{"id":495,"date":"2024-09-13T12:38:01","date_gmt":"2024-09-13T10:38:01","guid":{"rendered":"https:\/\/www.upo.es\/inmalab\/?page_id=495"},"modified":"2024-09-26T08:35:08","modified_gmt":"2024-09-26T06:35:08","slug":"difraccion-de-rayos-x","status":"publish","type":"page","link":"https:\/\/www.upo.es\/inmalab\/difraccion-de-rayos-x\/","title":{"rendered":"Difracci\u00f3n de rayos X"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"495\" class=\"elementor elementor-495\">\n\t\t\t\t<div class=\"elementor-element elementor-element-42cd071 e-con-full e-flex e-con e-parent\" data-id=\"42cd071\" data-element_type=\"container\" data-settings=\"{&quot;background_background&quot;:&quot;classic&quot;}\">\n\t\t\t\t<div class=\"elementor-element elementor-element-4f5f877 elementor-widget elementor-widget-heading\" data-id=\"4f5f877\" data-element_type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h2 class=\"elementor-heading-title elementor-size-default\">Difracci\u00f3n de rayos X<\/h2>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t<div class=\"elementor-element elementor-element-cb3fcee e-grid e-con-boxed e-con e-parent\" data-id=\"cb3fcee\" data-element_type=\"container\">\n\t\t\t\t\t<div class=\"e-con-inner\">\n\t\t\t\t<div class=\"elementor-element elementor-element-5cdfe2c elementor-widget elementor-widget-text-editor\" data-id=\"5cdfe2c\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<h4>\u00a0<\/h4><p><img fetchpriority=\"high\" decoding=\"async\" class=\"wp-image-2089  alignleft\" src=\"https:\/\/www.upo.es\/inmalab\/wp-content\/uploads\/2024\/09\/XRD-1024x768.jpg\" alt=\"\" width=\"284\" height=\"213\" \/>La difracci\u00f3n de rayos X se basa en la interacci\u00f3n de los rayos X con la estructura at\u00f3mica de un material. Cuando un haz de rayos X incide sobre una muestra cristalina, los electrones en los \u00e1tomos difractan la radiaci\u00f3n en distintas direcciones. Debido a la disposici\u00f3n peri\u00f3dica de los \u00e1tomos en el cristal, los rayos difractados pueden interferir constructivamente en ciertas direcciones cuando se satisface la ley de Bragg.<\/p><p style=\"text-align: left;\">El Laboratorio de Difracci\u00f3n de Rayos X de INMALAB est\u00e1 concebido para ofrecer soluciones integrales a investigadores y empresas de diversos sectores, como el minero, aeroespacial y muchos m\u00e1s. Contamos con equipos de \u00faltima generaci\u00f3n que permiten realizar an\u00e1lisis detallados de estructura cristalina, identificaci\u00f3n de fases y caracterizaci\u00f3n de tensiones residuales en diferentes materiales.<\/p><p style=\"text-align: left;\">Nuestro laboratorio est\u00e1 equipado con tecnolog\u00eda avanzada que incluye difract\u00f3metros de alta precisi\u00f3n, capaces de realizar an\u00e1lisis en polvo, s\u00f3lidos y pel\u00edculas delgadas, as\u00ed como t\u00e9cnicas de microdifracci\u00f3n para estudios localizados. Adem\u00e1s, ofrecemos servicios especializados de mapeo del espacio rec\u00edproco, reflectometr\u00eda y an\u00e1lisis de texturas. Con el respaldo de un equipo de expertos, INMALAB est\u00e1 preparado para atender las necesidades espec\u00edficas de cada proyecto, proporcionando resultados precisos y fiables en cada estudio.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t<div class=\"elementor-element elementor-element-c357bea e-flex e-con-boxed e-con e-parent\" data-id=\"c357bea\" data-element_type=\"container\">\n\t\t\t\t\t<div class=\"e-con-inner\">\n\t\t\t\t<div class=\"elementor-element elementor-element-ac2fdbc e-n-tabs-mobile elementor-widget elementor-widget-n-tabs\" data-id=\"ac2fdbc\" data-element_type=\"widget\" data-settings=\"{&quot;tabs_justify_horizontal&quot;:&quot;start&quot;,&quot;horizontal_scroll&quot;:&quot;disable&quot;}\" data-widget_type=\"nested-tabs.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<div class=\"e-n-tabs\" data-widget-number=\"180551100\" aria-label=\"Pesta\u00f1as. Abre elementos con Intro o Espacio, ci\u00e9rralos con Escape y navega con las fechas.