{"id":1828,"date":"2013-09-10T15:26:55","date_gmt":"2013-09-10T18:26:55","guid":{"rendered":"http:\/\/ifm.ufpel.edu.br\/pgfisica\/site\/?p=1828"},"modified":"2013-09-10T15:26:55","modified_gmt":"2013-09-10T18:26:55","slug":"selecao-de-bolsista-pnpd-na-area-de-fisica-estatistica","status":"publish","type":"post","link":"https:\/\/wp.ufpel.edu.br\/pgfisica\/2013\/09\/10\/selecao-de-bolsista-pnpd-na-area-de-fisica-estatistica\/","title":{"rendered":"Sele\u00e7\u00e3o de bolsista PNPD na \u00e1rea de F\u00edsica Estat\u00edstica"},"content":{"rendered":"<p style=\"text-align: justify\">O Programa de P\u00f3s-Gradua\u00e7\u00e3o em F\u00edsica da UFPel est\u00e1 selecionando <span style=\"color: #0000ff\"><strong>1<\/strong> <strong>(um)<\/strong><\/span> bolsista rec\u00e9m-doutor <span style=\"color: #0000ff\"><strong>PNPD\/CAPES<\/strong><\/span>, para atuar na \u00e1rea de <span style=\"color: #ff0000\"><strong>F\u00edsica<\/strong><strong> Estat\u00edstica &#8211; Modelagem Computacional de Macromol\u00e9culas<\/strong><\/span>. A sele\u00e7\u00e3o estar\u00e1 aberta de <span style=\"color: #0000ff\"><strong>06\/09\/13<\/strong><\/span> a <span style=\"color: #0000ff\"><strong>06\/10\/13<\/strong><\/span>.<\/p>\n<p style=\"text-align: justify\">O edital completo pode ser encontrado <a href=\"http:\/\/ifm.ufpel.edu.br\/pgfisica\/site\/wp-content\/uploads\/2013\/edital_selecao_estatistica_2013.pdf\" target=\"_blank\">aqui<\/a>.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>O Programa de P\u00f3s-Gradua\u00e7\u00e3o em F\u00edsica da UFPel est\u00e1 selecionando 1 (um) bolsista rec\u00e9m-doutor PNPD\/CAPES, para atuar na \u00e1rea de F\u00edsica Estat\u00edstica &#8211; Modelagem Computacional de Macromol\u00e9culas. A sele\u00e7\u00e3o estar\u00e1 aberta de 06\/09\/13 a 06\/10\/13. O edital completo pode ser encontrado aqui.<\/p>\n","protected":false},"author":220,"featured_media":0,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"_jetpack_newsletter_access":"","_jetpack_dont_email_post_to_subs":false,"_jetpack_newsletter_tier_id":0,"_jetpack_memberships_contains_paywalled_content":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":"","jetpack_publicize_message":"","jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":false,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2}},"categories":[20],"tags":[],"class_list":["post-1828","post","type-post","status-publish","format-standard","hentry","category-noticias"],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p94N8p-tu","_links":{"self":[{"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/posts\/1828","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/users\/220"}],"replies":[{"embeddable":true,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/comments?post=1828"}],"version-history":[{"count":0,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/posts\/1828\/revisions"}],"wp:attachment":[{"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/media?parent=1828"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/categories?post=1828"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/tags?post=1828"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}