TY - GEN
T1 - Head scatter factor calculation considering characteristics of scattered photon
AU - Miyashita, Hisayuki
AU - Hatanaka, Shogo
AU - Fujita, Yukio
AU - Myojyoyama, Atsushi
AU - Saitoh, Hidetoshi
N1 - Copyright:
Copyright 2021 Elsevier B.V., All rights reserved.
PY - 2009
Y1 - 2009
N2 - The head scatter factor Sh is one of the important parameters for MU calculation. It is defined as a ratio of absorbed dose of arbitrary field to that of reference field. The Sh can be determined by using two physical quantities. One is energy fluence of primary photons generated from target and scattered photons from several components of treatment head. Another is backscattered radiation from collimator jaws into monitor chamber. In this study, to determine Sh for intricate field shaped with MLC, primary and scattered photons from several head components were simulated using Monte Carlo method and output variation caused by backscattered radiation into monitor chamber was measured using a miniphantom. In the simulation, geometry and materials of head component were precisely coded on the BEAMnrc, and the particles from the head components and incident into isocenter region were sampled into the phase space files. The emit positions of scattered photons at the base of flattening filter were analyzed by using information of the phase space file and the energy fluence distribution of scattered photons as a function of radius at base of flattening filter was obtained. The Sh was determined by integration of the energy fluence distribution within range defined by the field shape and contribution of backscatter into monitor chamber. The calculated Sh agreed with the measured one within 0.3 %.
AB - The head scatter factor Sh is one of the important parameters for MU calculation. It is defined as a ratio of absorbed dose of arbitrary field to that of reference field. The Sh can be determined by using two physical quantities. One is energy fluence of primary photons generated from target and scattered photons from several components of treatment head. Another is backscattered radiation from collimator jaws into monitor chamber. In this study, to determine Sh for intricate field shaped with MLC, primary and scattered photons from several head components were simulated using Monte Carlo method and output variation caused by backscattered radiation into monitor chamber was measured using a miniphantom. In the simulation, geometry and materials of head component were precisely coded on the BEAMnrc, and the particles from the head components and incident into isocenter region were sampled into the phase space files. The emit positions of scattered photons at the base of flattening filter were analyzed by using information of the phase space file and the energy fluence distribution of scattered photons as a function of radius at base of flattening filter was obtained. The Sh was determined by integration of the energy fluence distribution within range defined by the field shape and contribution of backscatter into monitor chamber. The calculated Sh agreed with the measured one within 0.3 %.
KW - Backscattered radiation
KW - Head scatter factor
KW - Monte Carlo method energy fluence
KW - Scattered photons
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U2 - 10.1007/978-3-642-03474-9_197
DO - 10.1007/978-3-642-03474-9_197
M3 - Conference contribution
AN - SCOPUS:77950456312
SN - 9783642034725
T3 - IFMBE Proceedings
SP - 700
EP - 703
BT - World Congress on Medical Physics and Biomedical Engineering
PB - Springer Verlag
T2 - World Congress on Medical Physics and Biomedical Engineering: Radiation Oncology
Y2 - 7 September 2009 through 12 September 2009
ER -