{"id":12044,"date":"2001-06-07T00:00:00","date_gmt":"2001-06-07T00:00:00","guid":{"rendered":"https:\/\/www.deberes.net\/tesis\/sin-categoria\/electroproduccion-de-charm-en-hera\/"},"modified":"2001-06-07T00:00:00","modified_gmt":"2001-06-07T00:00:00","slug":"electroproduccion-de-charm-en-hera","status":"publish","type":"post","link":"https:\/\/www.deberes.net\/tesis\/fisica\/electroproduccion-de-charm-en-hera\/","title":{"rendered":"Electroproducci\u00f3n de charm en hera"},"content":{"rendered":"<h2>Tesis doctoral de <strong> Ignacio Redondo Fer\u00e1ndez <\/strong><\/h2>\n<p>Los datos del experimento zeus tomados durante los a\u00f1os 1996-2000 se analizan en la primera parte de esta tesis. La electroproducci\u00f3n de charm se selecciona a trav\u00e9s de la identificaci\u00f3n del lept\u00f3n dispersado y de la reconstrucci\u00f3n de un mes\u00f3n d*. El mes\u00f3n d* se reconstruye en este estudio usando el canal de destintegraci\u00f3n d*=&gt; pi d0 (=&gt;pi k) la secci\u00f3n eficaz de producci\u00f3n de mensones d* se mide en una regi\u00f3n cinem\u00e1tica restringida en funci\u00f3n de diversas variables. Los datos se comparan con predicciones de nlo pqcd que incluyen tres sabores ligeros y el glu\u00f3n como partones en el prot\u00f3n. Adem\u00e1s se estudian efectos debidos a la fragmentaci\u00f3n. Estos c\u00e1lculos se usan posteriormente para extrapolar las medias a todo el espacio de fase de las variables del mes\u00f3n d* con el prop\u00f3sito de extraer la contribuciones de charm a f2. El acuerdo con los c\u00e1lculos supone una confirmaci\u00f3n de la universidad de las distribuciones patronicas del prot\u00f3n, y en particular de la del glu\u00f3n, dado que describen al mismo tiempo las violaciones de escala de f2 y la secci\u00f3n eficaz de producci\u00f3n de charm.  en la segunda parte de esta tesis se exploran futuras perspectivas del an\u00e1lisis de la primera parte. El nuevo detector de v\u00e9rtices de zeus (mvd), basado en tecnolog\u00eda de silicio, permitir\u00e1 la medida de v\u00e9rtices secundarios. adem\u00e1s, se extender\u00e1 hacia delante (direcci\u00f3n del prot\u00f3n) la regi\u00f3n en la que se pueden medir trazas. La tesis incluye estudios de prueba de haz sobre sensores de silicio que ir\u00e1n colocados en la regi\u00f3n de delante. Estos detectores se caracterizan por una inusual geometr\u00eda trapezoidal. Despu\u00e9s de un completo programa de pruebas con haz llegamos a la conclusi\u00f3n que muestran un comportamiento similar al de los sensores de geometr\u00eda rectangular mas est\u00e1ndar que se encontraran en la zona central del mvd. Medimos una resoluci\u00f3n en posici\u00f3n de unas 10 micras. Las perspectivas que presentan la electropro<\/p>\n<p>&nbsp;<\/p>\n<h3>Datos acad\u00e9micos de la tesis doctoral \u00ab<strong>Electroproducci\u00f3n de charm en hera<\/strong>\u00ab<\/h3>\n<ul>\n<li><strong>T\u00edtulo de la tesis:<\/strong>\u00a0 Electroproducci\u00f3n de charm en hera <\/li>\n<li><strong>Autor:<\/strong>\u00a0 Ignacio Redondo Fer\u00e1ndez <\/li>\n<li><strong>Universidad:<\/strong>\u00a0 Aut\u00f3noma de Madrid<\/li>\n<li><strong>Fecha de lectura de la tesis:<\/strong>\u00a0 06\/07\/2001<\/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>Luis Labarga Echeverr\u00eda<\/li>\n<\/ul>\n<\/li>\n<li><strong>Tribunal<\/strong>\n<ul>\n<li>Presidente del tribunal: sigmund Brandt <\/li>\n<li>h.g.j.m. Tieche (vocal)<\/li>\n<li> Yndurain mu\u00f1oz Francisco j. (vocal)<\/li>\n<li>Javier Berdurgo p\u00e9rez (vocal)<\/li>\n<\/ul>\n<\/li>\n<\/ul>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Tesis doctoral de Ignacio Redondo Fer\u00e1ndez Los datos del experimento zeus tomados durante los a\u00f1os 1996-2000 se analizan en la [&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":[199,39473,1432,27034],"tags":[39477,39474,39478,39475,39476,2787],"class_list":["post-12044","post","type-post","status-publish","format-standard","hentry","category-fisica","category-fisica-de-la-energia","category-fisica-teorica","category-leptones","tag-h-g-j-m-tieche","tag-ignacio-redondo-ferandez","tag-javier-berdurgo-perez","tag-luis-labarga-echeverria","tag-sigmund-brandt","tag-yndurain-munoz-francisco-j"],"_links":{"self":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/12044","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=12044"}],"version-history":[{"count":0,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/posts\/12044\/revisions"}],"wp:attachment":[{"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/media?parent=12044"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/categories?post=12044"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.deberes.net\/tesis\/wp-json\/wp\/v2\/tags?post=12044"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}