{"title":"临界正则框架下的无压阻尼Euler-Riesz系统","authors":"Meiling Chi, Ling-Yun Shou, Jiang Xu","doi":"10.1007/s00021-025-00964-w","DOIUrl":null,"url":null,"abstract":"<div><p>We are concerned with a system governing the evolution of the pressureless compressible Euler equations with Riesz interaction and damping in <span>\\(\\mathbb {R}^{d}\\)</span> (<span>\\(d\\ge 1\\)</span>), where the interaction force is given by <span>\\(\\nabla (-\\Delta )^{(\\alpha -d)/2}\\rho \\)</span> with <span>\\(d-2<\\alpha <d\\)</span>. It is observed by the eigenvalue analysis that the density exhibits fractional heat diffusion behavior at low frequencies, which enables us to establish the global existence and large-time behavior of solutions to the Cauchy problem in the critical <span>\\(L^p\\)</span> framework. Precisely, the density and its <span>\\(\\sigma \\)</span>-order derivative converge to the equilibrium at the <span>\\(L^p\\)</span>-rate <span>\\((1+t)^{-(\\sigma -\\sigma _1)/(\\alpha -d+2)}\\)</span> with <span>\\(-d/p-1\\le \\sigma _1< d/p-1\\)</span>, consistent with the rate of solutions for the frictional heat equation. A non-local hypercoercivity argument and the effective unknown <span>\\(z=u+\\nabla \\Lambda ^{\\alpha -d}\\rho \\)</span> associated with the Darcy law are introduced to overcome the difficulty from the absence of hyperbolic symmetrization for first-order dissipative systems.</p></div>","PeriodicalId":649,"journal":{"name":"Journal of Mathematical Fluid Mechanics","volume":"27 4","pages":""},"PeriodicalIF":1.3000,"publicationDate":"2025-08-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The Pressureless Damped Euler-Riesz System in the Critical Regularity Framework\",\"authors\":\"Meiling Chi, Ling-Yun Shou, Jiang Xu\",\"doi\":\"10.1007/s00021-025-00964-w\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We are concerned with a system governing the evolution of the pressureless compressible Euler equations with Riesz interaction and damping in <span>\\\\(\\\\mathbb {R}^{d}\\\\)</span> (<span>\\\\(d\\\\ge 1\\\\)</span>), where the interaction force is given by <span>\\\\(\\\\nabla (-\\\\Delta )^{(\\\\alpha -d)/2}\\\\rho \\\\)</span> with <span>\\\\(d-2<\\\\alpha <d\\\\)</span>. It is observed by the eigenvalue analysis that the density exhibits fractional heat diffusion behavior at low frequencies, which enables us to establish the global existence and large-time behavior of solutions to the Cauchy problem in the critical <span>\\\\(L^p\\\\)</span> framework. Precisely, the density and its <span>\\\\(\\\\sigma \\\\)</span>-order derivative converge to the equilibrium at the <span>\\\\(L^p\\\\)</span>-rate <span>\\\\((1+t)^{-(\\\\sigma -\\\\sigma _1)/(\\\\alpha -d+2)}\\\\)</span> with <span>\\\\(-d/p-1\\\\le \\\\sigma _1< d/p-1\\\\)</span>, consistent with the rate of solutions for the frictional heat equation. A non-local hypercoercivity argument and the effective unknown <span>\\\\(z=u+\\\\nabla \\\\Lambda ^{\\\\alpha -d}\\\\rho \\\\)</span> associated with the Darcy law are introduced to overcome the difficulty from the absence of hyperbolic symmetrization for first-order dissipative systems.</p></div>\",\"PeriodicalId\":649,\"journal\":{\"name\":\"Journal of Mathematical Fluid Mechanics\",\"volume\":\"27 4\",\"pages\":\"\"},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2025-08-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Mathematical Fluid Mechanics\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s00021-025-00964-w\",\"RegionNum\":3,\"RegionCategory\":\"数学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATHEMATICS, APPLIED\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Mathematical Fluid Mechanics","FirstCategoryId":"100","ListUrlMain":"https://link.springer.com/article/10.1007/s00021-025-00964-w","RegionNum":3,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATHEMATICS, APPLIED","Score":null,"Total":0}
The Pressureless Damped Euler-Riesz System in the Critical Regularity Framework
We are concerned with a system governing the evolution of the pressureless compressible Euler equations with Riesz interaction and damping in \(\mathbb {R}^{d}\) (\(d\ge 1\)), where the interaction force is given by \(\nabla (-\Delta )^{(\alpha -d)/2}\rho \) with \(d-2<\alpha <d\). It is observed by the eigenvalue analysis that the density exhibits fractional heat diffusion behavior at low frequencies, which enables us to establish the global existence and large-time behavior of solutions to the Cauchy problem in the critical \(L^p\) framework. Precisely, the density and its \(\sigma \)-order derivative converge to the equilibrium at the \(L^p\)-rate \((1+t)^{-(\sigma -\sigma _1)/(\alpha -d+2)}\) with \(-d/p-1\le \sigma _1< d/p-1\), consistent with the rate of solutions for the frictional heat equation. A non-local hypercoercivity argument and the effective unknown \(z=u+\nabla \Lambda ^{\alpha -d}\rho \) associated with the Darcy law are introduced to overcome the difficulty from the absence of hyperbolic symmetrization for first-order dissipative systems.
期刊介绍:
The Journal of Mathematical Fluid Mechanics (JMFM)is a forum for the publication of high-quality peer-reviewed papers on the mathematical theory of fluid mechanics, with special regards to the Navier-Stokes equations. As an important part of that, the journal encourages papers dealing with mathematical aspects of computational theory, as well as with applications in science and engineering. The journal also publishes in related areas of mathematics that have a direct bearing on the mathematical theory of fluid mechanics. All papers will be characterized by originality and mathematical rigor. For a paper to be accepted, it is not enough that it contains original results. In fact, results should be highly relevant to the mathematical theory of fluid mechanics, and meet a wide readership.