{"created":"2023-05-15T12:17:03.246541+00:00","id":643,"links":{},"metadata":{"_buckets":{"deposit":"baad8a7a-9ab6-4c46-a702-0c5008419afd"},"_deposit":{"created_by":3,"id":"643","owners":[3],"pid":{"revision_id":0,"type":"depid","value":"643"},"status":"published"},"_oai":{"id":"oai:tuis.repo.nii.ac.jp:00000643","sets":["1:4:200:201"]},"author_link":["2865","2872","2866","2873"],"control_number":"643","item_8_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2021-12-10","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"1","bibliographicPageEnd":"20","bibliographicPageStart":"11","bibliographicVolumeNumber":"25","bibliographic_titles":[{"bibliographic_title":"東京情報大学研究論集","bibliographic_titleLang":"ja"}]}]},"item_8_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"ノード破壊によってネットワークが分断され，多くのノードが通信できなくなった時の破壊割合をパーコレーション閾値と呼ぶ．Cohenらによるパーコレーション理論閾値，そして本研究で提案する破壊後のネットワークのリンク数から導かれる理論閾値の両方をノード破壊シミュレーションの値と比較を行った．その結果，スケールフリーネットワーク以外で両理論値とネットワークの広さ（直径）のピーク位置をパーコレーション閾値とした値が一致した．しかし，スケールフリーネットワークの一種であるバラバシアルバートモデルでは値が一致しないため，理論の修正が必要である．","subitem_description_type":"Other"}]},"item_8_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"東京情報大学","subitem_publisher_language":"ja"}]},"item_creator":{"attribute_name":"著者","attribute_type":"creator","attribute_value_mlt":[{"creatorNames":[{"creatorName":"河野, 涼太郎","creatorNameLang":"ja"},{"creatorName":"コウノ, リョウタロウ","creatorNameLang":"ja-Kana"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"森口, 一郎","creatorNameLang":"ja"},{"creatorName":"モリグチ, イチロウ","creatorNameLang":"ja-Kana"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Kouno, Ryoutarou","creatorNameLang":"en"}],"nameIdentifiers":[{}]},{"creatorNames":[{"creatorName":"Moriguchi, Ichirou","creatorNameLang":"en"}],"nameIdentifiers":[{}]}]},"item_files":{"attribute_name":"ファイル情報","attribute_type":"file","attribute_value_mlt":[{"accessrole":"open_date","date":[{"dateType":"Available","dateValue":"2021-12-13"}],"displaytype":"detail","filename":"r25-1-m2.pdf","filesize":[{"value":"8.7 MB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"r25-1-m2.pdf","url":"https://tuis.repo.nii.ac.jp/record/643/files/r25-1-m2.pdf"},"version_id":"09c8714b-0cb6-4285-8f01-cc2d60d496a7"}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"ネットワーク破壊","subitem_subject_language":"ja","subitem_subject_scheme":"Other"},{"subitem_subject":"Molloy-Reed criterion","subitem_subject_language":"ja","subitem_subject_scheme":"Other"},{"subitem_subject":"パーコレーション閾値","subitem_subject_language":"ja","subitem_subject_scheme":"Other"},{"subitem_subject":"ネットワーク直径","subitem_subject_language":"ja","subitem_subject_scheme":"Other"},{"subitem_subject":"Network breakdown","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"Molloy-Reed criterion","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"Percolation threshold","subitem_subject_language":"en","subitem_subject_scheme":"Other"},{"subitem_subject":"Network diameter","subitem_subject_language":"en","subitem_subject_scheme":"Other"}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"jpn"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"other","resourceuri":"http://purl.org/coar/resource_type/c_1843"}]},"item_title":"ネットワークのパーコレーション閾値","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"ネットワークのパーコレーション閾値","subitem_title_language":"ja"},{"subitem_title":"Percolation Thresholds of Networks","subitem_title_language":"en"}]},"item_type_id":"8","owner":"3","path":["201"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2021-12-13"},"publish_date":"2021-12-13","publish_status":"0","recid":"643","relation_version_is_last":true,"title":["ネットワークのパーコレーション閾値"],"weko_creator_id":"3","weko_shared_id":-1},"updated":"2023-12-21T02:06:31.561410+00:00"}