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dc.contributor.authorKii, T.en
dc.contributor.authorOmer, M.en
dc.contributor.authorNegm, H.en
dc.contributor.authorChoi, Y. W.en
dc.contributor.authorKinjo, R.en
dc.contributor.authorYoshida, K.en
dc.contributor.authorKonstantin, T.en
dc.contributor.authorKimura, N.en
dc.contributor.authorIshida, K.en
dc.contributor.authorImon, H.en
dc.contributor.authorShibata, M.en
dc.contributor.authorShimahashi, K.en
dc.contributor.authorKomai, T.en
dc.contributor.authorOkumura, K.en
dc.contributor.authorZen, H.en
dc.contributor.authorMasuda, K.en
dc.contributor.authorHori, T.en
dc.contributor.authorOhgaki, H.en
dc.contributor.alternative紀井, 俊輝ja
dc.contributor.alternative金城, 良太ja
dc.contributor.alternative吉田, 恭平ja
dc.contributor.alternative木村, 尚樹ja
dc.contributor.alternative石田, 啓一ja
dc.contributor.alternative井門, 秀和ja
dc.contributor.alternative柴田, 茉莉江ja
dc.contributor.alternative島橋, 享兵ja
dc.contributor.alternative駒井, 琢也ja
dc.contributor.alternative奥村, 健祐ja
dc.contributor.alternative全, 炳俊ja
dc.contributor.alternative増田, 開ja
dc.contributor.alternative堀, 利匡ja
dc.contributor.alternative大垣, 英明ja
dc.date.accessioned2023-09-20T00:24:14Z-
dc.date.available2023-09-20T00:24:14Z-
dc.date.issued2013-
dc.identifier.urihttp://hdl.handle.net/2433/285188-
dc.description11th International Conference on Synchrotron Radiation Instrumentation (SRI 2012)en
dc.description.abstractA monochromatic gamma ray beam is attractive for isotope-specific material/medical imaging or non-destructive inspection. A laser Compton scattering (LCS) gamma ray source which is based on the backward Compton scattering of laser light on high-energy electrons can generate energy variable quasi-monochromatic gamma ray. Due to the principle of the LCS gamma ray, the direction of the gamma beam is limited to the direction of the high-energy electrons. Then the target object is placed on the beam axis, and is usually moved if spatial scanning is required. In this work, we proposed an electron beam transport system consisting of four bending magnets which can stick the collision point and control the electron beam direction, and a laser system consisting of a spheroidal mirror and a parabolic mirror which can also stick the collision point. Then the collision point can be placed on one focus of the spheroid. Thus gamma ray direction and collision angle between the electron beam and the laser beam can be easily controlled. As the results, travelling direction of the LCS gamma ray can be controlled under the limitation of the beam transport system, energy of the gamma ray can be controlled by controlling incident angle of the colliding beams, and energy spread can be controlled by changing the divergence of the laser beam.en
dc.language.isoeng-
dc.publisherIOP Publishingen
dc.rightsPublished under licence by IOP Publishing Ltden
dc.titleDesign Study for Direction Variable Compton Scattering Gamma Rayen
dc.typeconference paper-
dc.type.niitypeConference Paper-
dc.identifier.jtitleJournal of Physics: Conference Seriesen
dc.identifier.volume425-
dc.relation.doi10.1088/1742-6596/425/19/192020-
dc.textversionpublisher-
dc.identifier.artnum192020-
dcterms.accessRightsopen access-
dc.identifier.pissn1742-6588-
dc.identifier.eissn1742-6596-
出現コレクション:学術雑誌掲載論文等

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