{"id":537371,"date":"2017-10-02T13:00:00","date_gmt":"2017-10-02T10:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=80002de6e17e8894fcb9d44b20ce50e3"},"modified":"2017-10-02T13:00:00","modified_gmt":"2017-10-02T10:00:00","slug":"effective-one-dimensional-coupling-in-the-highly-frustrated-square-lattice-itinerant-magnet-mathrmcaco_2%e2%88%92ymathrmas_2","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=537371","title":{"rendered":"Effective One-Dimensional Coupling in the Highly Frustrated Square-Lattice Itinerant Magnet ${\\mathrm{CaCo}}_{2\u2212y}{\\mathrm{As}}_{2}$"},"content":{"rendered":"<p>Author(s): A. Sapkota, B.\u2009G. Ueland, V.\u2009K. Anand, N.\u2009S. Sangeetha, D.\u2009L. Abernathy, M.\u2009B. Stone, J.\u2009L. Niedziela, D.\u2009C. Johnston, A. Kreyssig, A.\u2009I. Goldman, and R.\u2009J. McQueeney<\/p>\n<p>A rare example of a highly frustrated metal is identified, where the frustration is due to competing exchange interactions of spins, and not due to the spin geometry.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.119.147201.png\" width=\"200\" height=\\\"100\\\"><\/p>\n<p>[Phys. Rev. Lett. 119, 147201] Published Mon Oct 02, 2017<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): A. Sapkota, B.&thinsp;G. Ueland, V.&thinsp;K. Anand, N.&thinsp;S. Sangeetha, D.&thinsp;L. Abernathy, M.&thinsp;B. Stone, J.&thinsp;L. Niedziela, D.&thinsp;C. Johnston, A. Kreyssig, A.&thinsp;I. Goldman, and R.&thinsp;J. McQueeney<\/p>\n<p>A rare example of a highly frustrated metal is identified, where the frustration is due to competing exchange interactions of spins, and not due to the spin geometry.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.119.147201.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 119, 147201] Published Mon Oct 02, 2017<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_genesis_hide_title":false,"_genesis_hide_breadcrumbs":false,"_genesis_hide_singular_image":false,"_genesis_hide_footer_widgets":false,"_genesis_custom_body_class":"","_genesis_custom_post_class":"","_genesis_layout":"","footnotes":""},"categories":[182],"tags":[],"class_list":{"0":"post-537371","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-rss-teadus","7":"entry"},"_links":{"self":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/537371","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=537371"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/537371\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=537371"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=537371"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=537371"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}