{"id":114941,"date":"2013-03-12T00:00:00","date_gmt":"2013-03-12T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/on-supermembrane-in-d4-multiple-m0-brane-in-d11-and-supersymmetric-higher-spin-theories\/"},"modified":"2013-03-12T00:00:00","modified_gmt":"2013-03-12T00:00:00","slug":"on-supermembrane-in-d4-multiple-m0-brane-in-d11-and-supersymmetric-higher-spin-theories","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica-teorica\/on-supermembrane-in-d4-multiple-m0-brane-in-d11-and-supersymmetric-higher-spin-theories\/","title":{"rendered":"On supermembrane in d=4, multiple m0-brane in d=11 and supersymmetric higher spin theories"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Carlos Meliveo Garcia <\/strong><\/h2>\n<p>En este tesis se ha obtenido y estudiado el conjunto completo de las ecuaciones del movimiento en supercampos para el sistema en interacci\u00f3n de supermembrana d=4 y multiplete escalar din\u00e1mico. Este estudio proporciona el primer ejemplo de ecuaciones en supercampos para un sistema en interacci\u00f3n de supercampos de materia y un objeto supersim\u00e9trico extendido, as\u00ed como el primer conjunto de ecuaciones del movimiento en supercampos para un sistema din\u00e1mico que incluye a la supermembrana.Tambi\u00e9n se ha obtenido el conjunto completo de ecuaciones del movimiento para el sistema en interacci\u00f3n de supergravedad din\u00e1mica d=4 n=1 y supermembrana a partir de las ecuaciones en supercampos y, para esto, se ha desarrollado el enfoque de tipo de wess-zumino a la supergravedad minimal especial de grisaru-siegel-gates-ovrut-waldram, caracterizada por una constante cosmol\u00f3gica generada din\u00e1micamente. En el sistema en interacci\u00f3n, la supermembrana produce una renormalizaci\u00f3n de dicha constante cosmol\u00f3gica, por lo que su valor es diferente en las dos ramas del espaciotiempo separadas por el volumen-mundo de la supermembrana.Se han encontrado las ecuaciones en supercampos en superespacios tensoriales n-extendidos con n=2, 4, 8 que describen los supermultipletes d=4(,6,10) de la teor\u00eda de campos conformes de espines altos sin masa.Hemos obtenido y estudiado las ecuaciones del movimiento del sistema de m\u00faltiples m0-branas (mm0) que se derivan de la acci\u00f3n supersim\u00e9trica covariante y kappa-sim\u00e9trica. Se ha demostrado que todos los esatdos bps del sistema son 1\/2 bps, preservan 1\/2 de supersimetr\u00eda, y tienen las mismas propiedades  que los estados bps de una sola m0-brama.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>On supermembrane in d=4, multiple m0-brane in d=11 and supersymmetric higher spin theories<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 On supermembrane in d=4, multiple m0-brane in d=11 and supersymmetric higher spin theories <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Carlos Meliveo Garcia <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Pa\u00eds vasco\/euskal herriko unibertsitatea<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 03\/12\/2013<\/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>Igor Bandos<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Jos\u00e9 adolfo Azc\u00e1rraga feliu <\/li>\n<li>dmytro Sorokin &#8212; (vocal)<\/li>\n<li>yolanda Lozano g\u00f3mez (vocal)<\/li>\n<li>i\u00f1igo Luis Egusquiza egusquiza (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Carlos Meliveo Garcia En este tesis se ha obtenido y estudiado el conjunto completo de las ecuaciones [&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":[1432,12909],"tags":[227618,227619,118938,227620,197848,29956],"class_list":["post-114941","post","type-post","status-publish","format-standard","hentry","category-fisica-teorica","category-pais-vasco-euskal-herriko-unibertsitatea","tag-carlos-meliveo-garcia","tag-dmytro-sorokin","tag-igor-bandos","tag-inigo-luis-egusquiza-egusquiza","tag-jose-adolfo-azcarraga-feliu","tag-yolanda-lozano-gomez"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/114941","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=114941"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/114941\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=114941"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=114941"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=114941"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}