{"id":50543,"date":"2021-06-07T22:08:09","date_gmt":"2021-06-07T22:08:09","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/modelo-de-estructura-atomica-de-la-aleacion-amorfa-ge-sub-32-se-sub-64-te-sub-04\/"},"modified":"2021-06-07T22:08:09","modified_gmt":"2021-06-07T22:08:09","slug":"modelo-de-estructura-atomica-de-la-aleacion-amorfa-ge-sub-32-se-sub-64-te-sub-04","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/modelo-de-estructura-atomica-de-la-aleacion-amorfa-ge-sub-32-se-sub-64-te-sub-04\/","title":{"rendered":"Modelo de estructura atomica de la aleacion amorfa: ge sub 32 se sub 64 te sub 04."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Gonzalo Alvarez De Toledo Bandeira <\/strong><\/h2>\n<p>La rdf calculada a partir de las intensidades de difraccion de rayos x medidas en dos experimentos presenta un primer maximo en r=2 35 de area 2 48 atomos.  siguiendo el metodo de monte carlo se genero un modelo de estructura -que se ci\u00f1e a las conclusiones obtenidas en el estudio del orden local- que ajusta de modo correcto las curvas experimentales  con o elevado a 2 entre la rdf del modelo y la experimental de 0 0287; tambien otro modelo de fases separadas una de gese sub 2 y la otra de te describe correctamente los datos  con o elevado a 2 = 0 0290. Otros modelos construidos no consiguen un razonable ajuste de algunas zonas de las curvas experimentales. Un analisis de las dos estructuras mas representativas nos permitio encontrar diferencias claras entre ellas  aunque por las conclusiones a las que se llega en un estudio expectroscopico de aleaciones de este sistema y por los resultados obtenidos de la observacion de la muestra por el sem se propone el primero de ellos como mas representativo de la estructura media de la aleacion.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Modelo de estructura atomica de la aleacion amorfa: ge sub 32 se sub 64 te sub 04.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Modelo de estructura atomica de la aleacion amorfa: ge sub 32 se sub 64 te sub 04. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Gonzalo Alvarez De Toledo Bandeira <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Navarra<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1982<\/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>Francisco Sanz Ruiz<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Diego Ramirez Duro <\/li>\n<li>Severino Garcia-blanco Gutierrez (vocal)<\/li>\n<li>Sagrario Martinez Carrera (vocal)<\/li>\n<li>  (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Gonzalo Alvarez De Toledo Bandeira La rdf calculada a partir de las intensidades de difraccion 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 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