{"created":"2023-05-15T14:52:51.737316+00:00","id":72174,"links":{},"metadata":{"_buckets":{"deposit":"fd5edc98-dbb7-4574-ac77-145f7764c77a"},"_deposit":{"created_by":1,"id":"72174","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"72174"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00072174","sets":["10:28"]},"author_link":["710686","710681","710672","710695","710690","710676","710671","710674","710688","710687","710692","710682","710677","710691","710678","710696","710679","710685","710689","710680","710693","710694","710675","710697","710684","710683","710673"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2016-10-18","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"MHD　stability　and　its　active　control　of　reference　JT-60SA　scenarios　is　numerically　studied　with particular attention to high β N　plasmas. The qualification of high performance tokamak scenarios is one of the main missions of the JT-60SA device, both in support to ITER and in view of the definition of an optimized DEMO　design.　Neoclassical　Tearing　Modes　and　Resistive　Wall　Modes　will　be　probably　among　the　most challenging　MHD　instabilities　to　be　overcome　in　order　to　reach　this　final　goal.　In　the　framework　of　the European-Japanese　collaboration　on　JT-60SA　preparation,　the　main　effort　presented　in　this　paper　is　the development　and　application　of　some　of　the　main　European　MHD　codes　to　JT-60SA　specific　issues.　The implementation　of　these　numerical　tools　is　described,　taking　into　account　a　careful　description　of　the　main sources of instability and including the possibility of their active control. Two plasmas, representative in one case of the full current, Single Null, inductive reference scenario (Scenario2, according to the JT-60SA Research Plan definition) and in the second case of the high β N , fully non inductive reference scenario (Scenario 5), are taken as inputs. For the Scenario 2-like plasma, Neoclassical Tearing Modes are studied as most relevant MHD instabilities　and　the　active　stabilization　of　(2,1)　mode　provided　by　electron　cyclotron　waves　is　numerically investigated. Resistive Wall Modes are instead considered as the most challenging limiting MHD instability in the Scenario 5-like case and the development of a fully 3D model including closed loop active control by a set of active coils is presented.","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":"26th IAEA Fusion Energy ","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":"Bolzonella, T."}],"nameIdentifiers":[{"nameIdentifier":"710671","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Bettini, P."}],"nameIdentifiers":[{"nameIdentifier":"710672","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"L., Figini"}],"nameIdentifiers":[{"nameIdentifier":"710673","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Guo, S.C."}],"nameIdentifiers":[{"nameIdentifier":"710674","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Liu, Y.Q."}],"nameIdentifiers":[{"nameIdentifier":"710675","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Marchiori, G."}],"nameIdentifiers":[{"nameIdentifier":"710676","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Matsunaga, Go"}],"nameIdentifiers":[{"nameIdentifier":"710677","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Mastrostefano, S."}],"nameIdentifiers":[{"nameIdentifier":"710678","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"S., Nowak"}],"nameIdentifiers":[{"nameIdentifier":"710679","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"L., Pigatto"}],"nameIdentifiers":[{"nameIdentifier":"710680","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sauter O."}],"nameIdentifiers":[{"nameIdentifier":"710681","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Takechi, Manabu"}],"nameIdentifiers":[{"nameIdentifier":"710682","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"F., Villone"}],"nameIdentifiers":[{"nameIdentifier":"710683","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"X., Xu"}],"nameIdentifiers":[{"nameIdentifier":"710684","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Aiba, Nobuyuki"}],"nameIdentifiers":[{"nameIdentifier":"710685","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"J., Garcia"}],"nameIdentifiers":[{"nameIdentifier":"710686","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"L., Garzotti"}],"nameIdentifiers":[{"nameIdentifier":"710687","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Hayashi, Nobuhiko"}],"nameIdentifiers":[{"nameIdentifier":"710688","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Ph., Lauber"}],"nameIdentifiers":[{"nameIdentifier":"710689","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"M., Romanelli"}],"nameIdentifiers":[{"nameIdentifier":"710690","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Shiraishi, Junya"}],"nameIdentifiers":[{"nameIdentifier":"710691","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sozzi, C."}],"nameIdentifiers":[{"nameIdentifier":"710692","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"松永 剛","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710693","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"武智 学","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710694","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"相羽 信行","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710695","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"林 伸彦","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710696","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"白石 淳也","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"710697","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 object","resourceuri":"http://purl.org/coar/resource_type/c_c94f"}]},"item_title":"Securing High βN JT-60SA Operational Space by MHD Stability and Active Control Modelling","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Securing High βN JT-60SA Operational Space by MHD Stability and Active Control Modelling"}]},"item_type_id":"10005","owner":"1","path":["28"],"pubdate":{"attribute_name":"公開日","attribute_value":"2017-03-10"},"publish_date":"2017-03-10","publish_status":"0","recid":"72174","relation_version_is_last":true,"title":["Securing High βN JT-60SA Operational Space by MHD Stability and Active Control Modelling"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T19:42:55.006904+00:00"}