{"id":81555,"date":"1999-10-12T00:00:00","date_gmt":"1999-10-12T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/modelo-de-manhattan-en-la-red-hexagonal\/"},"modified":"1999-10-12T00:00:00","modified_gmt":"1999-10-12T00:00:00","slug":"modelo-de-manhattan-en-la-red-hexagonal","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/modelo-de-manhattan-en-la-red-hexagonal\/","title":{"rendered":"Modelo de manhattan en la red hexagonal"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Jos\u00e9 Damian Catala Galindo <\/strong><\/h2>\n<p>Estudiamos las propiedades de un nuevo modelo din\u00e1mico determinista en un entorno aleatorio. El modelo consiste en una red hexagonal en que se establecen giros de forma aleatoria en los puntos de la misma, con la caracter\u00edstica de que dichos giros no var\u00edan con el tiempo.  nos centramos en el an\u00e1lisis de los puntos cr\u00edticos y establecemos la existencia de una l\u00ednea cr\u00edtica en el espacio de fases. La distribuci\u00f3n del n\u00famero de pasos de las trayectorias en funci\u00f3n de las probabilidades de giro queda establecida mediante dos exponentes cr\u00edticos, que determinamos en distintos puntos del espacio de fases.  analizamos los conceptos relativos a objetos fractales para aplicarlos a las trayectorias extendidas de nuestro modelo y creamos el algoritmo necesario para la determinaci\u00f3n de la dimensi\u00f3n fractal de nuestras trayectorias a lo largo de la l\u00ednea cr\u00edtica.  para determinados valores de las probabilidades de giro, el m\u00e9todo es equivalente a la percolaci\u00f3n de sitios y constituye una potente herramienta para la determinaci\u00f3n precisa de la probabilidad cr\u00edtica de percolaci\u00f3n. Desde el punto de vista num\u00e9rico, nuestro modelo es el m\u00e1s eficiente hasta la fecha para la generaci\u00f3n de per\u00edmetros externos de percolaci\u00f3n, por lo que es posible utilizarlo para la determinaci\u00f3n de probabilidades cr\u00edticas de percolaci\u00f3n. El valor de la probabilidad critica de percolaci\u00f3n lo hemos obtenido mediante dos m\u00e9todos, uno directo y otro siguiendo nuestro modelo. la compraci\u00f3n de ambos m\u00e9todos nos permite evaluar la alta eficacia de nuestros resultados.  estudiamos las propiedades estad\u00edsticas de las distancias medias de las trayectorias desde su origen hasta su extremo en funci\u00f3n del n\u00famero de pasos que \u00e9stas describen. Tambi\u00e9n calculamos la relaci\u00f3n entre el diametro medio de una trayectoria cerrada y su n\u00famero de pasos.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Modelo de manhattan en la red hexagonal<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Modelo de manhattan en la red hexagonal <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Jos\u00e9 Damian Catala Galindo <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Murcia<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 10\/12\/1999<\/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>Miguel Ortu\u00f1o Ortin<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: rafael Garc\u00eda molina <\/li>\n<li>pedro j. Carpena s\u00e1nchez (vocal)<\/li>\n<li>Antonio Perez garrido (vocal)<\/li>\n<li>pedro Bernaola galvan (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Jos\u00e9 Damian Catala Galindo Estudiamos las propiedades de un nuevo modelo din\u00e1mico determinista en un entorno aleatorio. [&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":[199,202,201,8235],"tags":[102868,173971,62559,173972,117355,52365],"class_list":["post-81555","post","type-post","status-publish","format-standard","hentry","category-fisica","category-mecanica","category-mecanica-estadistica","category-murcia","tag-antonio-perez-garrido","tag-jose-damian-catala-galindo","tag-miguel-ortuno-ortin","tag-pedro-bernaola-galvan","tag-pedro-j-carpena-sanchez","tag-rafael-garcia-molina"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/81555","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=81555"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/81555\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=81555"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=81555"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=81555"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}