{"created":"2023-09-21T01:16:56.442446+00:00","id":2000045,"links":{},"metadata":{"_buckets":{"deposit":"e626b406-8f27-4bc3-8de9-5c92381b0eb4"},"_deposit":{"created_by":20,"id":"2000045","owner":"20","owners":[20],"pid":{"revision_id":0,"type":"depid","value":"2000045"},"status":"published"},"_oai":{"id":"oai:nifs-repository.repo.nii.ac.jp:02000045","sets":["6:7"]},"author_link":["127205","66665","66603","66524","66751","66755","66754","126267","127345"],"item_10001_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2023-09-06","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"9","bibliographicPageStart":"095105","bibliographicVolumeNumber":"13","bibliographic_titles":[{"bibliographic_title":"AIP Advances","bibliographic_titleLang":"en"}]}]},"item_10001_description_4":{"attribute_name":"著者ID","attribute_value_mlt":[{"subitem_description":"ORCID 0000-0002-4501-1956","subitem_description_type":"Other"}]},"item_10001_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"In magnetically confined fusion plasmas, a gyrotron is an essential auxiliary heating device for generating and sustaining plasma through electron cyclotron resonance heating owing to its ability to generate high-power microwaves. Microwaves emitted from a gyrotron are often transmitted through waveguides, and the transmitted power is monitored by a power monitor with a multi-hole directional coupler at the miter bend of the transmission line. Recently, a high-power dual-frequency gyrotron has been installed and operated in the Large Helical Device. A power monitor with good sensitivity to multiple frequencies is required to monitor the power transmission of the different frequencies at the same transmission line. In order to realize the power monitor, which can couple with the multiple-frequency microwaves, we focused on a sub-waveguide shape in the power monitor and investigated the influence of the tapered sub-waveguide by conducting electromagnetic simulations using a simple model. We also performed the high-power test using a power monitor with a tapered sub-waveguide. The experimental result was different from the simulation, but enough receiving power was obtained at both 116 and 154 GHz.","subitem_description_language":"en","subitem_description_type":"Abstract"}]},"item_10001_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"American Institute of Physics","subitem_publisher_language":"en"}]},"item_10001_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type":"isIdenticalTo","subitem_relation_type_id":{"subitem_relation_type_id_text":"https://doi.org/10.1063/5.0159136","subitem_relation_type_select":"DOI"}}]},"item_10001_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_name":[{"subitem_relation_name_text":"Publisher version"}],"subitem_relation_type_id":{"subitem_relation_type_id_text":"https://doi.org/10.1063/5.0159136","subitem_relation_type_select":"DOI"}}]},"item_10001_rights_15":{"attribute_name":"権利","attribute_value_mlt":[{"subitem_rights":"This article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. This article appeared in AIP Advances 13, 095105 (2023) and may be found at https://doi.org/10.1063/5.0159136","subitem_rights_language":"en"}]},"item_10001_source_id_9":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"2158-3226","subitem_source_identifier_type":"ISSN"}]},"item_10001_text_23":{"attribute_name":"NAIS","attribute_value_mlt":[{"subitem_text_value":"13940"}]},"item_10001_version_type_20":{"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":"YANAI, Ryoma","creatorNameLang":"en"},{"creatorName":"YANAI, Ryohma","creatorNameLang":"en"}],"familyNames":[{"familyName":"YANAI","familyNameLang":"en"},{"familyName":"YANAI","familyNameLang":"en"}],"givenNames":[{"givenName":"Ryoma","givenNameLang":"en"},{"givenName":"Ryohma","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"127205","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"TAKEUCHI, T.","creatorNameLang":"en"}],"familyNames":[{"familyName":"TAKEUCHI","familyNameLang":"en"}],"givenNames":[{"givenName":"T.","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"66665","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"MIZUNO, Yoshinori","creatorNameLang":"en"}],"familyNames":[{"familyName":"MIZUNO","familyNameLang":"en"}],"givenNames":[{"givenName":"Yoshinori","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"66603","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"YOSHIMURA, Yasuo","creatorNameLang":"en"}],"familyNames":[{"familyName":"YOSHIMURA","familyNameLang":"en"}],"givenNames":[{"givenName":"Yasuo","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"66524","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"NISHIURA, Masaki","creatorNameLang":"en"}],"familyNames":[{"familyName":"NISHIURA","familyNameLang":"en"}],"givenNames":[{"givenName":"Masaki","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"66751","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"IGAMI, Hiroe","creatorNameLang":"en"}],"familyNames":[{"familyName":"IGAMI","familyNameLang":"en"}],"givenNames":[{"givenName":"Hiroe","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"66755","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"TAKAHASHI, Hiromi","creatorNameLang":"en"}],"familyNames":[{"familyName":"TAKAHASHI","familyNameLang":"en"}],"givenNames":[{"givenName":"Hiromi","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"66754","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"TSUJIMIRA, Toru","creatorNameLang":"ja"},{"creatorName":"TSUJIMURA, Toru Ii","creatorNameLang":"ja-Kana"}],"familyNames":[{"familyName":"TSUJIMIRA","familyNameLang":"ja"},{"familyName":"TSUJIMURA","familyNameLang":"ja-Kana"}],"givenNames":[{"givenName":"Toru","givenNameLang":"ja"},{"givenName":"Toru Ii","givenNameLang":"ja-Kana"}],"nameIdentifiers":[{"nameIdentifier":"126267","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"KENMOCHI, Naoki","creatorNameLang":"en"}],"familyNames":[{"familyName":"KENMOCHI","familyNameLang":"en"}],"givenNames":[{"givenName":"Naoki","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"127345","nameIdentifierScheme":"WEKO"}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_access","date":[{"dateType":"Available","dateValue":"2023-09-21"}],"filename":"13940_AIP.Adv.pdf","filesize":[{"value":"4.2 MB"}],"format":"application/pdf","licensetype":"license_0","url":{"url":"https://nifs-repository.repo.nii.ac.jp/record/2000045/files/13940_AIP.Adv.pdf"},"version_id":"9bed1132-6458-4706-a062-647aea2b2527"}]},"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":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"Multi-hole coupling power monitor with tapered sub-waveguide for dual-frequency high-power gyrotron","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Multi-hole coupling power monitor with tapered sub-waveguide for dual-frequency high-power gyrotron","subitem_title_language":"en"}]},"item_type_id":"10001","owner":"20","path":["7"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2023-09-21"},"publish_date":"2023-09-21","publish_status":"0","recid":"2000045","relation_version_is_last":true,"title":["Multi-hole coupling power monitor with tapered sub-waveguide for dual-frequency high-power gyrotron"],"weko_creator_id":"20","weko_shared_id":-1},"updated":"2023-09-21T02:31:33.662286+00:00"}