{"id":43885,"date":"2018-07-30T15:35:53","date_gmt":"2018-07-30T15:35:53","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/estudio-teorico-experimental-del-hamiltoniano-de-heisenberg\/"},"modified":"2018-07-30T15:35:53","modified_gmt":"2018-07-30T15:35:53","slug":"estudio-teorico-experimental-del-hamiltoniano-de-heisenberg","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/estudio-teorico-experimental-del-hamiltoniano-de-heisenberg\/","title":{"rendered":"Estudio teorico-experimental del hamiltoniano de heisenberg."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Rafael Navarro Linares <\/strong><\/h2>\n<p>Se ha realizado un estudio teorico-experimental del hamietoniano isotropico de heisenberg  con solo vecinos mas proximos  para distintas dimensiones de la red magnetocristalina  utilizando los desarrollos exactos en series de potencias y las predicciones de la teoria de ondas espinoriales. Para ello se ha revisado comparativamente el desarrollo actual de las tres modelos simples de ising  de x-y u de heisemberg  resaltando los aspectos comunes en segundo lugar se ha realizado un estudio exhaustivo de las tecnicas de aproximantes de pade aplicados a la obtencion de extensiones analiticas de los desarrollos truncados en series de potencias de las magnitudes termodinamicas mas utiles en la realizacion de comparaci ones teoria-experiencia las tecnicas de aproximantes de pade han sido utilizadas en la investigacion de la existencia y posicion de la singularidad ferromagnetica  comparando sus predicciones con las estimaciones empiricas existentes para la susceptibilidad en este tipo de red. Paralelamente se ha realizado el mismo tipo de estudio con aproximantes de pade  y teoria proyectada de ondas espinoriales para las dos redes planas no compactas  con interaccion isotropicayantiferromagnetica obteniendo generos excelentes entre nuestras predicciones y los puntos experimentales de sistemas magneticos cuasi-bidimensionales de la familia xmf4<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Estudio teorico-experimental del hamiltoniano de heisenberg.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Estudio teorico-experimental del hamiltoniano de heisenberg. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Rafael Navarro Linares <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Zaragoza<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 01\/01\/1977<\/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> Jongh L. J. De<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Domingo Gonzalez Alvarez <\/li>\n<li>J. Huiskamp W. (vocal)<\/li>\n<li>Alberto Galindo Texaire (vocal)<\/li>\n<li>Salvador Miracle Sole (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Rafael Navarro Linares Se ha realizado un estudio teorico-experimental del hamietoniano isotropico de heisenberg con solo vecinos [&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":[199,1008,1007,13610],"tags":[108472,13308,108471,108470,18125,108473],"class_list":["post-43885","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-del-estado-solido","category-propiedades-magneticas-de-los-solidos","category-zaragoza","tag-alberto-galindo-texaire","tag-domingo-gonzalez-alvarez","tag-j-huiskamp-w","tag-jongh-l-j-de","tag-rafael-navarro-linares","tag-salvador-miracle-sole"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/43885","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=43885"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/43885\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=43885"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=43885"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=43885"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}