{"id":107,"date":"2018-10-12T08:30:43","date_gmt":"2018-10-12T08:30:43","guid":{"rendered":"http:\/\/cyprusconferences.org\/isnps2020\/?page_id=107"},"modified":"2021-11-16T15:17:37","modified_gmt":"2021-11-16T15:17:37","slug":"program","status":"publish","type":"page","link":"https:\/\/cyprusconferences.org\/stimulate2021\/program\/","title":{"rendered":"Program"},"content":{"rendered":"<p>[et_pb_section fb_built=&#8221;1&#8243; _builder_version=&#8221;3.17.2&#8243; use_background_color_gradient=&#8221;on&#8221; background_color_gradient_start=&#8221;#0972c1&#8243; background_color_gradient_end=&#8221;rgba(41,196,169,0)&#8221;][et_pb_row custom_padding=&#8221;28px|0px|29px|0px|false|false&#8221; _builder_version=&#8221;3.16.1&#8243;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;3.16.1&#8243; parallax=&#8221;off&#8221; parallax_method=&#8221;on&#8221;][et_pb_text _builder_version=&#8221;3.19.3&#8243; text_font=&#8221;||||||||&#8221;]<\/p>\n<p style=\"text-align: center;\"><span style=\"font-size: xx-large; color: #ffffff;\">SCIENTIFIC\u00a0 PROGRAM\u00a0<\/span><\/p>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; _builder_version=&#8221;3.16.1&#8243; custom_padding=&#8221;0|0px|190.297px|0px|false|false&#8221;][et_pb_row _builder_version=&#8221;3.16.1&#8243;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;3.16.1&#8243; parallax=&#8221;off&#8221; parallax_method=&#8221;on&#8221;][et_pb_accordion _builder_version=&#8221;3.19.3&#8243;][et_pb_accordion_item title=&#8221;Monday, November 22&#8243; open=&#8221;on&#8221; _builder_version=&#8221;3.19.3&#8243; title_text_shadow_horizontal_length=&#8221;0em&#8221; title_text_shadow_vertical_length=&#8221;0em&#8221; title_text_shadow_blur_strength=&#8221;0em&#8221; body_text_shadow_horizontal_length=&#8221;0em&#8221; body_text_shadow_vertical_length=&#8221;0em&#8221; body_text_shadow_blur_strength=&#8221;0em&#8221;]<\/p>\n<p><span><div class=\"wptb-container-legacy\" data-table-id=\"2934\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(80, 227, 194); width: 100px;\" data-x-index=\"0\" data-y-index=\"0\" data-wptb-own-bg-color=\"#50E3C2FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-29\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\"><p>09:15-09:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(80, 227, 194); width: 541px;\" data-x-index=\"1\" data-y-index=\"0\" data-wptb-own-bg-color=\"#50E3C2FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-30\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Welcome<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Andreas Fommer - Computing Matrix Functions<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Stefan K\u00fchn - Noisy intermediate-scale quantum computers: strategies for circuit design and error mitigation<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Peter Messmer-Coupled multi-physics workflows on modern GPU supercomputers<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Pan Kessel- On the Relation between General Relativity and Explanation Methods for Neural Networks<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-15:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Fabio Schifano-Challenges in Programming Recent HPC Processors<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:00-15:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Gustavo Ramirez -&nbsp;Coarsest-Level Improvements of Multigrid for Lattice QCD on Large-Scale Computers<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-19\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:30-16:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-20\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Malak Diab -&nbsp;Splitting Methods for Coupled Field-Circuit DAEs<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-21\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:00-16:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-22\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-23\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:30-17:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-24\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Mostafa Nasr Khalil -&nbsp;A Multilevel Approach to Stochastic Estimation of the Trace<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-25\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:00-17:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-26\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Giovanni Iannelli - Noisy Bayesian optimization for variational quantum eigensolver<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px; background-color: rgb(248, 231, 28);\" data-x-index=\"0\" data-y-index=\"13\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-27\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:00-19:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px; background-color: rgb(248, 231, 28);\" data-x-index=\"1\" data-y-index=\"13\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-28\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Welcome Reception<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n<\/span><\/p>\n<p>&nbsp;<\/p>\n<p>[\/et_pb_accordion_item][et_pb_accordion_item title=&#8221;Tuesday, November 23&#8243; open=&#8221;off&#8221; _builder_version=&#8221;3.19.3&#8243; title_text_shadow_horizontal_length=&#8221;0em&#8221; title_text_shadow_vertical_length=&#8221;0em&#8221; title_text_shadow_blur_strength=&#8221;0em&#8221; body_text_shadow_horizontal_length=&#8221;0em&#8221; body_text_shadow_vertical_length=&#8221;0em&#8221; body_text_shadow_blur_strength=&#8221;0em&#8221;]<\/p>\n<p><span><div