{"id":1684,"date":"2023-06-08T16:33:50","date_gmt":"2023-06-08T08:33:50","guid":{"rendered":"https:\/\/blog.vanabel.cn\/?p=1684"},"modified":"2023-06-08T16:33:50","modified_gmt":"2023-06-08T08:33:50","slug":"morse-index-stability-of-willmore-immersions-i","status":"publish","type":"post","link":"https:\/\/blog.vanabel.cn\/?p=1684","title":{"rendered":"Morse Index Stability of Willmore Immersions I"},"content":{"rendered":"<p>Title: Morse Index Stability of Willmore Immersions I<br \/>\nAuthors: Alexis Michelat and Tristan Rivi\\`ere<br \/>\nCategories: math.DG math.AP<br \/>\nComments: 96 pages<br \/>\nMSC-class: 35J35, 35J48, 35R01, 49Q10, 53A05, 53A10, 53A30, 53C42<br \/>\n\\\\<br \/>\n In a recent work, F. Da Lio, M. Gianocca, and T. Rivi\\`ere developped a new<br \/>\nmethod to show upper semi-continuity results in geometric analysis, which they<br \/>\napplied to conformally invariant Lagrangians in dimension $2$ (that include<br \/>\nharmonic maps). In this article, we apply this method to show that the sum of<br \/>\nthe Morse index and the nullity of Willmore immersions is upper<br \/>\nsemi-continuous, provided that the limiting immersions and the bubbles are free<br \/>\nof branch points. Our result covers the case of degenerating Riemann surfaces<br \/>\nfor which the ratio of the second residue (considered by P. Laurain and T.<br \/>\nRivi\\`ere in their work on the energy quantization of Willmore surfaces) and<br \/>\nthe length of the minimal shrinking geodesic of the underlying sequence of<br \/>\nRiemann surfaces is smaller than a universal constant.<br \/>\n\\\\ ( https:\/\/arxiv.org\/abs\/2306.04608 ,  68kb)<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Title: Morse Index Stability of Willmore Immersions I A&hellip; <a class=\"more-link\" href=\"https:\/\/blog.vanabel.cn\/?p=1684\">\u7ee7\u7eed\u9605\u8bfb<span class=\"screen-reader-text\">Morse Index Stability of Willmore Immersions I<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[248],"tags":[304,303,300,227,301,299,302],"class_list":["post-1684","post","type-post","status-publish","format-standard","hentry","category-arxiv","tag-branch-points","tag-bubbles","tag-conformally-invariant-lagrangians","tag-harmonic-maps","tag-morse-index","tag-upper-semi-continuity-results","tag-willmore-immersions","entry"],"_links":{"self":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/1684","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=1684"}],"version-history":[{"count":1,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/1684\/revisions"}],"predecessor-version":[{"id":1685,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/1684\/revisions\/1685"}],"wp:attachment":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1684"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=1684"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=1684"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}