{"id":796,"date":"2020-02-09T22:35:16","date_gmt":"2020-02-10T06:35:16","guid":{"rendered":"https:\/\/math.berkeley.edu\/wp\/apde\/?p=796"},"modified":"2020-02-09T22:35:16","modified_gmt":"2020-02-10T06:35:16","slug":"johannes-sjostrand-imb","status":"publish","type":"post","link":"https:\/\/wp.math.berkeley.edu\/apde\/2020\/02\/09\/johannes-sjostrand-imb\/","title":{"rendered":"CANCELLED: Johannes Sj\u00f6strand (IMB)"},"content":{"rendered":"\n\t\t\t\t\n<p> The APDE seminar on Monday, 03\/16 will be given by Johannes Sj\u00f6strand in Evans 939 from 4:10 to 5pm. <\/p>\n\n\n\n<p>Title:  Resonances over a potential well in an island.<\/p>\n\n\n\n<p>Abstract:  Recent work with M. Zerzeri. Let V : R^n \u2192 R be a sufficiently analytic potential which tends to 0 at infinity. Assume that for an E &gt; 0 we have V^{-1}(]- &infin; ,E[)=U(E) &#8852; S(E), where <SPAN STYLE=\"text-decoration:overline\">U(E)<\/SPAN> &cap; <SPAN STYLE=\"text-decoration:overline\">S(E)<\/SPAN> =  &empty; , with U(E) connected and bounded (the well) and S(E) connected (the sea). The distribution of the resonances of -h^2 \u0394 + V near E has been thoroughly studied since more than 30 years. If we increase E a natural scenario is that the decomposition persists until the closures of U(E) and S(E) intersect at a critical energy E = E_0. Under some natural assumptions we show that near E_0 most of the resonances are close to the real axis and obey a Weyl law. In one dimension there are more detailed results (Fujiie-Ramond &#8217;98).<\/p>\n\t\t","protected":false},"excerpt":{"rendered":"<p>The APDE seminar on Monday, 03\/16 will be given by Johannes Sj\u00f6strand in Evans 939 from 4:10 to 5pm. Title: Resonances over a potential well in an island. Abstract: Recent work with M. Zerzeri. Let V : R^n \u2192 R be a sufficiently analytic potential which tends to 0 at infinity. Assume that for an [&hellip;]<\/p>\n","protected":false},"author":109,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-796","post","type-post","status-publish","format-standard","hentry","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/posts\/796","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/users\/109"}],"replies":[{"embeddable":true,"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/comments?post=796"}],"version-history":[{"count":0,"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/posts\/796\/revisions"}],"wp:attachment":[{"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/media?parent=796"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/categories?post=796"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/wp.math.berkeley.edu\/apde\/wp-json\/wp\/v2\/tags?post=796"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}