{"id":240,"date":"2016-02-23T10:47:46","date_gmt":"2016-02-23T10:47:46","guid":{"rendered":"http:\/\/www.antonincoutant.fr\/?page_id=240"},"modified":"2025-02-27T19:18:52","modified_gmt":"2025-02-27T19:18:52","slug":"laboratory-seminars","status":"publish","type":"page","link":"http:\/\/www.antonincoutant.fr\/?page_id=240","title":{"rendered":"Laboratory seminars and webinars"},"content":{"rendered":"<p><strong>2024<\/strong><\/p>\n<ul>\n<li>&#8220;Topological invisibility in chiral mirror lattices&#8221;, <em>MetaMAT weekly webinar<\/em>, 14 May (2024).<\/li>\n<\/ul>\n<p><strong>2023<\/strong><\/p>\n<ul>\n<li>&#8220;Topological invisibility in chiral mirror lattices&#8221;,<em> Institute of Mathematics of Bourgogne<\/em> (France), November 28.<\/li>\n<li>&#8220;Scattering of topological edge waves in Kekule lattices&#8221;,<em> Institut Pprime de Poitiers<\/em> (France), June 7.<\/li>\n<li>&#8220;Topological invisibility in Kekule lattices&#8221;, <em>LAGA MSC team<\/em> (France), 15 May.<\/li>\n<\/ul>\n<p><strong>2022<\/strong><\/p>\n<ul>\n<li>&#8220;Topologically protected modes in acoustic networks&#8221;, <em>Ecole Polytechnique F\u00e9d\u00e9rale de Lausanne <\/em>(Suisse), September 1.<\/li>\n<li>&#8220;Topologically protected modes in acoustic networks&#8221;, <em>Laboratoire de M\u00e9canique et d&#8217;Acoustique<\/em>, Marseille (France), January 18.<\/li>\n<\/ul>\n<p><strong>2021<\/strong><\/p>\n<ul>\n<li>&#8220;Modes topologiques localis\u00e9s en r\u00e9seau acoustique&#8221;, <em>GdR MecaWave webinar<\/em>, March 4.<\/li>\n<li>&#8220;Waves in fast flows&#8221;, <em>Institute Jean Le Rond d&#8217;Alembert<\/em> (France), February 4.<\/li>\n<\/ul>\n<p><strong>2020<\/strong><\/p>\n<ul>\n<li>&#8220;Higher order topological insulators <em>\u00e0 la<\/em> Su-Schrieffer-Heeger in acoustic networks&#8221;, <em>Institute of Mathematics of Bourgogne<\/em> (France), December 2.<\/li>\n<\/ul>\n<p><strong>2019<\/strong><\/p>\n<ul>\n<li>&#8220;Slow-sound analogues of black holes and laser effect in lined flow ducts,&#8221; <em>Institut Pprime de Poitiers<\/em> (France), October 23.<\/li>\n<li>&#8220;Slow-sound analogues of black holes and laser effect in lined flow ducts,&#8221;\u00a0<em>Laboratory of Acoustics of Le Mans University<\/em> (France), October 8.<\/li>\n<li>&#8220;Slow-sound analogues of black holes and laser effect in lined flow ducts,&#8221; <em>Laboratoire de M\u00e9canique et d&#8217;Acoustique<\/em>, Marseille (France), September 10.<\/li>\n<li>&#8220;Black hole superradiance in a bathtub vortex,&#8221; <em>Fluide Automatique et Syst\u00e8mes Thermiques<\/em> (France), 21 February.<\/li>\n<li>&#8220;Black hole in fluid flows,&#8221; <em>Laboratoire de Physique et mod\u00e9lisation des milieux condens\u00e9s<\/em> (France), 6 February.<\/li>\n<li>&#8220;Les trous noirs et la nature de la rivi\u00e8re espace-temps,&#8221; <em>Universit\u00e9 de Lorraine<\/em> (France), 31 January.<\/li>\n<\/ul>\n<p><strong>2018<\/strong><\/p>\n<ul>\n<li>&#8220;From Hawking radiation to undular jumps,&#8221; <em>Institute Jean Le Rond d&#8217;Alembert<\/em> (France), December 4.<\/li>\n<li>&#8220;Black hole horizons in one dimensional flows,&#8221; <em>Laboratory of Acoustics of Le Mans University<\/em> (France), November 27.<\/li>\n<li>&#8220;Dynamical instabilities and Quasi-Normal Modes in the Klein-Gordon equation,&#8221; <em>Institute of Mathematics of Bourgogne<\/em> (France), November 7.<\/li>\n<li>&#8220;From Hawking radiation to undular jumps,&#8221; <em>Institute of Mathematics of Bordeaux<\/em> (France), July 9.<\/li>\n<\/ul>\n<p><strong>2017<\/strong><\/p>\n<ul>\n<li>&#8220;Mimicking black holes in fluids,&#8221; <em>LMPT Tours<\/em> (France), November 9.