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dc.contributor.author | Ali, Khaled | en |
dc.contributor.author | Ohgaki, Hideaki | en |
dc.contributor.author | Zen, Heishun | en |
dc.contributor.author | Kii, Toshiteru | en |
dc.contributor.author | Hayakawa, Takehito | en |
dc.contributor.author | Shizuma, Toshiyuki | en |
dc.contributor.author | Toyokawa, Hiroyuki | en |
dc.contributor.author | Taira, Yoshitaka | en |
dc.contributor.author | Iancu, Violeta | en |
dc.contributor.author | Turturica, Gabriel | en |
dc.contributor.author | Ur, Calin Alexandru | en |
dc.contributor.author | Fujimoto, Masaki | en |
dc.contributor.author | Katoh, Masahiro | en |
dc.contributor.alternative | 大垣, 英明 | ja |
dc.contributor.alternative | 全, 炳俊 | ja |
dc.contributor.alternative | 紀井, 俊輝 | ja |
dc.contributor.alternative | 早川, 岳人 | ja |
dc.contributor.alternative | 静間, 俊行 | ja |
dc.contributor.alternative | 豊川, 弘之 | ja |
dc.contributor.alternative | 平, 義隆 | ja |
dc.contributor.alternative | 藤本, 將輝 | ja |
dc.contributor.alternative | 加藤, 政博 | ja |
dc.date.accessioned | 2020-08-24T01:01:59Z | - |
dc.date.available | 2020-08-24T01:01:59Z | - |
dc.date.issued | 2020-08 | - |
dc.identifier.issn | 0018-9499 | - |
dc.identifier.uri | http://hdl.handle.net/2433/254063 | - |
dc.description.abstract | The isotope selectivity of computed tomography (CT) imaging based on nuclear resonance fluorescence (NRF) transmission method using a quasi-monochromatic laser Compton scattering (LCS) gamma-ray beam in the MeV region was demonstrated at the Ultra Violet Synchrotron Orbital Radiation–III (UVSOR-III) Synchrotron Radiation Facility (Institute of Molecular Science, National Institute of Natural Science) for two enriched lead isotope rods ( 206 Pb and 208 Pb) implanted in an aluminum cylinder. Since these two rods show the same gamma-ray attenuation in atomic processes, it is impossible to differentiate between them using a standard Gamma-CT technique based on atomic attenuation of gamma rays. The LCS gamma-ray beam had a maximum energy of 5.528 MeV and an intensity of approximately 5.5 photons/s/eV at the resonance energy ( Jπ=1− at 5.512 MeV in 208 Pb). A lead collimator with a hole diameter of 1 mm was used to define the size of the LCS gamma-ray beam at the CT target. The CT image of the 208 Pb rod was selectively obtained with a 2-mm pixel size resolution, which was determined by the horizontal step size of the CT stage. | en |
dc.format.mimetype | application/pdf | - |
dc.language.iso | eng | - |
dc.publisher | Institute of Electrical and Electronics Engineers (IEEE) | en |
dc.rights | This work is licensed under a Creative Commons Attribution 4.0 License. Formore information, see https://creativecommons.org/licenses/by/4.0/ | en |
dc.subject | Computed tomography (CT) | en |
dc.subject | isotope distribution | en |
dc.subject | laser Compton scattering (LCS) gamma-ray beam | en |
dc.subject | nuclear resonance fluorescence (NRF) | en |
dc.title | Selective Isotope CT Imaging Based on Nuclear Resonance Fluorescence Transmission Method | en |
dc.type | journal article | - |
dc.type.niitype | Journal Article | - |
dc.identifier.jtitle | IEEE Transactions on Nuclear Science | en |
dc.identifier.volume | 67 | - |
dc.identifier.issue | 8 | - |
dc.identifier.spage | 1976 | - |
dc.identifier.epage | 1984 | - |
dc.relation.doi | 10.1109/tns.2020.3004565 | - |
dc.textversion | publisher | - |
dcterms.accessRights | open access | - |
出現コレクション: | 学術雑誌掲載論文等 |

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