{"title":"Counterexamples to the comparison principle in the special Lagrangian potential equation","authors":"Karl K. Brustad","doi":"10.1007/s00526-024-02747-z","DOIUrl":null,"url":null,"abstract":"<p>For each <span>\\(k = 0,\\dots ,n\\)</span> we construct a continuous <i>phase</i> <span>\\(f_k\\)</span>, with <span>\\(f_k(0) = (n-2k)\\frac{\\pi }{2}\\)</span>, and viscosity sub- and supersolutions <span>\\(v_k\\)</span>, <span>\\(u_k\\)</span>, of the elliptic PDE <span>\\(\\sum _{i=1}^n \\arctan (\\lambda _i(\\mathcal {H}w)) = f_k(x)\\)</span> such that <span>\\(v_k-u_k\\)</span> has an isolated maximum at the origin. It has been an open question whether the comparison principle would hold in this second order equation for arbitrary continuous phases <span>\\(f:\\mathbb {R}^n\\supseteq \\Omega \\rightarrow (-n\\pi /2,n\\pi /2)\\)</span>. Our examples show it does not.\n</p>","PeriodicalId":2,"journal":{"name":"ACS Applied Bio Materials","volume":null,"pages":null},"PeriodicalIF":4.6000,"publicationDate":"2024-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Bio Materials","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1007/s00526-024-02747-z","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, BIOMATERIALS","Score":null,"Total":0}
引用次数: 0
Abstract
For each \(k = 0,\dots ,n\) we construct a continuous phase\(f_k\), with \(f_k(0) = (n-2k)\frac{\pi }{2}\), and viscosity sub- and supersolutions \(v_k\), \(u_k\), of the elliptic PDE \(\sum _{i=1}^n \arctan (\lambda _i(\mathcal {H}w)) = f_k(x)\) such that \(v_k-u_k\) has an isolated maximum at the origin. It has been an open question whether the comparison principle would hold in this second order equation for arbitrary continuous phases \(f:\mathbb {R}^n\supseteq \Omega \rightarrow (-n\pi /2,n\pi /2)\). Our examples show it does not.
对于每一个(k = 0,dots,n),我们构建一个连续相(f_k\ ),其中(f_k(0) = (n-2k)\frac\{pi }{2}\),以及粘度子溶体和超溶体(v_k\ )、\(u_k\), of the elliptic PDE \(\sum _{i=1}^n \arctan (\lambda _i(\mathcal {H}w)) = f_k(x)\) such that \(v_k-u_k\) has an isolated maximum at the origin.对于任意连续相 \(f:\mathbb {R}^n\supseteq \Omega \rightarrow (-n\pi /2,n\pi /2)\),比较原则在这个二阶方程中是否成立一直是个悬而未决的问题。我们的例子表明并不是这样。