<?xml version='1.0' encoding='UTF-8'?><?xml-stylesheet href="http://www.blogger.com/styles/atom.css" type="text/css"?><feed xmlns='http://www.w3.org/2005/Atom' xmlns:openSearch='http://a9.com/-/spec/opensearchrss/1.0/' xmlns:georss='http://www.georss.org/georss' xmlns:gd='http://schemas.google.com/g/2005' xmlns:thr='http://purl.org/syndication/thread/1.0'><id>tag:blogger.com,1999:blog-3975242521993377304</id><updated>2011-07-08T00:18:24.640-07:00</updated><category term='Location / Practical informations'/><category term='Sessions and Talks'/><category term='Schedule'/><category term='List of abstract: sessions B-C-D-E'/><category term='List of abstract: session A'/><category term='Home'/><category term='Program'/><category term='Invited speakers'/><title type='text'>Winter School and 9th ICOR on PDE  and Mathematical Biology</title><subtitle type='html'>FEBRUARY 15-26, 2010, La Habana, Cuba</subtitle><link rel='http://schemas.google.com/g/2005#feed' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/posts/default'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default?max-results=100'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/'/><link rel='hub' href='http://pubsubhubbub.appspot.com/'/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><generator version='7.00' uri='http://www.blogger.com'>Blogger</generator><openSearch:totalResults>46</openSearch:totalResults><openSearch:startIndex>1</openSearch:startIndex><openSearch:itemsPerPage>100</openSearch:itemsPerPage><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8804660953080208858</id><published>2009-10-23T02:40:00.000-07:00</published><updated>2010-02-08T05:06:15.416-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='Home'/><title type='text'></title><content type='html'>&lt;div style="text-align: justify;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;The goal of the Winter School and of the Sessions on PDE and Mathematical Biology is to promote research interplays between Cuba and other countries on recent developments on PDE mathematical investigations, with special interest on applications to Biology and other modelization areas.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;The Winter School is specially intended for graduate and PhD students, although it of course welcomes senior scientists as well. &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;br /&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;The Sessions on PDE and Mathematical Biology are organized in the frame of the 9th ICOR International Conference.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman',serif;"&gt;&lt;span class="Apple-style-span"  style="font-family:Georgia, serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;One can consult the &lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/06/tentative-program.html"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;program&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;, the &lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/07/sessions-and-talks.html"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;list of talks&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;, the &lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/07/participants.html"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;list of invited speakers&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;, and the website of the &lt;/span&gt;&lt;/span&gt;&lt;a href="http://www.ceremade.dauphine.fr/%7Emischler/EDPyAplicaciones.html"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;previous edition&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;. A detailed schedule will be posted &lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/10/schedule.html"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;here&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt; when available.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;br /&gt;Here is the page for the &lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/10/location.html"&gt;location and practical informations&lt;/a&gt; and here is the &lt;span class="Apple-style-span"  style=" ;font-family:Georgia, serif;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style=" ;font-size:medium;"&gt;&lt;a href="http://www.dma.ens.fr/%7Emouhot/2010"&gt;poster of the conference&lt;/a&gt;.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;br /&gt;For further informations, please contact the organizers (on the right).&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;Organizers and contact :&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Lucilla Corrias (Laboratoire d'Analyse et Probabilité, Université d'Evry, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Stéphane Mischler (CEREMADE, Université Paris-Dauphine, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Clément Mouhot (DMA, ÉNS Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Mariano Rodriguez Ricard (Departamento de Matematicas, Universidad de La Habana, Cuba)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Sponsors :&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;CEREMADE&lt;/b&gt;, Paris-Dauphine, France&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;font-size:14px;"&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="  font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;Laboratoire d'Analyse et Probabilité&lt;/b&gt;, Université d'Evry, France&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"   style="  font-weight: normal;font-family:Georgia,serif;font-size:16px;"&gt;&lt;span class="Apple-style-span"  style="font-family:Helvetica,serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"   style="  font-weight: normal;font-family:Georgia,serif;font-size:16px;"&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8804660953080208858?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8804660953080208858'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8804660953080208858'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/10/presentation.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-9009032886600843191</id><published>2009-06-28T02:26:00.000-07:00</published><updated>2010-02-08T05:09:40.246-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='Program'/><title type='text'></title><content type='html'>&lt;div class="ii gt" id=":20n"&gt;&lt;div&gt;&lt;div color="red" style="margin: 0px;"&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:large;"&gt;Program&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;br /&gt;&lt;/div&gt;&lt;div  style=" margin: 0px;color:red;"&gt;&lt;span style="font-size:large;"&gt;&lt;b&gt;WINTER SCHOOL on MATHEMATICAL BIOLOGY&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="margin: 0px;"&gt;Monday 15, Tuesday 16, Wednesday 17, Thursday 18&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;br /&gt;&lt;span style=" font-weight: bold;color:#ff6600;"&gt;&lt;span style="font-size:medium;"&gt;Courses:&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;span style=" font-weight: bold;color:#ff6600;"&gt;&lt;span class="Apple-style-span"  style=" font-weight: normal;color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;1. &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style=" font-weight: normal;color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;José Antonio Carrillo (Barcelona, Spain)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/jose.html"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Macroscopic and Kinetic Equations in Swarming and Chemotaxis&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;i&gt;&lt;/i&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;i&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span" style="font-style: normal;"&gt;''&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/jose.html"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;Ecuaciones cinéticas y macroscópicas en "Swarming" y quimiotaxis&lt;/span&gt;&lt;/a&gt;''&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;i&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;2. Benoît Perthame (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;span style="color:#000099;"&gt;&lt;i&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/benoit-perthame-universite-p.html"&gt;&lt;span style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Adaptive evolution: a population view&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;/i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;3. Marc Thiriet (Paris, France) &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="text-align: justify;"&gt;&lt;span style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/marc-thiriet-cnrs-universite-p.html"&gt;&lt;span style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Blood and air flows: from biomechanical simulations (patient-specific macroscopic scale investigations) to biomathematical approaches (coupling of short-term cell reactions at nano- and microscopic scales to flow-induced stresses)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;/i&gt;&lt;/span&gt;&lt;span style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="color: red; margin: 0px;"&gt;&lt;b&gt;&lt;br /&gt;SESSION on MATHEMATICAL BIOLOGY &lt;/b&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;Friday 19, Monday 22, Tuesday 23&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="margin: 0px; min-height: 14px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The talks of the Mathematical Biology session will be intended to present recent advances on topics such as :&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin: 0px;"&gt;&lt;ol&gt;&lt;span style="font-style: italic;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Structured Population Dynamic  &lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Fluid Mechanic in Human Environment &lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Chemotaxis&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Modelling of Biological Phenomena&lt;/span&gt;&lt;/span&gt;&lt;span style="  font-style: normal;font-family:Helvetica;font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;/span&gt;&lt;/ol&gt;&lt;/div&gt;&lt;div color="black" style=" margin: 0px; text-align: justify;"&gt;__________________________________________________&lt;/div&gt;&lt;div color="black" style=" margin: 0px; text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style=" margin: 0px; text-align: justify;color:black;"&gt;&lt;span class="Apple-style-span"   style="  font-weight: bold;font-size:large;color:red;"&gt;WINTER SCHOOL on PDE and applications&lt;/span&gt;&lt;/div&gt;&lt;div  style="margin: 0px; text-align: justify;color:black;"&gt;&lt;br /&gt;&lt;span style="font-weight: bold; color:#ff6600;"&gt;&lt;span style="font-size:medium;"&gt;Courses:&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; min-height: 14px; "&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; min-height: 14px; "&gt;&lt;span style="font-weight: bold; color:#ff6600;"&gt;&lt;span class="Apple-style-span"  style="font-weight: normal; color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;1. &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-weight: normal; color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;David Lannes (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; min-height: 14px; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; min-height: 14px; "&gt;&lt;span style="line-height: 14px; "&gt;&lt;span style="line-height: normal; "&gt;&lt;i&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-lannes.html"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;Stability/instability issues for two-fluid interfaces&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style="font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;2. François Murat (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; min-height: 14px; "&gt;&lt;i&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://www.dma.ens.fr/%7Emouhot/cours_Cuba.pdf"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;Basic homogenization&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/div&gt;&lt;/div&gt;&lt;div style="color: black; margin: 0px; text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="margin: 0px;"&gt;&lt;b&gt;&lt;span style="color:red;"&gt;SESSIONS on PDE and applications&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="margin: 0px;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin: 0px;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="color:#FF9900;"&gt;Opening Plenary Lecture,&lt;/span&gt; &lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span" style="font-weight: normal;"&gt;Monday 22 :&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="margin: 0px;"&gt;&lt;div  style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; color:black;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;&lt;span class="Apple-style-span" style="text-decoration: underline;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; color:black;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;P. L. Lions (Paris, France) &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/02/abstract-lions.html" style="color: red; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;An Introduction To Mean Field Games&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;br /&gt;&lt;i&gt;&lt;span&gt;&lt;span class="Apple-style-span" style="font-style: normal; font-weight: bold; -webkit-text-decorations-in-effect: underline; "&gt;&lt;span class="Apple-style-span"  style="color:#FF9900;"&gt;Plenary Lecture&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-weight: bold; -webkit-text-decorations-in-effect: underline; "&gt;&lt;span class="Apple-style-span"  style="color:#FF9900;"&gt; :&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div color="black" style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; "&gt;&lt;span&gt;&lt;span style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;I. Gamba (Austin, USA) &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div color="black" style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; "&gt;&lt;span&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-gamba.html" style="color: red; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Non-conservative models of multi-linear particle interactions&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span style="line-height: 14px; "&gt;&lt;span style="line-height: normal; "&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px; "&gt;&lt;span style="line-height: normal; "&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div color="black" style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; "&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div style="margin: 0px;"&gt;&lt;span style="color:red;"&gt;&lt;/span&gt;&lt;span style="color:red;"&gt;&lt;b&gt;&lt;span style=" font-weight: normal;color:black;"&gt;Tuesday 23, Wednesday 24, Thursday 25, &lt;/span&gt;&lt;span style=" font-weight: normal;color:black;"&gt;Friday 26 &lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;div  style=" font-style: italic; margin: 0px;color:black;"&gt;&lt;ol&gt;&lt;li&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Fluid Mechanic and Coastal Dynamic&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Mean Field Games&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Classical and Quantum Kinetic Equations&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style=" font-style: italic;color:black;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Homogenization, Inverse Problems and Control&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;/ol&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-9009032886600843191?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/9009032886600843191'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/9009032886600843191'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/06/tentative-program.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8953311004899614632</id><published>2009-06-20T04:36:00.000-07:00</published><updated>2010-03-12T08:49:34.660-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='Sessions and Talks'/><title type='text'>Sessions and Talks</title><content type='html'>&lt;b&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;A. Mathematical Biology&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;br /&gt;&lt;ol&gt;&lt;span style="line-height: 26px;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;D. Ambrosi (Milano, Italia) &lt;i&gt;&lt;span style="color:#cc0000;"&gt;"&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/12/abstract-ambrosi.html"&gt;&lt;span style="color:#cc0000;"&gt;The electromechanical coupling in cardiac mechanics&lt;/span&gt;&lt;/a&gt;&lt;span style="color:#cc0000;"&gt;"&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style=" line-height: 18px;font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;V. Calvez (Lyon, France)&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt; &lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;''&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: normal;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/vincent-calvez-cnrs-ens-lyon-france.html"&gt;&lt;span style="color:#cc0000;"&gt;The geometry of one-dimensional self-attracting&lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 18px;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/vincent-calvez-cnrs-ens-lyon-france.html"&gt;&lt;span style="color:#cc0000;"&gt; &lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/vincent-calvez-cnrs-ens-lyon-france.html"&gt;&lt;span style="color:#cc0000;"&gt;particles&lt;/span&gt;&lt;/a&gt;" &lt;span class="Apple-style-span"  style="color:#000099;"&gt;(&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/Calvez.pdf"&gt;pdf file&lt;/a&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;M. R. D'Orsogna (Los Angeles, USA) &lt;/span&gt;&lt;/span&gt;&lt;span style="color:red;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;"&lt;/span&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/12/maria-rita-dorsigna-california-state.html"&gt;&lt;span style="color:#cc0000;"&gt;Modelling viral entry dynamics&lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;/i&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="line-height: normal;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;M. Doumic-Jauffret (INRIA, France) &lt;i&gt;&lt;span style="color:#cc0000;"&gt;"&lt;a href="http://icor2010pde.blogspot.com/2010/01/marie-doumic-aggregationfragmentation.html"&gt;&lt;span style="color:#cc0000;"&gt;Aggregation/fragmentation models for protein polymerization&lt;/span&gt;&lt;/a&gt;" &lt;/span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/DOUMIC.pdf"&gt;(pdf file)&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;L. Dumas (Paris, France) &lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=" line-height: normal;color:#cc0000;"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/laurent-dumas-numerical-simulation-of.html"&gt;&lt;span style="color:#cc0000;"&gt;A numerical simulation of the human arterial network based on non invasive measurements&lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;/i&gt;&lt;span style="font-family:'times new roman';"&gt;" &lt;i&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/Dumas.pdf"&gt;(pdf file)&lt;/a&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;K. Fellner (Cambridge, UK) &lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;"&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: normal;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/02/klemens-fellner-cambridge-uk-stability.html"&gt;&lt;span class="Apple-style-span"  style="color:#cc0000;"&gt;Stability of stationary states of non-local evolution equations&lt;/span&gt;&lt;/a&gt;" &lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/Fellner.pdf"&gt;(pdf file)&lt;/a&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="line-height: normal;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;T. Hillen (University of Alberta, Canada)  &lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;"&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/thomas-hillen-university-of-alberta.html"&gt;&lt;span style="color:#cc0000;"&gt;Pointwise weak steady states of transport equations for cell movement in network tissue&lt;/span&gt;&lt;/a&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;P.