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A novel estimation method of water-equivalent thicknesses of secondary particle tracks using secondary electron bremsstrahlung emitted from therapeutic ion beams for attenuation correction
https://repo.qst.go.jp/records/49260
https://repo.qst.go.jp/records/4926072036894-a34f-4dfe-8a10-d33389750115
Item type | 学術雑誌論文 / Journal Article(1) | |||||
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公開日 | 2018-10-17 | |||||
タイトル | ||||||
タイトル | A novel estimation method of water-equivalent thicknesses of secondary particle tracks using secondary electron bremsstrahlung emitted from therapeutic ion beams for attenuation correction | |||||
言語 | ||||||
言語 | eng | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||
資源タイプ | journal article | |||||
アクセス権 | ||||||
アクセス権 | metadata only access | |||||
アクセス権URI | http://purl.org/coar/access_right/c_14cb | |||||
著者 |
Yamaguchi, Mitsutaka
× Yamaguchi, Mitsutaka× Sakai, Makoto× Nagao, Yuuto× Kikuchi, Mikiko× Arakawa, Kazuo× Kawachi, Naoki× Yamaguchi, Mitsutaka× Sakai, Makoto× Nagao, Yuuto× Kikuchi, Mikiko× Arakawa, Kazuo× Kawachi, Naoki |
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抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | Monitoring methods of therapeutic beams based on the measurement of secondary particles have been proposed and studied worldwide. Since secondary particles are influenced by substances in the human body before they reach detectors, estimation methods of the water-equivalent thickness of the tracks of the secondary particles are required for attenuation correction. In this work, we studied a novel estimation method of the water-equivalent thickness based on the observation of energy distribution of secondary electron bremsstrahlung (SEB) emitted from the trajectories of the therapeutic beams by Monte Carlo simulations. A 12C-ion beam with an energy of 290 MeV/u was injected into a water phantom. The phantom was surrounded by a collimator having a CdTe detector behind the collimator. A distribution of energy deposition due to SEB emission was recorded during beam injection. The simulation was iterated by varying the radius of the phantom. The simulation results were plotted as an R1 vs. R2 scatter plot, where R1 was defined as the ratio of the yield having a deposition energy between 30 and 40 keV to that between 20 and 30 keV, and R2 was defined as the ratio of the yield having a deposition energy between 60 and 70 keV to that between 20 and 30 keV. We found that clusters are formed at different positions on the scatter plot by different radii of the phantom and that the water-equivalent thickness of the secondary particle tracks could be estimated using the R1 vs. R2 plot. | |||||
書誌情報 |
Nuclear Instruments and Methods in Physics Research Section A 巻 954, 号 21, p. 161607-1-161607-6, 発行日 2018-11 |
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出版者 | ||||||
出版者 | Elsevier | |||||
ISSN | ||||||
収録物識別子タイプ | ISSN | |||||
収録物識別子 | 0168-9002 | |||||
DOI | ||||||
識別子タイプ | DOI | |||||
関連識別子 | 10.1016/j.nima.2018.11.066 | |||||
関連サイト | ||||||
識別子タイプ | DOI | |||||
関連識別子 | https://doi.org/10.1016/j.nima.2018.11.066 |