Simulation of a High-Energy Electron Beam Transmission Through Titanium and Kapton® Thin Films

T. Malykhina, S. Karpus, O. Shopen, V. Prystupa
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引用次数: 1

Abstract

The results of computer simulation of the high-energy electrons passage through thin layers of titanium (Ti) and polyimide Kaptonâ (C22H10N2O5) in the energy range from 3 MeV to 20 MeV are presented. Simulation is carried out using the Geant4 toolkit. The number of primary electrons is 6.24×107 for each series of calculations. The thickness of the titanium foil in the model experiment is 50 µm, the thickness of the Kaptonâ film is 110 µm. The energies of primary electrons are chosen as following: 3 MeV, 5 MeV, 10 MeV, 15 MeV, and 20 MeV. The purpose of the calculations is to reveal the possibility of using the Kaptonâ film in the output devices of linear electron accelerators. It was necessary to calculate the probable values of the energy absorbed in a Kaptonâ film and in a titanium foil for each value of primary electrons energy. Another important characteristic is the divergence radius of the electron beam at a predetermined distance from the film, or the electron scattering angle. As a result of calculations, the energy spectra of bremsstrahlung gamma-quanta, formed during the passage of electrons through the materials of the films, are obtained. The most probable values of the energy absorbed in the titanium foil and in the Kaptonâ film are calculated. The scattering radii of an electron beam for the Kaptonâ film and also for the titanium foil at a distance of 20 centimeters are estimated. These calculations are performed for electron energies of 3 MeV, 5 MeV, 10 MeV, 15 MeV, and 20 MeV. A comparative analysis of the obtained results of computational experiments is carried out. It is shown that the ratio of the total amount of bremsstrahlung gamma quanta in the case of use the Kaptonâ film is approximately 0.56 of the total amount of bremsstrahlung gamma quanta when using the titanium foil. The coefficients of the ratio of the electrons scattering radius most probable value after passing through Kaptonâ to the most probable value of the scattering radius after passing through titanium are from 0.62 at electrons energy of 3 MeV to 0.57 at electrons energy of 20 MeV. The analysis of the calculated data showed that the use of Kaptonâ (C22H10N2O5) as a material for the manufacture of output devices for high-energy electron beams is more preferable in comparison to titanium films, since the use of Kaptonâ instead of titanium makes it possible to significantly reduce the background of the generated bremsstrahlung gamma quanta and reduce the scattering radius of the electron beam.
高能电子束通过钛和卡普顿薄膜传输的模拟
本文给出了高能电子在3 ~ 20 MeV能量范围内通过钛(Ti)和聚酰亚胺kapton (C22H10N2O5)薄层的计算机模拟结果。仿真是使用Geant4工具包进行的。每一组计算的初级电子数为6.24×107。模型实验中钛箔的厚度为50µm, kapton膜的厚度为110µm。一次电子的能量选择如下:3mev、5mev、10mev、15mev和20mev。计算的目的是揭示在线性电子加速器的输出装置中使用kapton薄膜的可能性。有必要计算每个初级电子能量值在kapton薄膜和钛箔中吸收的能量的可能值。另一个重要的特性是电子束在离薄膜一定距离处的发散半径,或者说是电子散射角。通过计算,得到了电子在薄膜材料中通过时形成的轫致γ -量子能谱。计算了钛箔和kapton膜吸收能量的最可能值。估计了电子束对kapton薄膜和钛箔在20厘米距离上的散射半径。这些计算是在3 MeV、5 MeV、10 MeV、15 MeV和20 MeV的电子能量下进行的。并对计算实验结果进行了对比分析。结果表明,使用kapton薄膜时的韧致γ量子总量约为使用钛箔时的韧致γ量子总量的0.56。电子通过kapton后的最可能散射半径值与通过钛后的最可能散射半径值之比的系数从电子能量为3 MeV时的0.62到电子能量为20 MeV时的0.57。对计算数据的分析表明,与钛膜相比,使用kapton (C22H10N2O5)作为制造高能电子束输出器件的材料更可取,因为使用kapton代替钛可以显著降低产生的轫致γ量子的背景,减小电子束的散射半径。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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