{"created":"2023-05-15T14:56:34.068878+00:00","id":76773,"links":{},"metadata":{"_buckets":{"deposit":"00cc34b6-bd2c-4ab0-9fcc-825c0f968aeb"},"_deposit":{"created_by":1,"id":"76773","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"76773"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00076773","sets":["1"]},"author_link":["784993","784988","784992","784989","784990","784991"],"item_8_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2019-05","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"5","bibliographicPageStart":"052507","bibliographicVolumeNumber":"26","bibliographic_titles":[{"bibliographic_title":"Physics of Plasmas"}]}]},"item_8_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"An interplay between fluctuation driven toroidal axisymmetric flows (convective cell modes) and resistive ballooning mode turbulence after the pedestal collapse is numerically studied by a four-field reduced MHD model in the BOUT++ framework. The strong flow shear suppresses the radial transport of pressure filaments, and the pressure profile in the pedestal region is partially recovered. As a result, a secondary instability is quasilinearly excited, which yields a secondary collapse. The subsequent damped oscillation is also analyzed by phase diagram\nanalysis.","subitem_description_type":"Abstract"}]},"item_8_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"The American Institute of Physics"}]},"item_8_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1063/1.5086998","subitem_relation_type_select":"DOI"}}]},"item_8_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"https://aip.scitation.org/doi/10.1063/1.5086998","subitem_relation_type_select":"URI"}}]},"item_8_source_id_9":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"1070-664X","subitem_source_identifier_type":"ISSN"}]},"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":"Seto, Haruki"}],"nameIdentifiers":[{"nameIdentifier":"784988","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Xu, X.Q."}],"nameIdentifiers":[{"nameIdentifier":"784989","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Dudson, B.D."}],"nameIdentifiers":[{"nameIdentifier":"784990","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Yagi, Masatoshi"}],"nameIdentifiers":[{"nameIdentifier":"784991","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Seto, Haruki","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"784992","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Yagi, Masatoshi","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"784993","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":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"Interplay between fluctuation driven toroidal axisymmetric flows and resistive ballooning mode turbulence","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Interplay between fluctuation driven toroidal axisymmetric flows and resistive ballooning mode turbulence"}]},"item_type_id":"8","owner":"1","path":["1"],"pubdate":{"attribute_name":"公開日","attribute_value":"2019-09-13"},"publish_date":"2019-09-13","publish_status":"0","recid":"76773","relation_version_is_last":true,"title":["Interplay between fluctuation driven toroidal axisymmetric flows and resistive ballooning mode turbulence"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-16T00:10:50.042252+00:00"}