{"created":"2023-05-15T10:00:58.535738+00:00","id":5455,"links":{},"metadata":{"_buckets":{"deposit":"7b67d64a-55b2-451a-b9c1-64adb296fec1"},"_deposit":{"created_by":5,"id":"5455","owner":"5","owners":[5],"pid":{"revision_id":0,"type":"depid","value":"5455"},"status":"published"},"_oai":{"id":"oai:miyazaki-u.repo.nii.ac.jp:00005455","sets":["73","73:27"]},"author_link":["21431","29304","13413","29301"],"item_10001_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"1998-08","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"606","bibliographicPageStart":"595","bibliographicVolumeNumber":"1","bibliographic_titles":[{"bibliographic_title":"応用力学論文集"}]}]},"item_10001_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"In this paper, the motions for the small earthquakes are produced by a stochastic point source model with ω^-2 property. By summing the simulated motions and making use of the scaling relations between large and small earthquakes, the ground motions from an extended rupture too large to be treated as a point source model are simulated. To show a verification of the proposed method, the simulated ground motions are compared with the recorded ground motions.","subitem_description_type":"Abstract"}]},"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":[{"creatorAffiliations":[{"affiliationNameIdentifiers":[{"affiliationNameIdentifier":"","affiliationNameIdentifierScheme":"ISNI","affiliationNameIdentifierURI":"http://www.isni.org/isni/"}],"affiliationNames":[{"affiliationName":"","affiliationNameLang":"ja"}]}],"creatorNames":[{"creatorName":"大角, 恒雄","creatorNameLang":"ja"},{"creatorName":"オオスミ, ツネオ","creatorNameLang":"ja-Kana"},{"creatorName":"Ohsumi, Tsuneo","creatorNameLang":"en"}],"familyNames":[{"familyName":"大角","familyNameLang":"ja"},{"familyName":"オオスミ","familyNameLang":"ja-Kana"},{"familyName":"Ohsumi","familyNameLang":"en"}],"givenNames":[{"givenName":"恒雄","givenNameLang":"ja"},{"givenName":"ツネオ","givenNameLang":"ja-Kana"},{"givenName":"Tsuneo","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"21431","nameIdentifierScheme":"WEKO"}]},{"creatorAffiliations":[{"affiliationNameIdentifiers":[{"affiliationNameIdentifier":"","affiliationNameIdentifierScheme":"ISNI","affiliationNameIdentifierURI":"http://www.isni.org/isni/"}],"affiliationNames":[{"affiliationName":"","affiliationNameLang":"ja"}]}],"creatorNames":[{"creatorName":"Harada, Takanori","creatorNameLang":"en"},{"creatorName":"原田, 隆典","creatorNameLang":"ja"},{"creatorName":"ハラダ, タカノリ","creatorNameLang":"ja-Kana"}],"familyNames":[{"familyName":"Harada","familyNameLang":"en"},{"familyName":"原田","familyNameLang":"ja"},{"familyName":"ハラダ","familyNameLang":"ja-Kana"}],"givenNames":[{"givenName":"Takanori","givenNameLang":"en"},{"givenName":"隆典","givenNameLang":"ja"},{"givenName":"タカノリ","givenNameLang":"ja-Kana"}],"nameIdentifiers":[{"nameIdentifier":"13413","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"泉谷, 恭男"},{"creatorName":"イズタニ, ヤスオ","creatorNameLang":"ja-Kana"}],"nameIdentifiers":[{"nameIdentifier":"29301","nameIdentifierScheme":"WEKO"}]},{"creatorAffiliations":[{"affiliationNameIdentifiers":[{"affiliationNameIdentifier":"","affiliationNameIdentifierScheme":"ISNI","affiliationNameIdentifierURI":"http://www.isni.org/isni/"}],"affiliationNames":[{"affiliationName":"","affiliationNameLang":"ja"}]}],"creatorNames":[{"creatorName":"大角, 恒雄","creatorNameLang":"ja"},{"creatorName":"オオスミ, ツネオ","creatorNameLang":"ja-Kana"},{"creatorName":"Ohsumi, Tsuneo","creatorNameLang":"en"}],"familyNames":[{"familyName":"大角","familyNameLang":"ja"},{"familyName":"オオスミ","familyNameLang":"ja-Kana"},{"familyName":"Ohsumi","familyNameLang":"en"}],"givenNames":[{"givenName":"恒雄","givenNameLang":"ja"},{"givenName":"ツネオ","givenNameLang":"ja-Kana"},{"givenName":"Tsuneo","givenNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"21431","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Izutani, Yasuo","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"29304","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":"2020-06-21"}],"displaytype":"detail","filename":"digital_1998_harada.pdf","filesize":[{"value":"8.9 MB"}],"format":"application/pdf","licensetype":"license_note","mimetype":"application/pdf","url":{"label":"本文","url":"https://miyazaki-u.repo.nii.ac.jp/record/5455/files/digital_1998_harada.pdf"},"version_id":"759a2bc5-dad6-4c8e-b297-6cba6172fa79"}]},"item_keyword":{"attribute_name":"キーワード","attribute_value_mlt":[{"subitem_subject":"synthesis, trong ground motions, empirical Green's function, stochastic Green's function, earthquake source spectrum","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":"journal article","resourceuri":"http://purl.org/coar/resource_type/c_6501"}]},"item_title":"確率論的グリーン関数を用いた強震動の波形合成法とその検証例による震源パラメータの考察","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"確率論的グリーン関数を用いた強震動の波形合成法とその検証例による震源パラメータの考察","subitem_title_language":"ja"},{"subitem_title":"Digital Simulation of Ground Motions using Stochastic Green's Function and Consideration on Its Model Parameters","subitem_title_language":"en"}]},"item_type_id":"10001","owner":"5","path":["73","27"],"pubdate":{"attribute_name":"PubDate","attribute_value":"2020-06-21"},"publish_date":"2020-06-21","publish_status":"0","recid":"5455","relation_version_is_last":true,"title":["確率論的グリーン関数を用いた強震動の波形合成法とその検証例による震源パラメータの考察"],"weko_creator_id":"5","weko_shared_id":2},"updated":"2023-10-23T02:02:23.991839+00:00"}