{"id":83160,"date":"2023-05-29T11:29:56","date_gmt":"2023-05-29T08:29:56","guid":{"rendered":"https:\/\/myrtalycongress.gr\/?page_id=83160"},"modified":"2023-05-29T13:55:07","modified_gmt":"2023-05-29T10:55:07","slug":"abstracts-flux","status":"publish","type":"page","link":"https:\/\/myrtalycongress.gr\/en\/abstracts-flux\/","title":{"rendered":"Abstracts Flux"},"content":{"rendered":"<div class=\"wpb-content-wrapper\"><div id=\"fb-root\"><\/div>\n<div data-parent=\"true\" class=\"vc_row row-container\" id=\"row-unique-0\"><div class=\"row limit-width row-parent\"><div class=\"wpb_row row-inner\"><div class=\"wpb_column pos-top pos-center align_left column_parent col-lg-12 single-internal-gutter\"><div class=\"uncol style-light\"  ><div class=\"uncoltable\"><div class=\"uncell no-block-padding\" ><div class=\"uncont\" ><div class=\"uncode_text_column\" ><\/p>\n<table style=\"border-collapse: collapse; width: 100%; height: 692px;\">\n<tbody>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; text-align: center; height: 22px;\">\n<h4><span style=\"font-size: 12pt;\"><strong>NAME<\/strong><\/span><\/h4>\n<\/td>\n<td style=\"width: 63.7652%; text-align: center; height: 22px;\">\n<h4><span style=\"font-size: 12pt;\"><strong>TITLE<\/strong><\/span><\/h4>\n<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; text-align: left; height: 45px;\"><strong>Brun <\/strong>Allan Sacha<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">ON THE INTERPLAY BETWEEN FLUX EMERGENCE AND<br \/>\nTURBULENT CONVECTION<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Bellot Rubio<\/strong> Luis<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">UNIPOLAR AND BIPOLAR MAGNETIC FLUX APPEARANCE IN THE QUIET SUN INTERNETWORK<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Chintzoglou<\/strong> Georgios<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">COLLISIONAL SHEARING: A POSSIBLE MECHANISM PRODUCING RECURRENT EXPLOSIVE (FLARE AND CME) ACTIVITY IN SOLAR ACTIVE REGIONS<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Finley<\/strong> Adam<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">THE ROLE OF SURFACE DYNAMICS IN THE SOLAR DYNAMO<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Guglielmino<\/strong> Salvo<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">MULTIWAVELENGTH OBSERVATIONS OF SMALL-SCALE ERUPTIVE<br \/>\nPHENOMENA DURING FLUX EMERGENCE IN ACTIVE REGIONS<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Hansteen<\/strong> Viggo<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">THE MG II H&amp;K LINES AND FLUX EMERGENCE: HOW HIGH IS THE<br \/>\nCHROMOSPHERE<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Hotta<\/strong> Hideyuki<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">FLUX EMERGENCE SIMULATION FROM THE BASE OF THE<br \/>\nCONVECTION ZONE TO THE PHOTOSPHERE<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Jouve<\/strong> Laurene<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">PARAMETRIZING THE FLUX EMERGENCE PROCESS IN SIMPLIFIED<br \/>\nDYNAMO MODELS<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Leake<\/strong> James<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">ON THE PHOTOSPHERIC IMPRINTS OF SOLAR CORONAL ELECTRIC<br \/>\nCURRENTS<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>MacTaggart<\/strong> David<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">MAGNETIC WINDING AND THE STRUCTURE OF EMERGING ACTIVE<br \/>\nREGIONS<\/td>\n<\/tr>\n<tr style=\"height: 45px;\">\n<td style=\"width: 36.2348%; height: 45px;\"><strong>Martinez-Sykora<\/strong> Juan<\/td>\n<td style=\"width: 63.7652%; height: 45px;\">ON THE THERMAL AND FARLEY BULEMAN INSTABILITY IN FLUX<br \/>\nEMERGENCE<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Mathioudakis<\/strong> Mihalis<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">FLARE INDUCED PHOTOSPHERIC LINE ASYMMETRIES &#8211;<br \/>\nAPPLICATIONS TO SOLAR AND STELLAR