{"id":43822,"date":"2018-07-19T22:09:56","date_gmt":"2018-07-19T22:09:56","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/contribucion-a-la-formulacion-de-la-mecanica-cuantica-y-la-electrodinamica-estocastica-mediante-integrales-de-camino\/"},"modified":"2018-07-19T22:09:56","modified_gmt":"2018-07-19T22:09:56","slug":"contribucion-a-la-formulacion-de-la-mecanica-cuantica-y-la-electrodinamica-estocastica-mediante-integrales-de-camino","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/contribucion-a-la-formulacion-de-la-mecanica-cuantica-y-la-electrodinamica-estocastica-mediante-integrales-de-camino\/","title":{"rendered":"Contribucion a la formulacion de la mecanica cuantica y la electrodinamica estocastica mediante integrales de camino."},"content":{"rendered":"<h2>Tesis doctoral de <strong>  Nieto Salinas M. Paz <\/strong><\/h2>\n<p>Se parte de la formulacion de feymman de la mecanica cuantica mediante integrales de camino (path integrals).  se deduce una expresion de la probabilidad cuantica como suma de numeros reales (seudoprobabilidades) asociados a los posibles caminos (o trayectorias) en el espacio de configuracion. Se intenta que estos numeros reales sean no negativos para poder interpretarlos como probabilidades  lo que se consigue en algunos casos particulares. Se hace una formulacion analoga en el espacio de las fases utilizando la funcion de distribucion de wigner. En la segunda parte del trabajo se establece un metodo general para resolver ecuaciones diferenciales estocasticas mediante integrales de camino.  el metodo se aplica a la resolucion de algunos problemas particulares de electrodinamica estocastica  una teoria clasica que ha sido propuesta como posible alternativa a la mecanica cuantica.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Contribucion a la formulacion de la mecanica cuantica y la electrodinamica estocastica mediante integrales de camino.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Contribucion a la formulacion de la mecanica cuantica y la electrodinamica estocastica mediante integrales de camino. <\/li>\n<li><strong>Autor:<\/strong>\u00a0  Nieto Salinas M. Paz <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Valladolid<\/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>Emilio Santos Corchero<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: Jos\u00e9 Mart\u00ednez Salas <\/li>\n<li> Boya Balet Luis Joaquin (vocal)<\/li>\n<li> Gutierrez Suarez Juan  Jos\u00e9 (vocal)<\/li>\n<li>Emilio Santos Corchero (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Nieto Salinas M. Paz Se parte de la formulacion de feymman de la mecanica cuantica mediante integrales [&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":[199,1432,1431,12451],"tags":[28977,5143,108387,108386,108396],"class_list":["post-43822","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-teorica","category-teoria-cuantica-de-campos","category-valladolid","tag-boya-balet-luis-joaquin","tag-emilio-santos-corchero","tag-gutierrez-suarez-juan-jose","tag-jose-Martinez-salas","tag-nieto-salinas-m-paz"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/43822","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=43822"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/43822\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=43822"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=43822"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=43822"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}