class=\"wptb-container-legacy\" data-table-id=\"2928\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-wptb-responsive-directives=\"eyJyZXNwb25zaXZlRW5hYmxlZCI6ZmFsc2UsInJlc3BvbnNpdmVNb2RlIjoiYXV0byIsInByZXNlcnZlUm93Q29sb3IiOmZhbHNlLCJyZWxhdGl2ZVdpZHRoIjoid2luZG93IiwiaGVhZGVyRnVsbHlNZXJnZWQiOmZhbHNlLCJtb2RlT3B0aW9ucyI6eyJhdXRvIjp7ImRpc2FibGVkIjp7ImRlc2t0b3AiOmZhbHNlLCJ0YWJsZXQiOmZhbHNlLCJtb2JpbGUiOmZhbHNlfSwidG9wUm93QXNIZWFkZXIiOnsiZGVza3RvcCI6ZmFsc2UsInRhYmxldCI6dHJ1ZSwibW9iaWxlIjp0cnVlfSwicmVwZWF0TWVyZ2VkSGVhZGVyIjp7ImRlc2t0b3AiOnRydWUsInRhYmxldCI6dHJ1ZSwibW9iaWxlIjp0cnVlfSwic3RhdGljVG9wUm93Ijp7ImRlc2t0b3AiOmZhbHNlLCJ0YWJsZXQiOmZhbHNlLCJtb2JpbGUiOmZhbHNlfSwiY2VsbFN0YWNrRGlyZWN0aW9uIjp7ImRlc2t0b3AiOiJyb3ciLCJ0YWJsZXQiOiJyb3ciLCJtb2JpbGUiOiJyb3cifSwiY2VsbHNQZXJSb3ciOnsiZGVza3RvcCI6MSwidGFibGV0IjoxLCJtb2JpbGUiOjF9fX0sImJyZWFrcG9pbnRzIjp7ImRlc2t0b3AiOnsibmFtZSI6ImRlc2t0b3AiLCJ3aWR0aCI6MTAyNH0sInRhYmxldCI6eyJuYW1lIjoidGFibGV0Iiwid2lkdGgiOjcwMH0sIm1vYmlsZSI6eyJuYW1lIjoibW9iaWxlIiwid2lkdGgiOjMwMH19fQ==\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;Douglas Armstrong -&nbsp;Network Topology Analysis of the Synaptic Proteome<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nir Ben-Tal - Protein archaeology: How proteins emerged and evolve?<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Giulia Rosetti - Computational Biomedicine in neurodegenerative diseases<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Erik Lindahl -Multiscale Models of Human Skin and Permeation from Fitting Molecules and Simulations to CEMOVIS image data<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-15:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">George Spyrou -&nbsp;Network-based integration and inference for functional analysis and drug repurposing<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:00-15:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nikos Savva - Modelling of contact line phenomena on heterogeneous surfaces<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-21\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:45-16:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-22\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-23\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:00-16:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-24\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nicola Marzari - The great acceleration in materials design and discovery<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-25\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:45-17:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-26\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Giacomo Falcucci - Multiphase Lattice Boltzmann and Tolmann Length<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-53\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:30-18:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-54\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Fabio Guglietta -&nbsp;On the effect of membrane viscosity on loading and relaxation dynamics for a single red blood cell\"&nbsp;<br>&nbsp;<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px; background-color: rgb(126, 211, 33);\" data-x-index=\"0\" data-y-index=\"12\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-27\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:30-19:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px; background-color: rgb(126, 211, 33);\" data-x-index=\"1\" data-y-index=\"12\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-28\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\"><strong>Posters: Poster session&nbsp;&nbsp;<\/strong><\/p><p style=\"text-align: center;\"><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"13\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-29\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"13\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-30\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Maria Arnittali<\/em> -&nbsp;Understanding the Structure and Stability of Biomolecules via Atomistic Molecular Dynamics Simulations<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"14\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-31\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"14\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-32\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;<em>Evangelos Papaefthymiou,&nbsp; Orestis Pavlou<\/em> -&nbsp;Classification of local ultraluminous infrared galaxies and quasars with Kernel PCA<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"15\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-33\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"15\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-34\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Michalis Papadopoulos<\/em> -&nbsp;A Network Science approach for studying galaxy evolution<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"16\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-35\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"16\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-36\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Charalambia Varnava<\/em> -&nbsp;MCMC model fitting methods for studying galaxy evolution<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"17\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-37\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"17\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-38\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p class=\"\">&nbsp;<em>Agapi Maria Rissaki<\/em> -&nbsp;Reconstructing High Spectral Resolution Spectra of Galaxies Using Limited Photometry and Deep Generative Networks<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"18\" data-wptb-own-bg-color=\"#7ED321FF\"><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"18\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-40\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p class=\"\"><em>Dimitrios Kelesis<\/em> -&nbsp;Detecting and Analyzing the Topology of the Cosmic Web with Spatial Clustering Algorithms<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"19\" data-wptb-own-bg-color=\"#7ED321FF\"><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"19\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-56\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Nikolaos