-E. Jabin (Nice, France)  &lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;"&lt;span style="line-height: normal;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;i&gt;&lt;span style="font-size:medium;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/pierre-emmanuel-jabin-universite-de.html"&gt;&lt;span style="color:#cc0000;"&gt;Selection-mutation dynamics for the evolution of traits in a population&lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;" &lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;i&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/Jabin.pdf"&gt;(pdf file)&lt;/a&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;D. Levy (Maryland, USA) &lt;span style="color:#cc0000;"&gt;"G&lt;/span&gt;&lt;span style=" line-height: normal;font-size:medium;"&gt;&lt;i&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/12/doron-levy-university-of-maryland-usa.html"&gt;&lt;span style="color:#cc0000;"&gt;roup dynamics in phototaxis&lt;/span&gt;&lt;/a&gt;&lt;/i&gt;&lt;span style="color:#cc0000;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;S. Martin (Orsay, France) &lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;"&lt;a href="http://icor2010pde.blogspot.com/2010/01/sebastien-martin-modelling-of-air-flows.html"&gt;&lt;span style="color:#cc0000;"&gt;Modelling of air flows and gas exchange in the human lung&lt;/span&gt;&lt;/a&gt;" &lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/Martin.pdf"&gt;(pdf file)&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style=" line-height: normal;color:#333333;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;N. Meunier (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;span style="color:black;"&gt; &lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;"&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/01/nicolas-meunier-universite-france.html"&gt;&lt;span style="color:#cc0000;"&gt;Analysis of self-organization systems for cell polarization&lt;/span&gt;&lt;/a&gt;"&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;J. Mitchell (Wisconsin-Madison, USA) &lt;span style="color:#cc0000;"&gt;&lt;i&gt;"&lt;a href="http://icor2010pde.blogspot.com/2009/12/julie-mitchell.html"&gt;&lt;span style="color:#cc0000;"&gt;Using clustering and optimization in flexible protein docking&lt;/span&gt;&lt;/a&gt;&lt;span style="font-family:Helvetica,serif;"&gt;&lt;span style=" line-height: normal;font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:Helvetica,serif;"&gt;&lt;span style="line-height: normal;"&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-style: normal;"&gt;&lt;span style="font-size:medium;"&gt;G. Raoul &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style=" font-style: normal; line-height: 26px;font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;(Cachan, France) &lt;i&gt;&lt;span style="color:#cc0000;"&gt;"&lt;a href="http://icor2010pde.blogspot.com/2010/01/gael-raoul-ens-cachan-france-kimuras.html"&gt;&lt;span style="color:#cc0000;"&gt;Kimura's model : an integro-differential model to study evolution&lt;/span&gt;&lt;/a&gt;" &lt;/span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/raoul.pdf"&gt;(pdf file)&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:Helvetica,serif;"&gt;&lt;span style="line-height: normal;"&gt;&lt;i&gt;&lt;span style=" font-style: normal; line-height: 18px;font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;C. Schmeiser (Vienna, Austria)&lt;span style="color:#333333;"&gt; &lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: normal;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/12/christian-schmeiser-nonlinear-friction.html"&gt;&lt;span style="color:#cc0000;"&gt;Nonlinear friction in the cytoskeleton as a macroscopic limit of&lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;span style="line-height: 18px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/12/christian-schmeiser-nonlinear-friction.html"&gt;&lt;span style="color:#cc0000;"&gt; &lt;/span&gt;&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="  font-style: normal;font-family:Helvetica,serif;color:black;"&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/12/christian-schmeiser-nonlinear-friction.html"&gt;&lt;span style="color:#cc0000;"&gt;the activity of cytoskeletal proteins&lt;/span&gt;&lt;/a&gt;" &lt;/span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/Schmeiser.pdf"&gt;(pdf file)&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="line-height: normal;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;A. Vidal (Evry, France) &lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#cc0000;"&gt;''&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;i&gt;&lt;a href="http://icor2010pde.blogspot.com/2010/02/alexandre-vidal-universite-devry-val.html"&gt;&lt;span class="Apple-style-span"  style="color:#cc0000;"&gt;A model of the Gonadotropin Releasing Hormone secretion by hypothalamic neuron clusters&lt;/span&gt;&lt;/a&gt;&lt;/i&gt;&lt;span class="Apple-style-span"  style="color:#cc0000;"&gt;''&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;/span&gt;&lt;/ol&gt;&lt;div&gt;&lt;b&gt;&lt;span style="line-height: 21px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;B. &lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 21px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Fluid Mechanic and Coastal Dynamic&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;ol&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A. Alvarez Cruz (La Habana, Cuba) &lt;/span&gt;&lt;/span&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-alvarez.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Solving Mild Slope equation in Matlab with Domain decomposition method&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span class="Apple-style-span"  style="color:#333333;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;T. Kano (Kyoto, Japon)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-kano.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Tunamis on a deep open sea and on a gentle sloaping beach&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;  &lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A. Nachbin (Rio de Janeiro, Brazil) &lt;/span&gt;&lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-nachbin.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Asymptotic issues regarding nonlinear wave/topography interaction&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;C. &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Turner&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; (Cordoba, Argentina) &lt;/span&gt;&lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-turner.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Mathematical model for stratified fluids&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;B. Valiño Alonso (La Habana, Cuba) &lt;/span&gt;&lt;/span&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-valino.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Infinitely narrow solitons in shallow water equations&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;/ol&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="line-height: 21px;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;C. &lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 21px;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Mean Field Games&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;ol&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;I. Capuzzo Dolcetta (Roma, Italia) &lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-dolcetta.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A numerical approach to some mean field games problems&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;M. P. Gualdani (Austin, &lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;USA&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;) &lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-gualdani.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Global Existence of a Free Boundary Problem with Non-Standard Sources&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;  &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Aimé Lachapelle (Paris, France) &lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-lachapelle.html" style="color: red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Mean Field Games: a numerical methodology with application to a stylised model of technology switch&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;li style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;P. Markowich (Cambridge, UK and Vienna, Austria)&lt;/span&gt;&lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;span class="Apple-style-span"  style="color:red;"&gt;''&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"   style=" ;font-family:Helvetica;font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;&lt;a href="http://icor2010pde.blogspot.com/2009/12/peter-markowich-university-of-cambridge.html"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;On PDE Models for (some) Socio-Economic Problems: Price Formation, Opinion Formation and Crowd Modeling&lt;/span&gt;&lt;/a&gt;''&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;/ol&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="line-height: 21px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;D. &lt;/span&gt;&lt;/span&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;Classical and quantum kinetic equatio&lt;/span&gt;&lt;span style="line-height: normal;"&gt;ns&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;ol&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;M.J. Caceres (Granada, Espa&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;ñ&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;a) &lt;/span&gt;&lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-caceres.html" style="color: red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;A numerical solver for a nonlinear Fokker-Planck equation in Neuroscience&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;S. Calogero (Granada, España)  &lt;/span&gt;&lt;/span&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-calogero.html" style="color: red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Self-similar behavior &lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;a href="http://www.blogger.com/goog_1264080436004" style="color: red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;in relativistic galactic d&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-calogero.html" style="color: red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;ynamics&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;" &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;J.A. Cañizo (Barcelona, España)&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/absract-canizo.html" style="color: red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Entropy inequalities and speed of convergence to equilibrium for the growth-fragmentation equation&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;M. Escobedo (Bilbao, España) &lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;-&lt;/span&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i  style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;"&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-escobedo.html"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;Post Gel solutions for coagulation equations&lt;/span&gt;&lt;/a&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;span style="line-height: normal;"&gt;&lt;li style="text-align: justify;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;R. &lt;/span&gt;&lt;/span&gt;&lt;span style="color:#03ff08;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Galeano Andrades (Cartagena, Colombia) &lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/rafael-galeano-andrades-cartagena.html" style="color: red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Variational methods in stationary Boltzmann equation&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span style="color:red;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 14px;"&gt;&lt;span style="line-height: normal;"&gt;  &lt;/span&gt;&lt;/span&gt;&lt;/ol&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="line-height: 21px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;E. &lt;span style="line-height: 26px;"&gt;Homogenization, &lt;span style="line-height: 21px;"&gt;Inverse Problems and Control&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt; &lt;/b&gt;&lt;br /&gt;&lt;ol&gt;&lt;li&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;F. Dickstein (Rio de Janeiro, Brazil) &lt;span class="Apple-style-span"  style="color:red;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;"A&lt;/span&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;utomatic History Matching in Oil Reservoir Simulation"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;O. Kavian (Versailles, France) &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;- &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/01/abstract-kavian.html"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;Remarks on Inverse Problems arising from Electrical Impedance&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;"&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;li&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;&lt;span style="color:black;"&gt;N. Ghoussoub - &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span style="color:red;"&gt;"&lt;/span&gt;&lt;a href="http://icor2010pde.blogspot.com/2008/02/abstract-ghoussoub.html" style="color: red;"&gt;Homogenization of maximal monotone vector fields via selfdual variational calculus&lt;/a&gt;&lt;span style="color:red;"&gt;"&lt;/span&gt;&lt;/i&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:red;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/li&gt;&lt;/ol&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8953311004899614632?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8953311004899614632/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/07/sessions-and-talks.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8953311004899614632'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8953311004899614632'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/07/sessions-and-talks.html' title='Sessions and Talks'/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-7701033375471769776</id><published>2008-12-15T10:03:00.000-08:00</published><updated>2010-01-09T03:58:20.682-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;Davide Ambrosi&lt;/b&gt; &lt;/div&gt;&lt;div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;(Politecnico di &lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;Milano, Italia)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span style="line-height: 26px;"&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span" style="line-height: normal; "&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;The electromechanical coupling in cardiac mechanics&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/span&gt;&lt;div&gt;&lt;br /&gt;&lt;/div&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The coupling between cardiac mechanics and electric signalling can be  addressed in a two possible alternative framework: the electrical potential dictates the active stress or the active strain. In this talk the explore the second (less popular) strategy, obtained  thanks a factorization of the deformation tensor. After rewriting the equations in a deforming domain, we prove that neglecting the deformation of the substrate induces a non-negligible error in predicting celerity and width of the pulse, while the amplitude and the stability conditions are not affected by the electro--mechanical decoupling. Exact solutions of travelling front type can be found with explicit form  of the celerity and steepness. The role of visco-elasticity and the characterization of unstable initial conditions are discussed with the support of numerical simulations, both in one and two spatial dimensions. &lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;span style="color:black;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-7701033375471769776?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/7701033375471769776'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/7701033375471769776'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/12/abstract-ambrosi.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-591356699151456733</id><published>2008-10-23T11:52:00.000-07:00</published><updated>2010-02-20T17:40:08.886-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='Schedule'/><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="font-size: large;"&gt;Schedule&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="font-size: large;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="color: red;"&gt;&lt;span class="Apple-style-span" style="font-size: large;"&gt;Winter School on Mathematical Biology&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Monday 15, Tuesday 16, Wednesday 17, Thursday 18&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;The Winter School on Mathematical Biology will be held at the "Salón 250 Aniversario de la UH" in the Varona Building, located at one side of the Faculty of Mathematics and Computer Science inside the Campus.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/Schedule.pdf"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Click &lt;span class="Apple-style-span" style="color: #000099;"&gt;here&lt;/span&gt; to see the complete schedule of the Winter School on mathematical Biology.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;/div&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;/span&gt;&lt;br /&gt;&lt;div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span" style="font-family: Arial,serif;"&gt;&lt;span class="Apple-style-span" style="font-size: small;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;__________________________________________________________&lt;/div&gt;&lt;div&gt;&lt;br /&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: justify;"&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="color: red;"&gt;&lt;span class="Apple-style-span" style="font-size: large;"&gt;Session on Mathematical Biology&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Friday 19, Monday 22, Tuesday 23&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;The session on Mathematical Biology on Friday 19 and Monday 22 will be held at the "Salón 250 Aniversario de la UH" in the Varona Building, located at one side of the Faculty of Mathematics and Computer Science inside the Campus. &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman',serif;"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;On Tuesday 23, the session will be held at the Hotel Parque Central, in the Habana Vieja/Centro Habana district.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;a href="http://www.maths.univ-evry.fr/pages_perso/corrias/timetableBio.pdf"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Click &lt;/span&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;here&lt;/span&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; to see the complete schedule of the Mathematical Biology session.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;&lt;div&gt;__________________________________________________________&lt;/div&gt;&lt;div&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="color: red;"&gt;&lt;span class="Apple-style-span" style="font-size: large;"&gt;Sessions on PDE&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Opening lecture of Pierre-Louis Lions on monday 22 and Tuesday 23, Wednesday 24, Thursday 25, Friday 26.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman',serif;"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;The sessions on PDEs will be held at the Hotel Parque Central, in the Habana Vieja/Centro Habana district.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;a href="http://www.dma.ens.fr/%7Emouhot/Timetable-PDE.pdf"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Click &lt;/span&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;here&lt;/span&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; to see the complete schedule of the PDE session.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;br /&gt;&lt;br /&gt;__________________________________________________________&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div style="color: red;"&gt;&lt;span style="font-size: large;"&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="font-family: Arial;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span"&gt;Abredged schedule&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Monday, February 15 (Winter School)&lt;/b&gt;&lt;br /&gt;1:30-1:45pm: Welcome by the organizers&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;1:45-3:15pm: J. A. Carrillo&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Coffee break&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;3:30-5:00pm: J. A. Carrillo&lt;br /&gt;&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Tuesday, February 16 (Winter School)&lt;/b&gt;&lt;br /&gt;9:00-10:30am: &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;M. Thiriet&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span style="font-size: medium;"&gt;&lt;span style="font-family: 'times new roman';"&gt;C&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;offee break&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;10:45-12:15am: M. Thiriet&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;Lunch&lt;/i&gt;&lt;br /&gt;1:45-3:15&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;pm: J. A. Carrillo&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span style="font-size: medium;"&gt;&lt;span style="font-family: 'times new roman';"&gt;C&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;offee break&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;3:30-5:00&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;pm: J. A. Carrillo&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&amp;nbsp; &lt;br /&gt;&lt;b&gt;Wednesday, February 17 (Winter School)&lt;/b&gt;&lt;br /&gt;10:00-11:30am: B. Perthame&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Coffee break&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;11:45am-1:15pm: B. Perthame&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;Free afternoon&lt;/i&gt;&lt;br /&gt;&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Thursday, February 18 (Winter School)&lt;/b&gt;&lt;br /&gt;9:00-10:30am: M. Thiriet&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Coffee break&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;10:45-12:15am: M. Thiriet&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;Lunch&lt;/i&gt;&lt;br /&gt;1:45-3:15pm: B. Perthame&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Coffee break&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;3:30-5:00pm: B. Perthame&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Friday, February 19 (Biology session)&lt;/b&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;9:00-9:15am: &lt;i&gt;Welcome by the organizers&lt;/i&gt;&lt;br /&gt;9:15-10:00am: T. Hillen&lt;br /&gt;10:00-10:45am: P.