{"created":"2023-05-15T14:57:28.688874+00:00","id":78001,"links":{},"metadata":{"_buckets":{"deposit":"805c26c6-4391-403a-bf23-91c2d853b08c"},"_deposit":{"created_by":1,"id":"78001","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"78001"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00078001","sets":["1"]},"author_link":["1004430","1004425","1004427","1004426","1004429","1004432","1004431","1004428"],"item_8_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2019-12","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"214501-9","bibliographicPageStart":"214501-1","bibliographicVolumeNumber":"100","bibliographic_titles":[{"bibliographic_title":"Physical Review B"}]}]},"item_8_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"We use the Ginzburg-Landau theory for a chiral p-wave superconductor to describe the filamentary superconducting phase nucleating at temperatures higher than the bulk transition temperature near the interfaces between Ru metal and Sr2RuO4 in eutectic Sr2RuO4-Ru.The peculiar phase diagram of magnetic field versus temperature shows very distinct properties for different directions of the magnetic field. A clear feature of the magnetic fields in the basal plane of Sr2RuO4, perpendicular to the chiral axis (c axis), is the occurrence of a second superconducting transition with a new order parameter visible as a zero-bias anomaly in tunneling spectroscopy. For the field along the c axis of Sr2RuO4, two transitions merge, indicating that the field drives the second-order parameter through the paramagnetic coupling to a chiral supercurrent. The resulting phenomenology shows that the assumption of a chiral superconducting order parameter in Sr2RuO4 yields an image reproducing the qualitative properties observed in the experiment. This discussion is qualitatively analogous to thecorresponding chiral even- and odd-parity channels.\n","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.100.214501","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.100.214501","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":"Kaneyasu, Hirono"}],"nameIdentifiers":[{"nameIdentifier":"1004425","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Enokida, Yuya"}],"nameIdentifiers":[{"nameIdentifier":"1004426","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Nomura, Takuji"}],"nameIdentifiers":[{"nameIdentifier":"1004427","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Hasegawa, Yasumasa"}],"nameIdentifiers":[{"nameIdentifier":"1004428","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sakai, Toru"}],"nameIdentifiers":[{"nameIdentifier":"1004429","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sigrist, Manfred"}],"nameIdentifiers":[{"nameIdentifier":"1004430","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Takuji, Nomura","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"1004431","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Toru, Sakai","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"1004432","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":"Properties of the H-T phase diagram of the 3-K phase in eutectic Sr2RuO4-Ru: Evidence for chiral superconductivity","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Properties of the H-T phase diagram of the 3-K phase in eutectic Sr2RuO4-Ru: Evidence for chiral superconductivity"}]},"item_type_id":"8","owner":"1","path":["1"],"pubdate":{"attribute_name":"公開日","attribute_value":"2019-12-16"},"publish_date":"2019-12-16","publish_status":"0","recid":"78001","relation_version_is_last":true,"title":["Properties of the H-T phase diagram of the 3-K phase in eutectic Sr2RuO4-Ru: Evidence for chiral superconductivity"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T19:27:18.749181+00:00"}