{"id":203,"date":"2017-11-28T15:50:20","date_gmt":"2017-11-28T14:50:20","guid":{"rendered":"https:\/\/project.inria.fr\/bendali\/?page_id=203"},"modified":"2017-11-28T15:50:20","modified_gmt":"2017-11-28T14:50:20","slug":"pernet","status":"publish","type":"page","link":"https:\/\/project.inria.fr\/bendali\/program\/pernet\/","title":{"rendered":"S\u00e9bastien Pernet"},"content":{"rendered":"<p>ONERA<\/p>\n<h2>A posteriori error estimates for EFIE in electromagnetism<\/h2>\n<p>We present a localization technique which allows to construct a reliable, efficient and local a posteriori error estimate for the Electric Field Integral Equation (EFIE). This one is based on the choice of a generic operator which is used to transport the residual into L2 -type space.  Under appropriate conditions on the construction of this operator, we show that it is asymptotically exact with respect to an energy norm of the error.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>ONERA A posteriori error estimates for EFIE in electromagnetism We present a localization technique which allows to construct a reliable, efficient and local a posteriori error estimate for the Electric Field Integral Equation (EFIE). This one is based on the choice of a generic operator which is used to transport\u2026<\/p>\n<p> <a class=\"continue-reading-link\" href=\"https:\/\/project.inria.fr\/bendali\/program\/pernet\/\"><span>Continue reading<\/span><i class=\"crycon-right-dir\"><\/i><\/a> <\/p>\n","protected":false},"author":248,"featured_media":0,"parent":68,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-203","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/203","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/users\/248"}],"replies":[{"embeddable":true,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/comments?post=203"}],"version-history":[{"count":2,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/203\/revisions"}],"predecessor-version":[{"id":205,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/203\/revisions\/205"}],"up":[{"embeddable":true,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/68"}],"wp:attachment":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/media?parent=203"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}