-E. Jabin&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;Coffee break &lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;11:15-12:00am: C. Schmeiser&lt;br /&gt;12:00-12:45am: M. Rita D’Orsogna&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Lunch&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;2:15-3:00pm: D. Ambrosi&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;3:00-3:45pm: L. Dumas&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;Coffee break &lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;4:15-5:00pm: S. Martin&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Monday, February 22 (Biology session and opening lecture)&lt;/b&gt;&lt;b&gt;&lt;/b&gt;&lt;br /&gt;9:00-9:45am: V. Calvez&lt;br /&gt;9:45-10:30am: K. Fellner&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Coffee break&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;11:00-11:45am: M. Doumic&lt;br /&gt;11:45-12:30am: G. Raoul&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Lunch&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; 3:00-4:00pm: &lt;u&gt;Opening Plenary Lecture, P.-L. Lions&lt;/u&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Tuesday, February 23 (End Biology session and PDE sessions)&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;ICOR plenary speaker:&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;9:00-10:00am: B. Cornet&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;Coffee break&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Biology session&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;10:30-11:10am: J. Mitchell&lt;br /&gt;11:10-11:50am: A. Vidal&lt;br /&gt;11:50-12:30am: N. Meunier&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;PDE sessions&lt;/b&gt;&lt;i&gt;&lt;/i&gt;&lt;br /&gt;10:30-11:10am: P. Markowich&lt;br /&gt;11:10-11:50am: M. P. Gualdani&lt;br /&gt;11:50-12:30am: A. Lachapelle&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Lunch&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;2:00-3:20pm: D. Lannes (course 1)&lt;br /&gt;3:40-5:00pm: F. Murat (course 1)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;u&gt;Evening: Reception and Jazz concert&lt;/u&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Wednesday, February 24&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;ICOR plenary speaker:&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;9:00-10:00am: G. Still&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;Coffee break &lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;PDE sessions&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;10:30-11:10am: M. Escobedo&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; 11:10-11:50am: N. Ghoussoub&lt;br /&gt;11:50-12:30: O. Kavian&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Lunch&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; 2:00-2:40pm: &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;M. J. Caceres&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; 2:40-3:20pm: &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;J.A. Cañizo&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;in parallel with&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;2:00-3:20pm: D. Lannes (course 2)&lt;br /&gt;3:40-5:00pm: F. Murat (course 2)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Thursday, February 25&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;ICOR plenary speakers:&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;9:00-10:00am: A. Xavier&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;2:30-3:30pm: S. Méléard&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;PDE sessions&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;10:30-11:10: T. Kano &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;11:10-11:50am: B. Valiño Alonso&lt;br /&gt;11:50-12:30am: A. Nachbin&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Lunch&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;2:00-2:40: C. Turner&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;2:40-3:20: A. Alvarez Cruz&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;in parallel with&amp;nbsp;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;2:00-3:20pm: D. Lannes (course 3)&lt;br /&gt;3:40-5:00pm: F. Murat (course 3)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;u&gt;Evening: Social Diner &lt;/u&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;Friday, February 26&amp;nbsp;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;PDE sessions&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;ICOR plenary speaker: &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;9:00-10:00am: I. Gamba&lt;br /&gt;&lt;i&gt;Coffee Break&lt;/i&gt;&lt;br /&gt;10:30-11:10am: S. Calogero&lt;br /&gt;11:10-11:50am: R. Galeano Andrades&lt;b&gt; &lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;span class="Apple-style-span" style="font-family: Arial; font-size: small;"&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-591356699151456733?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/591356699151456733/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/10/schedule.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/591356699151456733'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/591356699151456733'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/10/schedule.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4464634772146523623</id><published>2008-10-23T02:52:00.000-07:00</published><updated>2010-02-11T14:23:17.257-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='Location / Practical informations'/><title type='text'>Location and Practical Information</title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Conferences location&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The Winter School (scheduled from February 15 to 18) as well as the first two days of the Session on "Mathematical Biology" (February 19 and February 22) will be held at the "Salón &lt;/span&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;250 Aniversario de la UH" in the Varona Building, located at one side of the Faculty of Mathematics and Computer Science inside the Campus of the La Havana University (Universidad de La Habana). &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The university is located at the intersection of the San Lázaro St., the Neptuno St. and L St. in the Vedado district, Ciudad Habana. &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;This is the main entrance with the stairs (escalinata) and the sculpture with the Alma Mater (see the picture on the right). Another entrance is located at the intersection of J St. and 27 de Noviembre St. in Vedado District. &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A map of the location can be found on Google Maps (http://maps.google.xx/): enter "23.134046, -82.382183".&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Current information will be located in front of the building of the Faculty of Mathematics and Computer Science, inside the Campus.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;From Tuesday 23 to Friday 26, every session will be held in the &lt;/span&gt;&lt;a href="http://www.hotelparquecentral.com/"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#333333;"&gt;Hotel Parque Central&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;, located in &lt;/span&gt;&lt;span class="Apple-style-span" style="line-height: 16px; "&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Neptuno street between the interceptions of Prado and Zulueta, in front of the Parque Central.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style=" font-weight: bold; font-family:georgia, serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;9th ICOR Registration&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Monday 22 is the opening day of the 9th ICOR. Besides the Mathematical Biology session and the Opening Plenary Lecture, it is devoted to individual registration. People already attending the Winter School on Matematical Biology but also interested to attend the 9th ICOR, should be registrated.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Talks&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Speakers will find slides projector and video projector connected to a computer which will accept your USB key (for a presentation with Acrobat or Power Point files) both in the University and in the Hotel Parque Central.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Accommodation/Hotel&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;According with your preferences, we recommend to be booked at a Hotel near the Campus or near the Capitolio. In addition, you can rent good rooms (can do so via internet) in hostals or family houses if they satisfy the official regulations (to our knowledge, can be booked good rooms near the Campus).&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Near the Campus (Vedado area):&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;br /&gt;Medium standing: Hotel Vedado, Hotel Colina, St.Johns&lt;br /&gt;&lt;br /&gt;High standing: Hotel Tryp Habana Libre&lt;br /&gt;&lt;br /&gt;Very high standing: Hotel Nacional&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Near the Capitolio (Habana Vieja area):&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;br /&gt;Medium standing: Hotel Caribbean, Hotel Deauville, Hotel Lido, Hotel Lincoln&lt;br /&gt;&lt;br /&gt;High standing: Hotel Inglaterra, Hotel Plaza, Hotel Sevilla, Ambos Mundos&lt;br /&gt;&lt;br /&gt;Very high standing: Hotel Telégrafo, Sta.Isabel, Los Frailes, Central Park&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Visa&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Each speaker will receive a "conference invitation" from the organizer committee. With that paper in hand one may ask to the cuban embassy a "scientific visa" (that is the only choice if you are coming from USA) or a "tourist card" (and, in that case, the conference invitation is obviously not necessary). The last procedure is quicker, cheaper and your travel agency should be able to do that formality for you. The only counterpart when you choose a "tourist card" is that you must be able to justify (hotel registration) that you have yet payed two nights in an hotel when you enter the cuban territory.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Money&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;There are two official currencies in Cuba. The "Peso Cubano" (CUP) (the usual money for cubans) and the "Peso Convertible " (1 CUC = 1.1 USD=24 CUP) with which foreigners must pay the Hotel, the Conference fees, and other services if required. Be careful, prices for both currency are ended by the $ sign! Of course in some places (Hotels, restaurants or in some Shopping Centers) the Visa card is also accepted. Traveller's checks and american express are refused. With Visa card one can get cash in a cash dispenser at the airport or in some hotels and places in some streets. It is also possible to bring cash and change it there (in CUC) when necessary. US dollar will be taxed on, 10% more than others currencies! Do not forget to change some money arriving at the airport (in order to pay the taxi to the hotel) &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Airport&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:georgia;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The arrival airport is the "José Marti's Aeropuerto" of La Habana. From the airport to the Habana center you must take a Taxi (no collective transport is available on that route). The journey from the airport to the town is between 10$ and 20$ (one must read $ = CUC here).&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4464634772146523623?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4464634772146523623/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/10/location.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4464634772146523623'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4464634772146523623'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/10/location.html' title='Location and Practical Information'/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-2842106721866637443</id><published>2008-07-07T08:00:00.000-07:00</published><updated>2010-02-14T03:32:21.064-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='Invited speakers'/><title type='text'>Invited speakers (to be confirmed)</title><content type='html'>&lt;ol style="font-family: georgia;"&gt;&lt;li&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman',serif;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman',Arial,sans-serif; font-size: medium; line-height: 18px;"&gt;A. Alvarez Cruz (La Habana, Cuba)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;D. Ambrosi (Milano, Italia)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;M.J. Caceres (Granada, España)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;S. Calogero (Granada, España)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;V. Calvez (Lyon, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;J.A. Cañizo (Barcelona, España)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;I. Capuzzo Dolcetta (Roma, Italia)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;J.A. Carrillo (Barcelona, España)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;F. Dickstein (Rio de Janeiro, Brazil)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;M.R. D'Orsogna (Los Angeles, USA)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;M. Doumic-Jauffret (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;L. Dumas (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;M. Escobedo (Bilbao, España)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;K. Fellner (Cambridge, UK)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;R. Galeano Andrades (Cartagena, Colombia)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;I. Gamba (Austin, USA)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;N. Ghoussoub (Vancouver, Canada) &lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;M.P. Gualdani (Austin, USA)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;T. Hillen (Alberta, Canada) &lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;P.-E. Jabin (Nice, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;T. Kano (Kyoto, Japon)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;O. Kavian (Versailles, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;D. Lannes (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;D. Levy (Maryland, USA)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;P.-L. Lions (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;P. Markowich (Cambridge, UK and Vienna, Austria)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;S. Martin (Orsay, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;N. Meunier (Paris, France)&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;J. Mitchell(Wisconsin-Madison, USA)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;F. Murat (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;A. Nachbin (Rio De Janeiro, Brazil)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;B. Perthame (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;G. Raoul (Cachan, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;C. Schmeiser (Vienna, Austria)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;M. Thiriet (Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;C. Turner (Cordoba, Argentina)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman',serif;"&gt;&lt;span class="Apple-style-span" style="font-family: 'times new roman',Arial,sans-serif; font-size: medium; line-height: 18px;"&gt;B. Valiño Alonso (La Habana, Cuba)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;li&gt;&lt;span style="font-family: 'times new roman';"&gt;&lt;span style="font-size: medium;"&gt;A. Vidal (Evry, France)&lt;/span&gt;&lt;/span&gt;&lt;/li&gt;&lt;/ol&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-2842106721866637443?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/2842106721866637443/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/07/participants.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2842106721866637443'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2842106721866637443'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/07/participants.html' title='Invited speakers (to be confirmed)'/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4567947391653105106</id><published>2008-02-03T13:29:00.000-08:00</published><updated>2010-02-03T13:31:00.735-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Nassif Ghoussoub&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Banf, Canada)&lt;/b&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red;"&gt;Homogenization of maximal monotone vector fields via selfdual variational calculus&lt;/span&gt;&lt;/div&gt;&lt;br /&gt;We use the theory of selfdual Lagrangians to give a variational approach to the homogenization of equations in divergence form, that are driven by a periodic family of maximal monotone vector fields. The approach has the advantage of using Gamma-convergence methods for corresponding  functionals just as in the classical case of convex potentials, as opposed to the graph convergence methods used in the absence of potentials. A new variational formulation for the homogenized equation is also given. &lt;br /&gt;This is joint work with Abbas Moameni and Ramon Zarate-Saiz&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4567947391653105106?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4567947391653105106/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/02/abstract-ghoussoub.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4567947391653105106'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4567947391653105106'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/02/abstract-ghoussoub.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4958876261248288849</id><published>2008-02-02T00:51:00.000-08:00</published><updated>2010-02-02T00:56:57.877-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Klemens Fellner&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(University of Cambridge, UK)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Stability of stationary states of non-local evolution equations&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;i&gt;&lt;br /&gt;&lt;/i&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:small;"&gt;(joint work with Gael Raoul, CMLA, ENS Cachan)&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We study non-local evolution equations for a density of individuals, which interact through a given symmetric potential. Such models appear in many applications such as swarming and flocking, opinion formation, inelastic materials, .... In particular, we are interested in interaction potentials, which behave locally repulsive, but aggregating over large scales. A particular example for such potentials was recently given in models of the alignment of the directions of filaments in the cytoskeleton.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We present results on the structure and stability of steady states. We shall show that stable stationary states of regular interaction potentials generically consist of sums of Dirac masses. However the amount of Diracs depends delicately on the interplay between local repulsion and aggregation. In particular we shall see that singular repulsive interaction potentials introduce diffusive effects in the sense that stationary state are rendered continuously.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p&gt;&lt;/p&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4958876261248288849?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4958876261248288849/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/02/klemens-fellner-cambridge-uk-stability.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4958876261248288849'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4958876261248288849'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/02/klemens-fellner-cambridge-uk-stability.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8831336723443403301</id><published>2008-02-01T13:56:00.000-08:00</published><updated>2010-02-01T14:21:10.389-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='List of abstract: sessions B-C-D-E'/><title type='text'></title><content type='html'>&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;div&gt;&lt;div&gt;&lt;div style="text-align: center; "&gt;&lt;div   style="font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; font-family:Helvetica;font-size:12px;"&gt;&lt;div style="text-align: center; "&gt;&lt;div style="text-align: center; "&gt;&lt;div style="text-align: center; "&gt;&lt;div style="font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; text-align: justify; "&gt;&lt;div style="text-align: justify; "&gt;&lt;div&gt;&lt;div style="text-align: justify; "&gt;&lt;div style="text-align: center; "&gt;&lt;span style="font-weight: bold; "&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Session B: Fluid mechanic and coastal dynamic&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A. C. Alvarez&lt;br /&gt;(Habana, Cuba)&lt;span class="Apple-style-span" style="font-weight: normal;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Solving Mild Slope equation in Matlab with &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Domain decomposition method&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(joint with M. Sarkis and D. Marchesin)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;In this paper the mild slope equation is solved on Matlab environmental. The method take into account physical processes waves as diffraction, refraction reflection, shoaling, port resonance and breaking. Further the effects of wave dissipation by friction, nonlinear amplitude dispersion are include. The algorithm is based on minimization of nonlinear functional using damped Newton iteration with Armijo-Goldstein line search strategy. Each linear problem is solved with Finite Element Method. Domain decomposition method with Schur complement is used in the linear case.