{"_buckets": {"deposit": "78a07cc7-7e56-4d75-a6a3-7b2d8b060df0"}, "_deposit": {"id": "1529", "owners": [], "pid": {"revision_id": 0, "type": "depid", "value": "1529"}, "status": "published"}, "_oai": {"id": "oai:soar-ir.repo.nii.ac.jp:00001529", "sets": ["150:151"]}, "item_6_biblio_info_6": {"attribute_name": "\u66f8\u8a8c\u60c5\u5831", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2011-11", "bibliographicIssueDateType": "Issued"}, "bibliographicIssueNumber": "21-22", "bibliographicPageEnd": "710", "bibliographicPageStart": "708", "bibliographicVolumeNumber": "471", "bibliographic_titles": [{"bibliographic_title": "PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS"}]}]}, "item_6_description_20": {"attribute_name": "\u6284\u9332", "attribute_value_mlt": [{"subitem_description": "We have measured tunnel conductance of spin-triplet superconductor Sr(2)RuO(4) (SRO) break junction which was made by micro fabrication technique with a focused ion beam. This is a new type of tunnel junctions made of SRO, which is different from those made of SRO and other materials. Since the tunnel conductance is sensitive to the internal phase of superconductivity, it enables us to examine the chiral p-wave pairing state, which is the most probable candidate of SRO. The tunnel conductance spectrum of the junction showed a broad zero-bias conductance peak whose shape is different from that of high-T(c) cuprate superconductors. The shape of the spectrum is in quite good agreement with the calculated spectrum of a chiral p-wave/insulator/normal metal junction.", "subitem_description_type": "Abstract"}]}, "item_6_description_30": {"attribute_name": "\u8cc7\u6e90\u30bf\u30a4\u30d7\uff08\u30b3\u30f3\u30c6\u30f3\u30c4\u306e\u7a2e\u985e\uff09", "attribute_value_mlt": [{"subitem_description": "Article", "subitem_description_type": "Other"}]}, "item_6_description_5": {"attribute_name": "\u5f15\u7528", "attribute_value_mlt": [{"subitem_description": "PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS. 471(21-22):708-710 (2011)", "subitem_description_type": "Other"}]}, "item_6_link_3": {"attribute_name": "\u4fe1\u5dde\u5927\u5b66\u7814\u7a76\u8005\u7dcf\u89a7\u3078\u306e\u30ea\u30f3\u30af", "attribute_value_mlt": [{"subitem_link_text": "Kambara, H", "subitem_link_url": "http://soar-rd.shinshu-u.ac.jp/profile/ja.HNnUWhLp.html"}]}, "item_6_link_67": {"attribute_name": "WoS", "attribute_value_mlt": [{"subitem_link_text": "Web of Science", "subitem_link_url": "http://gateway.isiknowledge.com/gateway/Gateway.cgi?\u0026GWVersion=2\u0026SrcAuth=ShinshuUniv\u0026SrcApp=ShinshuUniv\u0026DestLinkType=FullRecord\u0026DestApp=WOS\u0026KeyUT=000297433400032"}]}, "item_6_publisher_4": {"attribute_name": "\u51fa\u7248\u8005", "attribute_value_mlt": [{"subitem_publisher": "ELSEVIER SCIENCE BV"}]}, "item_6_relation_48": {"attribute_name": "DOI", "attribute_value_mlt": [{"subitem_relation_name": [{"subitem_relation_name_text": "10.1016/j.physc.2011.05.033"}], "subitem_relation_type_id": {"subitem_relation_type_id_text": "http://dx.doi.org/10.1016/j.physc.2011.05.033", "subitem_relation_type_select": "DOI"}}]}, "item_6_select_64": {"attribute_name": "\u8457\u8005\u7248\u30d5\u30e9\u30b0", "attribute_value_mlt": [{"subitem_select_item": "author"}]}, "item_6_source_id_35": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "0921-4534", "subitem_source_identifier_type": "ISSN"}]}, "item_6_source_id_39": {"attribute_name": "NII ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "0921-4534", "subitem_source_identifier_type": "ISSN"}]}, "item_6_source_id_40": {"attribute_name": "\u66f8\u8a8c\u30ec\u30b3\u30fc\u30c9ID", "attribute_value_mlt": [{"subitem_source_identifier": "AA11461984", "subitem_source_identifier_type": "NCID"}]}, "item_6_text_69": {"attribute_name": "wosonly authkey", "attribute_value_mlt": [{"subitem_text_value": "Ruthenates; Chiral p-wave; Proximity effect; Tunneling phenomena; Break junction"}]}, "item_6_text_70": {"attribute_name": "wosonly