{"created":"2023-05-15T14:53:43.678472+00:00","id":73164,"links":{},"metadata":{"_buckets":{"deposit":"05e0eced-8a89-4561-82a1-0d565ded7ab9"},"_deposit":{"created_by":1,"id":"73164","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"73164"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00073164","sets":["10:28"]},"author_link":["721017","721015","721016","721027","721021","721013","721025","721030","721018","721019","721026","721023","721014","721029","721028","721020","721024","721022"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2019-03-27","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"The fully non-inductive sustainment (Vloop~0) of high normalized beta (βN) plasmas is a crucial challenge for the steady-state operation of a tokamak reactor. Steady-state regimes have been explored at TCV during the 2017/18 EUROfusion MST1 campaign. The operating space has been extended towards plasmas closer to those expected in JT-60SA and ITER, i.e. with significant Neutral Beam Injection (NBI) and Electron Cyclotron Resonance Heating and Current Drive (ECRH/CD), bootstrap current and fast ion fraction. βN values up to 1.4 and 1.7 have been obtained in lower single null L-mode (H98(y,2) ∼ 0.8) and H-mode (H98(y,2) ∼ 1) plasmas, respectively, at zero time averaged loop voltage and q95 ∼ 6.","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":"10th IAEA Technical Meeting on the Steady State Operation of Magnetic Fusion Devices","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":"Piron, C."}],"nameIdentifiers":[{"nameIdentifier":"721013","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Garcia, J."}],"nameIdentifiers":[{"nameIdentifier":"721014","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Goodman, T."}],"nameIdentifiers":[{"nameIdentifier":"721015","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Agostini, M."}],"nameIdentifiers":[{"nameIdentifier":"721016","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Fontana, M."}],"nameIdentifiers":[{"nameIdentifier":"721017","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Giruzzi, G."}],"nameIdentifiers":[{"nameIdentifier":"721018","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Gobbin, M."}],"nameIdentifiers":[{"nameIdentifier":"721019","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Karpushov, A."}],"nameIdentifiers":[{"nameIdentifier":"721020","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Kong, M."}],"nameIdentifiers":[{"nameIdentifier":"721021","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Merle, A."}],"nameIdentifiers":[{"nameIdentifier":"721022","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Morales, J."}],"nameIdentifiers":[{"nameIdentifier":"721023","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Nowak, S."}],"nameIdentifiers":[{"nameIdentifier":"721024","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Pigatto, L."}],"nameIdentifiers":[{"nameIdentifier":"721025","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sauter, O."}],"nameIdentifiers":[{"nameIdentifier":"721026","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Testa, D."}],"nameIdentifiers":[{"nameIdentifier":"721027","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"M.Vallar"}],"nameIdentifiers":[{"nameIdentifier":"721028","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Yoshida, M."}],"nameIdentifiers":[{"nameIdentifier":"721029","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"吉田 麻衣子","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"721030","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":"Extension of the operating space of steady state regimes on TCV","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Extension of the operating space of steady state regimes on TCV"}]},"item_type_id":"10005","owner":"1","path":["28"],"pubdate":{"attribute_name":"公開日","attribute_value":"2019-01-26"},"publish_date":"2019-01-26","publish_status":"0","recid":"73164","relation_version_is_last":true,"title":["Extension of the operating space of steady state regimes on TCV"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T19:32:14.546967+00:00"}