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div class="post-body entry-content"&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Tadayoshi Kano&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Kyoto, Japan)&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style="text-align: center; color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;Tunamis on a deep open sea and on a gentle sloping beach&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: left; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Tunamis as shallow water waves:&lt;br /&gt;(1) The shallow water wave equations show that tunamis propagate on a deep open sea by, at least, the sound speed. (2) On a gentle sloping beach, the shallow water wave equations show that the diminution of propagation speed caused by the diminution of the water-depth results the deformation and, eventually, the break down of tunamis. The shallow water wave equation have a corresponding conservation law on a sloping beach and shock formation corresponding tunamis breaking on the shore.&lt;br /&gt;(3) A mathematical justification for tunamis as shallow water waves is given.&lt;/span&gt;&lt;/span&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="post-body entry-content" style="text-align: left; "&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;David Lannes&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Paris, France)&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style="text-align: center; color:red;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;A stability condition for two-fluid interfaces&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The aim of this talk is to derive a nonlinear stability condition for the interface between two fluids. This stability condition generalized the nonlinear Taylor criterion for the one fluid case and the linear Kelvin condition for the two fluid case. We show that it can explain the persistance of various natural phenomena such as waves and internal waves.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;div class="post-body entry-content" style="text-align: left; "&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Andre Nachbin&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Rio de Janeiro, Brasil)&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style="text-align: center; color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;Asymptotic issues regarding nonlinear wave/topography interaction&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The asymptotic issues of interest regard both the PDEs' (i.e. reduced models) as well as the solution's point of view. In particular for problems involving the interaction of coastal waves with quite arbitrary topography profiles. Phenomena studied are the apparent diffusion and waveform inversion of long waves in the presence of highly disordered topographies. I will report on recent results concerning the formulation of accurate reduced (PDE) models, where accuracy concerns asymptotic properties of solutions in respect to the full potential theory model.&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;div class="post-body entry-content"&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Cristina Turner&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Cordoba, Argentina)&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style="text-align: center; color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;Nonlinear stability of two-layer flows&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We study the dynamics of two–layer, stratiﬁed shallow water ﬂows. This is a model in which two scenarios for eventual mixing of stratiﬁed ﬂows (shear-instability and internal breaking waves) are, in principle, possible. We ﬁnd that unforced ﬂows cannot reach the threshold of shear-instability, at least without breaking ﬁrst. This is a fully nonlinear stability result for a model of stratiﬁed, sheared ﬂow. Mathematically, for 2X2 autonomous systems of mixed type, a criterium is found deciding whether the elliptic domain is reachable –smoothly– from hyperbolic initial conditions. If the characteristic ﬁelds depend smoothly on the system’s Riemann invariants, then the elliptic domain is unattainable. Otherwise, there are hyperbolic initial conditions that will lead to incursions into the elliptic domain, and the development of the associated instability. &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-body entry-content"&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-body entry-content"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-body entry-content"&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Baldomero Valiño Alonso&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(La Habana, Cuba)&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Infinitely narrow soliton in shallow water equations&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;(joint with Amaury Álvarez Cruz, Instituto de Oceanología, Cuba and Alex Méril, Université des Antilles et Guyana, Guadeloupe, France)&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;V.P.Maslov have shown that infinitely narrow solitons appear in Burgers’s equation as limit cases of singular solutions of Korteveg-De Fries’s equation. In this work we seek infinitely narrow solitons for shallow water equations, in the case when the profile of the depth has an isolated singular point. Following V. P. Maslov, we look for that singular solution as an asymptotical development with smooth coefficients in an appropriate algebra of generalized functions. Singular solutions of hyperbolic systems of partial differential equations in general position may have only a finite number of structuraly stable and self similar singular solutions. When the time evolves, the singular solution preserves the shape and structure of the initial condition. According to Maslov, the coeffcients of the formal asymptotic expansion of the singular solution satisfy an infinite chain of ordinary differential equations (the Hugoniot-Maslov chain corresponding to the singular solution involved). The truncation of the chain makes possible its aproximate calculation. From the point of view of numerical calculation, this approach is advantageous because it reduces the problem of solving numerically the nonlinear system of partial di¤erential equations to solving a closed system of ordinary differential equations. We interpret "infinitely narros solitons" as examples of simplified generalized functions in the sense of J. F. Colombeau and we use the rules of Colombeau’s differential algebras to do the calculations.&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-body entry-content"&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div class="post-body entry-content"&gt;&lt;div style="text-align: center; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span style="font-weight: bold; "&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Session C: Mean field games&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-body entry-content"&gt;&lt;div class="post-body entry-content"&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Italo Capuzzo Dolcetta&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Roma, Italy)&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A numerical approach to mean field games&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Mean ﬁelds games models introduced by Lasry-Lions describe through new systems of pde’s the asymptotic behavior of differential games in which the number of players tends to +∞. In the talk we discuss some recent work in collaboration with Y. Achdou and F. Camilli about numerical methods for the approximation of stationary and nonstationary versions of such models. Particular attention will be given to the optimal planning problem, in which the positions of a very large number of identical rational agents, with common value function, evolve from an initial given spatial density to a desired target density at the ﬁnal horizon time.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;span class="post-icons"&gt;&lt;span class="item-control blog-admin pid-1279762997"&gt;&lt;a href="http://www.blogger.com/post-edit.g?blogID=3975242521993377304&amp;amp;postID=4045447928341650846" title="Edit Post"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/a&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;a href="http://www.blogger.com/post-edit.g?blogID=3975242521993377304&amp;amp;postID=4045447928341650846" title="Edit Post"&gt;&lt;/a&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Maria Pia Gualdani&lt;br /&gt;(Austin, USA)&lt;span class="Apple-style-span" style="font-weight: normal;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style="text-align: center; color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;Global Existence of a Free Boundary Problem with Non-Standard Sources&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We consider a nonlinear free boundary problem, proposed by J.M.Lasry and P.L. Lions in 2006 in the framework of mean field games. The model describes the evolution of a scalar price which is realized as a free boundary of a diffusion equation with evolving sources. The talk focuses on global existence, uniqueness and regularity of solutions. The proof uses tools from non-interacting stochastic particle systems and multiscale analysis. Joint work with L. Chayes, M.d.M. Gonzalez and I. Kim.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;__________________________________________________________&lt;/span&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span" style="font-family: Georgia, serif; "&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Peter &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span style="line-height: 26px; "&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Markowich&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(University of Cambridge, UK &amp;amp; University of Vienna, Austria)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="color: rgb(0, 0, 0); font-style: normal; "&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;On PDE Models for (some) Socio-Economic Problems:&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Price Formation, Opinion Formation and Crowd Modeling&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify; "&gt;&lt;div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We present and analyse partial differential equation models in the socio-economic sciences:&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;1) a highly nonstandard free boundary problem in price formation&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;2) a Boltzmann equation for opinion formation in human societies with strong leaders&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;3) a continuity equation with an eikonal field equation coupling.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;div class="post-body entry-content"&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div class="post-body entry-content"&gt;&lt;div style="text-align: center; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span style="font-weight: bold; "&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Session D: Classical and quantum kinetic equations&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;María José Cáceres Granados&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A numerical solver for a nonlinear Fokker-Planck equation in Neuroscience&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Due to the huge number of neurons in the visual cortex network a kinetic approach can be considered. In such a way that the dynamic of the system is analyzed by mean of a distribution function. Therefore, the system of ODEs, which describes the integrate-and-fire models, is replaced with a system of PDEs. The advantage of the kinetic models is the reduction of the number of equations and consequently also the time of computation is reduced. In this talk we show a numerical scheme for the Fokker-Planck system, which models the visual cortex network dynamics. The deterministic numerical solutions are compared with Monte Carlo simulations. Our numerical solver allows us to obtain the evolution on time of the distribution functions and therefore the evolution of the macroscopic quantities, since they are moments of the pdf. As a consequence, we validate models which are obtained via moment closure.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="post-footer-line post-footer-line-1"&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center; "&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Simone Calogero&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Granada, España)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style="text-align: center; color:red;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;Self-similar behavior in relativistic galactic dynamics&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;In this talk I will present a short proof of existence of self-similar solution to the Ultra-Relativistic Vlasov-Poisson system in 3 dimensions. The proof is considerably simpler than the one presented recently by Lemou, Méhats &amp;amp; Raphaël and, at the same time, our existence result is more general. Moreover, our method works also for the massless Einstein-Vlasov system, for which the existence of self-similar solutions was previously unknown. This talk is based on a joint work with Óscar Sánchez.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: center; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;José Alfredo Cañizo &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Barcelona, España)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style="text-align: center;  color:red;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;Entropy inequalities and speed of convergence to equilibrium for the&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style="text-align: center; color:red;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;growth-fragmentation equation&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The growth-fragmentation equation models a group of cells which grow (or age) at a certain rate, and divide into two or more pieces. After a suitable rescaling, the shape of the distribution function of the population converges to a universal profile. By means of entropy-entropy dissipation inequalities for some unbounded fragmentation coefficients, we show that the speed of this convergence is exponential. This kind of inequalities may be used for other linear equations for which the General Relative Entropy principle is valid.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: center; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Rafael Galeano Andrades&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Cartagena, Colombia)&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div  style=" text-align: center; color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#FF0000;"&gt;A variational approach to the stationary Boltzmann equation&lt;/span&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div  style=" text-align: center; color:red;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(joint with Pedro Ortega Palencia)&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;We define a functional whose critical points coincide with stationary solutions of Boltzmann equation and by classical method to find the minimum of functionals we find critical point. &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;b&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8831336723443403301?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8831336723443403301/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/02/session-b-fluid-mechanic-and-coastal.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8831336723443403301'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8831336723443403301'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/02/session-b-fluid-mechanic-and-coastal.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8114883730479804915</id><published>2008-02-01T04:42:00.000-08:00</published><updated>2010-02-01T04:42:44.725-08:00</updated><title type='text'></title><content type='html'>&lt;div style="line-height: 1.3em; margin: 0px 0px 0.75em; text-align: center;"&gt;&lt;b&gt;David Lannes&lt;span style="font-weight: normal;"&gt;&amp;nbsp;&amp;nbsp;&lt;/span&gt;(Paris, France)&lt;/b&gt;&lt;/div&gt;&lt;div style="color: red; line-height: 1.3em; margin: 0px 0px 0.75em; text-align: center;"&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;A stability condition for two-fluid interfaces&lt;/span&gt;&lt;/div&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;The aim of this talk is to derive a nonlinear stability condition for the interface between two fluids. This stability condition generalized the nonlinear Taylor criterion for the one fluid case and the linear Kelvin condition for the two fluid case. We show that it can explain the persistance of various natural phenomena such as waves and internal waves.&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8114883730479804915?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8114883730479804915/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/02/abstract-lannes-talk.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8114883730479804915'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8114883730479804915'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/02/abstract-lannes-talk.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5266283006184987776</id><published>2008-02-01T03:32:00.000-08:00</published><updated>2010-02-01T03:33:55.921-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Pierre-Louis Lions&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Collège de France, Paris, France)&lt;/b&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red;"&gt;An Introduction To Mean Field Games&lt;/span&gt;&lt;/div&gt;&lt;br /&gt;This talk is an introduction to a new class of models called Mean Field Games that arise as the limits of Nash equilibria in a game where the number of players goes to infinity. The rigorous derivation of these models requires some new developments in Analysis that have other applications (to Statistical Physics and Mechanics). And we discuss some examples of such models (distribution of wealth in economics, population dynamics...).&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5266283006184987776?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5266283006184987776/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/02/abstract-lions.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5266283006184987776'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5266283006184987776'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/02/abstract-lions.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-71150060121988614</id><published>2008-01-25T14:08:00.000-08:00</published><updated>2010-01-26T13:36:26.958-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;José A. Carrillo de la Plata&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(ICREA &amp;amp; &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Universitat Autònoma de Barcelona, Spain&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(The lecture of Prof. J. A. Carrillo will likely be in spanish, &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#000099;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;depending on the audience)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Macroscopic and Kinetic Equations in Swarming and Chemotaxis&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;In these series of lectures I will review several models for the collective behavior of systems composed by many individuals. As a reference we will first discuss some swarming models proposed to describe some self-organized animal behaviors in fishes and birds for instance. Some typical principles of swarming will be described and minimal models derived. Continuum equations like kinetic or macroscopic equations appear when considering a large number of individuals and the corresponding mean-field limits and hydrodynamic equations will be treated. Some useful tools are distances between probability measures in which transport distances play an interesting role to connect to macroscopic models. At the macroscopic level, we will learn how to work with the transport distances in some typical examples. Classical chemotaxis models in which cells move due to a chemical response will be solved using this method and its use for some other aggregation equations in swarming will also be analysed.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#000000;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Ecuaciones cinéticas y macroscópicas en "Swarming" y quimiotaxis&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;/span&gt;&lt;/p&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;En esta serie de lecciones, haré un resumen del estudio de varios modelos del comportamiento colectivo de sistemas compuestos por muchos entes individuales. Como ejemplo de referencia, discutiremos algunos modelos del comportamiento de auto-organización en algunos animales como peces y pájaros, llamado "swarming". Los principios básicos del "swarming" darán lugar a modelos minimales para su descripción. Ecuaciones continuas de tipo cinética o macroscópicas se obtienen cuando el número de individuos es muy grande en lo que se conoce como límite de campo medio. Algunas herramientas matemáticas para estudiar dichos límites se analizarán como las distancias de tipo transporte entre medidas de probabilidad. Además, permiten conectar el estudio de dichas ecuaciones con ecuaciones macroscópicas. Modelos macroscópicos, entre ellos el de quimiotaxis en el que las células dirigen su movimiento hacia las regiones de mayor concentración de un cierto componente químico o algunos modelos de swarming, se pueden estudiar con dichas distancias.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;/span&gt;&lt;p&gt;&lt;/p&gt;&lt;/span&gt;&lt;p&gt;&lt;/p&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;/span&gt;&lt;p&gt;&lt;/p&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-71150060121988614?