{"title":"Instantaneous everywhere-blowup of parabolic SPDEs","authors":"","doi":"10.1007/s00440-024-01263-7","DOIUrl":null,"url":null,"abstract":"<h3>Abstract</h3> <p>We consider the following stochastic heat equation <span> <span>$$\\begin{aligned} \\partial _t u(t,x) = \\tfrac{1}{2} \\partial ^2_x u(t,x) + b(u(t,x)) + \\sigma (u(t,x)) {\\dot{W}}(t,x), \\end{aligned}$$</span> </span>defined for <span> <span>\\((t,x)\\in (0,\\infty )\\times {\\mathbb {R}}\\)</span> </span>, where <span> <span>\\({\\dot{W}}\\)</span> </span> denotes space-time white noise. The function <span> <span>\\(\\sigma \\)</span> </span> is assumed to be positive, bounded, globally Lipschitz, and bounded uniformly away from the origin, and the function <em>b</em> is assumed to be positive, locally Lipschitz and nondecreasing. We prove that the Osgood condition <span> <span>$$\\begin{aligned} \\int _1^\\infty \\frac{\\textrm{d}y}{b(y)}<\\infty \\end{aligned}$$</span> </span>implies that the solution almost surely blows up everywhere and instantaneously, In other words, the Osgood condition ensures that <span> <span>\\(\\textrm{P}\\{ u(t,x)=\\infty \\quad \\hbox { for all } t>0 \\hbox { and } x\\in {\\mathbb {R}}\\}=1.\\)</span> </span> The main ingredients of the proof involve a hitting-time bound for a class of differential inequalities (Remark 3.3), and the study of the spatial growth of stochastic convolutions using techniques from the Malliavin calculus and the Poincaré inequalities that were developed in Chen et al. (Electron J Probab 26:1–37, 2021, J Funct Anal 282(2):109290, 2022).</p>","PeriodicalId":20527,"journal":{"name":"Probability Theory and Related Fields","volume":"51 1","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2024-03-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Probability Theory and Related Fields","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1007/s00440-024-01263-7","RegionNum":1,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"STATISTICS & PROBABILITY","Score":null,"Total":0}
引用次数: 0
Abstract
We consider the following stochastic heat equation $$\begin{aligned} \partial _t u(t,x) = \tfrac{1}{2} \partial ^2_x u(t,x) + b(u(t,x)) + \sigma (u(t,x)) {\dot{W}}(t,x), \end{aligned}$$defined for \((t,x)\in (0,\infty )\times {\mathbb {R}}\), where \({\dot{W}}\) denotes space-time white noise. The function \(\sigma \) is assumed to be positive, bounded, globally Lipschitz, and bounded uniformly away from the origin, and the function b is assumed to be positive, locally Lipschitz and nondecreasing. We prove that the Osgood condition $$\begin{aligned} \int _1^\infty \frac{\textrm{d}y}{b(y)}<\infty \end{aligned}$$implies that the solution almost surely blows up everywhere and instantaneously, In other words, the Osgood condition ensures that \(\textrm{P}\{ u(t,x)=\infty \quad \hbox { for all } t>0 \hbox { and } x\in {\mathbb {R}}\}=1.\) The main ingredients of the proof involve a hitting-time bound for a class of differential inequalities (Remark 3.3), and the study of the spatial growth of stochastic convolutions using techniques from the Malliavin calculus and the Poincaré inequalities that were developed in Chen et al. (Electron J Probab 26:1–37, 2021, J Funct Anal 282(2):109290, 2022).
期刊介绍:
Probability Theory and Related Fields publishes research papers in modern probability theory and its various fields of application. Thus, subjects of interest include: mathematical statistical physics, mathematical statistics, mathematical biology, theoretical computer science, and applications of probability theory to other areas of mathematics such as combinatorics, analysis, ergodic theory and geometry. Survey papers on emerging areas of importance may be considered for publication. The main languages of publication are English, French and German.