{"id":5763,"date":"2022-08-11T14:45:04","date_gmt":"2022-08-11T17:45:04","guid":{"rendered":"https:\/\/wp.ufpel.edu.br\/pgfisica\/?p=5763"},"modified":"2022-08-11T14:45:27","modified_gmt":"2022-08-11T17:45:27","slug":"resultado-extra-de-doutorado-2022-2","status":"publish","type":"post","link":"https:\/\/wp.ufpel.edu.br\/pgfisica\/2022\/08\/11\/resultado-extra-de-doutorado-2022-2\/","title":{"rendered":"Homologa\u00e7\u00e3o dos Inscritos e Resultado da Sele\u00e7\u00e3o Extra de Doutorado 2022\/2"},"content":{"rendered":"<p>A Comiss\u00e3o de P\u00f3s-Gradua\u00e7\u00e3o do PPGFis, no papel de Comiss\u00e3o de Avalia\u00e7\u00e3o, divulga a homologa\u00e7\u00e3o dos inscritos e o resultado da Sele\u00e7\u00e3o Extra de Doutorado 2022\/2. A matr\u00edcula dos candidatos aprovados ocorrer\u00e1 dia 01\/09\/2022, em hor\u00e1rio a ser combinado com o Coordenador. <span dir=\"ltr\" role=\"presentation\">Recursos ao resultado da homologa\u00e7\u00e3o das candidaturas ou de qualquer uma das <\/span><span dir=\"ltr\" role=\"presentation\">fases da avalia\u00e7\u00e3o devem ser encaminhado por escrito para a Comiss\u00e3o de Avalia\u00e7\u00e3o, <\/span><span dir=\"ltr\" role=\"presentation\">no endere\u00e7o eletr\u00f4nico pg<\/span><span dir=\"ltr\" role=\"presentation\">fi<\/span><span dir=\"ltr\" role=\"presentation\">sica.ufpel@gmail.com, no prazo de at\u00e9 72h contadas a <\/span><span dir=\"ltr\" role=\"presentation\">partir da divulga\u00e7\u00e3o dos resultados.<\/span><\/p>\n<p><strong>HOMOLOGA\u00c7\u00c3O DAS INSCRI\u00c7\u00d5ES<\/strong><\/p>\n<table dir=\"ltr\" style=\"height: 115px;\" border=\"1\" width=\"898\" cellspacing=\"0\" cellpadding=\"0\">\n<colgroup>\n<col width=\"194\" \/>\n<col width=\"100\" \/>\n<col width=\"100\" \/><\/colgroup>\n<tbody>\n<tr>\n<td style=\"width: 904.683px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Candidato&quot;}\"><em>Candidato<\/em><\/td>\n<td style=\"width: 466.333px;\"><\/td>\n<td style=\"width: 663.983px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Situa\u00e7\u00e3o&quot;}\"><em>Situa\u00e7\u00e3o da Inscri\u00e7\u00e3o<br \/>\n<\/em><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 904.683px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Inaiara Leite Rodrigues&quot;}\">Inaiara Leite Rodrigues<\/td>\n<td style=\"width: 466.333px; text-align: center;\"><\/td>\n<td style=\"width: 663.983px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Homologado&quot;}\">Homologada<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 904.683px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Ramon de S\u00e1&quot;}\">Fabiano Pereira de Oliveira<\/td>\n<td style=\"width: 466.333px; text-align: center;\"><\/td>\n<td style=\"width: 663.983px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Homologado&quot;}\">Homologada<\/td>\n<\/tr>\n<tr>\n<td style=\"width: 904.683px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;FABIANO PEREIRA DE OLIVEIRA&quot;}\">Ramon de S\u00e1<\/td>\n<td style=\"width: 466.333px; text-align: center;\"><\/td>\n<td style=\"width: 663.983px; text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Homologado&quot;}\">Homologada<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p><strong>RESULTADO DA SELE\u00c7\u00c3O<br \/>\n<\/strong><\/p>\n<table dir=\"ltr\" border=\"1\" cellspacing=\"0\" cellpadding=\"0\">\n<colgroup>\n<col width=\"194\" \/>\n<col width=\"100\" \/><\/colgroup>\n<tbody>\n<tr>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Candidato&quot;}\">Candidato<\/td>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Classifica\u00e7\u00e3o&quot;}\">Classifica\u00e7\u00e3o<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Inaiara Leite Rodrigues&quot;}\">Inaiara Leite Rodrigues<\/td>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:3,&quot;3&quot;:1}\">1<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;Ramon de S\u00e1&quot;}\">Ramon de S\u00e1<\/td>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:3,&quot;3&quot;:2}\">2<\/td>\n<\/tr>\n<tr>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:2,&quot;2&quot;:&quot;FABIANO PEREIRA DE OLIVEIRA&quot;}\">Fabiano Pereira dos Santos<\/td>\n<td style=\"text-align: center;\" data-sheets-value=\"{&quot;1&quot;:3,&quot;3&quot;:3}\">Desclassificado seguindo o item 2.6 do Edital N\u00ba 130\/2022 :<br \/>\n<span dir=\"ltr\" role=\"presentation\">2.6 &#8211; As(os) candidatas(os) que obtiverem nota N1 ou N2 menor do que seis (6,0)<\/span><br role=\"presentation\" \/><span dir=\"ltr\" role=\"presentation\">ser\u00e3o automaticamente exclu\u00eddos do processo de sele\u00e7\u00e3o<\/span><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>A Comiss\u00e3o de P\u00f3s-Gradua\u00e7\u00e3o do PPGFis, no papel de Comiss\u00e3o de Avalia\u00e7\u00e3o, divulga a homologa\u00e7\u00e3o dos inscritos e o resultado da Sele\u00e7\u00e3o Extra de Doutorado 2022\/2. A matr\u00edcula dos candidatos aprovados ocorrer\u00e1 dia 01\/09\/2022, em hor\u00e1rio a ser combinado com o Coordenador. Recursos ao resultado da homologa\u00e7\u00e3o das candidaturas ou de qualquer uma das fases &hellip; <a href=\"https:\/\/wp.ufpel.edu.br\/pgfisica\/2022\/08\/11\/resultado-extra-de-doutorado-2022-2\/\" class=\"more-link\">Continue lendo <span class=\"screen-reader-text\">Homologa\u00e7\u00e3o dos Inscritos e Resultado da Sele\u00e7\u00e3o Extra de Doutorado 2022\/2<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":220,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_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":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","default_image_id":0,"font":"","enabled":false},"version":2},"jetpack_post_was_ever_published":false},"categories":[18],"tags":[],"class_list":["post-5763","post","type-post","status-publish","format-standard","hentry","category-sem-categoria"],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p94N8p-1uX","_links":{"self":[{"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/posts\/5763","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=5763"}],"version-history":[{"count":2,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/posts\/5763\/revisions"}],"predecessor-version":[{"id":5766,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/posts\/5763\/revisions\/5766"}],"wp:attachment":[{"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/media?parent=5763"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/categories?post=5763"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/wp.ufpel.edu.br\/pgfisica\/wp-json\/wp\/v2\/tags?post=5763"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}