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/71150060121988614/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/jose.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/71150060121988614'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/71150060121988614'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/jose.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-1180255290693598776</id><published>2008-01-25T04:52:00.000-08:00</published><updated>2010-01-25T04:53:59.182-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Aimé Lachapelle&lt;br /&gt;(Paris, France)&lt;br /&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red;"&gt; Mean Field Games: a numerical methodology with application to a stylised model of technology switch&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;Mean Field Games (MFG) have been recently introduced by Lasry and Lions, and  describe approximations of N-player games when N tends to infinity. After recalling briefly the mathematical framework, we will insist on the optimal control point of view. We will then present the monotonic algorithm we use for solving finite-horizon MFG problems. We will close with some simulations for a stylised model of technology switch involving non-uniqueness. Joint work with J. Salomon and G. Turinici.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-1180255290693598776?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/1180255290693598776/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-lachapelle.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/1180255290693598776'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/1180255290693598776'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-lachapelle.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-2960076547343674179</id><published>2008-01-25T04:20:00.000-08:00</published><updated>2010-01-25T04:22:33.857-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Otared Kavian&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Versaille, France)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;Remarks on Inverse Problems arising from Electrical Impedance Tomography&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;In this talk we present a few inverse problems related to the technique known as &lt;i&gt;Electrical Impedance Tomography&lt;/i&gt;, which has important applications in medical imaging. In particular we shall present some results recently published in joint paper with Y. Capdeboscq, J. Fehrenbach, F. de Gournay. In that paper, we discuss the reconstruction of the impedance from the local power density. This study is motivated by a new imaging principle which allows to recover interior measurements of the energy density by a non invasive method. We discuss the theoretical feasibility in two dimensions, and propose numerical algorithms to recover the conductivity in two and three dimension. The efficiency of this approach is documented by several numerical simulations.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-2960076547343674179?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/2960076547343674179/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-kavian.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2960076547343674179'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2960076547343674179'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-kavian.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4051007096058949838</id><published>2008-01-25T04:15:00.000-08:00</published><updated>2010-01-25T04:17:28.721-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Irene Gamba&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Austin, Texas, USA)&lt;br /&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;Non-conservative models of multi-linear particle interactions&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;We look at  extensions Kac N-particle model of pair interactions to an  N-particle model which includes  multi-particle interactions in Fourier/Laplace transformed space. Under molecular chaos assumption, one obtains a multi-linear integro-evolution equation that can be view as extensions of  Boltzmann model dynamics of Maxwell type for conservative or dissipative interactions.&lt;br /&gt;&lt;br /&gt;We shall study the evolution of the corresponding probability density solution. Under the assumption  temporal invariance  under scaling transformations of the  phase space and contractive properties,&lt;br /&gt;we obtain a full description of existence, uniqueness and long-time behavior to self-similar states, all from its spectral properties as well as the formation of power tails in their self similar state.&lt;br /&gt;&lt;br /&gt;We also focus on a couple  of new examples of multi-agent dynamics and information sharing and percolation models.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4051007096058949838?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4051007096058949838/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-gamba.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4051007096058949838'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4051007096058949838'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-gamba.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-7098287359520656057</id><published>2008-01-25T04:11:00.000-08:00</published><updated>2010-01-25T04:13:58.800-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Miguel Escobedo&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Bilbao, Spain)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red;"&gt;Post Gel solutions for coagulation equations&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;We shall briefly present and motivate the Smoluchowski coagulation esuation. We will describe the phenomena of gelation and recall the conjecture about the behaviour of the solutions after gelation. We will finally present a recent result about the existence of solutions with such a behaviour.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-7098287359520656057?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/7098287359520656057/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-escobedo.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/7098287359520656057'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/7098287359520656057'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-escobedo.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8653863620177688085</id><published>2008-01-21T08:31:00.000-08:00</published><updated>2010-01-21T08:47:07.111-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Baldomero Valiño Alonso&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(La Habana, Cuba)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red;"&gt;Infinitely narrow soliton in shallow water equations&lt;/span&gt;&lt;br /&gt;(joint with Amaury Álvarez Cruz, Instituto de Oceanología, Cuba and Alex Méril, Université des Antilles et Guyana, Guadeloupe, France)&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;V.P.Maslov have shown that infinitely narrow solitons appear in Burgers’s equation as limit cases of singular solutions of Korteveg-De Fries’s equation. In this work we seek infinitely narrow solitons for shallow water equations, in the case when the profile of the depth has an isolated singular point. Following V. P. Maslov, we look for that singular solution as an asymptotical development with smooth coefficients in an appropriate algebra of generalized functions. Singular solutions of hyperbolic systems of partial differential equations in general position may have only a finite number of structuraly stable and self similar singular solutions. When the time evolves, the singular solution preserves the shape and structure of the initial condition. According to Maslov, the coeffcients of the formal asymptotic expansion of the singular solution satisfy an infinite chain of ordinary differential equations (the Hugoniot-Maslov chain corresponding to the singular solution involved). The truncation of the chain makes possible its aproximate calculation. From the point of view of numerical calculation, this approach is advantageous because it reduces the problem of solving numerically the nonlinear system of partial di¤erential equations to solving a closed system of ordinary differential equations. We interpret "infinitely narros solitons" as examples of simplified generalized functions in the sense of J. F. Colombeau and we use the rules of Colombeau’s differential algebras to do the calculations.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8653863620177688085?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8653863620177688085/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-valino.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8653863620177688085'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8653863620177688085'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-valino.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-3358361120470562728</id><published>2008-01-21T08:28:00.000-08:00</published><updated>2010-01-21T08:30:19.898-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Tadayoshi Kano&lt;br /&gt;&lt;/b&gt; &lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Kyoto, Japan)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;Tunamis on a deep open sea and on a gentle sloping beach&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;Tunamis as shallow water waves:&lt;br /&gt;(1) The shallow water wave equations show that tunamis propagate on a deep open sea by, at least, the sound speed. (2) On a gentle sloping beach, the shallow water wave equations show that the diminution of propagation speed caused by the diminution of the water-depth results the deformation and, eventually, the break down of tunamis. The shallow water wave equation have a corresponding conservation law on a sloping beach and shock formation corresponding tunamis breaking on the shore.&lt;br /&gt;(3) A mathematical justification for tunamis as shallow water waves is given.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-3358361120470562728?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/3358361120470562728/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-kano.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3358361120470562728'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3358361120470562728'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-kano.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-3359283411639620548</id><published>2008-01-21T08:24:00.000-08:00</published><updated>2010-01-21T08:27:11.406-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Rafael Galeano Andrades&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Cartagena, Colombia)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;A variational approach to the stationary Boltzmann equation&lt;br /&gt;&lt;/div&gt;&lt;div style="color: red; text-align: center;"&gt;(joint with Pedro Ortega Palencia)&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;We define a functional whose critical points coincide with stationary solutions of Boltzmann equation and by classical method to find the minimum of functionals we find critical point.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-3359283411639620548?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/3359283411639620548/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/rafael-galeano-andrades-cartagena.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3359283411639620548'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3359283411639620548'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/rafael-galeano-andrades-cartagena.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4045447928341650846</id><published>2008-01-21T08:21:00.000-08:00</published><updated>2010-01-21T08:23:31.360-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Italo Capuzzo Dolcetta&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Roma, Italy)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red;"&gt;A numerical approach to mean field games&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;Mean ﬁelds games models introduced by Lasry-Lions describe through new systems of pde’s the asymptotic behavior of differential games in which the number of players tends to +∞. In the talk we discuss some recent work in collaboration with Y. Achdou and F. Camilli about numerical methods for the approximation of stationary and nonstationary versions of such models. Particular attention will be given to the optimal planning problem, in which the positions of a very large number of identical rational agents, with common value function, evolve from an initial given spatial density to a desired target density at the ﬁnal horizon time.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4045447928341650846?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4045447928341650846/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-dolcetta.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4045447928341650846'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4045447928341650846'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-dolcetta.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-6433383693483781118</id><published>2008-01-21T08:18:00.000-08:00</published><updated>2010-01-21T08:20:38.499-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Cristina Turner&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Cordoba, Argentina)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;Nonlinear stability of two-layer flows&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;We study the dynamics of two–layer, stratiﬁed shallow water ﬂows. This is a model in which two scenarios for eventual mixing of stratiﬁed ﬂows (shear-instability and internal breaking waves) are, in principle, possible. We ﬁnd that unforced ﬂows cannot reach the threshold of shear-instability, at least without breaking ﬁrst. This is a fully nonlinear stability result for a model of stratiﬁed, sheared ﬂow.  Mathematically, for 2X2 autonomous systems of mixed type, a criterium is found deciding whether the elliptic domain is reachable –smoothly– from hyperbolic initial conditions. If the characteristic ﬁelds depend smoothly on the system’s Riemann invariants, then the elliptic domain is unattainable. Otherwise, there are hyperbolic initial conditions that will lead to incursions into the elliptic domain, and the development of the associated instability. &lt;span style="color: #333333; font-family: Arial; font-size: small;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-6433383693483781118?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/6433383693483781118/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-turner.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/6433383693483781118'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/6433383693483781118'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-turner.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8172013711327843928</id><published>2008-01-21T08:16:00.000-08:00</published><updated>2010-01-21T08:17:51.930-08:00</updated><title type='text'></title><content type='html'>&lt;div style="margin: 1ex;"&gt;&lt;div style="text-align: center;"&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;Andre Nachbin&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Rio de Janeiro, Brasil)&lt;br /&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;Asymptotic issues regarding nonlinear wave/topography interaction &lt;br /&gt;&lt;/div&gt;&lt;br /&gt;The asymptotic issues of interest regard both the PDEs' (i.e. reduced models) as well as the solution's point of view.    In particular for problems involving the interaction of coastal waves with  quite arbitrary topography profiles. Phenomena studied are the apparent diffusion and waveform inversion of long waves in the presence of highly disordered topographies.   I will report on recent results concerning  the formulation of  accurate reduced (PDE) models, where accuracy concerns asymptotic properties of solutions in respect to the full potential theory model.&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8172013711327843928?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8172013711327843928/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-nachbin.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8172013711327843928'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8172013711327843928'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-nachbin.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4884547183250736664</id><published>2008-01-21T05:36:00.000-08:00</published><updated>2010-01-21T05:37:40.408-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;Maria Pia Gualdani &lt;br /&gt;(Austin, USA) &lt;br /&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;Global Existence of a Free Boundary Problem with Non-Standard Sources  &lt;br /&gt;&lt;/div&gt;&lt;br /&gt;We consider a nonlinear free boundary problem, proposed by J.M.Lasry and P.L. Lions in 2006 in the framework of mean field games. The model describes the evolution of a scalar price which is realized as a free boundary of a diffusion equation with evolving sources. The talk focuses on global existence, uniqueness and regularity of solutions. The proof uses tools from non-interacting stochastic particle systems and multiscale analysis. Joint work with L. Chayes, M.d.M. Gonzalez and I. Kim.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4884547183250736664?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4884547183250736664/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-gualdani.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4884547183250736664'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4884547183250736664'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-gualdani.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5982322723613173940</id><published>2008-01-21T05:30:00.000-08:00</published><updated>2010-01-21T05:32:10.465-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt; &lt;b&gt;Simone Calogero &lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;(Granada, España)&lt;/span&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;Self-similar behavior in relativistic  galactic dynamics&lt;/span&gt; &lt;span style="font-family: Helvetica; font-size: small;"&gt;&amp;nbsp;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;In this talk I will present a short  proof of existence of self-similar solution to the Ultra-Relativistic Vlasov-Poisson  system in 3 dimensions. The proof is considerably simpler than the one presented recently  by Lemou, Méhats &amp;amp; Raphaël and, at the same time, our existence result is more general. Moreover, our method works also for&amp;nbsp;the  massless Einstein-Vlasov system, for which the existence of self-similar solutions was previously  unknown. This talk is based on a joint work  with Óscar Sánchez.&lt;/span&gt;&lt;br /&gt;&lt;div style="margin: 1ex;"&gt;&lt;div&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5982322723613173940?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5982322723613173940/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-calogero.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5982322723613173940'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5982322723613173940'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-calogero.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8614042123867508679</id><published>2008-01-21T05:28:00.000-08:00</published><updated>2010-01-21T05:29:30.563-08:00</updated><title type='text'></title><content type='html'>&lt;div style="margin: 1ex;"&gt;&lt;div style="text-align: center;"&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: center;"&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;María José Cáceres Granados&lt;/span&gt;&amp;nbsp;&lt;/b&gt;&lt;br /&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red; font-family: Helvetica; font-size: small;"&gt;A numerical solver for a nonlinear  Fokker-Planck equation in Neuroscience&lt;/span&gt;&lt;span style="color: red;"&gt;&amp;nbsp;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;Due to the huge number of neurons  in the visual cortex network a kinetic&amp;nbsp; approach can be considered.  In such a way that the dynamic of the system is analyzed by mean of  a distribution function. Therefore, the system of ODEs, which  describes the integrate-and-fire models, is replaced&amp;nbsp; with a system  of&amp;nbsp; PDEs. The advantage of the kinetic models is the reduction  of the number of equations and consequently also the time of computation  is reduced.&amp;nbsp; In this talk we show a numerical scheme for the Fokker-Planck  system, which models the&amp;nbsp; visual cortex network dynamics. The deterministic numerical solutions  are compared with Monte Carlo simulations. Our numerical solver allows  us to obtain the evolution on time of the distribution functions and  therefore&amp;nbsp; the evolution of the macroscopic quantities, since they  are moments of the pdf. As a consequence, we validate models which are  obtained via moment closures &lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8614042123867508679?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8614042123867508679/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-caceres.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8614042123867508679'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8614042123867508679'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-caceres.