{"id":144224,"date":"1993-01-01T00:00:00","date_gmt":"1993-01-01T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/comportamiento-axial-del-campo-difractado-por-pupilas-sin-simetria-de-revolucion-aplicacion-al-diseno-de-apodizadores\/"},"modified":"1993-01-01T00:00:00","modified_gmt":"1993-01-01T00:00:00","slug":"comportamiento-axial-del-campo-difractado-por-pupilas-sin-simetria-de-revolucion-aplicacion-al-diseno-de-apodizadores","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/comportamiento-axial-del-campo-difractado-por-pupilas-sin-simetria-de-revolucion-aplicacion-al-diseno-de-apodizadores\/","title":{"rendered":"Comportamiento axial del campo difractado por pupilas sin simetria de revolucion. aplicacion al dise\u00f1o de apodizadores"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Manuel Martinez Corral <\/strong><\/h2>\n<p>En esta tesis se aborda el estudio de la distribucion tridimensional de amplitudes en el volumen focal haciendo uso de un nuevo planteamiento. Especificamente, se demuestra que la distribucion de amplitud compleja a lo largo de un eje arbitrario que pasa por el foco esta gobernada por la transformada de fourier unidimensional de una cierta version proyectada del promedio angular de la funcion pupila. Este formalismo, que es valido para cualquier valor es proximo a la unidad, para cualquiera de los ejes se produce un desplazamiento del maximo de irradiancia hacia el plano que contiene a la pupila.  esta formulacion constituye una poderosa herramienta matematica que permite a lo largo de esta tesis no solo analizar el comportamiento axial en difraccion de diferentes objetos, sino tambien el dise\u00f1o de filtros con los que modificar a voluntad la distribucion axial de irradiancia.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Comportamiento axial del campo difractado por pupilas sin simetria de revolucion. aplicacion al dise\u00f1o de apodizadores<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Comportamiento axial del campo difractado por pupilas sin simetria de revolucion. aplicacion al dise\u00f1o de apodizadores <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Manuel Martinez Corral <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Universitat de val\u00e9ncia (estudi general)<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1993<\/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>Pedro Andres Bou<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Carlos Ferreira Garcia <\/li>\n<li>Carlos Gomez Reino Carnota (vocal)<\/li>\n<li>Mar\u00eda  Josefa Yzuel Gimenez (vocal)<\/li>\n<li>Salvador X. Bar\u00e1 Vi\u00f1as (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Manuel Martinez Corral En esta tesis se aborda el estudio de la distribucion tridimensional de amplitudes en [&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":[199,1525,3024],"tags":[11734,11796,82106,7183,11935,65819],"class_list":["post-144224","post","type-post","status-publish","format-standard","hentry","category-fisica","category-optica","category-optica-fisica","tag-carlos-ferreira-garcia","tag-carlos-gomez-reino-carnota","tag-manuel-Martinez-corral","tag-maria-josefa-yzuel-gimenez","tag-pedro-andres-bou","tag-salvador-x-bara-vinas"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/144224","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=144224"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/144224\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=144224"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=144224"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=144224"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}