{"title":"特殊拉格朗日势能方程中比较原理的反例","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":9478,"journal":{"name":"Calculus of Variations and Partial Differential Equations","volume":"9 1","pages":""},"PeriodicalIF":2.1000,"publicationDate":"2024-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"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\":9478,\"journal\":{\"name\":\"Calculus of Variations and Partial Differential Equations\",\"volume\":\"9 1\",\"pages\":\"\"},\"PeriodicalIF\":2.1000,\"publicationDate\":\"2024-06-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Calculus of Variations and Partial Differential Equations\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.1007/s00526-024-02747-z\",\"RegionNum\":2,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Calculus of Variations and Partial Differential Equations","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1007/s00526-024-02747-z","RegionNum":2,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
引用次数: 0
摘要
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。
Counterexamples to the comparison principle in the special Lagrangian potential equation
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.
期刊介绍:
Calculus of variations and partial differential equations are classical, very active, closely related areas of mathematics, with important ramifications in differential geometry and mathematical physics. In the last four decades this subject has enjoyed a flourishing development worldwide, which is still continuing and extending to broader perspectives.
This journal will attract and collect many of the important top-quality contributions to this field of research, and stress the interactions between analysts, geometers, and physicists. The field of Calculus of Variations and Partial Differential Equations is extensive; nonetheless, the journal will be open to all interesting new developments. Topics to be covered include:
- Minimization problems for variational integrals, existence and regularity theory for minimizers and critical points, geometric measure theory
- Variational methods for partial differential equations, optimal mass transportation, linear and nonlinear eigenvalue problems
- Variational problems in differential and complex geometry
- Variational methods in global analysis and topology
- Dynamical systems, symplectic geometry, periodic solutions of Hamiltonian systems
- Variational methods in mathematical physics, nonlinear elasticity, asymptotic variational problems, homogenization, capillarity phenomena, free boundary problems and phase transitions
- Monge-Ampère equations and other fully nonlinear partial differential equations related to problems in differential geometry, complex geometry, and physics.