Patsalidis -&nbsp;<\/em>Hierarchical Computational Study of Polybutadiene\/Alumina Systems, via Ab-initio Calculations and Atomistic Simulations<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"20\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-45\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"20\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-46\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;<em>AIkaterini Keliri<\/em> -&nbsp;Application of RISE in Myocardial Perfusion SPECT Imaging, using a Cardiac Phantom<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"21\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-47\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"21\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-48\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;<em>Eirini Gkolfi<\/em> - Utilization of HPC for computational study of polymers with complex architecture in atomic scale<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"22\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-49\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"22\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-50\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Stavros Athanasiou<\/em> -&nbsp;Flow-based generative models for simulating the quantum harmonic and anharmonic oscillator<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"23\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-51\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"23\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-52\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Charalambos Chrysostomou<\/em> -&nbsp;Predict the Next Influenza Pandemic using Deep Learning Methodologies<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n<\/span><\/p>\n<p>[\/et_pb_accordion_item][et_pb_accordion_item title=&#8221;Wednesday, November 24&#8243; open=&#8221;off&#8221; _builder_version=&#8221;3.19.3&#8243; title_text_shadow_horizontal_length=&#8221;0em&#8221; title_text_shadow_vertical_length=&#8221;0em&#8221; title_text_shadow_blur_strength=&#8221;0em&#8221; body_text_shadow_horizontal_length=&#8221;0em&#8221; body_text_shadow_vertical_length=&#8221;0em&#8221; body_text_shadow_blur_strength=&#8221;0em&#8221;]<\/p>\n<p><span><div class=\"wptb-container-legacy\" data-table-id=\"2938\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-wptb-responsive-directives=\"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\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:00-09:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Oscar Palomino Hernandez -&nbsp;Conformational studies on alpha synuclein as contrasted by experiments<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Ke Zuo -&nbsp;The two redox states of the human NEET proteins\u2019 [2Fe\u20132S] clusters<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"2\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-31\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:00-10:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"2\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-32 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Henri-Baptiste Marjault -A novel anti-diabetic drug targeting NEET (CISD) proteins<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"3\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-33\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:30-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"3\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-34\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Guilherme Tegoni Goedert - Extreme events in Shell Models of Turbulence<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Lokahith Agasthya - Reconstruction and Modification of Turbulent Thermal Flows Using Eulerian and Lagrangian Approaches<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:00-12:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Daniele Simeoni -&nbsp;Algorithms for Relativistic Lattice Boltzmann<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-35\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:30-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-36\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Madeleine Dale -&nbsp;Baryon masses from full QCD+QED_C simulations<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"8\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-37\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-13:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"8\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-38\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Pietro Faccioli -&nbsp;From Quarks to Drugs: A journey in cross-disciplinary and translational applications of path integral methods<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>1330-14:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px; background-color: rgb(248, 231, 28);\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:30-18:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px; background-color: rgb(248, 231, 28);\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Excursion<\/p><p style=\"text-align: center;\"><br><\/p><p style=\"text-align: center;\"><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(255, 255, 255); width: 100px;\" data-wptb-own-bg-color=\"#FFFFFFFF\"><\/td><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(255, 255, 255); width: 541px;\" data-wptb-own-bg-color=\"#FFFFFFFF\"><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-x-index=\"0\" data-y-index=\"12\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-39\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>20:00-22:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-x-index=\"1\" data-y-index=\"12\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-40\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Dinner<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n<\/span><\/p>\n<p>[\/et_pb_accordion_item][et_pb_accordion_item