{"id":52894,"date":"2006-02-06T00:00:00","date_gmt":"2006-02-06T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/metodos-de-gran-n-aplicados-a-holografa%c2%ada-y-equivalencia-planar\/"},"modified":"2006-02-06T00:00:00","modified_gmt":"2006-02-06T00:00:00","slug":"metodos-de-gran-n-aplicados-a-holografa%c2%ada-y-equivalencia-planar","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/metodos-de-gran-n-aplicados-a-holografa%c2%ada-y-equivalencia-planar\/","title":{"rendered":"M\u00e9todos de gran n aplicados a holograf\u00eday equiValencia planar."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Carlos Hoyos Badajoz <\/strong><\/h2>\n<p>Antecedentes y estado actual:  uno de los temas actuales de investigaci\u00f3n m\u00e1s importantes dentro del campo de f\u00edsica te\u00f3rica de altas energ\u00edas es la correspondencia entre teor\u00edas gauge y teor\u00edas de gravedad. Seg\u00fan la correspondencia, ambas teor\u00edas son equivalentes bajo una identificaci\u00f3n adecuada de cantidades duales. En la dualidad juega un papel muy importante el hecho de que el rango del grupo gauge sea muy grande (gran n). En su mayor parte, la dualidad se ha estudiado en el l\u00edmite en que n es infinito (planar). Sin embargo, aunque correcciones de tipo 1\/n podr\u00edan modificar dr\u00e1sticamente la equiValencia, todav\u00eda no se sabe muy bien c\u00f3mo implementarlas.  por otro lado, la dualidad se establece cuando la teor\u00eda gauge est\u00e1 a acoplo fuerte, de forma que la curvatura del dual gravitatorio es peque\u00f1a. De esta forma, propiedades no perturbativas que no se pod\u00edan estudiar anal\u00edticamente en la teor\u00eda gauge, pueden ser extra\u00eddas de su dual gravitatorio. Actualmente se conocen modelos con diversas propiedades, incluyendo confinamiento, quarks, etc, por lo que se piensa que de esta forma se puede llegar a describir la f\u00edsica de las interacciones fuertes. Es e gran inter\u00e9s por tanto establecer c\u00f3mo las diversas caracter\u00edsticas de la teor\u00eda gauge est\u00e1n codificadas en la geometr\u00eda dual.  otra l\u00ednea de investigaci\u00f3n relacionada es la de equiValencia planar entre teor\u00eda supersim\u00e9tricas y teor\u00edas que no lo son. Muchas de las propiedades no perturbativas, para las que no hay una descripci\u00f3n rigurosa en el caso no supersim\u00e9trico, pueden describirse exactamente gracias a la supersimetr\u00eda. la equiValencia implicar\u00eda que los resultados obtenidos podr\u00edan trasladarse inmediatamente de unas a otras. Sin embargo, la validez de la equiValencia a nivel no perturbativo no est\u00e1 completamente establecida.  contenidos:  en primer lugar, se estudia c\u00f3mo la geometr\u00eda cl\u00e1sica de teor\u00edas garvitatorias se ve modificada cua<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>M\u00e9todos de gran n aplicados a holograf\u00eday equiValencia planar.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 M\u00e9todos de gran n aplicados a holograf\u00eday equiValencia planar. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Carlos Hoyos Badajoz <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Aut\u00f3noma de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 02\/06\/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>Jos\u00e9 Luis Fernandez Barbon<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Luis \u00e1lvarez gaum\u00e9 <\/li>\n<li>c\u00e9sar G\u00f3mez l\u00f3pez (vocal)<\/li>\n<li>alfonso V\u00e1zquez ramallo (vocal)<\/li>\n<li>Antonio Gonz\u00e1lez-arroyo espa\u00f1a (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Carlos Hoyos Badajoz Antecedentes y estado actual: uno de los temas actuales de investigaci\u00f3n m\u00e1s importantes dentro 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