{"id":37876,"date":"2018-03-09T09:37:11","date_gmt":"2018-03-09T09:37:11","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/heavy-quarkonium-and-nonrelativistic-effective-field-theories\/"},"modified":"2018-03-09T09:37:11","modified_gmt":"2018-03-09T09:37:11","slug":"heavy-quarkonium-and-nonrelativistic-effective-field-theories","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/heavy-quarkonium-and-nonrelativistic-effective-field-theories\/","title":{"rendered":"Heavy quarkonium and nonrelativistic effective field theories."},"content":{"rendered":"<h2>Tesis doctoral de <strong> Antonio  Miguel Pineda Ruiz <\/strong><\/h2>\n<p>Las primeras aplicaciones de esta tesis se concentraron en aplicaciones de hqet a sistemas de heavy quarkonium. Construimos un lagrangiano de tipo chiral con las simetr\u00edas de la hqet para quarks y antiquarks. Con esta teor\u00eda parametrizamos, en una forma independiente de modelo, algunos efectos no perturbativos. Tambi\u00e9n clarificamos la confusi\u00f3n existente respecto algunas dimensiones an\u00f3malas imaginarias.  tambi\u00e9n se estudio las correcciones no perturbativas estandar al quarkonium muy pesado. Se encontraron y calcularon nuevas correcciones no perturbativas al fine y al hyperfine splitting. Se chequearon determinadas desigualdades que son necesarias para que los resultados sean validos calculando las siguientes correcciones no perturbativas. Tambi\u00e9n se ha hallado la masa polo para el bottom y el charm con una precisi\u00f3n o(   ) y v con las correcciones no perturbativas dominantes.  hemos estudiado las teor\u00edas efectivas (nrqcd). Hemos construido una teor\u00eda con los ingredientes necesarios para describir los sistemas no relativistas de forma eficiente. Hemos calculado los coeficientes de los t\u00e9rminos de cuatro fermiones y el lamb shift utilizando regularizaci\u00f3n dimensional. Resultados parciales para el caso del positronium tambi\u00e9n se han obtenido.<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Heavy quarkonium and nonrelativistic effective field theories.<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Heavy quarkonium and nonrelativistic effective field theories. <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Antonio  Miguel Pineda Ruiz <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Barcelona<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 29\/01\/1998<\/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>Joan Soto Riera<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: pere Pascual de sans <\/li>\n<li>Francisco j. Yndurain mu\u00f1oz (vocal)<\/li>\n<li>Miguel angel Sanchis lozano (vocal)<\/li>\n<li>emili Bagan capella (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Antonio Miguel Pineda Ruiz Las primeras aplicaciones de esta tesis se concentraron en aplicaciones de hqet a [&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":[951,199,1432,11703],"tags":[78798,20183,98861,41866,98862,48152],"class_list":["post-37876","post","type-post","status-publish","format-standard","hentry","category-barcelona","category-fisica","category-fisica-teorica","category-particulas-elementales","tag-antonio-miguel-pineda-ruiz","tag-emili-bagan-capella","tag-francisco-j-yndurain-munoz","tag-joan-soto-riera","tag-miguel-angel-sanchis-lozano","tag-pere-pascual-de-sans"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/37876","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=37876"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/37876\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=37876"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=37876"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=37876"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}