{"created":"2023-05-15T14:37:28.622368+00:00","id":48337,"links":{},"metadata":{"_buckets":{"deposit":"63d21066-e3f2-4e68-8d8a-b0c3e1384296"},"_deposit":{"created_by":1,"id":"48337","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"48337"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00048337","sets":["1"]},"author_link":["485826","485825","485828","485827"],"item_8_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2017-06","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"8","bibliographicPageEnd":"086011-9","bibliographicPageStart":"086011-1","bibliographicVolumeNumber":"57","bibliographic_titles":[{"bibliographic_title":"Nuclear Fusion"}]}]},"item_8_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"The hot-tail (H-T) effect in disruption of impurity injections is considered. The contribution of the H-T effect to runaway electron (RE) current, which arises from fast thermal quenching, is studied using a two-dimensional Fokker–Planck simulation. It is found that in a high-density plasma the total RE current is reduced owing to the high collisionality. We also found that if the thermal quench is fast enough to invoke the H-T effect, the effect produces more seed REs than when the H-T effect is excluded even in high-density plasmas. In the high-density region (ne ∼ 1021 m−3) with fast thermal quenching, nevertheless the increment of the seed REs due to the H-T effect is generally small (tens of milliamperes) while the increment of the total RE current reached 2 MA owing to the avalanche effect.","subitem_description_type":"Abstract"}]},"item_8_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"IOPScience"}]},"item_8_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1088/1741-4326/aa7367","subitem_relation_type_select":"DOI"}}]},"item_8_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_name":[{"subitem_relation_name_text":"http://iopscience.iop.org/article/10.1088/1741-4326/aa7367/pdf"}],"subitem_relation_type_id":{"subitem_relation_type_id_text":"http://iopscience.iop.org/article/10.1088/1741-4326/aa7367/pdf","subitem_relation_type_select":"URI"}}]},"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":"Nuga, H."}],"nameIdentifiers":[{"nameIdentifier":"485825","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Yagi, M."}],"nameIdentifiers":[{"nameIdentifier":"485826","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Fukuyama, A."}],"nameIdentifiers":[{"nameIdentifier":"485827","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"矢木 雅敏","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"485828","nameIdentifierScheme":"WEKO"}]}]},"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":"Simulations of runaway electron generation including the hot-tail effect","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Simulations of runaway electron generation including the hot-tail effect"}]},"item_type_id":"8","owner":"1","path":["1"],"pubdate":{"attribute_name":"公開日","attribute_value":"2017-09-21"},"publish_date":"2017-09-21","publish_status":"0","recid":"48337","relation_version_is_last":true,"title":["Simulations of runaway electron generation including the hot-tail effect"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T23:29:15.943599+00:00"}