title=&#8221;Thursday, November 25&#8243; open=&#8221;off&#8221; _builder_version=&#8221;3.19.3&#8243; title_text_shadow_horizontal_length=&#8221;0em&#8221; title_text_shadow_vertical_length=&#8221;0em&#8221; title_text_shadow_blur_strength=&#8221;0em&#8221; body_text_shadow_horizontal_length=&#8221;0em&#8221; body_text_shadow_vertical_length=&#8221;0em&#8221; body_text_shadow_blur_strength=&#8221;0em&#8221;]<\/p>\n<table class=\"wp-list-table widefat fixed striped wptbtables\">\n<tbody id=\"the-list\" data-wp-lists=\"list:wptbtable\">\n<tr>\n<td class=\"shortcode column-shortcode\" data-colname=\"Shortcode\"><div class=\"wptb-container-legacy\" data-table-id=\"2942\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Silvia Morante -&nbsp;SARS-CoV-2 immune response evasion mediated by Zn ions: models, simulations and experiments<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Prof. Vangelis Harmandaris - Hierarchical Computational Modeling of Complex Nanostructured Materials Across Scales<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Massimo Cencini - Learning pursuing and evasion strategies at low Reynolds number<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Dr Michele Buzzicotti -&nbsp;AI meets turbulence: Lagrangian and Eulerian data-driven tools for optimal navigation and data-assimilation<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-15:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nazario Tantalo - Extraction of spectral densities from lattice correlators<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:00-15:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Martha Constantinou - The structure of the proton from numerical simulations of lattice QCD<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-19\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:45-16:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-20\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Fabio Montagnino - Introduction to innovation: from theory to practice<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-21\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:30-17:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-22\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-23\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:00-17:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-24\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Urs Wenger -&nbsp;Pion-pole contribution to the muon g-2 from Lattice QCD<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-27\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:30-18:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-28\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Floriano Manigrasso -&nbsp;Flavor decomposition for the proton unpolarized, helicity and transversity parton distribution functions<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-25\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:00-18:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-26\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Antonino Todaro -&nbsp;Neutron electric dipole moment using lattice QCD simulations at the physical point<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"13\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-29\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:30-19:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"13\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-30 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Ahmed Bakry -&nbsp;Topological terms in the effective string action<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>[\/et_pb_accordion_item][et_pb_accordion_item title=&#8221;Friday, November 26&#8243; open=&#8221;off&#8221; _builder_version=&#8221;3.19.3&#8243; title_text_shadow_horizontal_length=&#8221;0em&#8221; title_text_shadow_vertical_length=&#8221;0em&#8221; title_text_shadow_blur_strength=&#8221;0em&#8221; body_text_shadow_horizontal_length=&#8221;0em&#8221; body_text_shadow_vertical_length=&#8221;0em&#8221; body_text_shadow_blur_strength=&#8221;0em&#8221;]<\/p>\n<table class=\"wp-list-table widefat fixed striped wptbtables\">\n<tbody id=\"the-list\" data-wp-lists=\"list:wptbtable\">\n<tr>\n<td class=\"shortcode column-shortcode\" data-colname=\"Shortcode\"><div class=\"wptb-container-legacy\" data-table-id=\"2944\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Marcus Petschlies - Pion-Nucleon scattering in lattice QCD \u200b<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Kyriacos Hadjiyiannakou - Nucleon Spin on the Lattice<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Sinead Ryan - Heavy flavour spectroscopy from lattice QCD: a multiscale challenge<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Hartmut Wittig - Hadron Structure in Lattice QCD: Status and Challenges<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-x-index=\"0\" data-y-index=\"5\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-x-index=\"1\" data-y-index=\"5\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"6\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-14:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"6\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Jacob Finkenrath -&nbsp;Monte Carlo simulations of the 2D Schwinger Model via machine-learned flows in Global Correction steps<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:45-15:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Ferenc Pittler -&nbsp;Determining quark masses with lattice simulation<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>[\/et_pb_accordion_item][\/et_pb_accordion][\/et_pb_column][\/et_pb_row][\/et_pb_section]<\/p>\n","protected":false},"excerpt":{"rendered":"<p>SCIENTIFIC\u00a0 PROGRAM\u00a0<div