{"id":56522,"date":"2007-11-01T00:00:00","date_gmt":"2007-11-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/phenomenology-of-neutrino-mass-models\/"},"modified":"2007-11-01T00:00:00","modified_gmt":"2007-11-01T00:00:00","slug":"phenomenology-of-neutrino-mass-models","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/phenomenology-of-neutrino-mass-models\/","title":{"rendered":"Phenomenology of neutrino mass models"},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Villanova Del Moral Albert <\/strong><\/h2>\n<p>Los recientes resultados de experimentos de neutrinos han puesto en evidencia que el modelo est\u00e1ndar ha de ser extendido para explicar los datos experimentales. Ante esta situaci\u00f3n, multitud de modelos de masa de neutrinos han sido propuestos. Sin embargo,  el mecanismo responsable de la generaci\u00f3n de masas es todav\u00eda desconocido. Con la finalidad de comprenderlo, han de verificarse dos requisitos: por un lado, los modelos deben ser comprobables; por otro lado, diferentes modelos han de ser diferenciables. Por tanto, es necesario llevar a cabo un an\u00e1lisis en detalle de los diferentes modelos de masa de neutrinos para identificar sus caracter\u00edsticas diferenciadoras y sus espec\u00edficas implicaciones fenomenol\u00f3gicas. Este tipo de estudio ha sido precisamente la principal motivaci\u00f3n de esta tesis. De hecho, se trata del estudio de diferentes modelos de masa de neutrinos y de la investigaci\u00f3n de sus implicaciones. entre los modelos estudiados, algunos de ellos est\u00e1n basados en la simetr\u00eda discreta de sabor a4. Esta simetr\u00eda puede estar realizada de muy diversas formas dependiendo del contenido de part\u00edculas del modelo y de las propiedades de transformaci\u00f3n de \u00e9stas bajo a4. Una de las realizaciones estudiadas en detalle se trata de un modelo que predice masas de neutrinos cuasi degeneradas. El contenido de part\u00edculas es el mismo que en el modelo est\u00e1ndar supersim\u00e9trico m\u00ednimo, pero extendido con supercampos leptones, quarks y de higgs, singletes bajo su(2). Los principales resultados de este modelo son: las mezclas de los neutrinos y las de los sleptones est\u00e1n correlacionadas; predice la existencia de un slept\u00f3n con masa accesible en el lhc; establece una cota inferior a la escala de masa absoluta de majorana de los neutrinos; predice procesos que violan sabor lept\u00f3nico con cotas inferiores accesibles a los pr\u00f3ximos experimentos. en otra realizaci\u00f3n de la simetr\u00eda a4, el contenido de part\u00edculas es extendido respecto al del modelo est\u00e1ndar con<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Phenomenology of neutrino mass models<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Phenomenology of neutrino mass models <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Villanova Del Moral Albert <\/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 11\/01\/2007<\/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 Wagner<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: alfred Bartl <\/li>\n<li>Mar\u00eda Jos\u00e9 Herrero solans (vocal)<\/li>\n<li>walter Grimus (vocal)<\/li>\n<li>rudolf Porod werner (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Villanova Del Moral Albert Los recientes resultados de experimentos de neutrinos han puesto en evidencia que el [&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":[199,1432,27034,11703],"tags":[87353,58144,15514,124864,124862,124863],"class_list":["post-56522","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-teorica","category-leptones","category-particulas-elementales","tag-alfred-bartl","tag-furtado-valle-jose-wagner","tag-maria-jose-herrero-solans","tag-rudolf-porod-werner","tag-villanova-del-moral-albert","tag-walter-grimus"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/56522","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=56522"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/56522\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=56522"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=56522"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=56522"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}