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5496789989184933336</id><published>2008-01-21T05:24:00.000-08:00</published><updated>2010-01-21T08:38:21.283-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;A. C. Alvarez&lt;br /&gt;(Habana, Cuba) &lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color: red;"&gt;Solving Mild Slope equation in Matlab with Domain decomposition method&lt;/span&gt;&lt;br /&gt;(joint with M. Sarkis and D. Marchesin)&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;In this paper the mild slope equation is solved on Matlab environmental. The method take into account physical processes waves as diffraction, refraction reflection, shoaling, port resonance and breaking. Further the effects of wave dissipation by friction, nonlinear amplitude dispersion are include. The algorithm is based on minimization of nonlinear functional using damped Newton iteration with Armijo-Goldstein line search strategy. Each linear problem is solved with Finite Element Method. Domain decomposition method with Schur complement is used in the linear case.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5496789989184933336?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5496789989184933336/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-alvarez.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5496789989184933336'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5496789989184933336'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-alvarez.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8867508175078145036</id><published>2008-01-21T05:20:00.000-08:00</published><updated>2010-01-25T04:51:14.182-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;David Lannes&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;(Paris, France)&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;Stability/instability issues for two-fluid interfaces&lt;/div&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;&amp;nbsp;&lt;/span&gt; &lt;br /&gt;This short course is devoted to simple considerations on the stability of the interface between two fluids. With simple tools, we will exhibit the main phenomena responsable for possible (Kelvin-Helmholtz) instabilities and explain qualitatively the main steps of the full nonlinear analysis.&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8867508175078145036?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8867508175078145036/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-lannes.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8867508175078145036'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8867508175078145036'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/abstract-lannes.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-8761141012547397279</id><published>2008-01-21T05:01:00.000-08:00</published><updated>2010-01-21T05:19:37.768-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;&amp;nbsp;José Alfredo Cañizo&amp;nbsp;&lt;/span&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;&amp;nbsp;(Barcelona, España)&lt;/span&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;div style="color: red; text-align: center;"&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;Entropy inequalities and speed of  convergence to equilibrium for the&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="color: red;"&gt;&lt;/div&gt;&lt;div style="color: red; text-align: center;"&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;growth-fragmentation equation&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;br /&gt;&lt;br /&gt;&lt;br /&gt;&lt;span style="font-family: Helvetica; font-size: small;"&gt;The growth-fragmentation equation  models a group of cells which grow (or age) at a certain rate, and divide  into two or more pieces. After a suitable rescaling, the shape of  the distribution function of the population converges to a universal  profile. By means of entropy-entropy dissipation inequalities  for some unbounded fragmentation coefficients, we show  that the speed of this convergence is exponential. This kind of inequalities  may be used for other linear equations for which the General Relative  Entropy principle is valid.&lt;/span&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-8761141012547397279?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/8761141012547397279/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/absract-canizo.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8761141012547397279'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/8761141012547397279'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/absract-canizo.html' title=''/><author><name>Yes!</name><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='32' height='21' src='http://2.bp.blogspot.com/_7eONx2CJzc0/TU1D9uVUIKI/AAAAAAAAEs8/B8zlL2F-92U/s1600/yes_we_caire-d4a9a.jpg'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-3469206678005761616</id><published>2008-01-20T12:35:00.000-08:00</published><updated>2010-01-20T12:41:26.810-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Vincent Calvez&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;(CNRS &amp;amp; ENS-Lyon, France)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span" style="color: rgb(204, 0, 0); font-style: italic; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;The geometry of one-dimensional self-attracting&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="line-height: 18px; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;particles&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: small;"&gt;(&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: small;"&gt;joint work with José Antonio Carrillo, ICREA, Univiversidad Autònoma Barcelona)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;&lt;br /&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;&lt;i&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span" style="color: rgb(204, 0, 0); font-style: italic; "&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;p style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;We wish to present in this talk a brief overview of recent developments in the analysis of the generalized Keller-Segel system:&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;\[&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;\partial_t \rho(t,x) = \Delta\rho^m(t,x) + \chi \nabla\cdot \left(\rho(t,x) \nabla\left(\dfrac{|x|^{k}}{k}*\rho(t,x)\right)\right)\, , \quad t&gt;0\, , \quad x\in \mathbb{R}^N\, .&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;\]&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Here $\rho(t,x)$ denotes the density of diffusive cells which are self-attracted through a mean field potential. This model has raised a lot of interest in the field of mathematical biology since it generally exhibits a dichotomy between global existence (dispersion of the cells) and finite time blow-up (aggregation of the cells). We will explain how this system possesses the structure of a gradient flow for the Wasserstein metric on the space of probability densities. Interestingly enough the energy functional is the sum of two opposite contributions, being respectively convex and concave, and homogeneous. We will show some consequences of this gradient flow interpretation, concerning finite time blow-up and long time asymptotics.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;/span&gt;&lt;p&gt;&lt;/p&gt; &lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica; min-height: 14.0px"&gt;&lt;br /&gt;&lt;/p&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-3469206678005761616?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/3469206678005761616/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/vincent-calvez-cnrs-ens-lyon-france.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3469206678005761616'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3469206678005761616'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2008/01/vincent-calvez-cnrs-ens-lyon-france.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-7428067073740007518</id><published>2008-01-20T12:25:00.000-08:00</published><updated>2010-01-20T12:43:32.509-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Thomas Hillen&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(University of Alberta, Canada)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;''&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Pointwise weak steady states of transport equations for cell movement in network tissue''&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="font-style: normal; "&gt;&lt;span class="Apple-style-span"  style="font-size:small;"&gt;(joint work with K. Painter (Heriot-Watt), P. Hinow (Milwaukee) and Z.A. Wang (Vanderbilt))&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;i&gt;&lt;br /&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;i&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Some metastatic cancer cells use an interesting mechanism to move through network tissue, such as collagen networks. I will present a transport equation model, which describes the movement of these cells along network fibers and the network degradation due to proteolytic enzymes which are produced by the cells. In numerical implementation we find that the resulting models shows generation of networks which resemble vasculature formation. We believe that pointwise weak steady states are the organizing centres behind these network patterns. I will introduce the notion of pointwise weak steady states and discuss their use to understand network formation. &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-7428067073740007518?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/7428067073740007518/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/thomas-hillen-university-of-alberta.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/7428067073740007518'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/7428067073740007518'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/thomas-hillen-university-of-alberta.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-1807096346525714208</id><published>2008-01-12T12:59:00.000-08:00</published><updated>2010-01-13T06:50:23.824-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Nicolas Meunier&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;(Université Paris V, France)&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:17px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Analysis of self-organization systems for cell polarization&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:17px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:small;"&gt;(Joint work with V. Calvez and R. Voituriez)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:17px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="font-family: Helvetica; font-size-adjust: none; font-size: 17px; font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:11px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;In this work, we investigate the dynamics of a modified Keller-Segel type model. On the contrary to the classical configuration, the chemical production term is located on the boundary. In the one-dimensional case and in a particular case in dimension two, we prove, under suitable assumptions, the following dichotomy which is reminiscent of the two-dimensional Keller-Segel system. Solutions are global if the mass is below the critical mass and they blow-up in finite time above the critical mass. Furthermore, in the one-dimensional case, using entropy techniques, we provide quantitative convergence results for the subcritical case. This work is completed with a more realistic model (still one-dimensional) for modeling purpose. In this new setting, the chemical is supplied by a quantity which evolves by exchanging particles at the boundary. Finally some results are given for the two-dimensional case and we also provide some links with cell polarisation that is an essential step for many biological processes and that is involved for instance in cell migration, division, or morphogenesis.&lt;/span&gt;&lt;/span&gt;&lt;span style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-1807096346525714208?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/1807096346525714208/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/nicolas-meunier-universite-france.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/1807096346525714208'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/1807096346525714208'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/nicolas-meunier-universite-france.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4764568518226893506</id><published>2008-01-12T12:25:00.000-08:00</published><updated>2010-01-13T06:51:00.707-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;Pierre-Emmanuel Jabin&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;(Université de Nice Sophia-Antipolis, France)&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;"&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Selection-mutation Dynamics for the Evolution of Traits in a Population"&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;This talk aims at introducing some models describing the evolution of a large population of individuals with different biological "traits". The reproduction rate of each individual depends on its trait and on the competition for ressources within the population. In addition mutations may be included, enabling new traits to develop. These models leads to difficult asymptotic problems as the time scale of the mutations is usually much larger than the time scale of births and death. One such asymptotic will in particular be investigated, corresponding to frequent small mutations.&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4764568518226893506?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4764568518226893506/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/pierre-emmanuel-jabin-universite-de.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4764568518226893506'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4764568518226893506'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/pierre-emmanuel-jabin-universite-de.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5611787300989560569</id><published>2008-01-09T04:00:00.000-08:00</published><updated>2010-02-08T05:08:12.059-08:00</updated><category scheme='http://www.blogger.com/atom/ns#' term='List of abstract: session A'/><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-weight: bold;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Session A: Mathematical Biology&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;b&gt;&lt;span style="color:#666666;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Davide Ambrosi&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Politecnico di &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Milano, Italia)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="line-height: normal;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="line-height: 18px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The electromechanical coupling in cardiac mechanics&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The coupling between cardiac mechanics and electric signalling can be addressed in a two possible alternative framework: the electrical potential dictates the active stress or the active strain. In this talk the explore the second (less popular) strategy, obtained thanks a factorization of the deformation tensor. After rewriting the equations in a deforming domain, we prove that neglecting the deformation of the substrate induces a non-negligible error in predicting celerity and width of the pulse, while the amplitude and the stability conditions are not affected by the electro--mechanical decoupling. Exact solutions of travelling front type can be found with explicit form of the celerity and steepness. The role of visco-elasticity and the characterization of unstable initial conditions are discussed with the support of numerical simulations, both in one and two spatial dimension. &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;_________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span style=" font-style: italic;color:#cc0000;"&gt;&lt;/span&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center;"&gt;&lt;span style=" font-style: italic;color:#cc0000;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span style="font-style: normal;"&gt;&lt;span style="color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Vincent Calvez&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style=" font-style: italic;color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span style="font-style: normal;"&gt;&lt;span style="color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(CNRS &amp;amp; ENS-Lyon, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The geometry of one-dimensional self-attracting&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="line-height: 18px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;particles&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style=" font-style: italic;color:#cc0000;"&gt;&lt;span&gt;&lt;span style="font-style: normal;"&gt;&lt;span style="color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span style="font-style: normal;"&gt;&lt;span style="color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;joint work with José Antonio Carrillo, ICREA, Univiversidad Autònoma Barcelona)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span style=" font-style: italic;color:#cc0000;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span style="color:black;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We wish to present in this talk a brief overview of recent developments in the analysis of the generalized Keller-Segel system:&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;\[&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;\partial_t \rho(t,x) = \Delta\rho^m(t,x) + \chi \nabla\cdot \left(\rho(t,x) \nabla\left(\dfrac{|x|^{k}}{k}*\rho(t,x)\right)\right)\, , \quad t&amp;gt;0\, , \quad x\in \mathbb{R}^N\, .&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;\]&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Here $\rho(t,x)$ denotes the density of diffusive cells which are self-attracted through a mean field potential. This model has raised a lot of interest in the field of mathematical biology since it generally exhibits a dichotomy between global existence (dispersion of the cells) and finite time blow-up (aggregation of the cells). We will explain how this system possesses the structure of a gradient flow for the Wasserstein metric on the space of probability densities. Interestingly enough the energy functional is the sum of two opposite contributions, being respectively convex and concave, and homogeneous. We will show some consequences of this gradient flow interpretation, concerning finite time blow-up and long time asymptotics.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;_________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Maria Rita D'Orsogna&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;California State University at Northridge, Los Angeles, USA&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style=" line-height: 26px;color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Modelling viral entry dynamics&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Successful viral infection of a healthy cell requires complex host-pathogen interactions. In this talk we focus on the dynamics specific to the HIV virus entering a eucaryotic cell.  We model viral entry as a stochastic engagement of receptors and coreceptors on the cell surface. We also consider the transport of virus material to the cell nucleus by coupling microtubular motion to the concurrent biochemical transformations that render the viral material competent for nuclear entry. We discuss both mathematical and biological consequences of our model, such as the formulation of an effective integrodifferential boundary condition embodying a memory kernel and optimal timing in maximizing viral probabilities.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style="  font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;_________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style="color:black;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Marie Doumic-Jauffret&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(INRIA, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;div style="text-align: center;"&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Aggregation/fragmentation models for protein polymerization&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Abnormal protein polymerization is at the origin of a number of neuro-degenerative diseases, e.g. Prion (Madcow), Huntington or Alzheimer diseases. This phenomenon can be described mathematically either in a discrete or in a continuous setting, by equations of fragmentation-coagulation type. We review here some results and some open problems on the study of prion proliferation equations.