{"title":"Sign-changing solution for logarithmic elliptic equations with critical exponent","authors":"Tianhao Liu, Wenming Zou","doi":"10.1007/s00229-024-01535-5","DOIUrl":null,"url":null,"abstract":"<p>In this paper, we consider the logarithmic elliptic equations with critical exponent </p><span>$$\\begin{aligned} \\left\\{ \\begin{array}{ll} -\\Delta u=\\lambda u+ |u|^{2^*-2}u+\\theta u\\log u^2, \\\\ u \\in H_0^1(\\Omega ), \\quad \\Omega \\subset {{\\mathbb {R}}}^N. \\end{array}\\right. \\end{aligned}$$</span><p>Here, the parameters <span>\\(N\\ge 6\\)</span>, <span>\\(\\lambda \\in {{\\mathbb {R}}}\\)</span>, <span>\\(\\theta >0\\)</span> and <span>\\( 2^*=\\frac{2N}{N-2} \\)</span> is the Sobolev critical exponent. We prove the existence of a sign-changing solution with exactly two nodal domain for an arbitrary smooth bounded domain <span>\\(\\Omega \\subset {\\mathbb {R}}^{N}\\)</span>. When <span>\\(\\Omega =B_R(0)\\)</span> is a ball, we also construct infinitely many radial sign-changing solutions with alternating signs and prescribed nodal characteristic.\n</p>","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1007/s00229-024-01535-5","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In this paper, we consider the logarithmic elliptic equations with critical exponent
Here, the parameters \(N\ge 6\), \(\lambda \in {{\mathbb {R}}}\), \(\theta >0\) and \( 2^*=\frac{2N}{N-2} \) is the Sobolev critical exponent. We prove the existence of a sign-changing solution with exactly two nodal domain for an arbitrary smooth bounded domain \(\Omega \subset {\mathbb {R}}^{N}\). When \(\Omega =B_R(0)\) is a ball, we also construct infinitely many radial sign-changing solutions with alternating signs and prescribed nodal characteristic.