{"created":"2023-05-15T14:40:00.094467+00:00","id":54894,"links":{},"metadata":{"_buckets":{"deposit":"21b4aa46-d6ab-4169-abe6-bada9760fb8c"},"_deposit":{"created_by":1,"id":"54894","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"54894"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00054894","sets":["2"]},"author_link":["561349","561353","561354","561350","561351","561352","561348"],"item_10003_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2017-01","bibliographicIssueDateType":"Issued"},"bibliographic_titles":[{"bibliographic_title":"Proceedings of M&C 2017, Korean Nuclear Society"}]}]},"item_10003_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"We introduce a benchmark of an electromagnetic gyrokinetic model, dFEFI. dFEFI solves the gyrokinetic equation, closing the system with the Poisson and induction equations. We here present a comparison of linear properties with those done by GS2. We examine the nonlinear turbulence with different box-sizes of Ly/Lx. For the lower Ly/Lx cases, the turbulence exhibits so bursty that higher standard deviation is estimated. The probability distribution function (PDF) analysis indicates that the bursty behavior can be related to the electron heat transport. ","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.kns.org/files/int_paper/paper/MC2017_2017_11/P382S11-01MikiK.pdf"}],"subitem_relation_type_id":{"subitem_relation_type_id_text":"https://www.kns.org/files/int_paper/paper/MC2017_2017_11/P382S11-01MikiK.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":"三木, 一弘"}],"nameIdentifiers":[{"nameIdentifier":"561348","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Miyato, Naoaki"}],"nameIdentifiers":[{"nameIdentifier":"561349","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Scott, Bruce"}],"nameIdentifiers":[{"nameIdentifier":"561350","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Yagi, Masatoshi"}],"nameIdentifiers":[{"nameIdentifier":"561351","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"三木 一弘","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"561352","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"宮戸 直亮","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"561353","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"矢木 雅敏","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"561354","nameIdentifierScheme":"WEKO"}]}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"eng"}]},"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":"Benchmark of an electromagnetic gyrokinetic simulation code","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Benchmark of an electromagnetic gyrokinetic simulation code"}]},"item_type_id":"10003","owner":"1","path":["2"],"pubdate":{"attribute_name":"公開日","attribute_value":"2018-04-27"},"publish_date":"2018-04-27","publish_status":"0","recid":"54894","relation_version_is_last":true,"title":["Benchmark of an electromagnetic gyrokinetic simulation code"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T22:55:33.987627+00:00"}