{"created":"2023-05-15T11:43:18.892081+00:00","id":2978,"links":{},"metadata":{"_buckets":{"deposit":"961079de-2b67-414c-8beb-dd0b4f0f07e4"},"_deposit":{"created_by":1,"id":"2978","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"2978"},"status":"published"},"_oai":{"id":"oai:kanagawa-u.repo.nii.ac.jp:00002978","sets":["237:238:239"]},"author_link":["6131","6133","6132","6134","6135"],"item_9_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2007-11-15","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"36","bibliographicPageStart":"33","bibliographic_titles":[{"bibliographic_title":"Microwave Conference, 2007. KJMW 2007. Korea-Japan"}]}]},"item_9_description_4":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Exact propagation eigenmode for stripline with finite thickness is important for practical design of MIC.\nSo far propagation eigenmode for stripline with zero thickness is given exactly by conformal transformation method, but not for that with finite thickness. In order to treat this problem analytically, lateral equivaSlent network in general is derived and applied to obtain equivalent network of stripline structure along horizontal or vertical direction. Equivalent network for two direction are dirrerent, but gives same propagation eigenmode, which demonstrate the usefulness of the derivered lateral equivalent network.","subitem_description_type":"Abstract"}]},"item_9_description_42":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"subitem_description":"Article","subitem_description_type":"Other"}]},"item_9_publisher_35":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"IEEE"}]},"item_9_relation_11":{"attribute_name":"ISBN","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"978-1-4244-1556-4","subitem_relation_type_select":"ISBN"}}]},"item_9_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type":"isIdenticalTo","subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1109/KJMW.2007.4402233","subitem_relation_type_select":"DOI"}}]},"item_9_version_type_18":{"attribute_name":"著者版フラグ","attribute_value_mlt":[{"subitem_version_resource":"http://purl.org/coar/version/c_970fb48d4fbd8a85","subitem_version_type":"VoR"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"Ding, Kai"}],"nameIdentifiers":[{"nameIdentifier":"6131","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"平岡, 隆晴"}],"nameIdentifiers":[{"nameIdentifier":"6132","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Hiraoka, Takaharu"}],"nameIdentifiers":[{"nameIdentifier":"6133","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"許, 瑞邦"}],"nameIdentifiers":[{"nameIdentifier":"6134","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Hsu, Jui-Pang"}],"nameIdentifiers":[{"nameIdentifier":"6135","nameIdentifierScheme":"WEKO"}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2018-11-16"}],"displaytype":"detail","filename":"75 Calculation of Propagation.pdf","filesize":[{"value":"4.2 MB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"75 Calculation of Propagation.pdf","url":"https://kanagawa-u.repo.nii.ac.jp/record/2978/files/75 Calculation of Propagation.pdf"},"version_id":"c31614f8-c92f-4a7a-ac39-aad41cd1fcc0"}]},"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 paper","resourceuri":"http://purl.org/coar/resource_type/c_5794"}]},"item_title":"Calculation of Propagation Eigenmode for Stripline with Finite Thickness based on Equivalent Network along Horizontal or Vertical Direction","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Calculation of Propagation Eigenmode for Stripline with Finite Thickness based on Equivalent Network along Horizontal or Vertical Direction"}]},"item_type_id":"9","owner":"1","path":["239"],"pubdate":{"attribute_name":"公開日","attribute_value":"2011-02-08"},"publish_date":"2011-02-08","publish_status":"0","recid":"2978","relation_version_is_last":true,"title":["Calculation of Propagation Eigenmode for Stripline with Finite Thickness based on Equivalent Network along Horizontal or Vertical Direction"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T16:34:27.611715+00:00"}