{"id":60283,"date":"2018-03-09T22:48:07","date_gmt":"2018-03-09T22:48:07","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/interaccion-neutrino-nucleo-a-energias-intermedias\/"},"modified":"2018-03-09T22:48:07","modified_gmt":"2018-03-09T22:48:07","slug":"interaccion-neutrino-nucleo-a-energias-intermedias","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/interaccion-neutrino-nucleo-a-energias-intermedias\/","title":{"rendered":"Interaccion neutrino-nucleo a energias intermedias"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Manuel Valverde Hermosilla <\/strong><\/h2>\n<p>En este trabajo hemos desarrollado un modelo para estudiar las reacciones de dispersion de neutrinos por nucleos en la region del pico cuasi-elastico y un regimen de energias intermedias, relevante para experimentos de oscilacion de neutrinos.  Hemos estudiado reacciones mediadas por corrientes neutras y cargadas e inducidas tanto por neutrinos como por antineutrinos.Nuestro modelo parte de un gas de fermi en aproximacion de densidad local, pero incluye una serie de efectos debidos al medio nuclear relevantes: dispersion coulombiana del lepton cargado saliente, correlaciones de largo alcance (polarizacion delmedio tipo rpa), auto-energia del nucleon en el medio (final state interaction, fsi) . Hemos comprobado que la inclusion de estos efectos de dinamica nuclear, en particular rpa y fsi, producen modificaciones muy importantes de la respuesta del gas de fermi ante sondas debiles. La polarizacion del medio (rpa) resulta esencial para obtener una descripcion aceptable de los datos. Por otro lado, los efectos<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Interaccion neutrino-nucleo a energias intermedias<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Interaccion neutrino-nucleo a energias intermedias <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Manuel Valverde Hermosilla <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Granada<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 27\/07\/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>Jos\u00e9 Enrique Amaro Soriano<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: elvira Moya valga\u00f1\u00f3n <\/li>\n<li> Caballero carretero Juan  Antonio (vocal)<\/li>\n<li>eulogio Oset baguena (vocal)<\/li>\n<li>federico S\u00e1nchez nieto (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Manuel Valverde Hermosilla En este trabajo hemos desarrollado un modelo para estudiar las reacciones de dispersion 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 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