{"id":41269,"date":"2014-12-09T18:00:00","date_gmt":"2014-12-09T15:00:00","guid":{"rendered":"http:\/\/www.fyysika.ee\/?guid=0ce84ecb75fc41f150d9b069d7b5260d"},"modified":"2014-12-09T18:00:00","modified_gmt":"2014-12-09T15:00:00","slug":"su2xu1-gauge-invariance-and-the-shape-of-new-physics-in-rare-b-decays","status":"publish","type":"post","link":"https:\/\/www.fyysika.ee\/?p=41269","title":{"rendered":"SU(2)\u00d7U(1) Gauge Invariance and the Shape of New Physics in Rare B Decays"},"content":{"rendered":"<p>Author(s): R. Alonso, B. Grinstein, and J. Martin Camalich<\/p>\n<p> An effective field theory for physics beyond the electroweak scale, where symmetries of the Standard Model are assumed to apply, provides model-independent constraints on new physics from the branching ratios of <span style=\"font-style: italic;\">B<\/span> decays.<\/p>\n<p>[Phys. Rev. Lett. 113, 241802] Published Tue Dec 09, 2014<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Author(s): R. Alonso, B. Grinstein, and J. Martin Camalich An effective field theory for physics beyond the electroweak scale, where symmetries of the Standard Model are assumed to apply, provides model-independent constraints on new physics from the b&#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-41269","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\/41269","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=41269"}],"version-history":[{"count":0,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=\/wp\/v2\/posts\/41269\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=41269"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=41269"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fyysika.ee\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=41269"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}