{"created":"2023-05-15T15:02:37.781355+00:00","id":84917,"links":{},"metadata":{"_buckets":{"deposit":"81cabd2a-686c-4e5d-ae35-94d622f4e712"},"_deposit":{"created_by":1,"id":"84917","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"84917"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00084917","sets":["1"]},"author_link":["1040748","1040746","1040743","1040745","1040747","1040744"],"item_8_biblio_info_7":{"attribute_name":"書誌情報","attribute_value_mlt":[{"bibliographicIssueDates":{"bibliographicIssueDate":"2021-11","bibliographicIssueDateType":"Issued"},"bibliographicIssueNumber":"1","bibliographicPageEnd":"014428-12","bibliographicPageStart":"014428-1","bibliographicVolumeNumber":"105","bibliographic_titles":[{"bibliographic_title":"Physical Review B"}]}]},"item_8_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"Successive phase transitions in a rare-earth monoaxial chiral magnet DyNi 3 Ga9 have been investigated by resonant x-ray diffraction. Magnetic dipole and electric quadrupole degrees of freedom arising from the large angular moment of J = 15/2, in combination with the symmetric and antisymmetric exchange interactions and the crystal field anisotropy, give rise to competing ordered phases. We show that the antiferromagnetically coupled Dy moments in the c-plane form an incommensurate helimagnetic order with q ∼ (0, 0, 0.43) just below TN = 10 K, which further exhibits successive first-order transitions to the commensurate helimagnetic order with q = (0, 0, 0.5) at TN′ = 9 K, and to the canted antiferromagnetic order with q = (0, 0, 0) at TN′′ = 8.5 K. The relation of the magnetic helicity and the crystal chirality in DyNi3 Ga9 is also uniquely determined. Splitting of the (6, 0, 0) Bragg peak is observed below TN′′ , reflecting the lattice distortion due to the ferroquadrupole order. In the canted antiferromagnetic phase, a spin-flop transition takes place at 5 K when the temperature is swept in a weak magnetic field. We discuss these transitions from the viewpoint of competing energies described above.","subitem_description_type":"Abstract"}]},"item_8_relation_14":{"attribute_name":"DOI","attribute_value_mlt":[{"subitem_relation_type_id":{"subitem_relation_type_id_text":"10.1103/PhysRevB.105.014428","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.105.014428","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":"Tsukagoshi, M."}],"nameIdentifiers":[{"nameIdentifier":"1040743","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Matsumura, T."}],"nameIdentifiers":[{"nameIdentifier":"1040744","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Michimura, S."}],"nameIdentifiers":[{"nameIdentifier":"1040745","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Inami, Toshiya"}],"nameIdentifiers":[{"nameIdentifier":"1040746","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Ohara, S."}],"nameIdentifiers":[{"nameIdentifier":"1040747","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"Toshiya, Inami","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"1040748","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":"Competition between helimagnetic and ferroquadrupolar orderings in a monoaxial chiral magnet DyNi3Ga9 studied by resonant x-ray diffraction","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Competition between helimagnetic and ferroquadrupolar orderings in a monoaxial chiral magnet DyNi3Ga9 studied by resonant x-ray diffraction"}]},"item_type_id":"8","owner":"1","path":["1"],"pubdate":{"attribute_name":"公開日","attribute_value":"2021-11-01"},"publish_date":"2021-11-01","publish_status":"0","recid":"84917","relation_version_is_last":true,"title":["Competition between helimagnetic and ferroquadrupolar orderings in a monoaxial chiral magnet DyNi3Ga9 studied by resonant x-ray diffraction"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T17:24:38.398681+00:00"}