{"id":105,"date":"2018-09-11T08:07:19","date_gmt":"2018-09-11T08:07:19","guid":{"rendered":"http:\/\/teleparalleluniverses.usal.es\/?page_id=105"},"modified":"2018-11-24T12:44:22","modified_gmt":"2018-11-24T12:44:22","slug":"english-program","status":"publish","type":"page","link":"https:\/\/teleparalleluniverses.usal.es\/en\/english-program\/","title":{"rendered":"Program"},"content":{"rendered":"<p><\/p>\n<table border=\"0\" cellspacing=\"0\">\n<colgroup width=\"70\"><\/colgroup>\n<colgroup width=\"478\"><\/colgroup>\n<colgroup width=\"607\"><\/colgroup>\n<colgroup width=\"525\"><\/colgroup>\n<tbody>\n<tr>\n<td align=\"center\" valign=\"middle\" height=\"23\"><\/td>\n<td align=\"center\"><b><span style=\"font-family: Liberation Serif\">Monday<\/span><\/b><\/td>\n<td align=\"center\"><b><span style=\"font-family: Liberation Serif\">Tuesday<\/span><\/b><\/td>\n<td align=\"center\"><b><span style=\"font-family: Liberation Serif\">Wednesday<\/span><\/b><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" height=\"23\"><b><span style=\"font-family: Liberation Serif\">9:00 \u2013 9:30<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#DFCCE4\"><span style=\"font-family: Liberation Serif\">Registration and opening<\/span><\/td>\n<td align=\"center\"><\/td>\n<td align=\"center\"><\/td>\n<\/tr>\n<tr>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" height=\"92\"><b><span style=\"font-family: Liberation Serif\">9:30 \u2013 10:15<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#F37B70\"><b><span style=\"font-family: Liberation Serif\">Jose G. Pereira<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#F37B70\"><b><span style=\"font-family: Liberation Serif\">M.J. Guzm\u00e1n Monsalve<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#F37B70\"><b><span style=\"font-family: Liberation Serif\">T Ort\u00edn<\/span><\/b><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#F37B70\"><i><span style=\"font-family: Liberation Serif\">Teleparallel Gravity: Some Properties and Achievements<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#F37B70\"><i><span style=\"font-family: Liberation Serif\">Hamiltonian formalism of the Jordan and Einstein frame representations of f(T) gravity<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#F37B70\"><i><span style=\"font-family: Liberation Serif\">Higher-order terms in gravity theories: SEP and globally regular stringy black holes<\/span><\/i><\/td>\n<\/tr>\n<tr>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" height=\"46\"><b><span style=\"font-family: Liberation Serif\">10:30 \u2013 11:00<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">M. Krssak<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">Daniel Blixt<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">P. Antonio Cano<\/span><\/b><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">On the problem of energy-momentum in teleparallel gravity<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Hamiltonian analysis in new general relativity<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Higher-curvature gravity and the fate of black holes<\/span><\/i><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" height=\"23\"><b><span style=\"font-family: Liberation Serif\">11:00 \u2013 11:30<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Coffee break<\/span><\/td>\n<td align=\"center\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Coffee break<\/span><\/td>\n<td align=\"center\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Coffee break<\/span><\/td>\n<\/tr>\n<tr>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" height=\"92\"><b><span style=\"font-family: Liberation Serif\">11:30 \u2013 12:15<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#F37B70\"><b><span style=\"font-family: Liberation Serif\">M. Hohmann<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#F37B70\"><b><span style=\"font-family: Liberation Serif\">Y. Obukhov<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#F37B70\"><b><span style=\"font-family: Liberation Serif\">T. Zlosnik<\/span><\/b><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#F37B70\"><i><span style=\"font-family: Liberation Serif\">Scalar-torsion theories of gravity<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#F37B70\"><i><span style=\"font-family: Liberation Serif\">Premetric approach in teleparallel gravity theory<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#F37B70\"><i><span style=\"font-family: Liberation Serif\">Cartan geometry and gravity<\/span><\/i><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" height=\"46\"><b><span style=\"font-family: Liberation Serif\">12:30 \u2013 13:00<\/span><\/b><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#ADC5E7\"><span style=\"font-family: Liberation Serif\">Discussions<\/span><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#ADC5E7\"><span style=\"font-family: Liberation Serif\">Discussions<\/span><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#ADC5E7\"><span