class=\"wptb-container-legacy\" data-table-id=\"2934\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(80, 227, 194); width: 100px;\" data-x-index=\"0\" data-y-index=\"0\" data-wptb-own-bg-color=\"#50E3C2FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-29\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\"><p>09:15-09:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(80, 227, 194); width: 541px;\" data-x-index=\"1\" data-y-index=\"0\" data-wptb-own-bg-color=\"#50E3C2FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-30\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Welcome<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Andreas Fommer - Computing Matrix Functions<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Stefan K\u00fchn - Noisy intermediate-scale quantum computers: strategies for circuit design and error mitigation<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Peter Messmer-Coupled multi-physics workflows on modern GPU supercomputers<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Pan Kessel- On the Relation between General Relativity and Explanation Methods for Neural Networks<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-15:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Fabio Schifano-Challenges in Programming Recent HPC Processors<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:00-15:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Gustavo Ramirez -&nbsp;Coarsest-Level Improvements of Multigrid for Lattice QCD on Large-Scale Computers<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-19\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:30-16:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-20\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Malak Diab -&nbsp;Splitting Methods for Coupled Field-Circuit DAEs<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-21\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:00-16:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-22\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-23\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:30-17:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-24\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Mostafa Nasr Khalil -&nbsp;A Multilevel Approach to Stochastic Estimation of the Trace<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-25\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:00-17:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-26\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Giovanni Iannelli - Noisy Bayesian optimization for variational quantum eigensolver<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px; background-color: rgb(248, 231, 28);\" data-x-index=\"0\" data-y-index=\"13\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-27\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:00-19:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px; background-color: rgb(248, 231, 28);\" data-x-index=\"1\" data-y-index=\"13\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-28\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Welcome Reception<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n &nbsp; <div class=\"wptb-container-legacy\" data-table-id=\"2928\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-wptb-responsive-directives=\"eyJyZXNwb25zaXZlRW5hYmxlZCI6ZmFsc2UsInJlc3BvbnNpdmVNb2RlIjoiYXV0byIsInByZXNlcnZlUm93Q29sb3IiOmZhbHNlLCJyZWxhdGl2ZVdpZHRoIjoid2luZG93IiwiaGVhZGVyRnVsbHlNZXJnZWQiOmZhbHNlLCJtb2RlT3B0aW9ucyI6eyJhdXRvIjp7ImRpc2FibGVkIjp7ImRlc2t0b3AiOmZhbHNlLCJ0YWJsZXQiOmZhbHNlLCJtb2JpbGUiOmZhbHNlfSwidG9wUm93QXNIZWFkZXIiOnsiZGVza3RvcCI6ZmFsc2UsInRhYmxldCI6dHJ1ZSwibW9iaWxlIjp0cnVlfSwicmVwZWF0TWVyZ2VkSGVhZGVyIjp7ImRlc2t0b3AiOnRydWUsInRhYmxldCI6dHJ1ZSwibW9iaWxlIjp0cnVlfSwic3RhdGljVG9wUm93Ijp7ImRlc2t0b3AiOmZhbHNlLCJ0YWJsZXQiOmZhbHNlLCJtb2JpbGUiOmZhbHNlfSwiY2VsbFN0YWNrRGlyZWN0aW9uIjp7ImRlc2t0b3AiOiJyb3ciLCJ0YWJsZXQiOiJyb3ciLCJtb2JpbGUiOiJyb3cifSwiY2VsbHNQZXJSb3ciOnsiZGVza3RvcCI6MSwidGFibGV0IjoxLCJtb2JpbGUiOjF9fX0sImJyZWFrcG9pbnRzIjp7ImRlc2t0b3AiOnsibmFtZSI6ImRlc2t0b3AiLCJ3aWR0aCI6MTAyNH0sInRhYmxldCI6eyJuYW1lIjoidGFibGV0Iiwid2lkdGgiOjcwMH0sIm1vYmlsZSI6eyJuYW1lIjoibW9iaWxlIiwid2lkdGgiOjMwMH19fQ==\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;Douglas Armstrong -&nbsp;Network Topology Analysis of the Synaptic Proteome<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nir Ben-Tal - Protein archaeology: How proteins emerged and evolve?<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Giulia Rosetti - Computational Biomedicine in neurodegenerative diseases<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Erik Lindahl -Multiscale Models of Human Skin and Permeation from Fitting Molecules and Simulations to CEMOVIS image data<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-15:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">George Spyrou -&nbsp;Network-based integration and inference for functional analysis and drug repurposing<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:00-15:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nikos Savva - Modelling of contact line phenomena on heterogeneous surfaces<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-21\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:45-16:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-22\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-23\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:00-16:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-24\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nicola Marzari - The great acceleration in materials design and discovery<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-25\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:45-17:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-26\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Giacomo Falcucci - Multiphase Lattice Boltzmann and Tolmann