Chegeni Nahid, Pur Saleh Boveiry, Razmjoo Sasan, Hoseini Seydeh Khadijed
Ph.D. of Medical Physics, Assistant Professor, Department of Medical Physics, Faculty of Medicine, Ahvaz Jundishapur University of Medical Sciences: Ahvaz, Iran.
M.Sc. of Medical Physics, Department of Medical Physics, Faculty of Medicine, Ahvaz Jundishapur University of Medical Sciences: Ahvaz, Iran.
Electron Physician. 2017 Jun 25;9(6):4590-4596. doi: 10.19082/4590. eCollection 2017 Jun.
Today, electron accelerators are taken into consideration as photoneutron sources. Therefore, for maximum production of epithermal neutron flux, designing a photoneutron target is of significant importance. In this paper, the effect of thickness and geometric shape of a photoneutron target on neutron output were investigated.
In this study, a pencil photon source with 13, 15, 18, 20 and 25 MeV energies and a diameter of 2 mm was investigated using Monte Carlo simulation method using MCNP code. To optimize the design of the photoneutron target, the tungsten target with various geometries and thicknesses was investigated.
The maximum neutron flux produced for all target geometries and thicknesses occurred at neutron energy peak of around 0.46 MeV. As the thickness increased to 2 cm, neutron flux increased and then a decreasing trend was observed. For various geometrical shapes, the determining factor in photoneutron output was the effective target thickness in the photon interaction path that increased by the increase in the area of interaction. Another factor was the angle of the photon's incidence with the target surface that resulted in a significant decrease in photoneutron output in cone-shaped targets.
Three factors including the total neutron flux, neutrons energy spectrum, and convergence of neutrons plays an important role in the selection of geometry and shape of the target that should be investigated considering beam shaping assembly (BSA) shape.
如今,电子加速器被视为光中子源。因此,为了最大程度地产生超热中子通量,设计一个光中子靶具有重要意义。本文研究了光中子靶的厚度和几何形状对中子输出的影响。
在本研究中,使用MCNP代码通过蒙特卡罗模拟方法研究了能量为13、15、18、20和25 MeV且直径为2 mm的笔形光子源。为了优化光中子靶的设计,研究了具有各种几何形状和厚度的钨靶。
所有靶几何形状和厚度产生的最大中子通量出现在约0.46 MeV的中子能量峰值处。随着厚度增加到2 cm,中子通量增加,然后观察到下降趋势。对于各种几何形状,光中子输出的决定因素是光子相互作用路径中的有效靶厚度,其随着相互作用面积的增加而增加。另一个因素是光子与靶表面的入射角,这导致锥形靶中的光中子输出显著降低。
包括总中子通量、中子能谱和中子会聚在内的三个因素在靶的几何形状和形状选择中起着重要作用,应结合束流整形组件(BSA)的形状进行研究。