keywords", "attribute_value_mlt": [{"subitem_text_value": "SUPERCONDUCTING SR2RUO4; TUNNELING SPECTROSCOPY; BOUND-STATES; TRANSITION"}]}, "item_6_textarea_68": {"attribute_name": "wosonly abstract", "attribute_value_mlt": [{"subitem_textarea_value": "We have measured tunnel conductance of spin-triplet superconductor Sr(2)RuO(4) (SRO) break junction which was made by micro fabrication technique with a focused ion beam. This is a new type of tunnel junctions made of SRO, which is different from those made of SRO and other materials. Since the tunnel conductance is sensitive to the internal phase of superconductivity, it enables us to examine the chiral p-wave pairing state, which is the most probable candidate of SRO. The tunnel conductance spectrum of the junction showed a broad zero-bias conductance peak whose shape is different from that of high-T(c) cuprate superconductors. The shape of the spectrum is in quite good agreement with the calculated spectrum of a chiral p-wave/insulator/normal metal junction. (C) 2011 Elsevier B.V. All rights reserved."}]}, "item_creator": {"attribute_name": "\u8457\u8005", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "Kambara,  H"}], "nameIdentifiers": [{"nameIdentifier": "2394", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Kashiwaya,  S"}], "nameIdentifiers": [{"nameIdentifier": "2395", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Kashiwaya,  H"}], "nameIdentifiers": [{"nameIdentifier": "2396", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Tanaka,  Y"}], "nameIdentifiers": [{"nameIdentifier": "2397", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Maeno,  Y"}], "nameIdentifiers": [{"nameIdentifier": "2398", "nameIdentifierScheme": "WEKO"}]}]}, "item_files": {"attribute_name": "\u30d5\u30a1\u30a4\u30eb\u60c5\u5831", "attribute_type": "file", "attribute_value_mlt": [{"accessrole": "open_date", "date": [{"dateType": "Available", "dateValue": "2015-09-24"}], "displaytype": "detail", "download_preview_message": "", "file_order": 0, "filename": "Local_transport_characteristics_ break_junction.pdf", "filesize": [{"value": "664.4 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_free", "mimetype": "application/pdf", "size": 664400.0, "url": {"label": "Local_transport_characteristics_ break_junction.pdf", "url": "https://soar-ir.repo.nii.ac.jp/record/1529/files/Local_transport_characteristics_ break_junction.pdf"}, "version_id": "c95bfab5-069b-49c8-94af-f4c594119f7a"}]}, "item_keyword": {"attribute_name": "\u30ad\u30fc\u30ef\u30fc\u30c9", "attribute_value_mlt": [{"subitem_subject": "Ruthenates", "subitem_subject_scheme": "Other"}, {"subitem_subject": "Chiral p-wave", "subitem_subject_scheme": "Other"}, {"subitem_subject": "Proximity effect", "subitem_subject_scheme": "Other"}, {"subitem_subject": "Tunneling phenomena", "subitem_subject_scheme": "Other"}, {"subitem_subject": "Break junction", "subitem_subject_scheme": "Other"}]}, "item_language": {"attribute_name": "\u8a00\u8a9e", "attribute_value_mlt": [{"subitem_language": "eng"}]}, "item_resource_type": {"attribute_name": "\u8cc7\u6e90\u30bf\u30a4\u30d7", "attribute_value_mlt": [{"resourcetype": "journal article", "resourceuri": "http://purl.org/coar/resource_type/c_6501"}]}, "item_title": "Local transport characteristics of break junction in Sr(2)RuO(4) microbridge", "item_titles": {"attribute_name": "\u30bf\u30a4\u30c8\u30eb", "attribute_value_mlt": [{"subitem_title": "Local transport characteristics of break junction in Sr(2)RuO(4) microbridge"}]}, "item_type_id": "6", "owner": "1", "path": ["150/151"], "permalink_uri": "http://hdl.handle.net/10091/16129", "pubdate": {"attribute_name": "\u516c\u958b\u65e5", "attribute_value": "2012-12-06"}, "publish_date": "2012-12-06", "publish_status": "0", "recid": "1529", "relation": {}, "relation_version_is_last": true, "title": ["Local transport characteristics of break junction in Sr(2)RuO(4) microbridge"], "weko_shared_id": 3}