{"id":21,"date":"2026-02-19T15:18:01","date_gmt":"2026-02-19T15:18:01","guid":{"rendered":"https:\/\/teams.issibern.ch\/energizationprocesses\/?page_id=21"},"modified":"2026-02-25T14:37:18","modified_gmt":"2026-02-25T14:37:18","slug":"meeting","status":"publish","type":"page","link":"https:\/\/teams.issibern.ch\/energizationprocesses\/meeting\/","title":{"rendered":"Meeting"},"content":{"rendered":"<p><strong>First meeting (February 2026):<\/strong><\/p>\n<p>Schedule:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone  wp-image-34\" src=\"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-content\/uploads\/sites\/160\/2026\/02\/IMG_0026-copie-300x197.jpg\" alt=\"\" width=\"578\" height=\"379\" srcset=\"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-content\/uploads\/sites\/160\/2026\/02\/IMG_0026-copie-300x197.jpg 300w, https:\/\/teams.issibern.ch\/energizationprocesses\/wp-content\/uploads\/sites\/160\/2026\/02\/IMG_0026-copie-1024x673.jpg 1024w, https:\/\/teams.issibern.ch\/energizationprocesses\/wp-content\/uploads\/sites\/160\/2026\/02\/IMG_0026-copie-768x504.jpg 768w, https:\/\/teams.issibern.ch\/energizationprocesses\/wp-content\/uploads\/sites\/160\/2026\/02\/IMG_0026-copie-1536x1009.jpg 1536w, https:\/\/teams.issibern.ch\/energizationprocesses\/wp-content\/uploads\/sites\/160\/2026\/02\/IMG_0026-copie-2048x1345.jpg 2048w\" sizes=\"auto, (max-width: 578px) 100vw, 578px\" \/><\/p>\n<table style=\"width: 100%\" cellspacing=\"0\" cellpadding=\"0\">\n<tbody>\n<tr>\n<td style=\"width: 99.770115%\" colspan=\"3\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\"><b>Monday schedule<\/b><b><\/b><\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">9:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Introduction &amp; self-introduction<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">9:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Sergio Toledo-Redondo<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Statistics of the Warm Plasma Cloak and detached plasmaspheric plasma<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">10:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Inmaculada Albert<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Gaussian Mixture Model applied to cold plasma<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">11:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Coffee break<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">11:10<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Chris Cully<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Cold plasma structure relation to wave growth and high energy particle precipitation<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">11:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Jing Liao<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Identification of\u00a0the source of the warm plasma cloak<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">12:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Lunch<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">13:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Lynn Kistler<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; Contribution of the solar wind plasma to the plasma sheet<br \/>\n&#8211; Contributions of ionospheric ions accelerated at the near-earth reconnection region.<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">14:15<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Adam Michael<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; Global multi-fluid MHD simulations of the plasmaspheric evolution during and following storms<br \/>\n&#8211; Global test particle simulations of oxygen ion transport and heating<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">15:15<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Coffee break<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">15:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Guillaume Peyrichon<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Simulations of Kelvin-Helmholtz instability<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">16:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Jean-Fran\u00e7ois Ripoll <\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Simulations of wave-particle interactions in the radiation belts<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">16:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Alexandre Winant<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Ionization of the atmosphere, radiation belts and plasmasphere<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">17:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Welcome drink<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 99.770115%\" colspan=\"3\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\"><b>Tuesday schedule<\/b><b><\/b><\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">9:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Jean-Fran\u00e7ois Ripoll <\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Simulations of wave-particle interactions in the radiation belts<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">9:15<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">J\u00e9r\u00e9my Dargent<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Energy budgets of magnetic reconnection with cold ions<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">9:45<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Dan Welling<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; 3-fluid simulations of outflow &amp; multifluid coupling with a plasmasphere code<br \/>\n&#8211; New way to measure the total reconnection potential on the dayside<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">10:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Coffee break<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">10:45<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Alexandre Winant<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Ionization of the atmosphere, radiation belts and plasmasphere<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">11:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Cecilia Norgren<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Gaussian Mixture Model applied to cold plasma<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">12:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Lunch<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">13:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Alex Glocer<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; Overview of the ion outflow model in global MHD simulation<br \/>\n&#8211; Case studies tracking different plasma sources though the magnetosphere<br \/>\n&#8211; Other code and method improvements<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">14:30<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">End of presentation &amp; start of team work<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; Identification of the energization processes of interest<br \/>\n&#8211; Collaboration works<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">19:00<\/span><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">Social dinner<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 99.770115%\" colspan=\"3\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\"><b>Wednesday schedule<\/b><b><\/b><\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; Select dataset and\/or events with energization processes in presence of ionospheric plasma<br \/>\n&#8211; Collaboration works<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 99.770115%\" colspan=\"3\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\"><b>Thursday schedule<\/b><b><\/b><\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; Defining simulation setup associated with previously selected dataset\/events<br \/>\n&#8211; Collaboration works<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 99.770115%\" colspan=\"3\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\"><b>Friday schedule<\/b><b><\/b><\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 6.666667%\" valign=\"top\"><\/td>\n<td style=\"width: 44.597701%\" valign=\"top\"><span style=\"color: #000000;font-family: Helvetica Neue;font-size: small\">&#8211; Collaboration works<\/span><\/td>\n<td style=\"width: 48.505747%\" valign=\"top\"><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n","protected":false},"excerpt":{"rendered":"<p>First meeting (February 2026): Schedule: Monday schedule 9:00 Introduction &amp; self-introduction 9:30 Sergio Toledo-Redondo Statistics of the Warm Plasma Cloak and detached plasmaspheric plasma 10:30 Inmaculada Albert Gaussian Mixture Model applied to cold plasma 11:00 Coffee break 11:10 Chris Cully Cold plasma structure relation to wave growth and high energy particle precipitation 11:30 Jing Liao [&hellip;]<\/p>\n","protected":false},"author":189,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-21","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/pages\/21","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/users\/189"}],"replies":[{"embeddable":true,"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/comments?post=21"}],"version-history":[{"count":10,"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/pages\/21\/revisions"}],"predecessor-version":[{"id":38,"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/pages\/21\/revisions\/38"}],"wp:attachment":[{"href":"https:\/\/teams.issibern.ch\/energizationprocesses\/wp-json\/wp\/v2\/media?parent=21"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}