{"id":47361,"date":"2020-04-08T22:55:24","date_gmt":"2020-04-08T22:55:24","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/calculo-teorico-de-los-espectros-ii-electronicos-de-los-derivados-mono-y-dihidroxilados-del-11-elevado-a-1-22-elevado-a-1-y-12-elevado-a-1-azonaftaleno\/"},"modified":"2020-04-08T22:55:24","modified_gmt":"2020-04-08T22:55:24","slug":"calculo-teorico-de-los-espectros-ii-electronicos-de-los-derivados-mono-y-dihidroxilados-del-11-elevado-a-1-22-elevado-a-1-y-12-elevado-a-1-azonaftaleno","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/calculo-teorico-de-los-espectros-ii-electronicos-de-los-derivados-mono-y-dihidroxilados-del-11-elevado-a-1-22-elevado-a-1-y-12-elevado-a-1-azonaftaleno\/","title":{"rendered":"Calculo teorico de los espectros ii-electronicos de los derivados mono y dihidroxilados del 1,1 elevado a 1- 2,2 elevado a 1- y 1,2 elevado a 1-azonaftaleno."},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Guijarro Gonzalez M. Soledad <\/strong><\/h2>\n<p>Para el calculo de los espectros hemos utilizado el metodo mecano cuantico de panisen-parr-pople con niteracion de configuraciones. Primeramente tuvimos que escoger los parametros necesarios para poder emplear dicho metodo  para lo cual determinamos como afectaban a las porciones de las bandas del alfa-nafhol  el potencial de ionizacion y electroafinidad del oxigeno  la longitud del enlacec-o y la nitegral de resonancia beta sub c &#8211; o y las nitegrales beta sub c-n y beta sub n n en el 1 1 elevado a 1- azonaftaleno. Una vez elegido el conjunto de parametros calculamos los espectos de 217 derivados de los azonaftalenos  analizando despues para cada uno de estos derivados las siguientes propiedades: longitud de onda de la primera transicion del espectro  fuerza del oscilador correspondiente a esta transicion  momento dipolas pi de la molecula y densidades de carga pi electronica de los nitrogenos  oxigenos y anillos naftalenicos  sacandose conclusiones ante las variaciones de dichas propiedades.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Calculo teorico de los espectros ii-electronicos de los derivados mono y dihidroxilados del 1,1 elevado a 1- 2,2 elevado a 1- y 1,2 elevado a 1-azonaftaleno.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Calculo teorico de los espectros ii-electronicos de los derivados mono y dihidroxilados del 1,1 elevado a 1- 2,2 elevado a 1- y 1,2 elevado a 1-azonaftaleno. <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Guijarro Gonzalez M. Soledad <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Aut\u00f3noma de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1980<\/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> Fernandez Alonso Jos\u00e9 Ignacio<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal:  Fernandez Alonso  Jos\u00e9 Ignacio <\/li>\n<li>Rafael Perez Alvarez-osorio (vocal)<\/li>\n<li>Juan Sancho Gomez (vocal)<\/li>\n<li>Juan Bertr\u00e1n Rusca (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Guijarro Gonzalez M. Soledad Para el calculo de los espectros hemos utilizado el metodo mecano cuantico de [&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":[1625,199,560],"tags":[567,111878,1120,108187,109557],"class_list":["post-47361","post","type-post","status-publish","format-standard","hentry","category-espectroscopia-electronica","category-fisica","category-quimica-fisica","tag-fernandez-alonso-jose-ignacio","tag-guijarro-gonzalez-m-soledad","tag-juan-bertran-rusca","tag-juan-sancho-gomez","tag-rafael-perez-alvarez-osorio"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/47361","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=47361"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/47361\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=47361"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=47361"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=47361"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}