{"id":137002,"date":"2026-01-12T17:02:03","date_gmt":"2026-01-12T17:02:03","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/optica-de-rayos-x-para-lineas-de-radiacion-de-sincrotron-y-aplicacion-de-la-espectroscopia-de-absorcion-de-rayos-x-al-estudio-de-materiales-ordenados-y-desordenados-de-metales-de-transicion\/"},"modified":"2026-01-12T17:02:03","modified_gmt":"2026-01-12T17:02:03","slug":"optica-de-rayos-x-para-lineas-de-radiacion-de-sincrotron-y-aplicacion-de-la-espectroscopia-de-absorcion-de-rayos-x-al-estudio-de-materiales-ordenados-y-desordenados-de-metales-de-transicion","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/optica-de-rayos-x-para-lineas-de-radiacion-de-sincrotron-y-aplicacion-de-la-espectroscopia-de-absorcion-de-rayos-x-al-estudio-de-materiales-ordenados-y-desordenados-de-metales-de-transicion\/","title":{"rendered":"Optica de rayos x para lineas de radiacion de sincrotron y aplicacion de la espectroscopia de absorcion de rayos x al estudio de materiales ordenados y desordenados de metales de transicion."},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Sanchez Del Rio Manuel <\/strong><\/h2>\n<p>Presentamos un estudio de optica de rayos x duros para radiacion de sincrotron. Se desarrollaron modelos teoricos para la difraccion de rayos x y se implementaron en un programa de trazado de rayos x \u00abshadow\u00bb. En particular se consideraron, cristales tallados asimetricamente, curvados y cristales mosaico. Se dise\u00f1o la optica de un monocromador focalizante para el laboratorio scow de frascati.  en una segunda parte se estudian dos tipos de materiales mediante la espectroscopia de absorcion de rayos x.  i) soluciones diluidas de metales de transicion.  ii) impurezas diluidas de metales de transicion en cristales de mgo.  el analisis de los datos se realizara por comparacion directa de los datos experimentales con calculos tecnicos \u00abab initio\u00bb, basados en el formalismo multiple scattering.  se aislaron contribuciones de multiple scattering en los espectros exafs de las soluciones.  se determino el lugar de localizacion de las impurezas en la matriz mgo y la evolucion de estas impurezas al tratar el material termoquimicamente.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Optica de rayos x para lineas de radiacion de sincrotron y aplicacion de la espectroscopia de absorcion de rayos x al estudio de materiales ordenados y desordenados de metales de transicion.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Optica de rayos x para lineas de radiacion de sincrotron y aplicacion de la espectroscopia de absorcion de rayos x al estudio de materiales ordenados y desordenados de metales de transicion. <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Sanchez Del Rio Manuel <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Zaragoza<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1991<\/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>Joaquin Garcia Ruiz<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Domingo Gonzalez Alvarez <\/li>\n<li>Renzo Natoli Calogero (vocal)<\/li>\n<li>Felix Yndurain Mu\u00f1oz (vocal)<\/li>\n<li>Adolfo Savoia (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Sanchez Del Rio Manuel Presentamos un estudio de optica de rayos x duros para radiacion de sincrotron. [&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":[49616,199,1008,6064,1525,13610],"tags":[251525,13308,14806,72292,104772,251524],"class_list":["post-137002","post","type-post","status-publish","format-standard","hentry","category-espectroscopia-optica-de-absorcion","category-fisica","category-fisica-del-estado-solido","category-interaccion-de-la-radiacion-con-los-solidos","category-optica","category-zaragoza","tag-adolfo-savoia","tag-domingo-gonzalez-alvarez","tag-felix-yndurain-munoz","tag-joaquin-garcia-ruiz","tag-renzo-natoli-calogero","tag-sanchez-del-rio-manuel"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/137002","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=137002"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/137002\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=137002"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=137002"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=137002"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}