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Calculations of neutron dose equivalent exposures from range-modulated proton therapy beams

Jerimy C Polf et al 2005 Phys. Med. Biol. 50 3859-3873   doi: 10.1088/0031-9155/50/16/014  Help

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Jerimy C Polf1 and Wayne D Newhauser1,2
1 Department of Radiation Physics, Unit 130, The University of Texas M D Anderson Cancer Center, 1515 Holcombe Boulevard, Houston, TX 77030, USA
2 The University of Texas Graduate School of Biomedical Sciences at Houston, TX, USA
E-mail: jpolf@yahoo.com

Abstract. Passive beam spreading techniques have been used for most proton therapy treatments worldwide. This delivery method employs static scattering foils to spread the beam laterally and a range modulating wheel or ridge filter to spread the high dose region in depth to provide a uniform radiation dose to the treatment volume. Neutrons produced by interactions of the treatment beam with nozzle components, such as the range modulation wheel, can account for a large portion of the secondary dose delivered to healthy tissue outside the treatment volume. Despite this fact, little is known about the effects of range modulation on the secondary neutron exposures around passively scattered proton treatment nozzles. In this work, the neutron dose equivalent spectra per incident proton (H(E)/p) and total neutron dose equivalent per therapeutic absorbed dose (H/D) were studied using Monte Carlo techniques for various values of range modulation at 54 locations around a passive scattering proton therapy treatment nozzle. As the range modulator wheel step thickness increased from 1.0 to 11.5 cm, the peak values of H(E)/p decreased from approximately 1 × 10−17 mSv Gy−1 to approximately 2 × 10−18 mSv Gy−1 at 50 cm from isocentre along the beam's central axis. In general, H/D increased with increasing range modulation at all locations studied, and the maximum H/D exposures shifted away from isocentre.

Print publication: Issue 16 (21 August 2005)
Received 24 February 2005, in final form 25 May 2005
Published 3 August 2005

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