{"id":91732,"date":"2015-06-02T17:00:00","date_gmt":"2015-06-02T14:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=c14a0ca737559b5761e0b4bbed7f0f79"},"modified":"2015-06-02T17:00:00","modified_gmt":"2015-06-02T14:00:00","slug":"updated-next-to-next-to-leading-order-qcd-predictions-for-the-weak-radiative-b-meson-decays","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=91732","title":{"rendered":"Updated Next-to-Next-to-Leading-Order QCD Predictions for the Weak Radiative B-Meson Decays"},"content":{"rendered":"<p>Author(s): M. Misiak, H.\u2009M. Asatrian, R. Boughezal, M. Czakon, T. Ewerth, A. Ferroglia, P. Fiedler, P. Gambino, C. Greub, U. Haisch, T. Huber, M. Kami\u0144ski, G. Ossola, M. Poradzi\u0144ski, A. Rehman, T. Schutzmeier, M. Steinhauser, and J. Virto<\/p>\n<p>Precise standard-model theoretical predictions of the decay of a bottom-quark meson into a strange-quark and a photon allow better bounds on models of new physics, notably those with hypothetical charged Higgs bosons.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.114.221801.png\" width=\"200\" height=\"100\"><\/p>\n<p>[Phys. Rev. Lett. 114, 221801] Published Tue Jun 02, 2015<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): M. Misiak, H.&thinsp;M. Asatrian, R. Boughezal, M. Czakon, T. Ewerth, A. Ferroglia, P. Fiedler, P. Gambino, C. Greub, U. Haisch, T. Huber, M. Kami&#324;ski, G. Ossola, M. Poradzi&#324;ski, A. Rehman, T. Schutzmeier, M. Steinhauser, and J. Virto<\/p>\n<p>Precise standard-model theoretical predictions of the decay of a bottom-quark meson into a strange-quark and a photon allow better bounds on models of new physics, notably those with hypothetical charged Higgs bosons.<\/p>\n<p><img decoding=\"async\" src=\"http:\/\/d22izw7byeupn1.cloudfront.net\/journals\/PRL\/key_images\/10.1103\/PhysRevLett.114.221801.png\" width=\"200\" height='\"100\"'><br \/>[Phys. Rev. Lett. 114, 221801] Published Tue Jun 02, 2015<\/p>\n","protected":false},"author":0,"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-91732","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\/91732","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"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=91732"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/91732\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=91732"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=91732"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=91732"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}