{"created":"2023-05-15T14:48:38.441468+00:00","id":66636,"links":{},"metadata":{"_buckets":{"deposit":"531394a1-9454-40a6-9517-6943b2e68129"},"_deposit":{"created_by":1,"id":"66636","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"66636"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00066636","sets":["10:29"]},"author_link":["655347","655341","655345","655342","655346","655338","655343","655344","655339","655337","655340","655336"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2017-12-14","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"TOPICS, VMEC, FORTEC-3Dからなる統合フレームワークを用いてJT-60SAにおける外部印加摂動磁場が作る新古典トロイダル粘性(NTV)の評価を行う。JT-60SAでは6つの長方形誤差磁場補正コイルが上中下段にそれぞれ設置され、様々なパターンの磁場摂動スペクトルを印加できる。同じコイル電流であれば、印加パリティが異なっても同じ大きさのNTVが得られた。n=1の磁場摂動はn=3よりも大きなNTVを生じさせる。特に、n=1の共鳴磁場摂動印加はn=1の非共鳴磁場摂動印加に比べ、5倍大きな影響が出ることが分かった。","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":"閉じ込め・輸送研究会２０１７","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":"本多, 充"}],"nameIdentifiers":[{"nameIdentifier":"655336","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"佐竹, 真介"}],"nameIdentifiers":[{"nameIdentifier":"655337","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"鈴木, 康浩"}],"nameIdentifiers":[{"nameIdentifier":"655338","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"松永, 剛"}],"nameIdentifiers":[{"nameIdentifier":"655339","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"篠原, 孝司"}],"nameIdentifiers":[{"nameIdentifier":"655340","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"吉田, 麻衣子"}],"nameIdentifiers":[{"nameIdentifier":"655341","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"井手, 俊介"}],"nameIdentifiers":[{"nameIdentifier":"655342","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"本多 充","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"655343","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"松永 剛","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"655344","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"篠原 孝司","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"655345","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"吉田 麻衣子","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"655346","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"井手 俊介","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"655347","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":"Effects of the applied magnetic fields with various phasing on the neoclassical toroidal viscosity in JT-60SA","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Effects of the applied magnetic fields with various phasing on the neoclassical toroidal viscosity in JT-60SA"}]},"item_type_id":"10005","owner":"1","path":["29"],"pubdate":{"attribute_name":"公開日","attribute_value":"2018-03-08"},"publish_date":"2018-03-08","publish_status":"0","recid":"66636","relation_version_is_last":true,"title":["Effects of the applied magnetic fields with various phasing on the neoclassical toroidal viscosity in JT-60SA"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T20:46:40.971582+00:00"}