{"id":76117,"date":"2005-09-09T00:00:00","date_gmt":"2005-09-09T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/el-efecto-dielectrico-en-teoria-de-cuerdas-y-su-aplicacion-a-la-descripcion-microscopica-de-los-gravitones-gigantes\/"},"modified":"2005-09-09T00:00:00","modified_gmt":"2005-09-09T00:00:00","slug":"el-efecto-dielectrico-en-teoria-de-cuerdas-y-su-aplicacion-a-la-descripcion-microscopica-de-los-gravitones-gigantes","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/el-efecto-dielectrico-en-teoria-de-cuerdas-y-su-aplicacion-a-la-descripcion-microscopica-de-los-gravitones-gigantes\/","title":{"rendered":"El efecto dielectrico en teoria de cuerdas y su aplicacion a la descripcion microscopica de los  gravitones gigantes."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Diego Rodriguez Gomez <\/strong><\/h2>\n<p>El objeto de esta tesis es profundizar en la compresi\u00f3n del efecto diel\u00e9ctrico, y aplicarlo a la descripci\u00f3n microsc\u00f3pica de los gravitones gigantes. M\u00e1s concretamente los resultados obtenidos y expuestos en esta direcci\u00f3n en la tesis propuesta son:  . Gravit\u00f3n gigante en ads7 x s4 y dual en ads4x s7: es el caso m\u00e1s est\u00e1ndar, y en ambos casos debemos construir una s2 no conmutativa.  . Gravit\u00f3n gigantes y dual en ads3  x  s3 x  t4: a priori deberemos construir s1 no conmutativas, lo que no tiene sentido. Veremos que al final, con la ayuda de un escalar de t-dualidad lograremos construirun cilindro no conmutativo.  . Gravit\u00f3n gigante y dual en  ads5  x  s5: aunque a priori debemos construir una s3 no conmutativa, veremos que deberemos ver la s3 como un fibrado de hopf con base s2 y fibre s1. As\u00ed, s\u00f3lo la base s2 ser\u00e1 no conmutativa, mientras que el  u(1) extra ser\u00e1 clave t\u00e9cnicamente en nuestra descripci\u00f3n.  . Gravit\u00f3n gigante en ads4  x  s7  y dual  en  ads7 x s4: muy en sinton\u00edacon el  anterior  veremos que necesitaremos hacer uso de la isometr\u00eda interna en la s5 que ser\u00eda enprincipio el gravit\u00f3n, pero \u00e9sta vez de un modo mucho m\u00e1s elaborado. Al final la variedad no conmutativa a construir es un cp2. creemosque \u00e9ste es el primer ejemplo de un cp2 no conmutativo f\u00edsicamente motivado.  adem\u00e1s se ver\u00e1 en la tesis como la versi\u00f3n de teor\u00eda m propuesta por berenstein, maldacena y nastase en 2002 en el l\u00edmite de penrose de los ads en 11 dimensiones se puede obtener como l\u00edmite de la acci\u00f3n para gravitones coincidentes. usando \u00e9ste hecho en la tesis se expondr\u00e1 la primera descripci\u00f3n microsc\u00f3pica del vac\u00edo invariante so (6) de dicha  teor\u00eda.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>El efecto dielectrico en teoria de cuerdas y su aplicacion a la descripcion microscopica de los  gravitones gigantes.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 El efecto dielectrico en teoria de cuerdas y su aplicacion a la descripcion microscopica de los  gravitones gigantes. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Diego Rodriguez Gomez <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Oviedo<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 09\/09\/2005<\/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>Yolanda Lozano Gomez<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: alfonso V\u00e1zquez ramallo <\/li>\n<li>bert Janssen (vocal)<\/li>\n<li>roberto a. Emparan Garc\u00eda de salazar (vocal)<\/li>\n<li>tomas Otin Miguel (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Diego Rodriguez Gomez El objeto de esta tesis es profundizar en la compresi\u00f3n del efecto diel\u00e9ctrico, y [&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":[199,1432,164310,8846,14443],"tags":[2857,164312,164311,73105,164313,29956],"class_list":["post-76117","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-teorica","category-gravitones","category-oviedo","category-teoria-de-campos","tag-alfonso-vazquez-ramallo","tag-bert-janssen","tag-diego-rodriguez-gomez","tag-roberto-a-emparan-garcia-de-salazar","tag-tomas-otin-miguel","tag-yolanda-lozano-gomez"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/76117","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=76117"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/76117\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=76117"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=76117"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=76117"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}