{"id":90249,"date":"2015-05-27T17:00:00","date_gmt":"2015-05-27T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=c858be61392ebafda19808156da798ab"},"modified":"2015-05-27T17:00:00","modified_gmt":"2015-05-27T14:00:00","slug":"reentrant-superconductivity-driven-by-quantum-tricritical-fluctuations-in-urhge-evidence-from-59co-nmr-in-urh_0-9co_0-1ge","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=90249","title":{"rendered":"Reentrant Superconductivity Driven by Quantum Tricritical Fluctuations in URhGe: Evidence from ^{59}Co NMR in URh_{0.9}Co_{0.1}Ge"},"content":{"rendered":"<p>Author(s): Y. Tokunaga, D. Aoki, H. Mayaffre, S. Kr\u00e4mer, M.-H. Julien, C. Berthier, M. Horvati\u0107, H. Sakai, S. Kambe, and S. Araki<\/p>\n<p>NMR measurements near the quantum tricritical point show that reentrance of superconductivity at high fields requires longitudinal fluctuations (parallel to the applied field). These experimental results will require revision of theoretical work, which to date has included only transverse fluctuations.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.114.216401.png\" width=\"200\" height=\"100\"><\/p>\n<p>[Phys. Rev. Lett. 114, 216401] Published Wed May 27, 2015<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): Y. Tokunaga, D. Aoki, H. Mayaffre, S. Kr&auml;mer, M.-H. Julien, C. Berthier, M. Horvati&#263;, H. Sakai, S. Kambe, and S. Araki<\/p>\n<p>NMR measurements near the quantum tricritical point show that reentrance of superconductivity at high fields requires longitudinal fluctuations (parallel to the applied field). These experimental results will require revision of theoretical work, which to date has included only transverse fluctuations.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.114.216401.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 114, 216401] Published Wed May 27, 2015<\/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-90249","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\/90249","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=90249"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/90249\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=90249"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=90249"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=90249"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}