{"created":"2023-05-15T14:48:30.558713+00:00","id":66460,"links":{},"metadata":{"_buckets":{"deposit":"ff967864-1cf2-45c8-93ab-aea622c67a67"},"_deposit":{"created_by":1,"id":"66460","owners":[1],"pid":{"revision_id":0,"type":"depid","value":"66460"},"status":"published"},"_oai":{"id":"oai:repo.qst.go.jp:00066460","sets":["10:29"]},"author_link":["653814","653817","653815","653819","653818","653816","653813","653812"],"item_10005_date_7":{"attribute_name":"発表年月日","attribute_value_mlt":[{"subitem_date_issued_datetime":"2017-09-23","subitem_date_issued_type":"Issued"}]},"item_10005_description_5":{"attribute_name":"抄録","attribute_value_mlt":[{"subitem_description":"YbNi3Al9 は空間群 R32 に属し,鏡映面と反転心をもたない Chiral 結晶である。\nTN=3.4K で磁気転移し, c軸方向の伝播ベクトル q=(0,0,0.82) をもつらせん磁気構造を形成する。また、c面内に磁場をかけると HC=1.0kOe で強磁性に転移する。Ni を Cu で置換することで、 x=0.06 のとき TN は 6.5K, HC は 10kOe まで上昇し、伝播ベクトル q は (0,0,0.44) まで小さくなると同時に、Chiral Soliton Lattice (CSL) の形成を示唆する特徴的な磁化過程が見られるようになる。これまで我々は円偏光を用いた共鳴 X 線散乱により結晶の Chirality とらせん磁気秩序の Helicity との間に 1 対 1 の対応関係があること( DM 相互作用の存在)を示してきた。また、磁場を印加することで、らせん秩序の高調波成分が誘起されていくことから、 CSL が形成されている可能性があることも指摘してきた。本講演では、新しい実験結果も含めて,これまでの結果を考察する。","subitem_description_type":"Abstract"}]},"item_10005_description_6":{"attribute_name":"会議概要（会議名, 開催地, 会期, 主催者等）","attribute_value_mlt":[{"subitem_description":"日本物理学会 2017年秋季大会","subitem_description_type":"Other"}]},"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":"松村, 武"}],"nameIdentifiers":[{"nameIdentifier":"653812","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"喜多, 要介"}],"nameIdentifiers":[{"nameIdentifier":"653813","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"久保, 光野"}],"nameIdentifiers":[{"nameIdentifier":"653814","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"吉川, 雄吾"}],"nameIdentifiers":[{"nameIdentifier":"653815","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"道村, 真司"}],"nameIdentifiers":[{"nameIdentifier":"653816","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"稲見, 俊哉"}],"nameIdentifiers":[{"nameIdentifier":"653817","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"大原, 繁男"}],"nameIdentifiers":[{"nameIdentifier":"653818","nameIdentifierScheme":"WEKO"}]},{"creatorNames":[{"creatorName":"稲見 俊哉","creatorNameLang":"en"}],"nameIdentifiers":[{"nameIdentifier":"653819","nameIdentifierScheme":"WEKO"}]}]},"item_language":{"attribute_name":"言語","attribute_value_mlt":[{"subitem_language":"jpn"}]},"item_resource_type":{"attribute_name":"資源タイプ","attribute_value_mlt":[{"resourcetype":"conference object","resourceuri":"http://purl.org/coar/resource_type/c_c94f"}]},"item_title":"Yb(Ni1−xCux)3Al9 におけるらせん磁気構造とキラルソリトン格子の形成","item_titles":{"attribute_name":"タイトル","attribute_value_mlt":[{"subitem_title":"Yb(Ni1−xCux)3Al9 におけるらせん磁気構造とキラルソリトン格子の形成"}]},"item_type_id":"10005","owner":"1","path":["29"],"pubdate":{"attribute_name":"公開日","attribute_value":"2017-09-29"},"publish_date":"2017-09-29","publish_status":"0","recid":"66460","relation_version_is_last":true,"title":["Yb(Ni1−xCux)3Al9 におけるらせん磁気構造とキラルソリトン格子の形成"],"weko_creator_id":"1","weko_shared_id":-1},"updated":"2023-05-15T20:48:42.657219+00:00"}