{"created":"2023-06-20T15:16:17.653031+00:00","id":9991,"links":{},"metadata":{"_buckets":{"deposit":"3394c975-c7ba-4c1f-b472-b899aa61e540"},"_deposit":{"created_by":3,"id":"9991","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"9991"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:00009991","sets":["8:32"]},"author_link":["61910","61911","61909","61912"],"item_5_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"1995-05-01","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":"\"By modeling the typical orbital deviation and the deposition profile of tangentially injected neutral beams, the heating efficiency is derived in heliotron/ torsatrons.  It is found that the changes of the configuration due to the finite beta effects alter the NBI heating efficiency largely and that the magnetic well or hill condition, which is important for the  MHD stabilities, is also an important factor to determine the heating efficiency in a weak magnetic field.  By combining the energy confinement scaling law the reachable beta value is evaluated and it is found that there is the optimum value of the magnetic field strength to obtain the high plasma beta in point of view of the NBI heating efficiency.\"","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-354"}]},"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":"\"Murakami,  S.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Nakajima,  N.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Okamura,  S.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Okamoto,  M.\"","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"plasma beta","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"heliotron/ torsatron","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"neutral beam injection heating","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"beam orbit loss","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"heating efficiency","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"high beta experiments","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"the Compact Helical System","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":"Orbital Aspects of Reachable beta  Value in NBI Heated Heliotron/Torsatrons","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Orbital Aspects of Reachable beta  Value in NBI Heated Heliotron/Torsatrons","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":"9991","relation_version_is_last":true,"title":["Orbital Aspects of Reachable beta  Value in NBI Heated Heliotron/Torsatrons"],"weko_creator_id":"3","weko_shared_id":-1},"updated":"2023-06-20T20:54:51.171689+00:00"}