, Copenhagen, for their valued input and discussions.

Declaration of interest: Per Munck af Rosenschöld has a research agreement with Varian Medical Systems. The authors alone are responsible for the content and writing of the paper.

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