{"id":208706,"date":"2016-04-13T17:00:00","date_gmt":"2016-04-13T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=fe53f063b03530fb3734dec0fa56a610"},"modified":"2016-04-13T17:00:00","modified_gmt":"2016-04-13T14:00:00","slug":"universality-and-scaling-in-a-charge-two-channel-kondo-device","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=208706","title":{"rendered":"Universality and Scaling in a Charge Two-Channel Kondo Device"},"content":{"rendered":"<p>Author(s): A.\u2009K. Mitchell, L.\u2009A. Landau, L. Fritz, and E. Sela<\/p>\n<p>A two-channel Kondo model solved using the numerical renormalization group reproduces the temperature dependence of the conductance measured in recent experiments on Kondo nanostructures. This suggests that charge-Kondo devices constitute perfect quantum simulations of models exhibiting quantum criticality.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.116.157202.png\" width=\"200\" height=\"100\"><\/p>\n<p>[Phys. Rev. Lett. 116, 157202] Published Wed Apr 13, 2016<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): A.&thinsp;K. Mitchell, L.&thinsp;A. Landau, L. Fritz, and E. Sela<\/p>\n<p>A two-channel Kondo model solved using the numerical renormalization group reproduces the temperature dependence of the conductance measured in recent experiments on Kondo nanostructures. This suggests that charge-Kondo devices constitute perfect quantum simulations of models exhibiting quantum criticality.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.116.157202.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 116, 157202] Published Wed Apr 13, 2016<\/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-208706","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\/208706","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=208706"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/208706\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=208706"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=208706"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=208706"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}