{"id":10507,"date":"2026-08-05T14:44:19","date_gmt":"2026-08-05T19:44:19","guid":{"rendered":"https:\/\/editorial.udenar.edu.co\/?p=10507"},"modified":"2026-08-05T14:47:00","modified_gmt":"2026-08-05T19:47:00","slug":"teoria-de-fotones-masivos-en-las-coordenadas-de-plano-nulo","status":"publish","type":"post","link":"https:\/\/editorial.udenar.edu.co\/?p=10507","title":{"rendered":"Teor\u00eda de fotones masivos en las coordenadas de plano nulo"},"content":{"rendered":"<p><a href=\"https:\/\/editorial.udenar.edu.co\/wp-content\/uploads\/2026\/08\/Teoria-de-fotones.png\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-10509 alignleft\" src=\"https:\/\/editorial.udenar.edu.co\/wp-content\/uploads\/2026\/08\/Teoria-de-fotones.png\" alt=\"\" width=\"336\" height=\"436\" \/><\/a>\u00a0 Autores;\u00a0 German Enrique Ramos Zambrano;\u00a0 Bruto Max Pimentel<\/p>\n<p>Una manera alternativa de generar masa a los campos gauge consiste en romper simetr\u00eda a trav\u00e9s de mecanismos de Higgs. En Electrodin\u00e1mica cu\u00e1ntica es posible atribuir una masa al fot\u00f3n y aun mantener una teor\u00eda renormalizable y unitaria. Tal posibilidad no ocurre en teor\u00edas de gauge no abelianas, sin embargo, existe un mecanismo de rompimiento din\u00e1mico de simetr\u00eda donde los campos de la teor\u00eda se reorganizan generando el equivalente del bos\u00f3n de Higgs y campos de gauge masivos. Un ejemplo cl\u00e1sico de este tipo de teor\u00edas es el modelo de Nambu-Jona-Lasinio y el mecanismo es denominado rompimiento din\u00e1mico de simetr\u00eda. En este proyecto se estudiar\u00e1 la estructura can\u00f3nica de la densidad Lagrangiana propuesta por Cornwall que le da masa al campo electromagn\u00e9tico y aun garantiza la invariante de gauge de la teor\u00eda. Para cumplir este prop\u00f3sito, se utilizara la formulaci\u00f3n de Dirac y de Faddeev -Jackiw que permite deducir en forma natural la estructura simpl\u00e9ctica del espacio de fase y los par\u00e9ntesis generalizados de la teor\u00eda.<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<p>Tama\u00f1o:\u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0Formato:\u00a0 Digital\u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0Paginas: 167<\/p>\n<p>A\u00f1o:\u00a0 2026\u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0ISBN:\u00a0 978-628-7864-82-5\u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0 \u00a0Valor:\u00a0 <a href=\"https:\/\/sired.udenar.edu.co\/18633\/1\/18633.pdf\">Descarga Gratuita<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u00a0 Autores;\u00a0 German Enrique Ramos Zambrano;\u00a0 Bruto Max Pimentel Una manera alternativa de generar masa a los campos gauge consiste en romper simetr\u00eda a trav\u00e9s de mecanismos de Higgs. En Electrodin\u00e1mica cu\u00e1ntica es posible atribuir una masa al fot\u00f3n y aun mantener una teor\u00eda renormalizable y unitaria. Tal posibilidad no ocurre en teor\u00edas de gauge [&hellip;]<\/p>\n","protected":false},"author":4,"featured_media":10509,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_et_pb_use_builder":"","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"categories":[83,1],"tags":[],"class_list":["post-10507","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-83","category-sin-categoria"],"_links":{"self":[{"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/posts\/10507","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/users\/4"}],"replies":[{"embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=10507"}],"version-history":[{"count":10,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/posts\/10507\/revisions"}],"predecessor-version":[{"id":10519,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/posts\/10507\/revisions\/10519"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/media\/10509"}],"wp:attachment":[{"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=10507"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=10507"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=10507"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}