{"id":469,"date":"2022-01-20T22:07:01","date_gmt":"2022-01-20T13:07:01","guid":{"rendered":"http:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/?post_type=topics&#038;p=469"},"modified":"2022-01-21T12:54:47","modified_gmt":"2022-01-21T03:54:47","slug":"phase-diagram-of-a-distorted-kagome-antiferromagnet-and-application-to-y-kapellasite","status":"publish","type":"topics","link":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/topics\/phase-diagram-of-a-distorted-kagome-antiferromagnet-and-application-to-y-kapellasite\/","title":{"rendered":"Phase diagram of a distorted kagome antiferromagnet and application to Y-kapellasite"},"content":{"rendered":"<p>Antiferromagnets on kagome lattices are among the most interesting materials in the field of highly frustrated magnetism. We have studied a material that has, according to our density functional theory based energy mapping, a kagome lattice with a very interesting distortion. Classical calculations arrive at a phase diagram which contains, besides three ordered phases, a large classical spin liquid phase. The material Y-kapellasite which motivated the study and led to the discovery of this phase diagram is situated in a non-collinar coplanar ordered phase, in agreement with experiment.<\/p>\n<p>M. Hering, F. Ferrari, A. Razpopov, I. I. Mazin, R. Valenti, H. O. Jeschke, J. Reuther<\/p>\n<p>npj Comput. Mater. <b>8<\/b>, 10 (2022) <<a href=\"https:\/\/doi.org\/10.1038\/s41524-021-00689-0\" rel=\"noopener\" target=\"_blank\">https:\/\/doi.org\/10.1038\/s41524-021-00689-0<\/a>><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-content\/uploads\/2022\/01\/ykapellasitea.png\" alt=\"\" width=\"500\" height=\"653\" class=\"aligncenter size-full wp-image-281\" \/><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Antiferromagnets on kagome lattices are among the most interesting materials in  &#8230; <\/p>\n","protected":false},"author":2,"featured_media":457,"menu_order":0,"template":"","format":"standard","meta":{"footnotes":""},"categories":[],"tags":[],"class_list":["post-469","topics","type-topics","status-publish","format-standard","has-post-thumbnail","hentry"],"_links":{"self":[{"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/topics\/469","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/topics"}],"about":[{"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/types\/topics"}],"author":[{"embeddable":true,"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/users\/2"}],"version-history":[{"count":6,"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/topics\/469\/revisions"}],"predecessor-version":[{"id":478,"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/topics\/469\/revisions\/478"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/media\/457"}],"wp:attachment":[{"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/media?parent=469"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/categories?post=469"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.physics.okayama-u.ac.jp\/jeschke-otsuki-group\/wp-json\/wp\/v2\/tags?post=469"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}