\">\n\t\t\t<div class=\"e-n-tabs-heading\" role=\"tablist\">\n\t\t\t\t\t<button id=\"e-n-tab-title-1805511001\" class=\"e-n-tab-title\" aria-selected=\"true\" data-tab-index=\"1\" role=\"tab\" tabindex=\"0\" aria-controls=\"e-n-tab-content-1805511001\" style=\"--n-tabs-title-order: 1;\">\n\t\t\t\t\t\t<span class=\"e-n-tab-title-text\">\n\t\t\t\tEquipamiento\t\t\t<\/span>\n\t\t<\/button>\n\t\t\t\t<button id=\"e-n-tab-title-1805511002\" class=\"e-n-tab-title\" aria-selected=\"false\" data-tab-index=\"2\" role=\"tab\" tabindex=\"-1\" aria-controls=\"e-n-tab-content-1805511002\" style=\"--n-tabs-title-order: 2;\">\n\t\t\t\t\t\t<span class=\"e-n-tab-title-text\">\n\t\t\t\tAccesorios\t\t\t<\/span>\n\t\t<\/button>\n\t\t\t\t<button id=\"e-n-tab-title-1805511003\" class=\"e-n-tab-title\" aria-selected=\"false\" data-tab-index=\"3\" role=\"tab\" tabindex=\"-1\" aria-controls=\"e-n-tab-content-1805511003\" style=\"--n-tabs-title-order: 3;\">\n\t\t\t\t\t\t<span class=\"e-n-tab-title-text\">\n\t\t\t\tLaboratorio\t\t\t<\/span>\n\t\t<\/button>\n\t\t\t\t\t<\/div>\n\t\t\t<div class=\"e-n-tabs-content\">\n\t\t\t\t<div id=\"e-n-tab-content-1805511001\" role=\"tabpanel\" aria-labelledby=\"e-n-tab-title-1805511001\" data-tab-index=\"1\" style=\"--n-tabs-title-order: 1;\" class=\"e-active elementor-element elementor-element-ba4a5fa e-flex e-con-boxed e-con e-child\" data-id=\"ba4a5fa\" data-element_type=\"container\">\n\t\t\t\t\t<div class=\"e-con-inner\">\n\t\t<div class=\"elementor-element elementor-element-1a83001 e-con-full e-flex e-con e-child\" data-id=\"1a83001\" data-element_type=\"container\">\n\t\t\t\t<div class=\"elementor-element elementor-element-838159a elementor-widget elementor-widget-heading\" data-id=\"838159a\" data-element_type=\"widget\" data-widget_type=\"heading.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t<h6 class=\"elementor-heading-title elementor-size-default\">Bruker D8 Discover<\/h6>\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<div class=\"elementor-element elementor-element-39372ba elementor-widget elementor-widget-text-editor\" data-id=\"39372ba\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<p>El D8 DISCOVER es un difract\u00f3metro de Rayos X vers\u00e1til y de alto resoluci\u00f3n, Dise\u00f1ado para la caracterizaci\u00f3n estructural de una amplia gama de materiales, desde polvo, materiales amorfos y policristalinos hasta capas delgadas en condiciones ambientales o atm\u00f3sfera inerte. Equipado con una microfuente, permite realizar microdifracci\u00f3n con resoluci\u00f3n espacial precisa, as\u00ed como mediciones con incidencia rasante o reflectometr\u00eda. Adem\u00e1s, ofrece la capacidad de llevar a cabo estudios de tensiones residuales y an\u00e1lisis de texturas. Este equipo incluye un detector Eiger-200K de \u00faltima generaci\u00f3n, que posibilita la adquisici\u00f3n de datos de difracci\u00f3n en dos dimensiones, proporcionando una visi\u00f3n completa y detallada de las muestras analizadas.<\/p>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t<div id=\"e-n-tab-content-1805511002\" role=\"tabpanel\" aria-labelledby=\"e-n-tab-title-1805511002\" data-tab-index=\"2\" style=\"--n-tabs-title-order: 2;\" class=\" elementor-element elementor-element-44c618a e-con-full e-flex e-con e-child\" data-id=\"44c618a\" data-element_type=\"container\">\n\t\t<div class=\"elementor-element elementor-element-12bfcb3 e-flex e-con-boxed e-con e-child\" data-id=\"12bfcb3\" data-element_type=\"container\">\n\t\t\t\t\t<div class=\"e-con-inner\">\n\t\t\t\t<div class=\"elementor-element elementor-element-3416576 elementor-widget elementor-widget-text-editor\" data-id=\"3416576\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t\t<ul><li>Cuna de Euler: Integra las rotaciones chi y phi y traslaciones x-y-z en un \u00fanico soporte de muestras, otorgando 5 grados de libertad.<\/li><li>Panoramic evacuated flight tube de 350 mm: Minimiza la dispersi\u00f3n del haz de rayos x difractados, mejorando la relaci\u00f3n se\u00f1al-ruido.<\/li><li>Colimadores de 0.1, 0.5, 1 y 2 mm.<\/li><li>Portamuestras \u00a0de PMMA o cuarzo para an\u00e1lisis de polvo polvo PMMA.<\/li><li>Portamuestra \u00a0de PMMA para an\u00e1lisis de polvo en atm\u00f3sfera inerte.<\/li><li>Portamuestra de Silicio <em>zero-background<\/em> para an\u00e1lisis de polvo.<\/li><li>Portamuestra de Silicio <em>zero-background<\/em>\u00a0con c\u00fapula para an\u00e1lisis en atm\u00f3sfera inerte.