{"id":155484,"date":"2026-01-12T17:20:47","date_gmt":"2026-01-12T17:20:47","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/razones-de-ramificacion-y-momentos-electronicos-de-transicion-en-el-nitrogeno-y-oxigeno-moleculares\/"},"modified":"2026-01-12T17:20:47","modified_gmt":"2026-01-12T17:20:47","slug":"razones-de-ramificacion-y-momentos-electronicos-de-transicion-en-el-nitrogeno-y-oxigeno-moleculares","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/razones-de-ramificacion-y-momentos-electronicos-de-transicion-en-el-nitrogeno-y-oxigeno-moleculares\/","title":{"rendered":"Razones de ramificacion y momentos electronicos de transicion en el nitrogeno y oxigeno moleculares."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Rosalino Lorenzo Mu\u00f1iz <\/strong><\/h2>\n<p>En este trabajo se presentan medidas de intensidades de lineas, momentos electronicos de transicion y factores de franck condon, de estados electronicos del segundo sistema positivo de la molecula de n2 y del primer sistema negativo de la molecula de o2+ para ello se han dise\u00f1ado y puesto a punto dos monocromadores de distancia focal de un metro, uno de ellos de tipo seya namioka y el otro de tipo eagle. Se han obtenido las intensidades de 41 bandas del segundo sistema positivo de la molecula de n2 y las intensidades de 20 bandas de la molecula de o2+.  se han determinado tambien las probabilidades de transicion relativas de 80 lineas del ion atomico del o+ comprendidas entre 3700 y 4800 a.  se ha dise\u00f1ado y puesto a punto un sistema experimental para la obtencion de vidas medias de atomos y moleculas de gases reactivos.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Razones de ramificacion y momentos electronicos de transicion en el nitrogeno y oxigeno moleculares.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Razones de ramificacion y momentos electronicos de transicion en el nitrogeno y oxigeno moleculares. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Rosalino Lorenzo Mu\u00f1iz <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Complutense de Madrid<\/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>Jose Campos Gutierrez<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal:  Sanchez Del Rio Y Sierra Carlos <\/li>\n<li> Cabrera Jimenez Juan  Antonio (vocal)<\/li>\n<li> Martin Martinez M. Piedad (vocal)<\/li>\n<li>Antonio Cabello Albala (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Rosalino Lorenzo Mu\u00f1iz En este trabajo se presentan medidas de intensidades de lineas, momentos electronicos de transicion [&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":[986,5506,1271,199,1272],"tags":[22653,76955,4714,269588,269587,5508],"class_list":["post-155484","post","type-post","status-publish","format-standard","hentry","category-complutense-de-madrid","category-espectroscopia-molecular","category-estructura-molecular","category-fisica","category-fisica-molecular","tag-antonio-cabello-albala","tag-cabrera-jimenez-juan-antonio","tag-jose-campos-gutierrez","tag-martin-Martinez-m-piedad","tag-rosalino-lorenzo-muniz","tag-sanchez-del-rio-y-sierra-carlos"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/155484","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=155484"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/155484\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=155484"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=155484"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=155484"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}