style=\"font-family: Liberation Serif\">Discussions<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" height=\"64\"><b><span style=\"font-family: Liberation Serif\">13:00 \u2013 15:30<\/span><\/b><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Lunch<\/span><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Lunch<\/span><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Lunch<\/span><\/td>\n<\/tr>\n<tr>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" height=\"46\"><b><span style=\"font-family: Liberation Serif\">15:30 \u2013 16:00<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">Diego S\u00e1ez-Chill\u00f3n G\u00f3mez<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">Laur J\u00e4rv<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">S. Costa Ulhoa<\/span><\/b><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Some features of extended Teleparallel theories<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Flat spin connection for rotating vacuum spacetimes in teleparallel f(T) gravity<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">On the quantization of charge-mass ratio<\/span><\/i><\/td>\n<\/tr>\n<tr>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" height=\"46\"><b><span style=\"font-family: Liberation Serif\">16:00 \u2013 16:30<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">A. Finch<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">M. Adak<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">A. Jim\u00e9nez Cano<\/span><\/b><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Galactic Rotation Dynamics in f(T) gravity<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">The Lagrange formulation of the symmetric teleparallel gravity in terms of the exterior algebra<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Electromagnetism induced by projective symmetry in metric-affine gravity<\/span><\/i><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" height=\"23\"><b><span style=\"font-family: Liberation Serif\">16:30 \u2013 17:00<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Coffee break<\/span><\/td>\n<td align=\"center\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Coffee break<\/span><\/td>\n<td align=\"center\" bgcolor=\"#FFF9AE\"><span style=\"font-family: Liberation Serif\">Coffee break<\/span><\/td>\n<\/tr>\n<tr>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" height=\"46\"><b><span style=\"font-family: Liberation Serif\">17:00 \u2013 17:30<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">K. Dialektopoulos<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">G. Farrugia<\/span><\/b><\/td>\n<td align=\"center\" bgcolor=\"#BCE4E5\"><b><span style=\"font-family: Liberation Serif\">C. Bejarano<\/span><\/b><\/td>\n<\/tr>\n<tr>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Noether symmetries in teleparallel theories<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Gravitational Waves in General Teleparallel Theories of Gravity<\/span><\/i><\/td>\n<td align=\"center\" valign=\"middle\" bgcolor=\"#BCE4E5\"><i><span style=\"font-family: Liberation Serif\">Some relevant issues in 2+1 f(T) gravity<\/span><\/i><\/td>\n<\/tr>\n<tr>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" height=\"46\"><b><span style=\"font-family: Liberation Serif\">17:30 \u2013 18:00<\/span><\/b><\/td>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" bgcolor=\"#ADC5E7\"><span style=\"font-family: Liberation Serif\">Discussions<\/span><\/td>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" bgcolor=\"#ADC5E7\"><span style=\"font-family: Liberation Serif\">Discussions<\/span><\/td>\n<td rowspan=\"2\" align=\"center\" valign=\"middle\" bgcolor=\"#DFCCE4\"><span style=\"font-family: Liberation Serif\">Discussions and closing remarks<\/span><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p class=\"Standard\"><span lang=\"EN-US\">\u00a0<\/span><\/p>\n<p><\/p>","protected":false},"excerpt":{"rendered":"<p>Monday Tuesday Wednesday 9:00 \u2013 9:30 Registration and opening 9:30 \u2013 10:15 Jose G. Pereira M.J. Guzm\u00e1n Monsalve T Ort\u00edn Teleparallel Gravity: Some Properties and Achievements Hamiltonian formalism of the Jordan and Einstein frame representations of f(T) gravity Higher-order terms in gravity theories: SEP and globally regular stringy black holes 10:30 \u2013 11:00 M. Krssak &hellip; <a href=\"https:\/\/teleparalleluniverses.usal.es\/en\/english-program\/\" class=\"more-link\">Continue reading<span class=\"screen-reader-text\"> &#8220;Program&#8221;<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-105","page","type-page","status-publish","hentry"],"aioseo_notices":[],"aioseo_head":"\n\t\t<!-- All in One SEO 4.9.9 - aioseo.com -->\n\t<meta name=\"description\" content=\"Monday Tuesday Wednesday 9:00 \u2013 9:30 Registration and opening 9:30 \u2013 10:15 Jose G. Pereira M.J. 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