{"created":"2023-05-15T14:38:23.130692+00:00","id":49543,"links":{},"metadata":{"_buckets":{"deposit":"799c0d01-5fd0-4a8e-b891-db6a9f0a33de"},"_deposit":{"created_by":1,"id":"49543","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"49543"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00049543","sets":["1"]},"author_link":["772906","772909","772907","772905","772908"],"item_8_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2019-01","bibliographicIssueDateType":"Issued"},"bibliographicVolumeNumber":"88","bibliographic_titles":[{"bibliographic_title":"Journal of the Physical Society of Japan"}]}]},"item_8_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"We report a Keldysh-like model for the electron transition rate in dielectrics under an intense circularly polarized laser. We assume a parabolic two-band system and the Houston function as the time-dependent wave function of the valence and conduction bands. Our formula reproduces the experimental result for the ratio of the excitation rate between linear and circular polarizations for α-quartz. This formula can be easily introduced into simulations of nanofabrication using an intense circularly polarized laser.","subitem_description_type":"Abstract"}]},"item_8_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"物理系学術誌刊行センター"}]},"item_8_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.7566/JPSJ.88.024706","subitem_relation_type_select":"DOI"}}]},"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":"乙部, 智仁"}],"nameIdentifiers":[{"nameIdentifier":"772905","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"篠原康"}],"nameIdentifiers":[{"nameIdentifier":"772906","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"佐藤駿丞"}],"nameIdentifiers":[{"nameIdentifier":"772907","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"矢花一浩"}],"nameIdentifiers":[{"nameIdentifier":"772908","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Otobe, Tomohito","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"772909","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":"Theory for Electron Excitation in Dielectrics under an Intense Linear and Circularly Polarized Laser Fields","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Theory for Electron Excitation in Dielectrics under an Intense Linear and Circularly Polarized Laser Fields"}]},"item_type_id":"8","owner":"1","path":["1"],"pubdate":{"attribute_name":"公開日","attribute_value":"2018-11-09"},"publish_date":"2018-11-09","publish_status":"0","recid":"49543","relation_version_is_last":true,"title":["Theory for Electron Excitation in Dielectrics under an Intense Linear and Circularly Polarized Laser Fields"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-16T00:25:59.906505+00:00"}