{"id":41518,"date":"2014-10-16T17:00:00","date_gmt":"2014-10-16T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=7b7b55267f73b41e5857ec727659bb15"},"modified":"2014-10-16T17:00:00","modified_gmt":"2014-10-16T14:00:00","slug":"solvable-relativistic-hydrogenlike-system-in-supersymmetric-yang-mills-theory","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=41518","title":{"rendered":"Solvable Relativistic Hydrogenlike System in Supersymmetric Yang-Mills Theory"},"content":{"rendered":"<p>Author(s): Simon Caron-Huot and Johannes M. Henn<\/p>\n<p> A relativistic quantum field theory extension to the classical Kepler problem provides a new method to compute the bound states of massive <span style=\"font-style: italic;\">W<\/span> bosons in planar <span style=\"font-family: brush script mt italic;\">N<\/span>=4 super Yang-Mills.<\/p>\n<p>[Phys. Rev. Lett. 113, 161601] Published Thu Oct 16, 2014<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): Simon Caron-Huot and Johannes M. Henn A relativistic quantum field theory extension to the classical Kepler problem provides a new method to compute the bound states of massive W bosons in planar N=4 super Yang-Mills.[Phys. Rev. Lett. 113, 1&#8230;<\/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-41518","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\/41518","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=41518"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/41518\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=41518"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=41518"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=41518"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}