{"created":"2023-05-15T14:48:06.918005+00:00","id":65941,"links":{},"metadata":{"_buckets":{"deposit":"675d8749-3f6a-4738-a2e2-134a9bba1838"},"_deposit":{"created_by":1,"id":"65941","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"65941"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00065941","sets":["10:29"]},"author_link":["649529","649532","649527","649530","649528","649525","649531","649533","649526"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2016-08-09","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"三次元同位体分布計測の基礎研究を行う目的で、分子研UVSOR-IIIにおいて、蓄積リングを周回する高エネルギー電子と大強度レーザーとを用いたレーザー逆コンプトン散乱ガンマ線のビームラインを建設している。レーザーには1.94μmのファイバーレーザーと、UVSORの定常運転モードである750MeV、300mAの電子ビームを用いて、最大エネルギー5.4MeV、コリメータ無しでのガンマ線収量1x10^7photons/sを得ている。このガンマ線を用いて手始めに2次元の同位体分布をNRFの吸収法を用いて2次元CT画像の取得を試みた。CT用のサンプルターゲットには鉛、アルミニウム、ステンレススチールのロッドを５ｘ５のマトリックスに組み、これを透過してくるガンマ線を鉛ブロックのWitness Targetにて光核共鳴散乱（NRF）を起こさせて208-Pbの同定を行った。本会ではビームラインの概要と諸元について報告をおこなうとともに、NRF-CT画像取得結果について報告を行う。","subitem_description_type":"Abstract"}]},"item_10005_description_6":{"attribute_name":"会議概要（会議名, 開催地, 会期, 主催者等）","attribute_value_mlt":[{"subitem_description":"第１３回日本加速器学会年会","subitem_description_type":"Other"}]},"item_access_right":{"attribute_name":"アクセス権","attribute_value_mlt":[{"subitem_access_right":"metadata only access","subitem_access_right_uri":"http://purl.org/coar/access_right/c_14cb"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"大垣英明"}],"nameIdentifiers":[{"nameIdentifier":"649525","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"大東出"}],"nameIdentifiers":[{"nameIdentifier":"649526","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"豊川弘之"}],"nameIdentifiers":[{"nameIdentifier":"649527","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"早川, 岳人"}],"nameIdentifiers":[{"nameIdentifier":"649528","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"静間, 俊行"}],"nameIdentifiers":[{"nameIdentifier":"649529","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"加藤政博"}],"nameIdentifiers":[{"nameIdentifier":"649530","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"山崎潤一郎"}],"nameIdentifiers":[{"nameIdentifier":"649531","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"早川 岳人","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"649532","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"静間 俊行","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"649533","nameIdentifierScheme":"WEKO"}]}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"jpn"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"conference object","resourceuri":"http://purl.org/coar/resource_type/c_c94f"}]},"item_title":"UVSOR-IIIにおける逆コンプトン散乱ビームライン開発とNRF-CTへの応用","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"UVSOR-IIIにおける逆コンプトン散乱ビームライン開発とNRF-CTへの応用"}]},"item_type_id":"10005","owner":"1","path":["29"],"pubdate":{"attribute_name":"公開日","attribute_value":"2016-08-17"},"publish_date":"2016-08-17","publish_status":"0","recid":"65941","relation_version_is_last":true,"title":["UVSOR-IIIにおける逆コンプトン散乱ビームライン開発とNRF-CTへの応用"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T20:54:35.696005+00:00"}