{"id":54280,"date":"2018-03-09T22:42:00","date_gmt":"2018-03-09T22:42:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/termodinamica-de-d-particulas-en-el-imf-y-algunas-precisiones-importantes-sobre-el-problema-de-hagedorn\/"},"modified":"2018-03-09T22:42:00","modified_gmt":"2018-03-09T22:42:00","slug":"termodinamica-de-d-particulas-en-el-imf-y-algunas-precisiones-importantes-sobre-el-problema-de-hagedorn","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/termodinamica-de-d-particulas-en-el-imf-y-algunas-precisiones-importantes-sobre-el-problema-de-hagedorn\/","title":{"rendered":"Termodinamica de   d  particulas en el imf y algunas precisiones importantes sobre el problema de hagedorn."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Mar\u00eda Suarez Diez <\/strong><\/h2>\n<p>En la primera parte se estudia la funci\u00f3n de partici\u00f3n can\u00f3nica de una \u00fanica part\u00edcula en un espacio tiempo de once dimensiones, con una dimensi\u00f3n espacial compactificada en un c\u00edrculo de radio r. Se calcula primero para un observador gen\u00e9rico que, cuando lleva r a infinito,  recupera la covariancia lorentz en 11 dimensiones y despu\u00e9s para un observador en el imf. El objeto de este an\u00e1lisis es estudiar c\u00f3mo este observador recobra la covariancia en 11 dimensiones y aclarar la relaci\u00f3n entre la acci\u00f3n de dirac-born-infeld y la acci\u00f3n de super-yang-mills, que es la que corresponde a la descripci\u00f3n de la teor\u00eda de matrices en este sistema  de referencia  tan particular: el imf.  en la segunda parte de la tesis se estudian los efectos de la temperatura sobre gases ideales de cuerdas, prestando especial inter\u00e9s a  el efecto de la topolog\u00eda del espacio en el que se propagan las cuerdas y la importancia de la elecci\u00f3n de uno u otro colectivo estad\u00edstico en las conclusiones extra\u00eddas.  &#8211; cuerdas abiertas en un espacio abierto o con las dimensiones compactificadas en c\u00edrculos cuyos radios tienden a infinito, a energ\u00eda y temperatura fija y con potencial qu\u00edmico cero. Ambas descripciones son equivalentes a pesar de la ruptura de equipartici\u00f3n.  &#8211; cuerdas cerradas movi\u00e9ndose en un espacio toroidal de dimensiones tales que las cuerdas se pueden enrollar en \u00e9stas. Aqu\u00ed nuestros resultados difieren de los expuestos en el ya cl\u00e1sico trabajo de brandenberger  y  vafa.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Termodinamica de   d  particulas en el imf y algunas precisiones importantes sobre el problema de hagedorn.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Termodinamica de   d  particulas en el imf y algunas precisiones importantes sobre el problema de hagedorn. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Mar\u00eda Suarez Diez <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Oviedo<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 21\/07\/2006<\/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>Miguel Angel Ramos Osorio<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal:  Ma\u00f1es palacio Juan  Luis <\/li>\n<li>Jos\u00e9 Luis Fernandez barbon (vocal)<\/li>\n<li> Vazquez  mozo Miguel angel (vocal)<\/li>\n<li>tomas Ortin Miguel (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Mar\u00eda Suarez Diez En la primera parte se estudia la funci\u00f3n de partici\u00f3n can\u00f3nica de una \u00fanica [&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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