Optimal regularity and fine asymptotics for the porous medium equation in bounded domains

Tianling Jin, Xavier Ros-Oton, Jingang Xiong
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xmlns:m=\"http://www.w3.org/1998/Math/MathML\">\n <m:mrow>\n <m:msup>\n <m:mi>C</m:mi>\n <m:mrow>\n <m:mn>2</m:mn>\n <m:mo>,</m:mo>\n <m:mi>α</m:mi>\n </m:mrow>\n </m:msup>\n <m:mo>⁢</m:mo>\n <m:mrow>\n <m:mo stretchy=\"false\">(</m:mo>\n <m:mover accent=\"true\">\n <m:mi mathvariant=\"normal\">Ω</m:mi>\n <m:mo>¯</m:mo>\n </m:mover>\n <m:mo stretchy=\"false\">)</m:mo>\n </m:mrow>\n </m:mrow>\n </m:math>\n <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_crelle-2024-0014_eq_0398.png\" />\n <jats:tex-math>{C^{2,\\alpha}(\\overline{\\Omega})}</jats:tex-math>\n </jats:alternatives>\n </jats:inline-formula> in space, with <jats:inline-formula id=\"j_crelle-2024-0014_ineq_9997\">\n <jats:alternatives>\n <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\">\n <m:mrow>\n <m:mi>α</m:mi>\n <m:mo>=</m:mo>\n <m:mfrac>\n <m:mn>1</m:mn>\n <m:mi>m</m:mi>\n </m:mfrac>\n </m:mrow>\n </m:math>\n <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_crelle-2024-0014_eq_0460.png\" />\n <jats:tex-math>{\\alpha=\\frac{1}{m}}</jats:tex-math>\n </jats:alternatives>\n </jats:inline-formula>, and <jats:inline-formula id=\"j_crelle-2024-0014_ineq_9996\">\n <jats:alternatives>\n <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\">\n <m:msup>\n <m:mi>C</m:mi>\n <m:mi mathvariant=\"normal\">∞</m:mi>\n </m:msup>\n </m:math>\n <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_crelle-2024-0014_eq_0401.png\" />\n <jats:tex-math>{C^{\\infty}}</jats:tex-math>\n </jats:alternatives>\n </jats:inline-formula> in time (uniformly in <jats:inline-formula id=\"j_crelle-2024-0014_ineq_9995\">\n <jats:alternatives>\n <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\">\n <m:mrow>\n <m:mi>x</m:mi>\n <m:mo>∈</m:mo>\n <m:mover accent=\"true\">\n <m:mi mathvariant=\"normal\">Ω</m:mi>\n <m:mo>¯</m:mo>\n </m:mover>\n </m:mrow>\n </m:math>\n <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_crelle-2024-0014_eq_0732.png\" />\n <jats:tex-math>{x\\in\\overline{\\Omega}}</jats:tex-math>\n </jats:alternatives>\n </jats:inline-formula>), for <jats:inline-formula id=\"j_crelle-2024-0014_ineq_9994\">\n <jats:alternatives>\n <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\">\n <m:mrow>\n <m:mi>t</m:mi>\n <m:mo>></m:mo>\n <m:msup>\n <m:mi>T</m:mi>\n <m:mo>*</m:mo>\n </m:msup>\n </m:mrow>\n </m:math>\n <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_crelle-2024-0014_eq_0670.png\" />\n <jats:tex-math>{t>T^{*}}</jats:tex-math>\n </jats:alternatives>\n </jats:inline-formula>.