{"id":15884,"date":"2002-04-03T00:00:00","date_gmt":"2002-04-03T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/dinamica-no-lineal-de-sistemes-lasers-potencials-de-lyapunov-i-diagrames-de-bifurcacions\/"},"modified":"2002-04-03T00:00:00","modified_gmt":"2002-04-03T00:00:00","slug":"dinamica-no-lineal-de-sistemes-lasers-potencials-de-lyapunov-i-diagrames-de-bifurcacions","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/dinamica-no-lineal-de-sistemes-lasers-potencials-de-lyapunov-i-diagrames-de-bifurcacions\/","title":{"rendered":"Dinamica no lineal de sistemes lasers: potencials de lyapunov i diagrames de bifurcacions"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Catalina Mayol Serra <\/strong><\/h2>\n<p>En este trabjo se ha estudiado la din\u00e1mica de los l\u00e1seres de clase a y de clase b en t\u00e9rminos del potencial de lyapunos. En el caso que se inyecte una se\u00f1al al l\u00e1ser, o se modulen algunos de los par\u00e1metros, aparece un comportamiento, m\u00e1s complejo y se estudia el conjunto de bifurcaciones.  1)en los l\u00e1seres de clase a, la din\u00e1mica determinista se ha interpretado como el movimiento sobre el potencial de lyapunov. En la din\u00e1mica estoc\u00e1stica, aparece unn flujo sostenida por ruido pasa la fase del campo el\u00e9ctrico, que proviene de la interacci\u00f3n de los t\u00e9rminos conservativos y los t\u00e9rminos de ruido.  2)pasa los l\u00e1seres de clase a con se\u00f1al inyectada, se ha descrito el conjunto de bifurcaciones completo y se ha determinado el conjunto de amplitudes y frecuencias en el cu\u00e1l el l\u00e1ser responde ajustando su frecuencia a la del campo externo.  3)se ha obtenido un potencial de lyapunor para los l\u00e1seres de clase b valido en el caso determinista, que incluye los t\u00e9rminos de saturaci\u00f3n de ganancia y de emisi\u00f3n espont\u00e1nea.  4)se ha realizado un estudio del conjunto de bifurcaciones parcial alrededor del r\u00e9gimen de tipo ii de la singularidad hopf-silla-nodo en un l\u00e1ser de clase b con se\u00f1al inyectada.  5)se han identificado las respuestas optimas para los l\u00e1seres de semiconductor sometidos a modulaci\u00f3n peri\u00f3dica externa. Se han obtenido las curvas que dan la respuesta m\u00e1xima para cada tipo de resonancia en el plano definido por la amplitud y la frecuencia de modulaci\u00f3n. Se han considerado los t\u00e9rminos de saturaci\u00f3n de ganancia y de emisi\u00f3n esp\u00f3ntanea.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Dinamica no lineal de sistemes lasers: potencials de lyapunov i diagrames de bifurcacions<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Dinamica no lineal de sistemes lasers: potencials de lyapunov i diagrames de bifurcacions <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Catalina Mayol Serra <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Illes balears<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 04\/03\/2002<\/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>Raul Toral Garces<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Luis Pesquera gonzalez <\/li>\n<li>a. Natiello mario (vocal)<\/li>\n<li>jordi Garc\u00eda ojalvo (vocal)<\/li>\n<li>pere Colet rafecas (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Catalina Mayol Serra En este trabjo se ha estudiado la din\u00e1mica de los l\u00e1seres de clase a [&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":[199,19034,7179,1525],"tags":[50442,50441,19991,15904,50443,4056],"class_list":["post-15884","post","type-post","status-publish","format-standard","hentry","category-fisica","category-illes-balears","category-laseres","category-optica","tag-a-natiello-mario","tag-catalina-mayol-serra","tag-jordi-garcia-ojalvo","tag-luis-pesquera-gonzalez","tag-pere-colet-rafecas","tag-raul-toral-garces"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/15884","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=15884"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/15884\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=15884"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=15884"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=15884"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}