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dc.contributor.authorAli, Khaleden
dc.contributor.authorOhgaki, Hideakien
dc.contributor.authorZen, Heishunen
dc.contributor.authorKii, Toshiteruen
dc.contributor.authorHayakawa, Takehitoen
dc.contributor.authorShizuma, Toshiyukien
dc.contributor.authorToyokawa, Hiroyukien
dc.contributor.authorTaira, Yoshitakaen
dc.contributor.authorIancu, Violetaen
dc.contributor.authorTurturica, Gabrielen
dc.contributor.authorUr, Calin Alexandruen
dc.contributor.authorFujimoto, Masakien
dc.contributor.authorKatoh, Masahiroen
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.accessioned2020-08-24T01:01:59Z-
dc.date.available2020-08-24T01:01:59Z-
dc.date.issued2020-08-
dc.identifier.issn0018-9499-
dc.identifier.urihttp://hdl.handle.net/2433/254063-
dc.description.abstractThe 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.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherInstitute of Electrical and Electronics Engineers (IEEE)en
dc.rightsThis work is licensed under a Creative Commons Attribution 4.0 License. Formore information, see https://creativecommons.org/licenses/by/4.0/en
dc.subjectComputed tomography (CT)en
dc.subjectisotope distributionen
dc.subjectlaser Compton scattering (LCS) gamma-ray beamen
dc.subjectnuclear resonance fluorescence (NRF)en
dc.titleSelective Isotope CT Imaging Based on Nuclear Resonance Fluorescence Transmission Methoden
dc.typejournal article-
dc.type.niitypeJournal Article-
dc.identifier.jtitleIEEE Transactions on Nuclear Scienceen
dc.identifier.volume67-
dc.identifier.issue8-
dc.identifier.spage1976-
dc.identifier.epage1984-
dc.relation.doi10.1109/tns.2020.3004565-
dc.textversionpublisher-
dcterms.accessRightsopen access-
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