{"id":2,"date":"2021-12-09T11:43:17","date_gmt":"2021-12-09T11:43:17","guid":{"rendered":"https:\/\/defi-theo-climat.ipsl.fr\/?page_id=2"},"modified":"2026-03-27T15:04:58","modified_gmt":"2026-03-27T15:04:58","slug":"reseau","status":"publish","type":"page","link":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/reseau\/","title":{"rendered":"Organisation"},"content":{"rendered":"\n<p>Le GDR \u00ab\u00a0D\u00e9fis th\u00e9orique pour les sciences du climat\u00a0\u00bb est une structure de l&rsquo;Institut de Physique (INP) du CNRS soutenue par l&rsquo;Institut des Sciences de l&rsquo;Univers (INSU) et l&rsquo;Institut national des sciences math\u00e9matiques et de leurs interactions (INSMI).&nbsp;<\/p>\n\n\n\n<figure class=\"wp-block-image aligncenter is-resized size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"936\" height=\"154\" src=\"https:\/\/defi-theo-climat.ipsl.fr\/wp-content\/uploads\/2022\/01\/image-1.png\" alt=\"\" class=\"wp-image-298\" style=\"width:602px;height:auto\" srcset=\"https:\/\/defi-theo-climat.ipsl.fr\/wp-content\/uploads\/2022\/01\/image-1.png 936w, https:\/\/defi-theo-climat.ipsl.fr\/wp-content\/uploads\/2022\/01\/image-1-300x49.png 300w, https:\/\/defi-theo-climat.ipsl.fr\/wp-content\/uploads\/2022\/01\/image-1-768x126.png 768w\" sizes=\"auto, (max-width: 936px) 100vw, 936px\" \/><\/figure>\n\n\n\n<h2 class=\"wp-block-heading\"><a>Coordination<\/a><\/h2>\n\n\n\n<ul class=\"wp-block-list\">\n<li><a href=\"https:\/\/perso.ens-lyon.fr\/corentin.herbert\/\" data-type=\"link\" data-id=\"https:\/\/perso.ens-lyon.fr\/corentin.herbert\/\" target=\"_blank\" rel=\"noreferrer noopener\">Corentin Herbert<\/a> (CNRS, Laboratoire de Physique, ENS de Lyon)<\/li>\n\n\n\n<li><a href=\"https:\/\/www.lpsm.paris\/users\/fischer\/\" data-type=\"link\" data-id=\"https:\/\/www.lpsm.paris\/users\/fischer\/\" target=\"_blank\" rel=\"noreferrer noopener\">Aur\u00e9lie Fischer<\/a> (Universit\u00e9 Paris Cit\u00e9, Laboratoire de Probabilit\u00e9s, Statistique et Mod\u00e9lisation)<\/li>\n\n\n\n<li>Rym Msadek (CNRS, CECI\/CERFACS, Toulouse)<\/li>\n<\/ul>\n\n\n\n<h2 class=\"wp-block-heading\"><a>Bureau<\/a><\/h2>\n\n\n\n<ul class=\"wp-block-list\">\n<li><a href=\"https:\/\/web.lmd.jussieu.fr\/~fbrient\/fr\/index.html\" data-type=\"link\" data-id=\"https:\/\/web.lmd.jussieu.fr\/~fbrient\/fr\/index.html\" target=\"_blank\" rel=\"noreferrer noopener\">Florent Brient<\/a> (Sorbonne Universit\u00e9, Laboratoire de M\u00e9t\u00e9orologie Dynamique, Paris)<\/li>\n\n\n\n<li><a href=\"https:\/\/web.meteo.mcgill.ca\/cdufour\/\" data-type=\"link\" data-id=\"https:\/\/web.meteo.mcgill.ca\/cdufour\/\" target=\"_blank\" rel=\"noreferrer noopener\">Carolina Dufour<\/a> (Ifremer, Laboratoire d&rsquo;Oc\u00e9anographie Physique et Spatiale, Brest)<\/li>\n\n\n\n<li><a href=\"https:\/\/membres-ljk.imag.fr\/Florian.Lemarie\/\" data-type=\"link\" data-id=\"https:\/\/membres-ljk.imag.fr\/Florian.Lemarie\/\" target=\"_blank\" rel=\"noreferrer noopener\">Florian Lemari\u00e9<\/a> (INRIA, Laboratoire