{"id":78187,"date":"2006-10-01T00:00:00","date_gmt":"2006-10-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/flavor-changing-neutral-decay-effects-in-models-with-two-higos-boson-doublets-applications-to-lhc-physics\/"},"modified":"2006-10-01T00:00:00","modified_gmt":"2006-10-01T00:00:00","slug":"flavor-changing-neutral-decay-effects-in-models-with-two-higos-boson-doublets-applications-to-lhc-physics","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/flavor-changing-neutral-decay-effects-in-models-with-two-higos-boson-doublets-applications-to-lhc-physics\/","title":{"rendered":"Flavor changing neutral decay effects in models with two higos boson doublets: applications to lhc physics"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Santiago Bejar Latonda <\/strong><\/h2>\n<p>En esta tesis se estudian diferentes aplicaciones fenomenol\u00f3gicas de los efectos de cambio de sabor por corrientes neutras (flavour changing neutral orrents, fcnc) inducidos en extensiones del sector de higgs, en particular, en modelos gen\u00e9ricos de dos dobletes de bosones de higgs y extensiones supersim\u00e9tricas.  se calculan las ratios de decaimiento (branching ratios, br) de los bosones de higgs decayendo a quarks pesados como el quark top y el bottom. Tambi\u00e9n se estudian las se\u00f1ales experimentales que permitirian discernir la naturaleza de estos bosones de higgs en aceleradores hadr\u00f3nicos, especialmente el lhc (large hadron collider).  las se\u00f1ales que puedan provenir de estos decaimientos fcnc pueden ser de gran ayuda para discrimirar estos bosones de higgs respecto del bos\u00f3n de higgs de model estandard (ms), ya que se puede demostrar que las br fcnc del boson de higgs del ms est\u00e1n extraordin\u00e1riamente suprimidas. Por lo tanto, si estos procesos se llegasen a observar ser\u00eda una evidencia directa de f\u00edsica mas all\u00e1 del ms. en esta tesis se demuestra que los bosones de higgs del mssm (minimal supersymetric standard model) y los bosones de higgs del modelo gen\u00e9rico 2hdm (model de dos dobletes de higgs) pueden dar br susceptibles de ser detectadas en el acelerador lhc. adem\u00e1s, en esta tesis se calculan las secciones eficaces de producci\u00f3n asociadas alos decaimientos de los bosones de higgs y se demuestra que con las luminosidades previstas en el acelerador lhc se podr\u00edan recoger un n\u00famero considerable de estos sucesos.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Flavor changing neutral decay effects in models with two higos boson doublets: applications to lhc physics<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Flavor changing neutral decay effects in models with two higos boson doublets: applications to lhc physics <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Santiago Bejar Latonda <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Aut\u00f3noma de barcelona<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 10\/01\/2006<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n<h3>Direcci\u00f3n y tribunal<\/h3>\n<ul>\n<li><strong>Director de la tesis<\/strong>\n<ul>\n<li>Joan Sol\u00e1 Peracaula<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: ram\u00f3n Pascual <\/li>\n<li>sven Heinemeyer (vocal)<\/li>\n<li>Mar\u00eda no Quir\u00f3s (vocal)<\/li>\n<li>martine Bosman (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Santiago Bejar Latonda En esta tesis se estudian diferentes aplicaciones fenomenol\u00f3gicas de los efectos de cambio de [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"default","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"var(--ast-global-color-4)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-gradient":""}},"footnotes":""},"categories":[199,7330,41577],"tags":[87316,118481,64448,168143,168142,168144],"class_list":["post-78187","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-de-altas-energias","category-fisica-teorica-de-altas-energias","tag-joan-sola-peracaula","tag-maria-no-quiros","tag-martine-bosman","tag-ramon-pascual","tag-santiago-bejar-latonda","tag-sven-heinemeyer"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/78187","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/comments?post=78187"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/78187\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=78187"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=78187"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=78187"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}