Length<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-53\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:30-18:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-54\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Fabio Guglietta -&nbsp;On the effect of membrane viscosity on loading and relaxation dynamics for a single red blood cell\"&nbsp;<br>&nbsp;<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px; background-color: rgb(126, 211, 33);\" data-x-index=\"0\" data-y-index=\"12\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-27\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:30-19:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px; background-color: rgb(126, 211, 33);\" data-x-index=\"1\" data-y-index=\"12\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-28\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\"><strong>Posters: Poster session&nbsp;&nbsp;<\/strong><\/p><p style=\"text-align: center;\"><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"13\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-29\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"13\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-30\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Maria Arnittali<\/em> -&nbsp;Understanding the Structure and Stability of Biomolecules via Atomistic Molecular Dynamics Simulations<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"14\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-31\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"14\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-32\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;<em>Evangelos Papaefthymiou,&nbsp; Orestis Pavlou<\/em> -&nbsp;Classification of local ultraluminous infrared galaxies and quasars with Kernel PCA<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"15\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-33\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"15\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-34\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Michalis Papadopoulos<\/em> -&nbsp;A Network Science approach for studying galaxy evolution<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"16\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-35\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"16\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-36\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Charalambia Varnava<\/em> -&nbsp;MCMC model fitting methods for studying galaxy evolution<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"17\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-37\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"17\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-38\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p class=\"\">&nbsp;<em>Agapi Maria Rissaki<\/em> -&nbsp;Reconstructing High Spectral Resolution Spectra of Galaxies Using Limited Photometry and Deep Generative Networks<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"18\" data-wptb-own-bg-color=\"#7ED321FF\"><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"18\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-40\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p class=\"\"><em>Dimitrios Kelesis<\/em> -&nbsp;Detecting and Analyzing the Topology of the Cosmic Web with Spatial Clustering Algorithms<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"19\" data-wptb-own-bg-color=\"#7ED321FF\"><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"19\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-56\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Nikolaos Patsalidis -&nbsp;<\/em>Hierarchical Computational Study of Polybutadiene\/Alumina Systems, via Ab-initio Calculations and Atomistic Simulations<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"20\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-45\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"20\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-46\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;<em>AIkaterini Keliri<\/em> -&nbsp;Application of RISE in Myocardial Perfusion SPECT Imaging, using a Cardiac Phantom<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"21\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-47\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"21\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-48\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>&nbsp;<em>Eirini Gkolfi<\/em> - Utilization of HPC for computational study of polymers with complex architecture in atomic scale<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"22\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-49\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"22\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-50\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Stavros Athanasiou<\/em> -&nbsp;Flow-based generative models for simulating the quantum harmonic and anharmonic oscillator<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 100px;\" data-x-index=\"0\" data-y-index=\"23\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-51\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(126, 211, 33); width: 541px;\" data-x-index=\"1\" data-y-index=\"23\" data-wptb-own-bg-color=\"#7ED321FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-52\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p><em>Charalambos Chrysostomou<\/em> -&nbsp;Predict the Next Influenza Pandemic using Deep Learning Methodologies<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n<div class=\"wptb-container-legacy\" data-table-id=\"2938\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-wptb-responsive-directives=\"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\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:00-09:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Oscar Palomino Hernandez -&nbsp;Conformational