Estimation of photoneutron yield in linear accelerator with different collimation systems by Geant4 and MCNPX simulation codes

被引:10
|
作者
Kim, Yoon Sang [1 ]
Khazaei, Zeinab [2 ]
Ko, Junho [1 ]
Afarideh, Hossein [2 ]
Ghergherehchi, Mitra [3 ]
机构
[1] Korea Univ Technol & Educ, Dept Comp Sci & Engn, Cheonan, England
[2] Amirkabir Univ Technol, Dept Energy Engn & Phys, Tehran, Iran
[3] Sungkyunkwan Univ, Sch Elect & Elect Engn, Coll Informat & Commun Engn, Suwon, South Korea
来源
PHYSICS IN MEDICINE AND BIOLOGY | 2016年 / 61卷 / 07期
关键词
Monte Carlo simulation code; linear accelerator; collimator; photoneutron convertor; neutron yield; MONTE-CARLO-SIMULATION; NEUTRON; TARGETS; SPECTRA; BERYLLIUM; TUNGSTEN; COPPER;
D O I
10.1088/0031-9155/61/7/2762
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
At present, the bremsstrahlung photon beams produced by linear accelerators are the most commonly employed method of radiotherapy for tumor treatments. A photoneutron source based on three different energies (6, 10 and 15 MeV) of a linac electron beam was designed by means of Geant4 and Monte Carlo N-Particle eXtended (MCNPX) simulation codes. To obtain maximum neutron yield, two arrangements for the photo neutron convertor were studied: (a) without a collimator, and (b) placement of the convertor after the collimator. The maximum photon intensities in tungsten were 0.73, 1.24 and 2.07 photon/e at 6, 10 and 15 MeV, respectively. There was no considerable increase in the photon fluence spectra from 6 to 15 MeV at the optimum thickness between 0.8 mm and 2 mm of tungsten. The optimum dimensions of the collimator were determined to be a length of 140 mm with an aperture of 5 mm x 70 mm for iron in a slit shape. According to the neutron yield, the best thickness obtained for the studied materials was 30 mm. The number of neutrons generated in BeO achieved the maximum value at 6 MeV, unlike that in Be, where the highest number of neutrons was observed at 15 MeV. Statistical uncertainty in all simulations was less than 0.3% and 0.05% for MCNPX and the standard electromagnetic (EM) physics packages of Geant4, respectively. Differences among spectra in various regions are due to various cross-section and stopping power data and different simulations of the physics processes.
引用
收藏
页码:2762 / 2779
页数:18
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