{"id":1526,"date":"2023-06-01T14:55:50","date_gmt":"2023-06-01T06:55:50","guid":{"rendered":"https:\/\/blog.vanabel.cn\/?p=1526"},"modified":"2023-06-01T14:55:50","modified_gmt":"2023-06-01T06:55:50","slug":"the-geometry-of-phi_3-harmonic-maps","status":"publish","type":"post","link":"https:\/\/blog.vanabel.cn\/?p=1526","title":{"rendered":"The geometry of $\\Phi_{(3)}$-harmonic maps"},"content":{"rendered":"<p>Title: The geometry of $\\Phi_{(3)}$-harmonic maps<br \/>\nAuthors: Shuxiang Feng, Yingbo Han, Kaige Jiang and Shihshu Walter Wei<br \/>\nCategories: math.DG math-ph math.AP math.MP<br \/>\nComments: 46 pages, to appear in Nonlinear Analysis (2023). arXiv admin note:<br \/>\n text overlap with arXiv:1911.05855<br \/>\nMSC-class: 58E20, 53C21, 53C25<br \/>\n\\\\<br \/>\n In this paper, we motivate and extend the study of harmonic maps or<br \/>\n$\\Phi_{(1)}$-harmonic maps (cf [15], Remark 1.3 (iii)), $\\Phi$-harmonic maps or<br \/>\n$\\Phi_{(2)}$-harmonic maps (cf. [24], Remark 1.3 (v)), and explore geometric<br \/>\nproperties of $\\Phi_{(3)}$-harmonic maps by unified geometric analytic methods.<br \/>\nWe define the notion of $\\Phi_{(3)}$-harmonic maps and obtain the first<br \/>\nvariation formula and the second variation formula of the $\\Phi_{(3)}$-energy<br \/>\nfunctional $E_{\\Phi_{(3)}}$. By using a stress-energy tensor, the<br \/>\n$\\Phi_{(3)}$-conservation law, a monotonicity formula, and the asymptotic<br \/>\nassumption of maps at infinity, we prove Liouville type results for<br \/>\n$\\Phi_{(3)}$-harmonic maps. We introduce the notion of<br \/>\n$\\Phi_{(3)}$-Superstrongly Unstable ($\\Phi_{(3)}$-SSU) manifold and provide<br \/>\nmany interesting examples. By using an extrinsic average variational method in<br \/>\nthe calculus of variations (cf. [51, 49]), we find $\\Phi_{(3)}$-SSU manifold<br \/>\nand prove that for $i=1,2,3$, every compact $\\Phi_{(i)}$-$\\operatorname{SSU}$<br \/>\nmanifold is $\\Phi_{(i)}$-$\\operatorname{SU}$, and hence is<br \/>\n$\\Phi_{(i)}$-$\\operatorname{U}$ (cf. Theorem 9.3). As consequences, we obtain<br \/>\ntopological vanishing theorems and sphere theorems by employing a<br \/>\n$\\Phi_{(3)}$-harmoic map as a catalyst. This is in contrast to the approaches<br \/>\nof utilizing a geodesic ([45]), minimal surface, stable rectifiable current<br \/>\n([34, 29, 50]), $p$-harmonic map (cf. [53]), etc., as catalysts. These<br \/>\nmysterious phenomena are analogs of harmonic maps or $\\Phi_{(1)}$-harmonic<br \/>\nmaps, $p$-harmonic maps, $\\Phi_{S}$-harmonic maps, $\\Phi_{S,p}$-harmonic maps,<br \/>\n$\\Phi_{(2)}$-harmonic maps, etc., (cf. [21, 40, 42, 41, 12, 13]).<br \/>\n\\\\ ( https:\/\/arxiv.org\/abs\/2305.19503 ,  30kb)<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Title: The geometry of $\\Phi_{(3)}$-harmonic maps Autho&hellip; <a class=\"more-link\" href=\"https:\/\/blog.vanabel.cn\/?p=1526\">\u7ee7\u7eed\u9605\u8bfb<span class=\"screen-reader-text\">The geometry of $\\Phi_{(3)}$-harmonic maps<\/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":[280,276,283,277,281,234,230,278,285,279,284,282],"class_list":["post-1526","post","type-post","status-publish","format-standard","hentry","category-arxiv","tag-phi_3-conservation-law","tag-phi_3-harmonic-maps","tag-extrinsic-average-variational-method","tag-first-variation-formula","tag-liouville-type","tag-monotonicity-formula","tag-mustread","tag-second-variation-formula","tag-sphere-theorems","tag-stress-energy-tensor","tag-topological-vanishing-theorems","tag-unstable-manifolds","entry"],"_links":{"self":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/1526","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=1526"}],"version-history":[{"count":1,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/1526\/revisions"}],"predecessor-version":[{"id":1527,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/1526\/revisions\/1527"}],"wp:attachment":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1526"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=1526"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=1526"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}