{"id":131688,"date":"1996-01-01T00:00:00","date_gmt":"1996-01-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/desarrollo-de-un-modelo-teorico-para-la-interpretacion-de-difractogramas-de-rayos-x-de-alta-resolucion\/"},"modified":"1996-01-01T00:00:00","modified_gmt":"1996-01-01T00:00:00","slug":"desarrollo-de-un-modelo-teorico-para-la-interpretacion-de-difractogramas-de-rayos-x-de-alta-resolucion","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/ciencias-tecnologicas\/desarrollo-de-un-modelo-teorico-para-la-interpretacion-de-difractogramas-de-rayos-x-de-alta-resolucion\/","title":{"rendered":"Desarrollo de un modelo teorico para la interpretacion de difractogramas de rayos x de alta resolucion."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Alfredo Sanz Hervas <\/strong><\/h2>\n<p>En esta tesis doctoral se desarrolla un modelo de simulacion de difractogramas de rayos x de alta resolucion. Para ello se ha utilizado la teoria dinamica de difraccion y un modelo de elasticidad anisotropa aplicable a cristales con cualquier orientacion. El modelo teorico se aplica a la caracterizacion de estructuras de pozo cuantico multiple de ingaas\/gaas sobre sustratos de gaas con orientacion (001) y (111) b.  se demuestra la correccion del modelo de difraccion para la caracterizacion de este tipo de estructuras. Los parametros estructurales obtenidos concuerdan con los de otras tecnicas como fotoluminiscencia, fotocorriente y microscopia electronica. Se ha hecho un estudio de la relajacion en estas estructuras, encontrando un buen ajuste con un modelo de relajacion establecido.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Desarrollo de un modelo teorico para la interpretacion de difractogramas de rayos x de alta resolucion.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Desarrollo de un modelo teorico para la interpretacion de difractogramas de rayos x de alta resolucion. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Alfredo Sanz Hervas <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Polit\u00e9cnica de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1996<\/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> Abril Domingo Evaristo Jose<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Miguel Aguilar Fernandez <\/li>\n<li>Miguel Lopez Coronado (vocal)<\/li>\n<li>Elias Mu\u00f1oz Merino (vocal)<\/li>\n<li>Juan Barbolla Sanchez (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Alfredo Sanz Hervas En esta tesis doctoral se desarrolla un modelo de simulacion de difractogramas de rayos [&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":[332,9195,16187,16008,3706],"tags":[58645,78165,14753,9633,30700,12555],"class_list":["post-131688","post","type-post","status-publish","format-standard","hentry","category-ciencias-tecnologicas","category-diseno-de-circuitos","category-dispositivos-fotoelectricos","category-politecnica-de-madrid","category-tecnologia-electronica","tag-abril-domingo-evaristo-jose","tag-alfredo-sanz-hervas","tag-elias-munoz-merino","tag-juan-barbolla-sanchez","tag-miguel-aguilar-fernandez","tag-miguel-lopez-coronado"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/131688","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=131688"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/131688\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=131688"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=131688"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=131688"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}