{"id":13358,"date":"2018-03-09T08:59:36","date_gmt":"2018-03-09T08:59:36","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/phenomenology-of-bilinear-broken-r-parity\/"},"modified":"2018-03-09T08:59:36","modified_gmt":"2018-03-09T08:59:36","slug":"phenomenology-of-bilinear-broken-r-parity","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/phenomenology-of-bilinear-broken-r-parity\/","title":{"rendered":"Phenomenology of bilinear broken r-parity"},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Restrepo Quintero Diego A. <\/strong><\/h2>\n<p>El moselo estandar supersim\u00e9trico minimo es la extension con m\u00ednimo numero de particulas correspondientes a aquellas del modelo estandar, un doblete de higgs adicional y todos los compa\u00f1eros supersimetricos de las particulas del modelo estandar, adem\u00e1s tiene un numero minimo de acoplamientos posibles. El modelo estandar supersim\u00e9trica (mes), sin restricci\u00f3n en el n\u00famero de acoplamientos permite la aparici\u00f3n simultanea de t\u00e9rminos  que violan n\u00famero l\u00e9ptonico y bari\u00f3nico y de este mod es excluido debido a que el proton decae a trav\u00e9s de interacciones electrodebiles. Sin embargo, es bien conocido que la estabilidad del prot\u00f3n permite la presencia ya sea de violacion de numero lept\u00f3nico o de la violaci\u00f3n de numero bari\u00f3nico. de hecho si los neutrinos tienen masa coo es suberido por las anomalias solar y atmosferica, no existe raz\u00f3n de peso para asumir que los terminos que violan numero lept\u00f3nico esten ausentes del superpotencial. En este trabajo estuiaremos la realizaci\u00f3n del mes con conservacion de numero bari\u00f3nico y violaci\u00f3n m\u00ednima de numero lept\u00f3nico. Los \u00fanicos t\u00e9rminos con violacion de n\u00famero lept\u00f3nico en este caso provienen del termino de masa m\u00e1s general que permite la invarianza gauge en el superpotencial del mes. Al modelo correspondiente lo llameremos mess (modelo estandar supersim\u00e9trico superrenormalizable). el mess es m\u00e1s predictivo y teoricamente m\u00e1s atractivo que el mes con conservaci\u00f3n de n\u00famero bari\u00f3nico pero con terminos arbitrarios de violacion de n\u00famero lept\u00f3nico y en general satisface todas las restricciones que surgen de esa violaci\u00f3n.  en el mess la particula supersim\u00e9trica m\u00e1s liviana (psl) puede decaer. en particular estudiaremos la fenomenolog\u00eda esperada del neutralino en lep2. En el caso de particulas supersimetricas de mayor masa que la psl, los decaimientos que violan n\u00famero lept\u00f3nico pueden llegar a ser detectables en los aceleradores incluso en el caso de masa de neutrin<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Phenomenology of bilinear broken r-parity<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Phenomenology of bilinear broken r-parity <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Restrepo Quintero Diego A. <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Universitat de val\u00e9ncia (estudi general)<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 19\/10\/2001<\/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> Furtado Valle Jos\u00e9 W.<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Luis e. Iba\u00f1ez Santiago <\/li>\n<li>arcadi Santamaria luna (vocal)<\/li>\n<li>enrico Nardi (vocal)<\/li>\n<li>carmen Garcia garcia (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Restrepo Quintero Diego A. El moselo estandar supersim\u00e9trico minimo es la extension con m\u00ednimo numero de particulas [&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":[199,1432],"tags":[43399,14693,43400,43398,14446,43397],"class_list":["post-13358","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-teorica","tag-arcadi-santamaria-luna","tag-carmen-garcia-garcia","tag-enrico-nardi","tag-furtado-valle-jose-w","tag-luis-e-ibanez-santiago","tag-restrepo-quintero-diego-a"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/13358","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=13358"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/13358\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=13358"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=13358"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=13358"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}