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;_________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;b&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Laurent Dumas&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Université Paris VI, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style=" line-height: normal;color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A numerical simulation of the human arterial network based on non invasive measurements&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The numerical simulation of the human arterial network of a given patient in order to find the main characteristics of its arteries and thus to prevent from cardiovascular diseases is a major subject of interest. A simple fluid-structure interaction model for the simulation of blood flow in arteries is studied here. Derived from the general 3D equations, it computes the section area of the artery and the volumetric flux of the flow for each longitudinal position and time. The inverse problem corresponding to the identification of the main parameters of this model is successfully solved by using a reduced number of non invasive measurements. A discussion on the amount of information needed is in particular studied. Some first results based on experimental measurements with a Doppler technique called echotracking are also presented&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/div&gt;&lt;div   style="text-align: center; font-style: normal; font-variant: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Klemens&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;i&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt; &lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/i&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Fellner&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="text-align: center; font-style: normal; font-variant: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(University of Cambridge, UK)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="text-align: center; font-style: normal; font-variant: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="text-align: center; font-style: normal; font-variant: normal; line-height: normal; margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font-family:Helvetica;font-size:12px;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Stability of stationary states of non-local evolution equations&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"   style="font-family:'times new roman', serif;color:#CC0000;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(joint work with Gael Raoul, CMLA, ENS Cachan)&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We study non-local evolution equations for a density of individuals, which interact through a given symmetric potential. Such models appear in many applications such as swarming and flocking, opinion formation, inelastic materials, .... In particular, we are interested in interaction potentials, which behave locally repulsive, but aggregating over large scales. A particular example for such potentials was recently given in models of the alignment of the directions of filaments in the cytoskeleton.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; min-height: 14px; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We present results on the structure and stability of steady states. We shall show that stable stationary states of regular interaction potentials generically consist of sums of Dirac masses. However the amount of Diracs depends delicately on the interplay between local repulsion and aggregation. In particular we shall see that singular repulsive interaction potentials introduce diffusive effects in the sense that stationary state are rendered continuously.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p&gt;&lt;/p&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;div style="text-align: center;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style=" font-style: normal;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Thomas Hillen&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style=" font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(University of Alberta, Canada)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style=" font-style: normal;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span" style="font-style: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Pointwise weak steady states of transport equations for cell movement in network tissue&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style=" font-style: normal;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(joint work with K. Painter (Heriot-Watt), P. Hinow (Milwaukee) and Z.A. Wang (Vanderbilt))&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style=" font-style: normal;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:black;"&gt;&lt;span class="Apple-style-span" style="font-style: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Some metastatic cancer cells use an interesting mechanism to move through network tissue, such as collagen networks. I will present a transport equation model, which describes the movement of these cells along network fibers and the network degradation due to proteolytic enzymes which are produced by the cells. In numerical implementation we find that the resulting models shows generation of networks which resemble vasculature formation. We believe that pointwise weak steady states are the organizing centres behind these network patterns. I will introduce the notion of pointwise weak steady states and discuss their use to understand network formation.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style=" font-style: normal;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Pierre-Emmanuel Jabin&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Université de Nice Sophia-Antipolis, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;S&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;election-mutation dynamics for the evolution of traits in a population&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;This talk aims at introducing some models describing the evolution of a large population of individuals with different biological "traits". The reproduction rate of each individual depends on its trait and on the competition for ressources within the population. In addition mutations may be included, enabling new traits to develop. These models leads to difficult asymptotic problems as the time scale of the mutations is usually much larger than the time scale of births and death. One such asymptotic will in particular be investigated, corresponding to frequent small mutations.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;______________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;b&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Doron Levy&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;University of Maryland, USA&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="font-style: normal;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Group Dynamics in Phototaxis&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="color:#cc0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Microbes live in environments that are often limiting for growth. They have evolved sophisticated mechanisms to sense changes in environmental parameters such as light and nutrients, after which they swim or crawl into optimal conditions. This phenomenon is known as "chemotaxis" or "phototaxis." Using time-lapse video microscopy we have monitored the movement of phototactic bacteria, i.e., bacteria that move towards light. These movies suggest that single cells are able to move directionally but at the same time, the group dynamics is equally important. Following these observations, in this talk we will present a hierarchy of mathematical models for phototaxis: a stochastic model, an interacting particle system, and a system of PDEs. We will discuss the models, their simulations, and our theorems that show how the system of PDEs can be considered as the limit dynamics of the particle system. Time-permitting, we will overview our recent results on particle, kinetic, and fluid models for phototaxis. This is a joint work with Devaki Bhaya (Department of Plant Biology, Carnegie Institute), Tiago Requeijo (Math, Stanford), and Seung-Yeal Ha (Seoul, Korea).&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;_____________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;b&gt;&lt;span class="Apple-style-span" style="font-weight: normal;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;"&gt;&lt;div style="text-align: justify;"&gt;&lt;div&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Sébastien Martin&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Université Paris-Sud 11, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Modelling of air flows and gas exchange in the human lung&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;This talk aims at describing some models of the respiratory system. The mechanical response of the lung can be described by either sophisticated models based on (Navier-)Stokes flows or simple mass-spring models, that are accurate enough to predict the behaviour of the system during a complex dynamical situation (the forced inspiratory-expiratory maneuver that is performed during spirometric evaluations). Oxygen absorption models are also described in order to observe the effects of changes in the parameters of the mechanical model in the efficiency of the lung. In particular, the models suggest that the airway smooth muscle (which is directly related to the bronchial rigidity) could have a structural function, to confer transport optimized mechanical properties to the bronchial tree.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;_&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Nicolas Meunier&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Université Paris V, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:17px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Analysis of self-organization systems for cell polarization&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:17px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Joint work with V. Calvez and R. Voituriez)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;I&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;n this work, we investigate the dynamics of a modified Keller-Segel type model. On the contrary to the classical configuration, the chemical production term is located on the boundary. In the one- dimensional case and in a particular case in dimension two, we prove, under suitable assumptions, the following dichotomy which is reminiscent of the two-dimensional Keller-Segel system. Solutions are global if the mass is below the critical mass and they blow-up in finite time above the critical mass. Furthermore, in the one-dimensional case, using entropy techniques, we provide quantitative convergence results for the subcritical case. This work is completed with a more realistic model (still one-dimensional) for modeling purpose. In this new setting, the chemical is supplied by a quantity which evolves by exchanging particles at the boundary. Finally some results are given for the two-dimensional case and we also provide some links with cell polarisation that is an essential step for many biological processes and that is involved for instance in cell migration, division, or morphogenesis.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;______________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Julie Mitchell&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;University of Wisconsin - Madison, USA&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style=" line-height: 26px;color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Using clustering and optimization in flexible protein docking&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Modeling molecular flexibility continues to be a frontier in predicting how two proteins bind. Allowing full dynamic flexibility can be excessive, yet neither traditional rigid body docking nor small-scale rearrangements of amino acid side chains can capture many biologically relevant motions. We propose an intermediate approach, which is to combine rigid optimization with discrete deformations that represent a protein's ``natural'' motions. Through exhaustive low-resolution search, hierarchical clustering, and global optimization within each energy basin, we are able to achieve accurate docking predictions. Our optimization approach employs a Convex Global Underestimation method that has been adapted for energy functions defined on $R^3 \times SO(3)$.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;_________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Gael Raoul&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(ENS-Cachan, France)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Kimura's model: An integro-differential model to study evolution&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;/span&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Kimura's model is a simple intero-differential model used by theoretical biologists to study evolution. Simulations for this model can be run, and they show that that the population usually converges to a finite sum of Dirac Masses. This phenomenon is interpreted by biologists as a speciation process. We study the stability of such populations, and link our results to other existing theories used by biologists to study evolution.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Christian Schmeiser&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(University of Vienna, Austria)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div style="font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Nonlinear friction in the cytoskeleton as a macroscopic limit of&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;the activity of cytoskeletal proteins&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The mechanical stability of polymer networks in the cytoskeleton relies on the action of cross-linking proteins and transmembrane proteins creating adhesion to the substrate. It will be demonstrated that their averaged effect can be described as friction, when cross-linking and adhesion molecules are assumed as elastic and when their building and breaking are described as stochastic processes.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;__________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Alexandre Vidal&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Université d'Evry Val d'Essonne, France)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: center;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="color:#cc0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;A model of the Gonadotropin Releasing Hormone secretion by hypothalamic neuron clusters&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The secretion of Gonadotropin Releasing Hormone (GnRH) by specific hypothalamic neurons plays a major role in the neuroendocrine control of the reproduction function in mammals. While the qualitative properties of the physiological secretion pattern is common to all females, the quantitative properties characterize the specificities of the ovulatory cycle in each species. The difficulty to obtain in vivo time series of GnRH release by the hypothalamus spurs us on to develop a controllable model to study this complex biological system.&lt;br /&gt;&lt;br /&gt;I will describe the qualitative properties of the physiological GnRH secretion pattern and introduce the types of specifications that the biological knowledge can specify in various species. I will present a model of the GnRH neuron secreting activities based on reaction-diffusion coupling of fast-slow oscillators. Applying bifurcation theory and a fast-slow analysis to a reduced model, I will show the model ability to reproduce the qualitative and species-dependent quantitative properties of the GnRH secretion pattern. Finally, I will display and discuss the synchronization/desynchronization alternation of the cluster activities reproducing subtle observable features but biologically misunderstood.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style="  font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;b&gt;&lt;span style="font-weight: normal;"&gt;&lt;span style="color:#333333;"&gt;&lt;span style="color:black;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;________________________________________________________&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5611787300989560569?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5611787300989560569/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/session-mathematical-biology.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5611787300989560569'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5611787300989560569'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/session-mathematical-biology.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-2197411632372001446</id><published>2008-01-09T03:45:00.000-08:00</published><updated>2010-01-13T06:52:43.377-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;Marie Doumic-Jauffret&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;(INRIA, France)&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Aggregation/fragmentation models for protein polymerization&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style=" ;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;i&gt;&lt;br /&gt;&lt;/i&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style=" ;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;span style=" ;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;i&gt;&lt;/i&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span style=" ;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;i&gt;&lt;span style="color:black;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Abnormal protein polymerization is at the origin of a number of neuro-degenerative diseases, e.g. Prion (Madcow), Huntington or Alzheimer diseases. This phenomenon can be described mathematically either in a discrete or in a continuous setting, by equations of fragmentation-coagulation type. We review here some results and some open problems on the study of prion proliferation equations.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;span style=" ;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;i&gt;&lt;/i&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style=" ;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;br /&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-2197411632372001446?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/2197411632372001446/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/marie-doumic-aggregationfragmentation.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2197411632372001446'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2197411632372001446'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/marie-doumic-aggregationfragmentation.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-3588587324673060985</id><published>2008-01-09T03:25:00.000-08:00</published><updated>2010-01-13T06:54:03.352-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;Laurent Dumas&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;(Université Paris VI, Frane)&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="line-height: 26px;"&gt;&lt;span style=" line-height: normal;color:#cc0000;"&gt;&lt;i&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;A numerical simulation of the human arterial network based on non invasive measurements&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;The numerical simulation of the human arterial network of a given patient in order to find the main characteristics of its arteries and thus to prevent from cardiovascular diseases is a major subject of interest. A simple fluid-structure interaction model for the simulation of blood flow in arteries is studied here. Derived from the general 3D equations, it computes the section area of the artery and the volumetric flux of the flow for each longitudinal position and time. The inverse problem corresponding to the identification of the main parameters of this model is successfully solved by using a reduced number of non invasive measurements. A discussion on the amount of information needed is in particular studied. Some first results based on experimental measurements with a Doppler technique called echotracking are also presented.&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-3588587324673060985?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/3588587324673060985/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/laurent-dumas-numerical-simulation-of.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3588587324673060985'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3588587324673060985'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/laurent-dumas-numerical-simulation-of.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5520384971797487653</id><published>2007-12-23T14:54:00.000-08:00</published><updated>2010-01-09T03:59:16.724-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;b&gt;Christian Schmeiser&lt;/b&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;(University of Vienna, Austria)&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Nonlinear friction in the cytoskeleton as a macroscopic limit of&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;   the activity of cytoskeletal proteins&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;br /&gt;&lt;span class="Apple-style-span"   style="font-family:Georgia, serif;color:#000000;"&gt;&lt;span class="Apple-style-span" style="font-style: normal;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="color:black;"&gt;&lt;span style="font-size:medium;"&gt;The mechanical stability of polymer networks in the cytoskeleton relies on the action of cross-linking proteins and transmembrane proteins creating adhesion to the substrate. It will be demonstrated that their averaged effect can be described as friction, when cross-linking and adhesion molecules are assumed as elastic and when their building and breaking are described as stochastic processes.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="color:#cc0000;"&gt;&lt;i&gt;&lt;br /&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;span style="color:#cc0000;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;span style="font-family:'times new roman',serif;"&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5520384971797487653?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5520384971797487653/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/christian-schmeiser-nonlinear-friction.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5520384971797487653'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5520384971797487653'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/christian-schmeiser-nonlinear-friction.