Jean Kuntzmann, Grenoble)<\/li>\n\n\n\n<li>Sa\u00efd Qasmi (Centre National de Recherches M\u00e9t\u00e9orologiques, Toulouse)<\/li>\n<\/ul>\n\n\n\n<h2 class=\"wp-block-heading\"><a>Comit\u00e9 scientifique<\/a><\/h2>\n\n\n\n<p><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Climat, oc\u00e9an et atmosph\u00e8re :<\/strong> Jean Louis Dufresne (CNRS section 19, IPSL et LMD, Sorbonne Universit\u00e9), Davide Faranda (CNRS section 19 et 52, LSCE, IPSL, LMD, ENS), Guillaume Lapeyre (CNRS section 19, LMD ENS), Julien Le Sommer (CNRS section 19, IGE, Grenoble) et Rym Msadek (CNRS section 19, CECI\/CERFACS).<\/li>\n\n\n\n<li><strong>Machine learning et climat :<\/strong> Ronan Fablet (IMT Atlantique).<\/li>\n\n\n\n<li><strong>Math\u00e9matiques et climat &#8211; EDP :<\/strong> Didier Bresch (CNRS section 41, universit\u00e9 de Savoie) et Anne Laure Dalibard (Sorbonne Universit\u00e9).<\/li>\n\n\n\n<li><strong>Math\u00e9matiques et climat &#8211; Statistique :<\/strong> Anne Laure Foug\u00e8res (Universit\u00e9 Claude Bernard Lyon 1) et Philippe Naveau (CNRS section 19, CEA Saclay, LSCE).<\/li>\n\n\n\n<li><strong>Math\u00e9matiques et climat &#8211; Analyse num\u00e9rique et assimilation de donn\u00e9es :<\/strong> Marc Bocquet (CEREA, \u00c9cole des Ponts ParisTech et EdF R&amp;D), Laurent Debreu (INRIA, Grenoble).<\/li>\n\n\n\n<li><strong>Mod\u00e9lisation stochastique :<\/strong> \u00c9tienne M\u00e9min (INRIA, Rennes).<\/li>\n\n\n\n<li><strong>Physique et dynamique non-lin\u00e9aire et climat :<\/strong> Basile Gallet (CEA, SPEC, Saclay) et Antoine Venaille (CNRS section 02, et ENS de Lyon).<\/li>\n\n\n\n<li><strong>Physique statistique et climat :<\/strong> Freddy Bouchet (CNRS section 02, ENS de Lyon) et B\u00e9reng\u00e8re Dubrulle (CNRS section 02, CEA Saclay, SPEC).<\/li>\n\n\n\n<li><strong>Turbulence et \u00e9coulements g\u00e9ophysiques :<\/strong> J\u00e9r\u00e9mie Bec (CNRS section 10, CEMEF MINES ParisTech, SophiaAntipolis).<\/li>\n\n\n\n<li><strong>Relations entres observations, donn\u00e9es et int\u00e9gration dans les mod\u00e8les :<\/strong> Bertrand Chapron (LOPS, IFREMER\/Brest) et Claudia Stubenrauch (CNRS 19, LMD, Sorbonne Universit\u00e9).<\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>Le GDR \u00ab\u00a0D\u00e9fis th\u00e9orique pour les sciences du climat\u00a0\u00bb est une structure de l&rsquo;Institut de Physique (INP) du CNRS soutenue par l&rsquo;Institut des Sciences de [&#8230;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-2","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/pages\/2","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/comments?post=2"}],"version-history":[{"count":18,"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/pages\/2\/revisions"}],"predecessor-version":[{"id":404,"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/pages\/2\/revisions\/404"}],"wp:attachment":[{"href":"https:\/\/defi-theo-climat.ipsl.fr\/index.php\/wp-json\/wp\/v2\/media?parent=2"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}