{"id":10521,"date":"2026-08-05T14:54:51","date_gmt":"2026-08-05T19:54:51","guid":{"rendered":"https:\/\/editorial.udenar.edu.co\/?p=10521"},"modified":"2026-08-05T14:54:51","modified_gmt":"2026-08-05T19:54:51","slug":"electrodinamica-escalar-de-primer-orden-en-las-coordenadas-de-plano-nulo","status":"publish","type":"post","link":"https:\/\/editorial.udenar.edu.co\/?p=10521","title":{"rendered":"Electrodin\u00e1mica escalar de primer orden en las coordenadas de plano nulo"},"content":{"rendered":"<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-10523 alignleft\" src=\"https:\/\/editorial.udenar.edu.co\/wp-content\/uploads\/2026\/08\/Electrodinamica-escalar.png\" alt=\"\" width=\"336\" height=\"445\" \/>Autores; German Enrique Ramos Zambrano; Bruto Max Pimentel<\/p>\n<p>Duffin, Kemmer y Patiau propusieron a mediados del siglo XX una ecuaci\u00f3n de campo de primer orden que permit\u00eda describir part\u00edculas de esp\u00edn cero y esp\u00edn<br \/>\nuno, que se conoce como ecuaci\u00f3n de Duffin-Kemmer\ufffd Petiau (DKP). Esta ecuaci\u00f3n resulta ser muy semejante a la ecuaci\u00f3n matricial de Dirac, con una algebra distinta a la satisfecha por las matrices de Dirac. La electrodin\u00e1mica escalar de primer orden describe un campo de DKP en la representaci\u00f3n 5 \u00d7 5 con acoplamiento m\u00ednimo a un campo electromagn\u00e9tico.<\/p>\n<p>La estructura singular de la densidad lagrangiana que describe esta teor\u00eda requiere un procedimiento consistente que garantice la compatibilidad entre las ligaduras que resulten y la simetr\u00eda de gauge que caracteriza el sistema. El estudio de teor\u00eda se realiza en las coordenadas de plano nulo, lo que implico encontrar una adecuada representaci\u00f3n de las matrices de DKP que permita seleccionar las componentes f\u00edsicas de los campos fundamentales<\/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: 173<\/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 978-628-7864-36-8 \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\/17996\/1\/17996.pdf\">Descarga Gratuita<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Autores; German Enrique Ramos Zambrano; Bruto Max Pimentel Duffin, Kemmer y Patiau propusieron a mediados del siglo XX una ecuaci\u00f3n de campo de primer orden que permit\u00eda describir part\u00edculas de esp\u00edn cero y esp\u00edn uno, que se conoce como ecuaci\u00f3n de Duffin-Kemmer\ufffd Petiau (DKP). Esta ecuaci\u00f3n resulta ser muy semejante a la ecuaci\u00f3n matricial de [&hellip;]<\/p>\n","protected":false},"author":4,"featured_media":10523,"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-10521","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\/10521","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=10521"}],"version-history":[{"count":9,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/posts\/10521\/revisions"}],"predecessor-version":[{"id":10531,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/posts\/10521\/revisions\/10531"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=\/wp\/v2\/media\/10523"}],"wp:attachment":[{"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=10521"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=10521"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/editorial.udenar.edu.co\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=10521"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}