studies on alpha synuclein as contrasted by experiments<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Ke Zuo -&nbsp;The two redox states of the human NEET proteins\u2019 [2Fe\u20132S] clusters<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"2\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-31\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:00-10:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"2\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-32 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Henri-Baptiste Marjault -A novel anti-diabetic drug targeting NEET (CISD) proteins<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"3\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-33\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:30-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"3\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-34\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Guilherme Tegoni Goedert - Extreme events in Shell Models of Turbulence<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Lokahith Agasthya - Reconstruction and Modification of Turbulent Thermal Flows Using Eulerian and Lagrangian Approaches<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:00-12:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Daniele Simeoni -&nbsp;Algorithms for Relativistic Lattice Boltzmann<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-35\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:30-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-36\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Madeleine Dale -&nbsp;Baryon masses from full QCD+QED_C simulations<\/p><p><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"8\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-37\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-13:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"8\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-38\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Pietro Faccioli -&nbsp;From Quarks to Drugs: A journey in cross-disciplinary and translational applications of path integral methods<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>1330-14:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px; background-color: rgb(248, 231, 28);\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:30-18:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px; background-color: rgb(248, 231, 28);\" data-wptb-own-bg-color=\"#F8E71CFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Excursion<\/p><p style=\"text-align: center;\"><br><\/p><p style=\"text-align: center;\"><\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(255, 255, 255); width: 100px;\" data-wptb-own-bg-color=\"#FFFFFFFF\"><\/td><td class=\"wptb-cell\" data-y-index=\"11\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(255, 255, 255); width: 541px;\" data-wptb-own-bg-color=\"#FFFFFFFF\"><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-x-index=\"0\" data-y-index=\"12\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-39\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>20:00-22:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-x-index=\"1\" data-y-index=\"12\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-40\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Dinner<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n <div class=\"wptb-container-legacy\" data-table-id=\"2942\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Silvia Morante -&nbsp;SARS-CoV-2 immune response evasion mediated by Zn ions: models, simulations and experiments<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Prof. Vangelis Harmandaris - Hierarchical Computational Modeling of Complex Nanostructured Materials Across Scales<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Massimo Cencini - Learning pursuing and evasion strategies at low Reynolds number<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Dr Michele Buzzicotti -&nbsp;AI meets turbulence: Lagrangian and Eulerian data-driven tools for optimal navigation and data-assimilation<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"5\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-15:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"6\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Nazario Tantalo - Extraction of spectral densities from lattice correlators<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:00-15:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"7\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Martha Constantinou - The structure of the proton from numerical simulations of lattice QCD<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-19\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>15:45-16:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"8\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-20\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Fabio Montagnino - Introduction to innovation: from theory to practice<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-21\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>16:30-17:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"9\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-22\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-23\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:00-17:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"10\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-24\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Urs Wenger -&nbsp;Pion-pole contribution to the muon g-2 from Lattice QCD<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-27\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>17:30-18:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"11\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-28\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Floriano Manigrasso -&nbsp;Flavor decomposition for