ESTRO 2023 - Abstract Book

S774

Monday 15 May 2023

ESTRO 2023

Conclusion For the first time, measurements and simulations were compared for an advanced Markus chamber for the dosimetry of protons within MFs. For both MF strengths, there was a good agreement of k_(B,M,Q) between experimentally determined and MC calculated values in this study. By benchmarking the MC code for calculation of k_(B,M,Q) it can be used to calculate k_(B,M,Q) for various ionisation chamber models, MF strengths and proton energies in order to generate data needed for a dosimetry protocol for MRiPT. OC-0928 Comparison of cylindrical and plane-parallel ionization chambers in continuous and pulsed proton PBS G. Vilches-Freixas 1 , A. Lourenço 2,3 , A. Douralis 2 , J. Martens 1 , A. Meijers 4,5 , H. Palmans 2,6 , I. Rinaldi 1 , K. Salvo 7 , R. Thomas 2,3 , G. Bosmans 1 1 Department of Radiation Oncology (MAASTRO), GROW School for Oncology, Maastricht University Medical Centre+, Maastricht, The Netherlands; 2 National Physical Laboratory, (NPL), Teddington, United Kingdom; 3 University College London, (UCL), London, United Kingdom; 4 Department of Radiation Oncology, University Medical Center Groningen, University of Groningen, Groningen, The Netherlands; 5 Center for Proton Therapy, Paul Scherrer Institute, Villigen, Switzerland; 6 MedAustron Ion Therapy Center, Medical Physics Group, Wiener Neustadt, Austria; 7 Department of Radiotherapy, AZ Sint-Maarten, Mechelen, Belgium Purpose or Objective In this experimental work we compared dose measurements using four ionization chambers (ICs), i.e., three plane parallel (PP) chambers and one Farmer-type chamber, irradiated under the same conditions in one continuous cyclotron-accelerated proton beam (IBA Proteus PLUS) and in two pulsed-scanned synchrocyclotron-accelerated proton beams (IBA Proteus ONE and MEVION Hyperscan 250i). Materials and Methods Measurements were performed using a PTW-34045 Advanced Markus, PTW-34001 Roos, IBA-PPC05 and PTW-30012 Farmer. The chambers were positioned at 2 cm depth in a water phantom in four square-field single-energy scanned proton beams with nominal energies between 80 and 220 MeV and in the middle of a 10x10x10 cm3 dose cube centered at 10 cm depth in water. To reduce uncertainties due to traceability, all chambers were calibrated at the same primary standard laboratory. IC readings were corrected for ambient conditions, polarity, and ion recombination. We used the beam quality (kQ) correction factors for the chambers under investigation from IAEA TRS-398, newly calculated Monte Carlo (MC) values and IAEA TRS-398 updated recommendations (Palmans et al. 2022). For the Farmer-type chamber placed at 2cm depth of single-energy beams we used an empirical model to account for the displacement correction factor. For the PP chambers the water-equivalent thickness (WET) of the entrance window was accounted for in positioning the inner surface of the window at the measurement depth. Results The polarity correction factor was found to be unity for all chambers and beam qualities, within experimental uncertainties. Ion recombination factors increased with beam energy with values up to 0.7%, 3.5%, and 7.6% for the PTW Farmer 30012 (operated at 400V) and up to 0.2%, 2%, and 3.7% for the PTW Roos 34001 (operated at 300V) in the continuous, and in the two pulsed beams, respectively. Dose differences among the four chambers ranged between 0.8% and 3.0% using the TRS 398 kQ values and increased to between 1% and 3.4% with the newly recommended kQ values. The largest differences were observed between the IBA PPC05 and the rest of the chambers, which agreed within one standard deviation, as shown in Figure 1.