<\/li><\/ul>\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t<div id=\"e-n-tab-content-1805511003\" role=\"tabpanel\" aria-labelledby=\"e-n-tab-title-1805511003\" data-tab-index=\"3\" style=\"--n-tabs-title-order: 3;\" class=\" elementor-element elementor-element-18ee37c e-con-full e-flex e-con e-child\" data-id=\"18ee37c\" data-element_type=\"container\">\n\t\t\t\t<div class=\"elementor-element elementor-element-e4453fa elementor-icon-list--layout-traditional elementor-list-item-link-full_width elementor-widget elementor-widget-icon-list\" data-id=\"e4453fa\" data-element_type=\"widget\" data-widget_type=\"icon-list.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t<ul class=\"elementor-icon-list-items\">\n\t\t\t\t\t\t\t<li class=\"elementor-icon-list-item\">\n\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-icon-list-icon\">\n\t\t\t\t\t\t\t<svg aria-hidden=\"true\" class=\"e-font-icon-svg e-fas-map-marker-alt\" viewBox=\"0 0 384 512\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\"><path d=\"M172.268 501.67C26.97 291.031 0 269.413 0 192 0 85.961 85.961 0 192 0s192 85.961 192 192c0 77.413-26.97 99.031-172.268 309.67-9.535 13.774-29.93 13.773-39.464 0zM192 272c44.183 0 80-35.817 80-80s-35.817-80-80-80-80 35.817-80 80 35.817 80 80 80z\"><\/path><\/svg>\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-icon-list-text\">Universidad Pablo de Olavide<br>Edificio 47, Planta Baja Lab. B05<\/span>\n\t\t\t\t\t\t\t\t\t<\/li>\n\t\t\t\t\t\t\t\t<li class=\"elementor-icon-list-item\">\n\t\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-icon-list-icon\">\n\t\t\t\t\t\t\t<svg aria-hidden=\"true\" class=\"e-font-icon-svg e-fas-user\" viewBox=\"0 0 448 512\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\"><path d=\"M224 256c70.7 0 128-57.3 128-128S294.7 0 224 0 96 57.3 96 128s57.3 128 128 128zm89.6 32h-16.7c-22.2 10.2-46.9 16-72.9 16s-50.6-5.8-72.9-16h-16.7C60.2 288 0 348.2 0 422.4V464c0 26.5 21.5 48 48 48h352c26.5 0 48-21.5 48-48v-41.6c0-74.2-60.2-134.4-134.4-134.4z\"><\/path><\/svg>\t\t\t\t\t\t<\/span>\n\t\t\t\t\t\t\t\t\t\t<span class=\"elementor-icon-list-text\">Francisco Javier Garc\u00eda Moscoso<\/span>\n\t\t\t\t\t\t\t\t\t<\/li>\n\t\t\t\t\t\t<\/ul>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>Difracci\u00f3n de rayos X \u00a0 La difracci\u00f3n de rayos X se basa en la interacci\u00f3n de los rayos X con la estructura at\u00f3mica de un material. Cuando un haz de rayos X incide sobre una muestra cristalina, los electrones en los \u00e1tomos difractan la radiaci\u00f3n en distintas direcciones. Debido a la disposici\u00f3n peri\u00f3dica de los [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"elementor_header_footer","meta":{"site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"full-width-container","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":"disabled","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":"set","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"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-opacity":"","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-opacity":"","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-opacity":"","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-opacity":"","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-opacity":"","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-opacity":"","overlay-gradient":""}},"footnotes":""},"class_list":["post-495","page","type-page","status-publish","hentry"],"rttpg_featured_image_url":null,"rttpg_author":{"display_name":"inmalab","author_link":"https:\/\/www.upo.es\/inmalab\/author\/inmalab\/"},"rttpg_comment":0,"rttpg_category":null,"rttpg_excerpt":"Difracci\u00f3n de rayos X \u00a0 La difracci\u00f3n de rayos X se basa en la interacci\u00f3n de los rayos X con la estructura at\u00f3mica de un material. Cuando un haz de rayos X incide sobre una muestra cristalina, los electrones en los \u00e1tomos difractan la radiaci\u00f3n en distintas direcciones. Debido a la disposici\u00f3n peri\u00f3dica de los&hellip;","_links":{"self":[{"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/pages\/495","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/comments?post=495"}],"version-history":[{"count":95,"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/pages\/495\/revisions"}],"predecessor-version":[{"id":2098,"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/pages\/495\/revisions\/2098"}],"wp:attachment":[{"href":"https:\/\/www.upo.es\/inmalab\/wp-json\/wp\/v2\/media?parent=495"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}