FLARES<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Moraitis<\/strong> Kostas<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">THE ROLE OF MAGNETIC HELICITY IN EXPLAINING AN MHD FLUX<br \/>\nEMERGENCE SIMULATION<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Nindos<\/strong> Alexander<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">PROPERTIES OF THE MAGNETIC FIELD IN AN MHD SIMULATION<br \/>\nOF CORONAL JETS<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>N\u00f3brega-Siverio<\/strong> Daniel<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">AN OBSERVATIONAL STUDY OF MAGNETIC FLUX EMERGENCE LEADING TO A DARK BUBBLE, EB, SURGE, AND A UV BURST REACHING 1 MK<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Norton<\/strong> Aimee<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">WHY ARE ACTIVE REGION FLUX EMERGENCE RATES LOWER IN OBSERVATIONS THAN SIMULATIONS?<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Pariat<\/strong> Etienne<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">DYNAMICS OF MAGNETIC ENERGY AND MAGNETIC HELICITY IN ACTIVE REGIONS: RECENT NUMERICAL AND OBSERVATIONAL RESULTS<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Schmieder<\/strong> Brigitte<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">LONG-TERM EMERGING MAGNETIC FLUX AND INTERMITTENT BLOB SOLAR JETS<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Strugarek<\/strong> Antoine<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">MODELLING SOLAR ERUPTIVE EVENTS FROM THEIR ONSET TO THEIR PROPAGATION AT 1 AU<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Torok<\/strong> Tibor<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">SOLAR ERUPTIONS TRIGGERED BY FLUX EMERGENCE<\/td>\n<\/tr>\n<tr style=\"height: 22px;\">\n<td style=\"width: 36.2348%; height: 22px;\"><strong>Zhuleku<\/strong> Eugene<\/td>\n<td style=\"width: 63.7652%; height: 22px;\">MAGNETIC FLUX EMERGENCE SIMULATIONS OF TOROIDAL FLUX TUBES IN THE SUN AND CREATION OF JETS<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>\n<\/div><\/div><\/div><\/div><\/div><\/div><script id=\"script-row-unique-0\" data-row=\"script-row-unique-0\" type=\"text\/javascript\" class=\"vc_controls\">UNCODE.initRow(document.getElementById(\"row-unique-0\"));<\/script><\/div><\/div><\/div>\n<\/div>","protected":false},"excerpt":{"rendered":"NAME TITLE Brun Allan Sacha ON THE INTERPLAY BETWEEN FLUX EMERGENCE AND TURBULENT CONVECTION Bellot Rubio Luis UNIPOLAR AND BIPOLAR [...]","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_EventAllDay":false,"_EventTimezone":"","_EventStartDate":"","_EventEndDate":"","_EventStartDateUTC":"","_EventEndDateUTC":"","_EventShowMap":false,"_EventShowMapLink":false,"_EventURL":"","_EventCost":"","_EventCostDescription":"","_EventCurrencySymbol":"","_EventCurrencyCode":"","_EventCurrencyPosition":"","_EventDateTimeSeparator":"","_EventTimeRangeSeparator":"","_EventOrganizerID":[],"_EventVenueID":[],"_OrganizerEmail":"","_OrganizerPhone":"","_OrganizerWebsite":"","_VenueAddress":"","_VenueCity":"","_VenueCountry":"","_VenueProvince":"","_VenueState":"","_VenueZip":"","_VenuePhone":"","_VenueURL":"","_VenueStateProvince":"","_VenueLat":"","_VenueLng":"","_VenueShowMap":false,"_VenueShowMapLink":false,"footnotes":""},"class_list":["post-83160","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/myrtalycongress.gr\/en\/wp-json\/wp\/v2\/pages\/83160","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/myrtalycongress.gr\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/myrtalycongress.gr\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/myrtalycongress.gr\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/myrtalycongress.gr\/en\/wp-json\/wp\/v2\/comments?post=83160"}],"version-history":[{"count":0,"href":"https:\/\/myrtalycongress.gr\/en\/wp-json\/wp\/v2\/pages\/83160\/revisions"}],"wp:attachment":[{"href":"https:\/\/myrtalycongress.gr\/en\/wp-json\/wp\/v2\/media?parent=83160"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}