{"created":"2023-05-15T14:40:02.832317+00:00","id":54955,"links":{},"metadata":{"_buckets":{"deposit":"f701dadb-46d3-488d-81f3-a44942273d18"},"_deposit":{"created_by":1,"id":"54955","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"54955"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00054955","sets":["2"]},"author_link":["561961","561962","561965","561958","561959","561963","561964","561960","561966"],"item_10003_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2019-01","bibliographicIssueDateType":"Issued"},"bibliographic_titles":[{"bibliographic_title":"第15回日本加速器学会年会論文集"}]}]},"item_10003_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"In order to improve optical functions and emittance compensation conditions for space charge dominated electron\nbeam in the compact ERL at the KEK, we introduced a new 3D model of a 2-cell injector superconducting cavity instead\nof a cylindrical 2D model. The 3D model includes input and HOM couplers. By using the 3D model, we improved\nthe optical functions from the injector to the main superconducting linac. Because of the improvement of the optical\nfunctions, emittance growth at both the injector and the recirculation sections decreased for the bunch charge of 40 pC.","subitem_description_type":"Abstract"}]},"item_10003_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_name":[{"subitem_relation_name_text":"https://www.pasj.jp/web_publish/pasj2018/proceedings/PDF/WEP0/WEP032.pdf"}],"subitem_relation_type_id":{"subitem_relation_type_id_text":"https://www.pasj.jp/web_publish/pasj2018/proceedings/PDF/WEP0/WEP032.pdf","subitem_relation_type_select":"URI"}}]},"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":"宮島司"}],"nameIdentifiers":[{"nameIdentifier":"561958","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"布袋貴大"}],"nameIdentifiers":[{"nameIdentifier":"561959","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"本田洋介"}],"nameIdentifiers":[{"nameIdentifier":"561960","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"島田美帆"}],"nameIdentifiers":[{"nameIdentifier":"561961","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"高井良太"}],"nameIdentifiers":[{"nameIdentifier":"561962","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"帯名崇"}],"nameIdentifiers":[{"nameIdentifier":"561963","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"加藤龍好"}],"nameIdentifiers":[{"nameIdentifier":"561964","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"永井, 良治"}],"nameIdentifiers":[{"nameIdentifier":"561965","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"永井 良治","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"561966","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 paper","resourceuri":"http://purl.org/coar/resource_type/c_5794"}]},"item_title":"cERLにおける空間電荷効果が支配的な電子ビームの光学関数とエミッタンス補償条件の改善","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"cERLにおける空間電荷効果が支配的な電子ビームの光学関数とエミッタンス補償条件の改善"}]},"item_type_id":"10003","owner":"1","path":["2"],"pubdate":{"attribute_name":"公開日","attribute_value":"2019-01-10"},"publish_date":"2019-01-10","publish_status":"0","recid":"54955","relation_version_is_last":true,"title":["cERLにおける空間電荷効果が支配的な電子ビームの光学関数とエミッタンス補償条件の改善"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T22:54:59.718531+00:00"}