{"created":"2023-05-15T14:58:41.986260+00:00","id":79636,"links":{},"metadata":{"_buckets":{"deposit":"2bfcbd5f-c565-4fe9-b825-f3b616ea8df4"},"_deposit":{"created_by":1,"id":"79636","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"79636"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00079636","sets":["2"]},"author_link":["863816","863818","863814","863815","863813","863817","863812","863811"],"item_10003_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2020-03","bibliographicIssueDateType":"Issued"},"bibliographicPageEnd":"011039-6","bibliographicPageStart":"011039-1","bibliographicVolumeNumber":"30","bibliographic_titles":[{"bibliographic_title":"JPS Conference Proceedings"}]}]},"item_10003_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Eutectic Sr2RuO4-Ru samples show an onset of inhomogeneous \nsuperconductivity at around 3 K, which is above the bulk transition of \nSr2RuO4 (SRO) with Tc≈1.5Tc≈1.5 K. This superconducting state nucleates \nmost likely as a filamentary state at the interface between SRO and Ru-\ninclusions. Assuming that the superconducting phase of SRO has chiral \nsymmetry, the evolution towards the bulk phase involves an additional \nsymmetry breaking transition. Phenomenological theories based on a two-\ncomponent order parameter (ηxηx, ηyηy) suggest that first a time reversal symmetry conserving order parameter nucleates at the interface due to the symmetry reduction. A second transition yields a time reversal symmetry breaking phase through the appearance of a second order parameter component. In this study we show how this second transition can be influenced by external magnetic fields. For fields parallel to the basal plane of SRO the transition is suppressed. On the other hand, fields along the c-axis support the \nsecond order parameter component. This behavior is well visible in quasi\n-particle tunneling spectroscopy where a zero-bias peak indicates the \npresence of the second order parameter component. Our result reproduces \nexperimental results on a qualitative level very well and are compatible \nwith both chiral superconducting phases, px±ipypx±ipy-wave (spin triplet)\n and dxz±idyzdxz±idyz-wave (spin singlet) pairing.","subitem_description_type":"Abstract"}]},"item_10003_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.7566/JPSCP.30.011039","subitem_relation_type_select":"DOI"}}]},"item_10003_relation_17":{"attribute_name":"関連サイト","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"https://journals.jps.jp/doi/abs/10.7566/JPSCP.30.011039","subitem_relation_type_select":"URI"}}]},"item_10003_source_id_9":{"attribute_name":"ISSN","attribute_value_mlt":[{"subitem_source_identifier":"2435-3892","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":"863811","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Enokida, Yuya"}],"nameIdentifiers":[{"nameIdentifier":"863812","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Nomura, Takuji"}],"nameIdentifiers":[{"nameIdentifier":"863813","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Hasegawa, Yasumasa"}],"nameIdentifiers":[{"nameIdentifier":"863814","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sakai, Toru"}],"nameIdentifiers":[{"nameIdentifier":"863815","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sigrist, Manfred"}],"nameIdentifiers":[{"nameIdentifier":"863816","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Nomura, Takuji","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"863817","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Sakai, Toru","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"863818","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":"conference paper","resourceuri":"http://purl.org/coar/resource_type/c_5794"}]},"item_title":"Features of Chirality Generated by Paramagnetic Coupling to Magnetic  Fields in the 3 K-Phase of Sr2RuO4","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Features of Chirality Generated by Paramagnetic Coupling to Magnetic  Fields in the 3 K-Phase of Sr2RuO4"}]},"item_type_id":"10003","owner":"1","path":["2"],"pubdate":{"attribute_name":"公開日","attribute_value":"2020-03-25"},"publish_date":"2020-03-25","publish_status":"0","recid":"79636","relation_version_is_last":true,"title":["Features of Chirality Generated by Paramagnetic Coupling to Magnetic  Fields in the 3 K-Phase of Sr2RuO4"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T22:02:42.693906+00:00"}