{"created":"2023-06-20T15:16:11.917138+00:00","id":9892,"links":{},"metadata":{"_buckets":{"deposit":"6895d792-4285-47b4-ba48-68cb6e9a856a"},"_deposit":{"created_by":3,"id":"9892","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"9892"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:00009892","sets":["8:32"]},"author_link":["60631","60632","60630"],"item_5_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"1993-03-01","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":"\"It is demonstrated by three-dimensional simulations for resistive magnetohydrodynamic (MHD) plasmas with both \"\"spatially nonuniform resistivity eta\"\" and \"\"uniform eta\"\" that the attractor of the dissipative structure in the resistive MHD plasmas is given by nabla x (eta j) = (alpha/2)B which is derived from a novel self-organization theory based on the minimum dissipation late profile. It is shown by the simulations that the attractor is reduced to nabla x B = lambda B in the special case with the \"\"uniform eta\"\" and no pressure gradient.\"","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-212"}]},"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":"\"Kondoh,  Y.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Hosaka,  Y.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Liang,  J.-L.\"","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"self-organization","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"eigenfunction","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"dissipative dynamics operator","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"attractor","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"dissipative structure","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"3-D MHD simulation","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":"Demonstration for Novel Self-organization Theory by Three-Dimensional Magnetohydrodynamic Simulation","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Demonstration for Novel Self-organization Theory by Three-Dimensional Magnetohydrodynamic Simulation","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":"9892","relation_version_is_last":true,"title":["Demonstration for Novel Self-organization Theory by Three-Dimensional Magnetohydrodynamic Simulation"],"weko_creator_id":"3","weko_shared_id":-1},"updated":"2023-06-20T20:55:50.700851+00:00"}