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Influence of beam incidence and irradiation parameters on stray neutron doses to healthy organs of pediatric patients treated for an intracranial tumor with passive scattering proton therapy

​​​​​​​​​​​​​​​​​​​Physica Medica / Volume 32, Issue 4, Pages 590-599, April 2016

Document type > *Article de revue

Keywords >

Research Unit > IRSN/PRP-HOM/SDE/LDRI

Authors > BONFRATE Anthony, FARAH Jad, DE MARZI Ludovic, DELACROIX Sabine, HÉRAULT Joël, SAYAH Rima, LEE Choonsik, BOLCH Wesley

Publication Date > 01/04/2016

Summary

Purpose

In scattering proton therapy, the beam incidence, i.e. the patient’s orientation with respect to the beam axis, can significantly influence stray neutron doses although it is almost not documented in the literature.


Methods

MCNPX calculations were carried out to estimate stray neutron doses to 25 healthy organs of a 10-year-old female phantom treated for an intracranial tumor. Two beam incidences were considered in this article, namely a superior (SUP) field and a right lateral (RLAT) field. For both fields, a parametric study was performed varying proton beam energy, modulation width, collimator aperture and thickness, compensator thickness and air gap size.


Results

Using a standard beam line configuration for a craniopharyngioma treatment, neutron absorbed doses per therapeutic dose of 63 μGy Gy−1 and 149 μGy Gy−1 were found at the heart for the SUP and the RLAT fields, respectively. This dose discrepancy was explained by the different patient’s orientations leading to changes in the distance between organs and the final collimator where external neutrons are mainly produced. Moreover, investigations on neutron spectral fluence at the heart showed that the number of neutrons was 2.5 times higher for the RLAT field compared against the SUP field. Finally, the influence of some irradiation parameters on neutron doses was found to be different according to the beam incidence.


Conclusion

Beam incidence was thus found to induce large variations in stray neutron doses, proving that this parameter could be optimized to enhance the radiation protection of the patient.
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