Małgorzata Liszka1, Liliana Stolarczyk1,2, Magdalena Kłodowska1, Anna Kozera1, Dawid Krzempek1, Natalia Mojżeszek1, Anna Pędracka1, Michael Patrick Russell Waligórski3,4, Paweł Olko3. 1. Institute of Nuclear Physics Polish Academy of Sciences in Krakow (IFJ PAN), The Bronowice Cyclotron Centre (CCB), Radzikowskiego 152, Krakow, 31-342, Poland. 2. Skandionkliniken, von Kraemers Allé 26, Uppsala, 752 37, Sweden. 3. Institute of Nuclear Physics Polish Academy of Sciences in Krakow (IFJ PAN), Division of Applied Physics, Proton Radiotherapy Group, Radzikowskiego 152, Krakow, 31-342, Poland. 4. The Maria Skłodowska-Curie Memorial Centre of Oncology, Krakow Division, Garncarska 11, 31-115, Krakow, Poland.
Abstract
PURPOSE: To evaluate the effect on charge collection in the ionization chamber (IC) in proton pencil beam scanning (PBS), where the local dose rate may exceed the dose rates encountered in conventional MV therapy by up to three orders of magnitude. METHODS: We measured values of the ion recombination (ks ) and polarity (kpol ) correction factors in water, for a plane-parallel Markus TM23343 IC, using the cyclotron-based Proteus-235 therapy system with an active proton PBS of energies 30-230 MeV. Values of ks were determined from extrapolation of the saturation curve and the Two-Voltage Method (TVM), for planar fields. We compared our experimental results with those obtained from theoretical calculations. The PBS dose rates were estimated by combining direct IC measurements with results of simulations performed using the FLUKA MC code. Values of ks were also determined by the TVM for uniformly irradiated volumes over different ranges and modulation depths of the proton PBS, with or without range shifter. RESULTS: By measuring charge collection efficiency versus applied IC voltage, we confirmed that, with respect to ion recombination, our proton PBS represents a continuous beam. For a given chamber parameter, e.g., nominal voltage, the value of ks depends on the energy and the dose rate of the proton PBS, reaching c. 0.5% for the TVM, at the dose rate of 13.4 Gy/s. For uniformly irradiated regular volumes, the ks value was significantly smaller, within 0.2% or 0.3% for irradiations with or without range shifter, respectively. Within measurement uncertainty, the average value of kpol , for the Markus TM23343 IC, was close to unity over the whole investigated range of clinical proton beam energies. CONCLUSION: While no polarity effect was observed for the Markus TM23343 IC in our pencil scanning proton beam system, the effect of volume recombination cannot be ignored.
PURPOSE: To evaluate the effect on charge collection in the ionization chamber (IC) in proton pencil beam scanning (PBS), where the local dose rate may exceed the dose rates encountered in conventional MV therapy by up to three orders of magnitude. METHODS: We measured values of the ion recombination (ks ) and polarity (kpol ) correction factors in water, for a plane-parallel Markus TM23343 IC, using the cyclotron-based Proteus-235 therapy system with an active proton PBS of energies 30-230 MeV. Values of ks were determined from extrapolation of the saturation curve and the Two-Voltage Method (TVM), for planar fields. We compared our experimental results with those obtained from theoretical calculations. The PBS dose rates were estimated by combining direct IC measurements with results of simulations performed using the FLUKA MC code. Values of ks were also determined by the TVM for uniformly irradiated volumes over different ranges and modulation depths of the proton PBS, with or without range shifter. RESULTS: By measuring charge collection efficiency versus applied IC voltage, we confirmed that, with respect to ion recombination, our proton PBS represents a continuous beam. For a given chamber parameter, e.g., nominal voltage, the value of ks depends on the energy and the dose rate of the proton PBS, reaching c. 0.5% for the TVM, at the dose rate of 13.4 Gy/s. For uniformly irradiated regular volumes, the ks value was significantly smaller, within 0.2% or 0.3% for irradiations with or without range shifter, respectively. Within measurement uncertainty, the average value of kpol , for the Markus TM23343 IC, was close to unity over the whole investigated range of clinical proton beam energies. CONCLUSION: While no polarity effect was observed for the Markus TM23343 IC in our pencil scanning proton beam system, the effect of volume recombination cannot be ignored.
Authors: Ming Yang; Xiaochun Wang; Fada Guan; Uwe Titt; Kiminori Iga; Dadi Jiang; Takeshi Takaoka; Satoshi Tootake; Tadashi Katayose; Masumi Umezawa; Emil Schüler; Steven Frank; Steven H Lin; Narayan Sahoo; Albert C Koong; Radhe Mohan; X Ronald Zhu Journal: Phys Med Biol Date: 2022-08-05 Impact factor: 4.174
Authors: Eunsin Lee; Ana Mónica Lourenço; Joseph Speth; Nigel Lee; Anna Subiel; Francesco Romano; Russell Thomas; Richard A Amos; Yongbin Zhang; Zhiyan Xiao; Anthony Mascia Journal: Med Phys Date: 2022-07-14 Impact factor: 4.506