{"created":"2023-06-20T15:15:52.980256+00:00","id":9517,"links":{},"metadata":{"_buckets":{"deposit":"2bd7885a-9f12-40c1-8141-f57d510082ca"},"_deposit":{"created_by":3,"id":"9517","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"9517"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:00009517","sets":["8:32"]},"author_link":["67900","67899"],"item_5_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"1997-09-01","bibliographicIssueDateType":"Issued"},"bibliographic_titles":[{},{"bibliographic_title":"Research Report NIFS-Series","bibliographic_titleLang":"en"}]}]},"item_5_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Self-organization and generation of large shear flow component in turbulent resistive interchange convection in magnetized plasma is considered. The effect of plasma density-electrostatic potential coupling via the inertialess electron dynamics along the magnetic field is shown to play significant role in the onset of shear component. The results of large-scale numerical simulation and low-dimensional (reduced) model are presented and compared.","subitem_description_type":"Abstract"}]},"item_5_source_id_10":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"0915-633X","subitem_source_identifier_type":"ISSN"}]},"item_5_text_8":{"attribute_name":"報告書番号","attribute_value_mlt":[{"subitem_text_value":"NIFS-505"}]},"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":"Bazdenkov,  S.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Sato,  T.","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"plasma transport","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"turbulent convection","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"Edge Localized Modes","subitem_subject_language":"en","subitem_subject_scheme":"Other"}]},"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":"research report","resourceuri":"http://purl.org/coar/resource_type/c_18ws"}]},"item_title":"Low-Dimensional Model of Resistive Interchange Convection in Magnetized Plasmas","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Low-Dimensional Model of Resistive Interchange Convection in Magnetized Plasmas","subitem_title_language":"en"}]},"item_type_id":"5","owner":"3","path":["32"],"pubdate":{"attribute_name":"公開日","attribute_value":"2010-02-05"},"publish_date":"2010-02-05","publish_status":"0","recid":"9517","relation_version_is_last":true,"title":["Low-Dimensional Model of Resistive Interchange Convection in Magnetized Plasmas"],"weko_creator_id":"3","weko_shared_id":-1},"updated":"2023-06-20T20:47:03.925440+00:00"}