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Photon beam softening coefficients evaluation for a 6 MeV photon beam for an aluminum slab: Monte Carlo study using BEAMnrc Code,DOSXYZnrc Code,and BEAMDP code
Authors:Mohamed Bencheikh  Abdelmajid Maghnouj  Jaouad Tajmouati
Affiliation:1.LISTA Laboratory, Physics Department, Faculty of Sciences Dhar El-Mahraz,University of Sidi Mohamed Ben Abdellah,Fez,Morocco
Abstract:Determination and understanding the photon beam attenuation by the photon beam modifier and the radiation beam softening for clinical use is more important part of material study for the beam modifier enhancements and the linac improvements. A Monte Carlo model was used to simulate 6 MeV photon beams from a Varian Clinac 2100 accelerator with the flattening filter and the later was replaced by the aluminum slab with variable thickness. The Monte Carlo geometry was validated by a gamma index acceptance rate of 99% in PDD and 98% in dose profiles, the gamma criteria was 3% for dose difference and 3 mm for distance to agreement. The purpose was to investigate aluminum material attenuation and beam softening coefficients as a function of the inserted aluminum slab thickness and of off-axis distance. The attenuation and beam softening coefficients were not identical for the same off-axis distance and they varied as a function of aluminum slab thickness. The results of our study were shown that the beam softening coefficients were varied with thickness beam modifier material used for beam softening and the off-axis distance inside the irradiation field. Thereafter, the softening coefficient a 1 have a maximum of 2.5 × 10–1 cm–1 for the aluminum slab thickness of 1 mm, 1.4 × 10–1 cm–1 for the aluminum slab thickness of 1.5 mm and 4.47 × 10–2 cm–1 for the aluminum slab thickness of 2 mm. The maximum of the second softening coefficient a 2 was 1.02 × 10–2 cm–2 for the aluminum slab thickness of 1 mm, was 1.92 × 10–2 cm–2 for the aluminum slab thickness of 1.5 mm and was 1.93 × 10–2 cm–2 for the aluminum slab thickness of 2 mm. Our study can be a basic investigation of photon beam softening material that will be used in the future linac configuration and also in the photon beam modifiers.
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