{"title":"Transport of nonlinear oscillations along rays that graze a convex\n obstacle to any order","authors":"Wang, Jian, Williams, Mark","doi":"10.48550/arxiv.2309.05910","DOIUrl":null,"url":null,"abstract":"We provide a geometric optics description in spaces of low regularity, $L^2$ and $H^1$, of the transport of oscillations in solutions to linear and some semilinear second-order hyperbolic boundary problems along rays that graze the boundary of a convex obstacle to arbitrarily high finite or infinite order. The fundamental motivating example is the case where the spacetime manifold is $M=(\\mathbb{R}^n\\setminus \\mathcal{O})\\times \\mathbb{R}_t$, where $\\mathcal{O}\\subset \\mathbb{R}^n$ is an open convex obstacle with $C^\\infty$ boundary, and the governing hyperbolic operator is the wave operator $\\Box:=\\Delta-\\partial_t^2$.","PeriodicalId":496270,"journal":{"name":"arXiv (Cornell University)","volume":"73 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv (Cornell University)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.48550/arxiv.2309.05910","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 provide a geometric optics description in spaces of low regularity, $L^2$ and $H^1$, of the transport of oscillations in solutions to linear and some semilinear second-order hyperbolic boundary problems along rays that graze the boundary of a convex obstacle to arbitrarily high finite or infinite order. The fundamental motivating example is the case where the spacetime manifold is $M=(\mathbb{R}^n\setminus \mathcal{O})\times \mathbb{R}_t$, where $\mathcal{O}\subset \mathbb{R}^n$ is an open convex obstacle with $C^\infty$ boundary, and the governing hyperbolic operator is the wave operator $\Box:=\Delta-\partial_t^2$.