the proton unpolarized, helicity and transversity parton distribution functions<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-25\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:00-18:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"12\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-26\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Antonino Todaro -&nbsp;Neutron electric dipole moment using lattice QCD simulations at the physical point<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"13\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-29\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>18:30-19:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"13\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-30 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">&nbsp;Ahmed Bakry -&nbsp;Topological terms in the effective string action<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n <div class=\"wptb-container-legacy\" data-table-id=\"2944\">\n    <table class=\"wptb-preview-table wptb-element-main-table_setting-2928\" data-reconstraction=\"1\" style=\"border: 1px solid rgb(209, 209, 209);\" data-wptb-table-tds-sum-max-width=\"704\" data-wptb-extra-styles=\"LyogRW50ZXIgeW91ciBjdXN0b20gQ1NTIHJ1bGVzIGhlcmUgKi8=\" role=\"table\" data-wptb-odd-row-background-color=\"#9AEDFFFF\" data-table-columns=\"2\"><tbody><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-1\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>09:30-10:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"0\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\" data-wptb-cell-vertical-alignment=\"top\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-2\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Marcus Petschlies - Pion-Nucleon scattering in lattice QCD \u200b<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-3\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>10:15-11:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"1\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-4\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Kyriacos Hadjiyiannakou - Nucleon Spin on the Lattice<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-5\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:00-11:30<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"2\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-6 edit-active\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Coffee Break<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-9\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>11:30-12:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"3\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-wptb-own-bg-color=\"#9AEDFFFF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-10\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Sinead Ryan - Heavy flavour spectroscopy from lattice QCD: a multiscale challenge<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"0\" style=\"border: 1px solid rgb(209, 209, 209); width: 100px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-11\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>12:15-13:00<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" data-y-index=\"4\" data-x-index=\"1\" style=\"border: 1px solid rgb(209, 209, 209); width: 541px;\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-12\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Hartmut Wittig - Hadron Structure in Lattice QCD: Status and Challenges<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 100px;\" data-x-index=\"0\" data-y-index=\"5\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-13\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>13:00-14:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(184, 233, 134); width: 541px;\" data-x-index=\"1\" data-y-index=\"5\" data-wptb-own-bg-color=\"#B8E986FF\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-14\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Lunch<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\" style=\"background-color: rgb(154, 237, 255);\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"6\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-15\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:15-14:45<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"6\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-16\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Jacob Finkenrath -&nbsp;Monte Carlo simulations of the 2D Schwinger Model via machine-learned flows in Global Correction steps<\/p><\/div><\/div><\/td><\/tr><tr class=\"wptb-row\"><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 100px;\" data-x-index=\"0\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-17\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p>14:45-15:15<\/p><\/div><\/div><\/td><td class=\"wptb-cell\" style=\"border: 1px solid rgb(209, 209, 209); background-color: rgb(154, 237, 255); width: 541px;\" data-x-index=\"1\" data-y-index=\"7\"><div class=\"wptb-text-container wptb-ph-element wptb-element-text-18\" style=\"color: rgb(74, 85, 104); font-size: 15px;\"><div class=\"\" style=\"position: relative;\"><p style=\"text-align: center;\">Ferenc Pittler -&nbsp;Determining quark masses with lattice simulation<\/p><\/div><\/div><\/td><\/tr><\/tbody><\/table>\n<\/div>\n<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":""},"_links":{"self":[{"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/pages\/107"}],"collection":[{"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/comments?post=107"}],"version-history":[{"count":13,"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/pages\/107\/revisions"}],"predecessor-version":[{"id":2951,"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/pages\/107\/revisions\/2951"}],"wp:attachment":[{"href":"https:\/\/cyprusconferences.org\/stimulate2021\/wp-json\/wp\/v2\/media?parent=107"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}