{"created":"2023-05-15T14:48:53.884484+00:00","id":66982,"links":{},"metadata":{"_buckets":{"deposit":"40e621e9-8312-4efe-a10f-2533d9ec253c"},"_deposit":{"created_by":1,"id":"66982","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"66982"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00066982","sets":["10:29"]},"author_link":["658399","658396","658397","658393","658395","658398","658394","658400"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2019-03-16","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Al-27は核物質の非破壊分析において、散乱強度を求める際の基準として用いるため、励起準位の共鳴幅やスピン・パリティなどの詳細な情報が必要である。そこで、米国デューク大学において、レーザーコンプトンガンマ線ビームを用いて、Al-27原子核の核共鳴蛍光散乱実験を行った。中心エネルギー3.0MeV、半値幅約4%のレーザーコンプトンガンマ線ビームを、Al-27ターゲットに照射し、散乱ターゲットからの共鳴散乱ガンマ線を6台の高純度ゲルマニウム検出器を用いて測定し、入射ガンマ線の偏光面に対する散乱ガンマ線の角度分布を測定した。その結果、励起エネルギー3.004MeV準位の共鳴幅が7meV、スピン・パリティが9/2+であることがわかった。また、殻模型を用いた理論解析を行い、3.004MeV準位の核構造について調べた。","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":"日本物理学会年会","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":"静間, 俊行"}],"nameIdentifiers":[{"nameIdentifier":"658393","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"アブデルサナド, モハマドオマルナギー"}],"nameIdentifiers":[{"nameIdentifier":"658394","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"羽島, 良一"}],"nameIdentifiers":[{"nameIdentifier":"658395","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"小泉光生"}],"nameIdentifiers":[{"nameIdentifier":"658396","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"宇都野穣"}],"nameIdentifiers":[{"nameIdentifier":"658397","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"静間 俊行","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"658398","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"アブデルサナド モハマドオマルナギー","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"658399","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"羽島 良一","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"658400","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":"レーザーコンプトンガンマ線を用いたAl-27の核共鳴蛍光散乱実験","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"レーザーコンプトンガンマ線を用いたAl-27の核共鳴蛍光散乱実験"}]},"item_type_id":"10005","owner":"1","path":["29"],"pubdate":{"attribute_name":"公開日","attribute_value":"2018-11-19"},"publish_date":"2018-11-19","publish_status":"0","recid":"66982","relation_version_is_last":true,"title":["レーザーコンプトンガンマ線を用いたAl-27の核共鳴蛍光散乱実験"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T20:42:48.242745+00:00"}