{"title":"中的三维不可压缩欧拉方程解的有限时间奇异性\\(\\:C^{\\infty}(\\mathbb{R}^3 \\setminus \\{0\\})\\cap C^{1,\\alpha}\\cap L^2\\)","authors":"Diego Córdoba, Luis Martinez-Zoroa, Fan Zheng","doi":"10.1007/s40818-025-00214-2","DOIUrl":null,"url":null,"abstract":"<div><p>We introduce a novel mechanism that reveals finite time singularities within the 1D De Gregorio model and the 3D incompressible Euler equations. Remarkably, we do not construct our blow up using self-similar coordinates, but build it from infinitely many regions with vorticity, separated by vortex-free regions in between. It yields solutions of the 3D incompressible Euler equations in <span>\\(\\mathbb{R}^3\\times [-T,0]\\)</span> such that the velocity is in the space <span>\\(C^{\\infty}(\\mathbb{R}^3 \\setminus \\{0\\})\\cap C^{1,\\alpha}\\cap L^2\\)</span> where <span>\\(0 < \\alpha \\ll 1\\)</span> for times <span>\\(t\\in (-T,0)\\)</span> and is not <span>\\(C^1\\)</span> at time 0.</p></div>","PeriodicalId":36382,"journal":{"name":"Annals of Pde","volume":"11 2","pages":""},"PeriodicalIF":2.6000,"publicationDate":"2025-07-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s40818-025-00214-2.pdf","citationCount":"0","resultStr":"{\"title\":\"Finite Time Singularities to the 3D Incompressible Euler Equations for Solutions in\\\\(\\\\:C^{\\\\infty}(\\\\mathbb{R}^3 \\\\setminus \\\\{0\\\\})\\\\cap C^{1,\\\\alpha}\\\\cap L^2\\\\)\",\"authors\":\"Diego Córdoba, Luis Martinez-Zoroa, Fan Zheng\",\"doi\":\"10.1007/s40818-025-00214-2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We introduce a novel mechanism that reveals finite time singularities within the 1D De Gregorio model and the 3D incompressible Euler equations. Remarkably, we do not construct our blow up using self-similar coordinates, but build it from infinitely many regions with vorticity, separated by vortex-free regions in between. It yields solutions of the 3D incompressible Euler equations in <span>\\\\(\\\\mathbb{R}^3\\\\times [-T,0]\\\\)</span> such that the velocity is in the space <span>\\\\(C^{\\\\infty}(\\\\mathbb{R}^3 \\\\setminus \\\\{0\\\\})\\\\cap C^{1,\\\\alpha}\\\\cap L^2\\\\)</span> where <span>\\\\(0 < \\\\alpha \\\\ll 1\\\\)</span> for times <span>\\\\(t\\\\in (-T,0)\\\\)</span> and is not <span>\\\\(C^1\\\\)</span> at time 0.</p></div>\",\"PeriodicalId\":36382,\"journal\":{\"name\":\"Annals of Pde\",\"volume\":\"11 2\",\"pages\":\"\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2025-07-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1007/s40818-025-00214-2.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Annals of Pde\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s40818-025-00214-2\",\"RegionNum\":1,\"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":"Annals of Pde","FirstCategoryId":"100","ListUrlMain":"https://link.springer.com/article/10.1007/s40818-025-00214-2","RegionNum":1,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATHEMATICS","Score":null,"Total":0}
Finite Time Singularities to the 3D Incompressible Euler Equations for Solutions in\(\:C^{\infty}(\mathbb{R}^3 \setminus \{0\})\cap C^{1,\alpha}\cap L^2\)
We introduce a novel mechanism that reveals finite time singularities within the 1D De Gregorio model and the 3D incompressible Euler equations. Remarkably, we do not construct our blow up using self-similar coordinates, but build it from infinitely many regions with vorticity, separated by vortex-free regions in between. It yields solutions of the 3D incompressible Euler equations in \(\mathbb{R}^3\times [-T,0]\) such that the velocity is in the space \(C^{\infty}(\mathbb{R}^3 \setminus \{0\})\cap C^{1,\alpha}\cap L^2\) where \(0 < \alpha \ll 1\) for times \(t\in (-T,0)\) and is not \(C^1\) at time 0.