{"created":"2023-05-15T14:39:56.824692+00:00","id":54820,"links":{},"metadata":{"_buckets":{"deposit":"de3d3bbe-53c9-4425-9b71-0e70757b5f43"},"_deposit":{"created_by":1,"id":"54820","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"54820"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00054820","sets":["2"]},"author_link":["560456","560457","560458","560461","560460","560459"],"item_10003_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2017-12","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"383","bibliographicPageStart":"379","bibliographic_titles":[{"bibliographic_title":"Proceedings of the 14th Annual Meeting of Particle Accelerator Society of Japan August 1-3, 2017, Sapporo, Japan"}]}]},"item_10003_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"As a part of Engineering Validation and Engineering Design Activities (EVEDA) of the International Fusion Materials Irradiation Facility (IFMIF), a prototype accelerator to validate the key technology to realize IFMIF is under construction and testing at the International Fusion Energy Research Center (IFERC) in Rokkasho, Japan. Since April 2015, the ion source commissioning has been started and a 100 keV/144 mA/CW deuterium beam with <0.25 π mm mrad normalized emittance in rms was obtained. In order to understand and control the space charge effect in the Low Energy Beam Transport (LEBT) that deteriorates the beam emittance, we injected Kr gas into the LEBT and measured the emittance, beam current and a spatial potential. Kr gas injection reduced the beam emittance and lowered the spatial potential in the LEBT.","subitem_description_type":"Abstract"}]},"item_10003_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"日本加速器学会"}]},"item_10003_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_name":[{"subitem_relation_name_text":"http://www.pasj.jp/web_publish/pasj2017/proceedings/PDF/TUP0/TUP030.pdf"}],"subitem_relation_type_id":{"subitem_relation_type_id_text":"http://www.pasj.jp/web_publish/pasj2017/proceedings/PDF/TUP0/TUP030.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":"一宮, 亮"}],"nameIdentifiers":[{"nameIdentifier":"560456","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"杉本, 昌義"}],"nameIdentifiers":[{"nameIdentifier":"560457","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"春日井, 敦"}],"nameIdentifiers":[{"nameIdentifier":"560458","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"一宮 亮","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"560459","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"杉本 昌義","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"560460","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"春日井 敦","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"560461","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":"IFMIF/EVEDA原型加速器のLEBTにおける空間電荷効果の評価と抑制策","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"IFMIF/EVEDA原型加速器のLEBTにおける空間電荷効果の評価と抑制策"}]},"item_type_id":"10003","owner":"1","path":["2"],"pubdate":{"attribute_name":"公開日","attribute_value":"2018-01-04"},"publish_date":"2018-01-04","publish_status":"0","recid":"54820","relation_version_is_last":true,"title":["IFMIF/EVEDA原型加速器のLEBTにおける空間電荷効果の評価と抑制策"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T22:56:25.201109+00:00"}