\nFurthermore, this allows us to refine the asymptotics of solutions for large times, improving the best known results so far in two ways: we establish a faster rate of convergence <jats:inline-formula id=\"j_crelle-2024-0014_ineq_9993\">\n <jats:alternatives>\n <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\">\n <m:mrow>\n <m:mi>O</m:mi>\n <m:mo>⁢</m:mo>\n <m:mrow>\n <m:mo stretchy=\"false\">(</m:mo>\n <m:msup>\n <m:mi>t</m:mi>\n <m:mrow>\n <m:mrow>\n <m:mo>-</m:mo>\n <m:mn>1</m:mn>\n </m:mrow>\n <m:mo>-</m:mo>\n <m:mi>γ</m:mi>\n </m:mrow>\n </m:msup>\n <m:mo stretchy=\"false\">)</m:mo>\n </m:mrow>\n </m:mrow>\n </m:math>\n <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_crelle-2024-0014_eq_0421.png\" />\n <jats:tex-math>{O(t^{-1-\\gamma})}</jats:tex-math>\n </jats:alternatives>\n </jats:inline-formula>, and we prove that the convergence holds in the <jats:inline-formula id=\"j_crelle-2024-0014_ineq_9992\">\n <jats:alternatives>\n <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\">\n <m:mrow>\n <m:msup>\n <m:mi>C</m:mi>\n <m:mrow>\n <m:mn>1</m:mn>\n <m:mo>,</m:mo>\n <m:mi>α</m:mi>\n </m:mrow>\n </m:msup>\n <m:mo>⁢</m:mo>\n <m:mrow>\n <m:mo stretchy=\"false\">(</m:mo>\n <m:mover accent=\"true\">\n <m:mi mathvariant=\"normal\">Ω</m:mi>\n <m:mo>¯</m:mo>\n </m:mover>\n <m:mo stretchy=\"false\">)</m:mo>\n </m:mrow>\n </m:mrow>\n </m:math>\n <jats:inline-graphic xmlns:xlink=\"http://www.w3.org/1999/xlink\" xlink:href=\"graphic/j_crelle-2024-0014_eq_0393.png\" />\n <jats:tex-math>{C^{1,\\alpha}(\\overline{\\Omega})}</jats:tex-math>\n </jats:alternatives>\n </jats:inline-formula> topology.</jats:p>","PeriodicalId":508691,"journal":{"name":"Journal für die reine und angewandte Mathematik (Crelles Journal)","volume":"39 8","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-03-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal für die reine und angewandte Mathematik (Crelles Journal)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/crelle-2024-0014","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

We prove the optimal global regularity of nonnegative solutions to the porous medium equation in smooth bounded domains with the zero Dirichlet boundary condition after certain waiting time T * {T^{*}} . More precisely, we show that solutions are C 2 , α ( Ω ¯ ) {C^{2,\alpha}(\overline{\Omega})} in space, with α = 1 m {\alpha=\frac{1}{m}} , and C {C^{\infty}} in time (uniformly in x Ω ¯ {x\in\overline{\Omega}} ), for t > T * {t>T^{*}} . Furthermore, this allows us to refine the asymptotics of solutions for large times, improving the best known results so far in two ways: we establish a faster rate of convergence O ( t - 1 - γ ) {O(t^{-1-\gamma})} , and we prove that the convergence holds in the C 1 , α ( Ω ¯ ) {C^{1,\alpha}(\overline{\Omega})} topology.
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有界域多孔介质方程的最优正则性和精细渐近线
我们证明了多孔介质方程在光滑有界域中的非负解的最优全局正则性,该方程具有零 Dirichlet 边界条件,经过一定的等待时间 T * {T^{*}} 。 更确切地说,我们证明解是 C 2 , α ( Ω¯ ) {C^{2,\alpha}(\overline{Omega})} 在空间中,α = 1 m {\alpha=\frac{1}{m}} 在时间上,C ∞ {C^{infty}} (在 x∈ Ω ¯ {x\in\overline{Omega}} 中均匀分布)。 ),对于 t > T * {t>T^{*}} 。 此外,这使我们能够完善大时间解的渐近性,从两个方面改进了迄今已知的最佳结果:我们建立了一个更快的收敛速率 O ( t - 1 - γ ) {O(t^{-1-\gamma})}。 我们证明收敛在 C 1 , α ( Ω ¯ ) 中成立 {C^{1,\alpha}(\overline{\Omega})} 拓扑中收敛成立。
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