{"id":1505,"date":"2019-04-22T17:55:12","date_gmt":"2019-04-22T15:55:12","guid":{"rendered":"http:\/\/umi.dm.unibo.it\/congresso2019\/?page_id=1505"},"modified":"2023-09-06T12:56:51","modified_gmt":"2023-09-06T10:56:51","slug":"s2-equazione-differenziali-alle-derivate-parziali","status":"publish","type":"page","link":"https:\/\/umi.dm.unibo.it\/congresso2023\/programma\/sezioni\/s2-equazione-differenziali-alle-derivate-parziali\/","title":{"rendered":"S2 &#8211; Equazione differenziali alle derivate parziali"},"content":{"rendered":"<p><strong>Le comunicazioni si svolgeranno<br \/>\n&#8211; mercoled\u00ec 6, Polo Carmignani, Aula Magna<br \/>\n&#8211; gioved\u00ec 7, Polo Carmignani, Aula Magna<br \/>\n&#8211; venerd\u00ec 8 settembre, Polo Carmignani,, Aula 2<\/strong><\/p>\n<p>&nbsp;<\/p>\n<table border=\"0\" frame=\"VOID\" rules=\"NONE\" cellspacing=\"0\">\n<colgroup>\n<col width=\"114\" \/>\n<col width=\"114\" \/>\n<col width=\"114\" \/>\n<col width=\"114\" \/><\/colgroup>\n<tbody>\n<tr>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Giovanni S.<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Alberti<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Genova<\/span><\/td>\n<td align=\"LEFT\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">Regularity theory for Maxwell\u2019s equations<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 14.30-14.50, venerd\u00ec 8 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Alessandro<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Audrito<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">ETH Zurich<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Il problema dell&#8217;ostacolo parabolico con diffusione fully nonlinear<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 12.20-12.40, mercoled\u00ec 6 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Paolo<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Bonicatto<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">University of Warwick, UK<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Transport of currents and geometric Rademacher-type theorems<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 11.20-11.40, gioved\u00ec 7 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Elia<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Bru\u00e8<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Bocconi, Milano<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Anomalous dissipation for the 3D Navier-Stokes equations<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 11.00-11.20, gioved\u00ec 7 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Laura<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Caravenna<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Padova<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Stime di stabilit\u00e0 per leggi di conservazione<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 16.10-16.30, venerd\u00ec 8 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Annalisa<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Cesaroni<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Padova<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Mean field games with aggregating interaction potentials of nonlocal type<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 11.40-12.00, gioved\u00ec 7 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Eleonora<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Cinti<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Bologna<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">On the evolution of sets by fractional mean curvature flow<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 15.30-15.50, venerd\u00ec 8 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Matteo<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Cozzi<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Milano<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">A quantitative version of Gidas-Ni-Nirenberg theorem<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 15.50-16.10, venerd\u00ec 8 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Cristiana<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">De Filippis<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Parma<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Unconventional Double Phase energies<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 11.20-11.40, mercoled\u00ec 6 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Michele<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Dolce<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">\u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Taylor dispersion and phase mixing in the Boltzmann equation<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 11.40-12.00, mercoled\u00ec 6 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Simone<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Dovetta<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Politecnico di Torino<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Action versus energy ground states in nonlinear Schroedinger equations<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 12.00-12.20, gioved\u00ec 7 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Isabella<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Ianni<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Roma La Sapienza<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">On the uniqueness of positive solutions of the Lane-Emden problem<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 14.50-15.10, venerd\u00ec 8 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Elio<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Marconi<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 di Padova<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Mixing and enhanced dissipation rates for 2d autonomous vector fields<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 12.00-12.20, mercoled\u00ec 6 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Alberto<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Maspero<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">SISSA<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Full description of Benjamin-Feir instability of Stokes waves in finite and deep water.<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 11.00-11.20, mercoled\u00ec 6 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Luigi<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Montoro<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Universit\u00e0 della Calabria<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Symmetry results for solutions of vectorial $p$-Stokes systems<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 15.10-15.30, venerd\u00ec 8 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Gianmarco<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Sperone<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Politecnico di Milano<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Steady-state Navier-Stokes flow in an obstructed pipe under mixed boundary conditions and with a prescribed transversal flux rate<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 12.40-13.00, mercoled\u00ec 6 settembre<\/span><\/td>\n<\/tr>\n<tr>\n<td align=\"LEFT\" height=\"22\"><span style=\"color: #000000; font-family: Helvetica;\">Riccardo<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Tione<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">Max Planck Institute for Mathematics in the Sciences (Leipzig)<\/span><\/td>\n<td align=\"LEFT\"><span style=\"color: #000000; font-family: Helvetica;\">On Stationary Points of Polyconvex Functionals<\/span><\/td>\n<td align=\"LEFT\" nowrap=\"nowrap\" width=\"auto\"><span style=\"color: #000000; font-family: Helvetica;\">ore 12.40-13.00, gioved\u00ec 7 settembre<\/span><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Le comunicazioni si svolgeranno &#8211; mercoled\u00ec 6, Polo Carmignani, Aula Magna &#8211; gioved\u00ec 7, Polo Carmignani, Aula Magna &#8211; venerd\u00ec 8 settembre, Polo Carmignani,, Aula 2 &nbsp; Giovanni S. Alberti Universit\u00e0 di Genova Regularity theory for Maxwell\u2019s equations ore 14.30-14.50, venerd\u00ec 8 settembre Alessandro Audrito ETH Zurich Il problema dell&#8217;ostacolo parabolico con diffusione fully nonlinear [&hellip;]<\/p>\n","protected":false},"author":3,"featured_media":0,"parent":205,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v21.0 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>S2 - Equazione differenziali alle derivate parziali - Congresso UMI 2023<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/umi.dm.unibo.it\/congresso2023\/programma\/sezioni\/s2-equazione-differenziali-alle-derivate-parziali\/\" \/>\n<meta property=\"og:locale\" content=\"it_IT\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"S2 - Equazione differenziali alle derivate parziali - Congresso UMI 2023\" \/>\n<meta property=\"og:description\" content=\"Le comunicazioni si svolgeranno &#8211; mercoled\u00ec 6, Polo Carmignani, Aula Magna &#8211; gioved\u00ec 7, Polo Carmignani, Aula Magna &#8211; venerd\u00ec 8 settembre, Polo Carmignani,, Aula 2 &nbsp; Giovanni S. 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