<\/li>\n<li>&#8220;Black hole superradiance in a bathtub vortex,&#8221;\u00a0<em>Institut Pprime de Poitiers<\/em> (France), November 6.<\/li>\n<li>&#8220;Mimicking black holes in fluids,&#8221; <em>LPTMS Orsay<\/em> (France), September 20.<\/li>\n<li>&#8220;A black hole in your bathtub,&#8221; <em>ENS Lyon<\/em> (France), September 19.<\/li>\n<li>&#8220;A black hole in your bathtub,&#8221; <em>PMMH<\/em>, Paris (France), September 15.<\/li>\n<li>&#8220;Black hole superradiance in a bathtub vortex,&#8221; <em>Perimeter Institute<\/em> (Canada), June 15.<\/li>\n<li>&#8220;Unitary and non-unitary transitions around a cosmological bounce,&#8221; <em>Perimeter Institute<\/em> (Canada), June 15.<\/li>\n<li>&#8220;Black hole superradiance in a bathtub vortex,&#8221; <em>University of Durham<\/em> (UK), May 12.<\/li>\n<li>&#8220;Reproducing Black Hole physics in fluids,&#8221; <em>LUTH, Observatoire de Paris<\/em> (France), March 30.<\/li>\n<li>&#8220;Reproducing Black Hole physics in fluids,&#8221; <em>DAMTP, Cambridge <\/em>(UK), February 10.<\/li>\n<li>&#8220;Observing Black Hole superradiance in fluids,&#8221; <em>Laboratoire d&#8217;acoustique de l&#8217;universit\u00e9 du Maine<\/em> (France), January 31.<\/li>\n<\/ul>\n<p><strong>2016<\/strong><\/p>\n<ul>\n<li>&#8220;Observing Black Hole superradiance in fluids,&#8221; <em>Institut d&#8217;Astrophysique de Paris<\/em> (France), October 31.<\/li>\n<li>&#8220;Scattering theory in dispersive wave equations with a background flow,&#8221; <em>Physics faculty of Wien Universit\u00e4t<\/em> (Austria), May 19.<\/li>\n<li>&#8220;Introduction to analog gravity,&#8221; <em>IQOQI<\/em> (Vienna), May 18.<\/li>\n<li>&#8220;The birth of a black hole instability,&#8221; <em>Sheffield University<\/em> (UK), April 18.<\/li>\n<li>&#8220;Almost black holes in flowing water,&#8221; <em>Imperial College<\/em> (London), March 17.<\/li>\n<li>&#8220;A black hole in your bathtub,&#8221; <em>University Medical Center of Geneva<\/em> (Switzerland), March 11.<\/li>\n<li>&#8220;Almost black holes in flowing water,&#8221; <em>LMPT Tours<\/em> (France), March 3.<\/li>\n<li>&#8220;Almost black holes in flowing water,&#8221; <em>Laboratoire de physique de l\u2019ENS de Lyon<\/em> (France), February 18.<\/li>\n<li>&#8220;Almost black holes in flowing water,&#8221; <em>Institut Pprime de Poitiers<\/em> (France), February 16.<\/li>\n<li>&#8220;Almost black holes in flowing water,&#8221; <em>Laboratoire de Physique Th\u00e9orique d&#8217;Orsay<\/em> (France), February 10.<\/li>\n<\/ul>\n<p><strong>2015<\/strong><\/p>\n<ul>\n<li>&#8220;The black hole laser instability in Bose-Einstein condensates,&#8221; <em>Vienna Center for Quantum Science and Technology<\/em> (Austria), November 13.<\/li>\n<li>&#8220;The black hole laser instability in Bose-Einstein condensates,&#8221; <em>School of mathematical science of the University of Nottingham<\/em> (UK), October 21.<\/li>\n<li>&#8220;Hawking radiation in Bose-Einstein condensates,&#8221; <em>Freie Universit\u00e4t<\/em> (Berlin), April 17.<\/li>\n<li>&#8220;Hawking radiation in Bose-Einstein condensates,&#8221; <em>Instituto Superior T\u00e9cnico<\/em> (Lisbon), March 5.<\/li>\n<li>&#8220;Unitary and non-unitary transitions around a cosmological bounce,&#8221; <em>Center for Theoretical Physics<\/em> (Marseille, France), February 2.<\/li>\n<\/ul>\n<p><strong>2014<\/strong><\/p>\n<ul>\n<li>&#8220;Hawking radiation in fluid flows,&#8221; <em>Institute for Gravitation and the Cosmos<\/em>, Penn State University (USA), October 24.