{"created":"2023-05-15T14:52:50.774818+00:00","id":72152,"links":{},"metadata":{"_buckets":{"deposit":"d669de4e-260b-4055-9e16-c2fb486db489"},"_deposit":{"created_by":1,"id":"72152","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"72152"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00072152","sets":["10:28"]},"author_link":["710441","710437","710436","710439","710440","710442","710438"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2017-01-26","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"絶縁体キャピラリーに入射したイオンビームがその電荷やエネルギーを維持したまま集束または偏向して出射するガイド効果の存在を調べるため、4 MeVのC+及びC4+を一対の凹凸ガラス円筒面の隙間（ガラス円筒面間チャネル）に入射し、入口を支点としてビームと垂直な軸周りでチルト回転（回転角θ）したときの出射粒子のエネルギーを測定した。その結果、幾何学的にはビームがガラス円筒面間チャネルを通過できないθ= ±2.5º以上チルトさせても、出射した粒子のエネルギー分布は入射時のそれをほぼ維持していることが分かり、ガラス円筒面間チャネルによる高速イオンのガイド効果が確認された。","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":"第１回QST高崎研シンポジウム","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":"本橋, 健次"}],"nameIdentifiers":[{"nameIdentifier":"710436","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"齋藤, 勇一"}],"nameIdentifiers":[{"nameIdentifier":"710437","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"宮脇, 信正"}],"nameIdentifiers":[{"nameIdentifier":"710438","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"鳴海, 一雅"}],"nameIdentifiers":[{"nameIdentifier":"710439","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"齋藤 勇一","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710440","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"宮脇 信正","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710441","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"鳴海 一雅","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710442","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":"ガラス円筒面間チャネルでガイドされた4 MeV-Cq+イオン(q = 1, 4)のエネルギー分布","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"ガラス円筒面間チャネルでガイドされた4 MeV-Cq+イオン(q = 1, 4)のエネルギー分布"}]},"item_type_id":"10005","owner":"1","path":["28"],"pubdate":{"attribute_name":"公開日","attribute_value":"2017-02-03"},"publish_date":"2017-02-03","publish_status":"0","recid":"72152","relation_version_is_last":true,"title":["ガラス円筒面間チャネルでガイドされた4 MeV-Cq+イオン(q = 1, 4)のエネルギー分布"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T19:43:10.778842+00:00"}