{"id":33502,"date":"1997-12-12T00:00:00","date_gmt":"1997-12-12T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/las-simetrias-fundamentales-a-alta-temperatura\/"},"modified":"1997-12-12T00:00:00","modified_gmt":"1997-12-12T00:00:00","slug":"las-simetrias-fundamentales-a-alta-temperatura","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/las-simetrias-fundamentales-a-alta-temperatura\/","title":{"rendered":"Las simetrias fundamentales a alta temperatura."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Silvia Teresa Vargas Castrillon <\/strong><\/h2>\n<p>Las relaciones de dispersi\u00f3n fermionicas en un plasma cuyas interacciones estan controladas por el moledo estandar m\u00ednimo de la f\u00edsica de part\u00edculas han sido calculadas num\u00e9ricamente. Por tanto, hemos obtenido las correcciones de temperatura dominantes y subdominantes en la expansi\u00f3n de alta temperatura, obteni\u00e9ndose as\u00ed resultados originales, tal como la diferencia entre las masas efectivas t\u00e9rmicas de los fermiones en la fase electrodebil rota y en la no rota.  hemos estudiado el comportamiento a alta temperatura de algunas de las simetr\u00edas del modelo estandar, tanto globales como locales, entre las globales, hemos estudiado la simetr\u00eda quiral de la cromodin\u00e1mica cu\u00e1ntica. En lo referente a simetr\u00edas locales, hemos estudiado la simetr\u00eda gauge su(2) x u (1) del modelo estandar tanto en el r\u00e9gimen perturbativo como en el de un higgs acoplado fuertemente correspondiente al r\u00e9gimen no perturbativo. En este \u00faltimo caso, hemos utilizado las t\u00e9cnicas de lagrangianos quirales. Restauraci\u00f3n de simetr\u00edas es la conclusi\u00f3n.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Las simetrias fundamentales a alta temperatura.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Las simetrias fundamentales a alta temperatura. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Silvia Teresa Vargas Castrillon <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Aut\u00f3noma de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 12\/12\/1997<\/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>Belen Gavela Legazpi<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: renaud Pene olivier <\/li>\n<li>Mar\u00eda Jos\u00e9 Herrero solans (vocal)<\/li>\n<li>Luis e. Iba\u00f1ez Santiago (vocal)<\/li>\n<li>nuria Rius dionis (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Silvia Teresa Vargas Castrillon Las relaciones de dispersi\u00f3n fermionicas en un plasma cuyas interacciones estan controladas por [&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":[199,1432,11703],"tags":[30132,14446,15514,58141,91328,91327],"class_list":["post-33502","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-teorica","category-particulas-elementales","tag-belen-gavela-legazpi","tag-luis-e-ibanez-santiago","tag-maria-jose-herrero-solans","tag-nuria-rius-dionis","tag-renaud-pene-olivier","tag-silvia-teresa-vargas-castrillon"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/33502","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=33502"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/33502\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=33502"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=33502"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=33502"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}