{"id":143868,"date":"1993-01-01T00:00:00","date_gmt":"1993-01-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/determinacion-de-parametros-electrodebiles-del-modelo-estandar-por-medio-de-la-reaccion-ee-tt-en-el-detector-delphi-del-acelerador-lep\/"},"modified":"1993-01-01T00:00:00","modified_gmt":"1993-01-01T00:00:00","slug":"determinacion-de-parametros-electrodebiles-del-modelo-estandar-por-medio-de-la-reaccion-ee-tt-en-el-detector-delphi-del-acelerador-lep","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/determinacion-de-parametros-electrodebiles-del-modelo-estandar-por-medio-de-la-reaccion-ee-tt-en-el-detector-delphi-del-acelerador-lep\/","title":{"rendered":"Determinacion de parametros electrodebiles del modelo estandar por medio de la reaccion e+e-  t+t- en el detector delphi del acelerador lep."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Francisco Matorras   Weinig <\/strong><\/h2>\n<p>Dentro del colisionador electron positron lep, trabajando a una energia centro de masas en torno a la resonancia del z, se ha estudiado el acoplamiento del lepton mas pesado de los conocidos, el    con este boson de intercambio comprobando asi aspectos fundamentales del sector electrodebil del modelo estandar de la fisica de particulas. Para ello se han medido distintos observables basicos de la reaccion e+e- 2+2-, la seccion eficaz, la asimetria de carga, la polarizacion promedio y la asimetria de polarizacion, utilizando los cerca de 500000z detectados y registrados por delphi durante los a\u00f1os 1990 y 1991.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Determinacion de parametros electrodebiles del modelo estandar por medio de la reaccion e+e-  t+t- en el detector delphi del acelerador lep.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Determinacion de parametros electrodebiles del modelo estandar por medio de la reaccion e+e-  t+t- en el detector delphi del acelerador lep. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Francisco Matorras   Weinig <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Cantabria<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1993<\/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>Alberto Ruiz Jimeno<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Enrique Fernandez Sanchez <\/li>\n<li>Marcos Cerrada Canales (vocal)<\/li>\n<li>Antonio Pich Zardoya (vocal)<\/li>\n<li>Pedro Trancoso Vaz (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Francisco Matorras Weinig Dentro del colisionador electron positron lep, trabajando a una energia centro de masas en [&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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