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-672626405180328755</id><published>2007-12-19T15:08:00.000-08:00</published><updated>2010-01-20T12:48:10.703-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Maria Rita D'Orsigna&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;(&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;California State University at Northridge, Los Angeles, USA&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style=" font-style: italic; line-height: 26px;color:#cc0000;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Modelling viral entry dynamics&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span" style="line-height: 26px;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Successful viral infection of a healthy cell requires complex host-pathogen interactions. In this talk we focus on the dynamics specific to the HIV virus entering a eucaryotic cell.  We model viral entry as a stochastic engagement of receptors and coreceptors on the cell surface. We also consider the transport of virus material to the cell nucleus by coupling microtubular motion to the concurrent biochemical transformations that render the viral material competent for nuclear entry. We discuss both mathematical and biological consequences of our model, such as the formulation of an effective integrodifferential boundary condition embodying a memory kernel and optimal timing in maximizing viral probabilities.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-672626405180328755?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/672626405180328755/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/maria-rita-dorsigna-california-state.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/672626405180328755'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/672626405180328755'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/maria-rita-dorsigna-california-state.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-2407562916748293232</id><published>2007-12-19T15:01:00.000-08:00</published><updated>2010-01-09T03:59:37.047-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;Doron Levy&lt;/b&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;(&lt;/span&gt;&lt;/span&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;University of Maryland, USA&lt;/span&gt;&lt;/span&gt;&lt;span style="font-size:medium;"&gt;&lt;span style="font-family:'times new roman';"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;&lt;i&gt;&lt;span style="color:#cc0000;"&gt;Group Dynamics in Phototaxis&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div face="Helvetica" size="12px" style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px;"&gt;&lt;br /&gt;&lt;/div&gt;&lt;div   style=" font-size-adjust: none;  font-stretch: normal; font-style: normal; font-variant: normal; font-weight: normal; line-height: normal; margin: 0px; text-align: justify;font-family:Helvetica;font-size:12px;"&gt;&lt;span style="font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;span style="color:black;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;Microbes live in environments that are often limiting for growth. They have evolved sophisticated mechanisms to sense changes in environmental parameters such as light and nutrients, after which they swim or crawl into optimal conditions. This phenomenon is known as "chemotaxis" or "phototaxis."  Using time-lapse video microscopy we have monitored the movement of phototactic bacteria, i.e., bacteria that move towards light. These movies suggest that single cells are able to move directionally but at the same time, the group dynamics is equally important.   Following these observations, in this talk we will present a hierarchy of mathematical models for phototaxis: a stochastic model, an interacting particle system, and a system of PDEs.  We will discuss the models, their simulations, and our theorems that show how the system of PDEs can be considered as the limit dynamics of the particle system.  Time-permitting, we will overview our recent results on particle, kinetic, and fluid models for phototaxis.  This is a joint work with Devaki Bhaya (Department of Plant Biology, Carnegie Institute), Tiago Requeijo (Math, Stanford), and Seung-Yeal Ha (Seoul, Korea).&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;span style=" ;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;i&gt;&lt;/i&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-2407562916748293232?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/2407562916748293232/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/doron-levy-university-of-maryland-usa.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2407562916748293232'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2407562916748293232'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/doron-levy-university-of-maryland-usa.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5674214486875250095</id><published>2007-12-19T14:46:00.000-08:00</published><updated>2010-02-01T13:47:32.467-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Peter &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;span style="line-height: 26px;"&gt;&lt;b&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Markowich&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(University of Cambridge, UK &amp;amp; University of Vienna, Austria)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span" style="color: rgb(0, 0, 0); font-style: normal; "&gt;&lt;div&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;On PDE Models for (some) Socio-Economic Problems: &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/div&gt;&lt;div&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Price Formation, Opinion Formation and Crowd Modeling&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/div&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We present and analyse partial differential equation models in the socio-economic sciences:&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;1) a highly nonstandard free boundary problem in price formation &lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;2) a Boltzmann equation for opinion formation in human societies with strong leaders&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;3) a  continuity equation with an eikonal field equation coupling.&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;/div&gt;&lt;div&gt;&lt;span&gt;&lt;span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;span&gt;&lt;span style=" ;font-family:Helvetica;font-size:medium;"&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5674214486875250095?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5674214486875250095/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/peter-markowich-university-of-cambridge.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5674214486875250095'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5674214486875250095'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/peter-markowich-university-of-cambridge.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5141167702650032049</id><published>2007-12-15T13:54:00.000-08:00</published><updated>2010-01-09T09:18:22.147-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-weight: bold;"&gt;Julie Mitchell&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="font-size:medium;"&gt;(&lt;/span&gt;&lt;span style="font-family:Helvetica,serif;"&gt;&lt;span style="font-family:'times new roman';"&gt;&lt;span style="font-size:medium;"&gt;University of Wisconsin - Madison, USA&lt;/span&gt;&lt;/span&gt;&lt;span style="font-family:Georgia,serif;"&gt;&lt;span style="font-size:medium;"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;br /&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span style="  font-style: italic; line-height: 26px;font-family:'times new roman',serif;color:#cc0000;"&gt;&lt;span style="font-size:medium;"&gt;Using clustering and optimization in flexible protein docking&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span" style="line-height: 26px;"&gt;&lt;span class="Apple-style-span"  style="font-family:Georgia, serif;"&gt;&lt;span class="Apple-style-span" style="line-height: normal;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span" style="font-size: medium;"&gt;Modeling molecular flexibility continues to be a frontier in predicting how two proteins bind. Allowing full dynamic flexibility can be excessive, yet neither traditional rigid body docking nor small-scale rearrangements of amino acid side chains can capture many biologically relevant motions. We propose an intermediate approach, which is to combine rigid optimization with discrete deformations that represent a protein's ``natural'' motions. Through exhaustive low-resolution search, hierarchical clustering, and global optimization within each energy basin, we are able to achieve accurate docking predictions.  Our optimization approach employs a Convex Global Underestimation method that has been adapted for energy functions defined on $R^3 \times SO(3)$.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5141167702650032049?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5141167702650032049/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/julie-mitchell.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5141167702650032049'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5141167702650032049'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2009/12/julie-mitchell.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-5308968373440928606</id><published>2007-02-01T00:54:00.000-08:00</published><updated>2010-02-01T01:00:57.632-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Alexandre Vidal&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Université d'Evry Val d'Essonne, France)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;i&gt;A model of the Gonadotropin Releasing Hormone secretion by hypothalamic neuron clusters&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: justify;"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span" style="color: rgb(0, 0, 0); "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The secretion of Gonadotropin Releasing Hormone (GnRH) by specific hypothalamic neurons plays a major role in the neuroendocrine control of the reproduction function in mammals. While the qualitative properties of the physiological secretion pattern is common to all females, the quantitative properties characterize the specificities of the ovulatory cycle in each species. The difficulty to obtain in vivo time series of GnRH release by the hypothalamus spurs us on to develop a controllable model to study this complex biological system.&lt;br /&gt;&lt;br /&gt;I will describe the qualitative properties of the physiological GnRH secretion pattern and introduce the types of specifications that the biological knowledge can specify in various species. I will present a model of the GnRH neuron secreting activities based on reaction-diffusion coupling of fast-slow oscillators. Applying bifurcation theory and a fast-slow analysis to a reduced model, I will show the model ability to reproduce the qualitative and species-dependent quantitative properties of the GnRH secretion pattern. Finally, I will display and discuss the synchronization/desynchronization alternation of the cluster activities reproducing subtle observable features but biologically misunderstood.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-5308968373440928606?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/5308968373440928606/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/02/alexandre-vidal-universite-devry-val.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5308968373440928606'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/5308968373440928606'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/02/alexandre-vidal-universite-devry-val.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-3479450685210598005</id><published>2007-01-20T13:03:00.000-08:00</published><updated>2010-01-20T13:11:54.870-08:00</updated><title type='text'></title><content type='html'>&lt;div&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Marc Thiriet&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(CNRS, Université P. et M. Curie and INRIA &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Rocquencourt, France&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Lecture 1 :  &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-weight: normal; "&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Physiological flows -- a macroscopic point of view with application to blood circulation and body's ventilation.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/b&gt;&lt;/p&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;- Basic equations: mass and momentum conservation (Navier-Stokes equations).&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: left;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;- Main features: unsteady, developing, three-dimensional flows of Newtonian or non-Newtonian fluid in deformable pipes (distensible and collapsible ducts).&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; min-height: 14px; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Lecture 2 : &lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span" style="font-weight: normal; "&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Physiological flows -- a nano/microscopic point of view. &lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/b&gt;&lt;/p&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Biological conduit walls are living tissues that react to the stress field applied to them by flowing fluid (mechanotransduction) and adapt vessel lumen size accordingly. Additional behavioral equation must be coupled to correct the computational domain size predicted by the Navier-Stokes solution.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;br /&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-3479450685210598005?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/3479450685210598005/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/marc-thiriet-cnrs-universite-p.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3479450685210598005'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3479450685210598005'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/marc-thiriet-cnrs-universite-p.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-2581185010602964915</id><published>2007-01-17T05:34:00.000-08:00</published><updated>2010-01-17T05:46:57.345-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;b&gt;&lt;br /&gt;&lt;/b&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Sébastien Martin&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(Université Paris-Sud 11, France)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Modelling of air flows and gas exchange in the human lung&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;i&gt;&lt;/i&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="color:#000000;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;This talk aims at describing some models of the respiratory system. The mechanical response of the lung can be described by either sophisticated models based on (Navier-)Stokes flows or simple mass-spring models, that are accurate enough to predict the behaviour of the system during a complex dynamical situation (the forced inspiratory-expiratory maneuver that is performed during spirometric evaluations). Oxygen absorption models are also described in order to observe the effects of changes in the parameters of the mechanical model in the efficiency of the lung. In particular, the models suggest that the airway smooth muscle (which is directly related to the bronchial rigidity) could have a structural function, to confer transport optimized mechanical properties to the bronchial tree.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;/i&gt;&lt;/span&gt;&lt;p&gt;&lt;/p&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-2581185010602964915?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/2581185010602964915/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/sebastien-martin-modelling-of-air-flows.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2581185010602964915'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/2581185010602964915'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/sebastien-martin-modelling-of-air-flows.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-4022829515660376570</id><published>2006-01-13T12:34:00.000-08:00</published><updated>2010-01-13T12:56:49.358-08:00</updated><title type='text'></title><content type='html'>&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;Gael Raoul&lt;/span&gt;&lt;/span&gt;&lt;/b&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;(ENS-Cachan, France)&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div style="text-align: center;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;Kimura's model: An integro-differential model to study evolution&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px Helvetica"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;&lt;i&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;Kimura's model is a simple intero-differential model used by theoretical biologists to study evolution. Simulations for this model can be run, and they show that that the population usually converges to a finite sum of Dirac Masses. This phenomenon is interpreted by biologists as a speciation process. We study the stability of such populations, and link our results to other existing theories used by biologists to study evolution.&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;/span&gt;&lt;/span&gt;&lt;/div&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-4022829515660376570?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/4022829515660376570/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/gael-raoul-ens-cachan-france-kimuras.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4022829515660376570'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/4022829515660376570'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/gael-raoul-ens-cachan-france-kimuras.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry><entry><id>tag:blogger.com,1999:blog-3975242521993377304.post-3627318212171860902</id><published>2006-01-13T12:17:00.000-08:00</published><updated>2010-01-13T12:57:18.242-08:00</updated><title type='text'></title><content type='html'>&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;b&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Benoît Perthame&lt;/span&gt;&lt;/b&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;(&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;Université P. et M.  Curie, INRIA-Rocquencourt and Institut Universitaire de France, France&lt;/span&gt;&lt;/span&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;)&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: center;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;span class="Apple-style-span"  style="color:#CC0000;"&gt;Adaptive evolution: a population view&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman', serif;"&gt;&lt;span class="Apple-style-span"  style=" ;font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;The two processes of mutations and selection, proposed by C. Darwin, can be written in mathematical words. In a very simple,  general and idealized description, the  environment can be considered as a nutrient shared by all the population. This  alllows  certain individuals, characterized by a 'phenotypical trait', to multiply faster because they are better adapted to use the environment.  This leads to select the 'fittest trait' in the population.  On the other hand, the new-born individuals undergo small variations of  the trait under the effect of mutations. In these circumstances, is it possible to observ 'speciation' and to describe the dynamical evolution of the 'fittest' traits?&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; min-height: 14px; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;We will give a class of self-contained mathematical models of such population dynamics and show that an asymptotic view allows us to formalize precisely the concepts of monomorphic or polymorphic populations. We can describe the evolution of the 'fittest traits' and various forms of branching points. We will also show that numerical solutions are consistant with individual based stochastic simulations. &lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; min-height: 14px; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;&lt;br /&gt;&lt;/span&gt;&lt;/span&gt;&lt;/p&gt; &lt;p style="text-align: justify;margin-top: 0px; margin-right: 0px; margin-bottom: 0px; margin-left: 0px; font: normal normal normal 12px/normal Helvetica; "&gt;&lt;span class="Apple-style-span"  style="font-family:'times new roman';"&gt;&lt;span class="Apple-style-span"  style="font-size:medium;"&gt;Eventhough the model is very simple, its analysis relates to remarkable recent progresses of nonlinear analysis. &lt;/span&gt;&lt;/span&gt;&lt;/p&gt;&lt;div class="blogger-post-footer"&gt;&lt;img width='1' height='1' src='https://blogger.googleusercontent.com/tracker/3975242521993377304-3627318212171860902?l=icor2010pde.blogspot.com' alt='' /&gt;&lt;/div&gt;</content><link rel='replies' type='application/atom+xml' href='http://icor2010pde.blogspot.com/feeds/3627318212171860902/comments/default' title='Post Comments'/><link rel='replies' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/benoit-perthame-universite-p.html#comment-form' title='0 Comments'/><link rel='edit' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3627318212171860902'/><link rel='self' type='application/atom+xml' href='http://www.blogger.com/feeds/3975242521993377304/posts/default/3627318212171860902'/><link rel='alternate' type='text/html' href='http://icor2010pde.blogspot.com/2010/01/benoit-perthame-universite-p.html' title=''/><author><name>Stéphane</name><uri>http://www.blogger.com/profile/04486306289362065219</uri><email>noreply@blogger.com</email><gd:image rel='http://schemas.google.com/g/2005#thumbnail' width='16' height='16' src='http://img2.blogblog.com/img/b16-rounded.gif'/></author><thr:total>0</thr:total></entry></feed>