<\/li>\n<li>&#8220;Unitary and non-unitary transitions around a cosmological bounce,&#8221; <em>Tufts Institute for Cosmology<\/em>, Tufts University (USA), October 14.<\/li>\n<li>&#8220;Hawking radiation in fluid flows,&#8221; <em>Perimeter Institute<\/em> (Canada), October 9.<\/li>\n<li>\u201cHawking radiation in acoustic black and white holes,\u201d <em>Laboratoire de Math\u00e9matiques et Physique Th\u00e9orique in Tours<\/em> (France), April 17.<\/li>\n<li>\u201cHawking radiation in acoustic black and white holes,\u201d <em>Institut d\u2019Astrophysique de Paris<\/em> (France), April 14.<\/li>\n<li>\u201cUnitary and non-unitary transitions around a cosmological bounce,\u201d <em>Institute for theoretical physics of the K\u00f6ln Universit\u00e4t<\/em> (Germany), April 8.<\/li>\n<li>\u201cHawking radiation in acoustic black and white holes,\u201d <em>School of mathematical science of the University of Nottingham<\/em> (UK), February 20.<\/li>\n<li>\u201cBirth of laser instability in black hole geometries,\u201d <em>Fundamental Interaction group of the Universit\u00e9 Libre de Bruxelles<\/em> (Belgium), January 27.<\/li>\n<li>\u201cBirth of laser instability in black hole geometries,\u201d <em>Gravitation group of the Wien Universit\u00e4t<\/em> (Austria), January 23.<\/li>\n<\/ul>\n<p><strong>2013<\/strong><\/p>\n<ul>\n<li>\u201cHawking radiation in acoustic black holes,\u201d <em>mechanics and gravitation group of the Mons University<\/em> (Belgium), June 10.<\/li>\n<\/ul>\n<p><strong>2012<\/strong><\/p>\n<ul>\n<li>\u201cUndulations in analog gravity flows,\u201d <em>theoretical physics group of the LadHyX, \u00e9cole Polytechnique<\/em> (France), October 26.<\/li>\n<li>\u201cBlack hole radiation with short distance dispersion,\u201d <em>Laboratoire de physique de l\u2019ENS de Lyon<\/em> (France), February 27.<\/li>\n<li>\u201cBlack hole radiation with short distance dispersion,\u201d<em> Max Planck Institute for gravitational physics<\/em> (Potsdam, Germany), January 10.<\/li>\n<\/ul>\n<p><strong>2011<\/strong><\/p>\n<ul>\n<li>\u201cBlack hole laser, a mode analysis,\u201d<em> Institute of Sciences of the Cosmos of the Barcelona University<\/em> (Spain), December 2.<\/li>\n<li>\u201cHawking radiation turned into laser instability,\u201d<em> Max Planck Institute for gravitational physics<\/em> (Potsdam, Germany), May 6.<\/li>\n<\/ul>\n","protected":false},"excerpt":{"rendered":"<p>2024 &#8220;Topological invisibility in chiral mirror lattices&#8221;, MetaMAT weekly webinar, 14 May (2024). 2023 &#8220;Topological invisibility in chiral mirror lattices&#8221;, Institute of Mathematics of Bourgogne (France), November 28. &#8220;Scattering of topological edge waves in Kekule lattices&#8221;, Institut Pprime de Poitiers (France), June 7. &#8220;Topological invisibility in Kekule lattices&#8221;, LAGA MSC team (France), 15 May. 2022 [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"page-templates\/full-width.php","meta":{"footnotes":""},"class_list":["post-240","page","type-page","status-publish","hentry"],"jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/P3HWNU-3S","_links":{"self":[{"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=\/wp\/v2\/pages\/240","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=240"}],"version-history":[{"count":32,"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=\/wp\/v2\/pages\/240\/revisions"}],"predecessor-version":[{"id":847,"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=\/wp\/v2\/pages\/240\/revisions\/847"}],"wp:attachment":[{"href":"http:\/\/www.antonincoutant.fr\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=240"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}