Ana Lourenço1,2, Hugo Bouchard3, Sebastian Galer1, Gary Royle2, Hugo Palmans1,4. 1. Medical Radiation Science, National Physical Laboratory, Teddington, TW11 0LW, UK. 2. Department of Medical Physics and Biomedical Engineering, University College London, London, WC1E 6BT, UK. 3. Département de Physique, Université de Montréal, Québec, 2900 Boulevard Edouard-Montpetit, Montréal, QC, H3T 1J4, Canada. 4. Medical Physics Group, EBG MedAustron GmbH, A-2700, Wiener Neustadt, Austria.
Abstract
PURPOSE: In all recent protocols for the reference dosimetry of clinical proton beams, ionization chamber perturbation factors are assumed to be unity. In this work, such factors were computed using the FLUKA Monte Carlo code for three ionization chamber types, with particular attention to the influence of nuclear interactions. METHODS: The accuracy of the transport algorithms implemented in FLUKA was first evaluated by performing a Fano cavity test. Ionization chamber perturbation factors were computed for the PTW-34001 Roos® and the PTW-34070 and PTW-34073 Bragg peak® chambers for proton beams of 60-250 MeV using the same transport parameters that were needed to pass the Fano test. RESULTS: FLUKA was found to pass the Fano test within 0.15%. Ionization chamber simulation results show that the presence of the air cavity and the wall results in dose perturbations of the order of 0.6% and 0.8%, respectively. The perturbation factors are shown to be energy dependent and nuclear interactions must be taken into account for accurate calculation of the ionization chamber's response. CONCLUSION: Ionization chamber perturbations can amount to 1% in high-energy proton beams and therefore need to be considered in dosimetry procedures.
PURPOSE: In all recent protocols for the reference dosimetry of clinical proton beams, ionization chamber perturbation factors are assumed to be unity. In this work, such factors were computed using the FLUKA Monte Carlo code for three ionization chamber types, with particular attention to the influence of nuclear interactions. METHODS: The accuracy of the transport algorithms implemented in FLUKA was first evaluated by performing a Fano cavity test. Ionization chamber perturbation factors were computed for the PTW-34001 Roos® and the PTW-34070 and PTW-34073 Bragg peak® chambers for proton beams of 60-250 MeV using the same transport parameters that were needed to pass the Fano test. RESULTS: FLUKA was found to pass the Fano test within 0.15%. Ionization chamber simulation results show that the presence of the air cavity and the wall results in dose perturbations of the order of 0.6% and 0.8%, respectively. The perturbation factors are shown to be energy dependent and nuclear interactions must be taken into account for accurate calculation of the ionization chamber's response. CONCLUSION:Ionization chamber perturbations can amount to 1% in high-energy proton beams and therefore need to be considered in dosimetry procedures.