{"created":"2023-06-20T15:16:18.484231+00:00","id":10009,"links":{},"metadata":{"_buckets":{"deposit":"546643a7-13ac-4127-83df-945fb194d14d"},"_deposit":{"created_by":3,"id":"10009","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"10009"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:00010009","sets":["8:32"]},"author_link":["62318","62319","62320","62317"],"item_5_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2000-07-01","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 both experimentally and theoretically demonstrated that ion flow velocity at an arbitrary angle with respect to the magnetic field can be measured with a directional Langmuir probe. Based on the symmetry argument, we show that the effect of magnetic field on directional probe current is exactly canceled in determining the ion flow velocity, and obtain the generalized relation between flow velocity and directional probe currents valid for any flowing direction. The absolute value of the flow velocity is determined by an textit{in situ} calibration method of the probe. The applicability limit of the present method to a strongly ion-magnetized plasma is experimentally examined.\"","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-638"}]},"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":"\"Nagaoka,  K.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Okamoto,  A.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Yoshimura,  S.","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Tanaka,  M.Y.\"","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"plasma flow","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"directional Langmuir probe","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"Mach probe","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"magnetic field effect","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"calibration method","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"E x B drift","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":"Plasma Flow Measurement Using Directional Langmuir Probe under Weakly Ion-Magnetized Conditions","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Plasma Flow Measurement Using Directional Langmuir Probe under Weakly Ion-Magnetized Conditions","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":"10009","relation_version_is_last":true,"title":["Plasma Flow Measurement Using Directional Langmuir Probe under Weakly Ion-Magnetized Conditions"],"weko_creator_id":"3","weko_shared_id":-1},"updated":"2023-06-20T20:54:35.881425+00:00"}