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Simulation of a high-energy electron beam transmission through titanium and Kapton\(^\circledR\) thin films
The results of computer simulation of the high-energy electrons passage through thin layers of titanium (Ti) and polyimide Kapton\(^\circledR\) in the energy range from 3 to 20 MeV are presented. Simulation is carried out using the Geant4 toolkit. The thickness of the Ti foil in the model experiment...
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description | The results of computer simulation of the high-energy electrons passage through thin layers of titanium (Ti) and polyimide Kapton\(^\circledR\) in the energy range from 3 to 20 MeV are presented. Simulation is carried out using the Geant4 toolkit. The thickness of the Ti foil in the model experiment is 50 microns, the thickness of the Kapton\(^\circledR\) film is 110 microns. The purpose of the calculations is to reveal the possibility of using the Kapton\(^\circledR\) film in the output devices of linear electron accelerators. It was necessary to calculate the probable values of the energy absorbed in a Kapton\(^\circledR\) film and in a Ti 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 Ti foil and in the Kapton\(^\circledR\) film are calculated. The scattering radii of an electron beam for the Kapton\(^\circledR\) film and also for the Ti foil at a distance of 20 cm are estimated. It is shown that the ratio of the total amount of bremsstrahlung gamma quanta in the case of use the Kapton\(^\circledR\) film is approximately 0.56 of the total amount of bremsstrahlung gamma quanta when using the Ti foil. The analysis of the calculated data showed that the use of Kapton\(^\circledR\) as a material for the manufacture of output devices for high-energy electron beams is more preferable in comparison to Ti films. The use of Kapton\(^\circledR\) instead of Ti makes it possible to significantly reduce the background of the generated bremsstrahlung gamma quanta and reduce the scattering radius of the electron beam. |
doi_str_mv | 10.48550/arxiv.2112.07487 |
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Simulation is carried out using the Geant4 toolkit. The thickness of the Ti foil in the model experiment is 50 microns, the thickness of the Kapton\(^\circledR\) film is 110 microns. The purpose of the calculations is to reveal the possibility of using the Kapton\(^\circledR\) film in the output devices of linear electron accelerators. It was necessary to calculate the probable values of the energy absorbed in a Kapton\(^\circledR\) film and in a Ti 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 Ti foil and in the Kapton\(^\circledR\) film are calculated. The scattering radii of an electron beam for the Kapton\(^\circledR\) film and also for the Ti foil at a distance of 20 cm are estimated. It is shown that the ratio of the total amount of bremsstrahlung gamma quanta in the case of use the Kapton\(^\circledR\) film is approximately 0.56 of the total amount of bremsstrahlung gamma quanta when using the Ti foil. The analysis of the calculated data showed that the use of Kapton\(^\circledR\) as a material for the manufacture of output devices for high-energy electron beams is more preferable in comparison to Ti films. The use of Kapton\(^\circledR\) instead of Ti makes it possible to significantly reduce the background of the generated bremsstrahlung gamma quanta and reduce the scattering radius of the electron beam.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2112.07487</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Bremsstrahlung ; Computer simulation ; Electron accelerators ; Electron beams ; Energy ; Energy spectra ; High energy electrons ; Kapton (trademark) ; Metal foils ; Polyimide resins ; Scattering angle ; Simulation ; Thickness ; Thin films ; Titanium</subject><ispartof>arXiv.org, 2021-12</ispartof><rights>2021. This work is published under http://creativecommons.org/licenses/by-nc-nd/4.0/ (the “License”). 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Simulation is carried out using the Geant4 toolkit. The thickness of the Ti foil in the model experiment is 50 microns, the thickness of the Kapton\(^\circledR\) film is 110 microns. The purpose of the calculations is to reveal the possibility of using the Kapton\(^\circledR\) film in the output devices of linear electron accelerators. It was necessary to calculate the probable values of the energy absorbed in a Kapton\(^\circledR\) film and in a Ti 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 Ti foil and in the Kapton\(^\circledR\) film are calculated. The scattering radii of an electron beam for the Kapton\(^\circledR\) film and also for the Ti foil at a distance of 20 cm are estimated. It is shown that the ratio of the total amount of bremsstrahlung gamma quanta in the case of use the Kapton\(^\circledR\) film is approximately 0.56 of the total amount of bremsstrahlung gamma quanta when using the Ti foil. The analysis of the calculated data showed that the use of Kapton\(^\circledR\) as a material for the manufacture of output devices for high-energy electron beams is more preferable in comparison to Ti films. 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Simulation is carried out using the Geant4 toolkit. The thickness of the Ti foil in the model experiment is 50 microns, the thickness of the Kapton\(^\circledR\) film is 110 microns. The purpose of the calculations is to reveal the possibility of using the Kapton\(^\circledR\) film in the output devices of linear electron accelerators. It was necessary to calculate the probable values of the energy absorbed in a Kapton\(^\circledR\) film and in a Ti 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 Ti foil and in the Kapton\(^\circledR\) film are calculated. The scattering radii of an electron beam for the Kapton\(^\circledR\) film and also for the Ti foil at a distance of 20 cm are estimated. It is shown that the ratio of the total amount of bremsstrahlung gamma quanta in the case of use the Kapton\(^\circledR\) film is approximately 0.56 of the total amount of bremsstrahlung gamma quanta when using the Ti foil. The analysis of the calculated data showed that the use of Kapton\(^\circledR\) as a material for the manufacture of output devices for high-energy electron beams is more preferable in comparison to Ti films. The use of Kapton\(^\circledR\) instead of Ti makes it possible to significantly reduce the background of the generated bremsstrahlung gamma quanta and reduce the scattering radius of the electron beam.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2112.07487</doi><oa>free_for_read</oa></addata></record> |
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subjects | Bremsstrahlung Computer simulation Electron accelerators Electron beams Energy Energy spectra High energy electrons Kapton (trademark) Metal foils Polyimide resins Scattering angle Simulation Thickness Thin films Titanium |
title | Simulation of a high-energy electron beam transmission through titanium and Kapton\(^\circledR\) thin films |
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