{"id":63109,"date":"2018-03-09T22:51:02","date_gmt":"2018-03-09T22:51:02","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/estudio-de-las-regularidades-en-el-ensanchamiento-stark-de-los-gases-nobles-una-vez-ionizados\/"},"modified":"2018-03-09T22:51:02","modified_gmt":"2018-03-09T22:51:02","slug":"estudio-de-las-regularidades-en-el-ensanchamiento-stark-de-los-gases-nobles-una-vez-ionizados","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica-atomica\/estudio-de-las-regularidades-en-el-ensanchamiento-stark-de-los-gases-nobles-una-vez-ionizados\/","title":{"rendered":"Estudio de las regularidades en el ensanchamiento stark de los gases nobles una vez ionizados"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Ram\u00f3n Javier Pel\u00e1ez De Fuentes <\/strong><\/h2>\n<p>En esta tesis se presentan las medidas de par\u00e1metros stark de algunos gases nobles ionizados. Estos par\u00e1metros at\u00f3micos se han medido en un plasma generado por descarga pulsada. La densidad de electrones, n_e, est\u00e1 en torno a 10^23 m^-3 y la temperatura electr\u00f3nica, t_e, var\u00eda de 2 a 4 ev dependiendo del experimento. Se ha analizado espectrosc\u00f3picamente la luz emergente de una regi\u00f3n homog\u00e9nea del plasma. Utilizando instrumentaci\u00f3n espectrosc\u00f3pica de gran resoluci\u00f3n se han registrado las l\u00edneas espectrales con una precisi\u00f3n del orden de pm. Mediante ajustes del tipo anchura-n_e y desplazamiento-n_e, se ha calibrado la anchura y el desplazamiento stark para cada una de las l\u00edneas.  en total se han medido m\u00e1s de 80 par\u00e1metros stark para l\u00edneas de ne ii, 180 para xe ii y 80 para xe iii. Pr\u00e1cticamente la mitad de estos par\u00e1metros son completamente nuevos en la bibliograf\u00eda.  la segunda parte de la tesis ha consistido en analizar las tendencias sistem\u00e1ticas que presentan las anchuras stark a lo largo de la serie hom\u00f3loga de los gases nobles ionizados i.E. Ne ii, ar ii, kr ii y xe ii. Se ha analizado la relaci\u00f3n entre la anchura stark y la energ\u00eda de ionizaci\u00f3n del nivel superior de la transici\u00f3n y el n\u00famero at\u00f3mico. Se han mejorado los ajustes anteriores, siendo el error promedio inferior al 20%, valor realmente bajo para este tipo de ajustes.  las tendencias obtenidas y los par\u00e1metros medidos en este trabajo tienen dos aplicaciones fundamentalmente. (1) diagn\u00f3stico no intrusivo de plasmas de car\u00e1cter industrial, astrof\u00edsico o bien de las zonas fr\u00edas de los plasmas de fusi\u00f3n. (2) predicci\u00f3n precisa de par\u00e1metros stark no medidos y mejora de los modelos te\u00f3ricos de predicci\u00f3n de par\u00e1metros stark.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Estudio de las regularidades en el ensanchamiento stark de los gases nobles una vez ionizados<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Estudio de las regularidades en el ensanchamiento stark de los gases nobles una vez ionizados <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Ram\u00f3n Javier Pel\u00e1ez De Fuentes <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Valladolid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 25\/02\/2008<\/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>Santiago Mar Sarda\u00f1a<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: julio alfonso Alonso mart\u00edn <\/li>\n<li>Luis Roso franco (vocal)<\/li>\n<li>bernardo Zurro hern\u00e1ndez (vocal)<\/li>\n<li>Antonio Sola d\u00edaz (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Ram\u00f3n Javier Pel\u00e1ez De Fuentes En esta tesis se presentan las medidas de par\u00e1metros stark de algunos [&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":[23557,5086,10842,12451],"tags":[95540,31875,136255,12394,139351,10846],"class_list":["post-63109","post","type-post","status-publish","format-standard","hentry","category-espectroscopia-optica-de-emision","category-fisica-atomica","category-fisica-de-plasmas","category-valladolid","tag-antonio-sola-diaz","tag-bernardo-zurro-hernandez","tag-julio-alfonso-alonso-martin","tag-luis-roso-franco","tag-ramon-javier-pelaez-de-fuentes","tag-santiago-mar-sardana"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/63109","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=63109"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/63109\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=63109"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=63109"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=63109"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}