{"created":"2023-05-15T15:01:29.370790+00:00","id":83411,"links":{},"metadata":{"_buckets":{"deposit":"ed3e47fc-c1fa-49c7-8ca8-2e4da3ebc841"},"_deposit":{"created_by":1,"id":"83411","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"83411"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00083411","sets":["1"]},"author_link":["1064476","1064478","1064480","1064481","1064479","1064477"],"item_8_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2021-09","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"9","bibliographicPageStart":"094419","bibliographicVolumeNumber":"104","bibliographic_titles":[{"bibliographic_title":"Physical Review B"}]}]},"item_8_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"We propose sum rules of x-ray magnetic circularly polarized emission (XMCPE) at L edges for 3d transition metals. By making use of combinations of incident and emitted photon helicities, z-component expectation values of spin, orbital, magnetic dipole, and quadrupole terms can be obtained separately. The fundamental difference in the sum rules between x-ray magnetic circular dichroism and XMCPE arises from the variety of electron transitions involving core states split by the spin-orbit interaction. The additional electron transition in XMCPE causes complicated angular dependence of the sum rule relation for the spin moment. Our findings promote future L-edge XMCPE measurements, which have not been observed at present","subitem_description_type":"Abstract"}]},"item_8_publisher_8":{"attribute_name":"出版者","attribute_value_mlt":[{"subitem_publisher":"アメリカ物理学会"}]},"item_8_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1103/PhysRevB.104.094419","subitem_relation_type_select":"DOI"}}]},"item_8_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"https://journals.aps.org/prb/abstract/10.1103/PhysRevB.104.094419","subitem_relation_type_select":"URI"}}]},"item_8_source_id_9":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"2469-9950","subitem_source_identifier_type":"ISSN"}]},"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":"Akihiro, Koide"}],"nameIdentifiers":[{"nameIdentifier":"1064476","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Takuji, Nomura"}],"nameIdentifiers":[{"nameIdentifier":"1064477","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Toshiya, Inami"}],"nameIdentifiers":[{"nameIdentifier":"1064478","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Akihiro, Koide","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"1064479","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Takuji, Nomura","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"1064480","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Toshiya, Inami","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"1064481","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":"Sum rules of L-edge x-ray magnetic circularly polarized emission for 3d transition metals","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Sum rules of L-edge x-ray magnetic circularly polarized emission for 3d transition metals"}]},"item_type_id":"8","owner":"1","path":["1"],"pubdate":{"attribute_name":"公開日","attribute_value":"2021-09-15"},"publish_date":"2021-09-15","publish_status":"0","recid":"83411","relation_version_is_last":true,"title":["Sum rules of L-edge x-ray magnetic circularly polarized emission for 3d transition metals"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T16:48:35.062127+00:00"}