{"title":"Removing parametrized rays symplectically","authors":"B. Stratmann","doi":"10.4310/jsg.2022.v20.n2.a4","DOIUrl":null,"url":null,"abstract":"Extracting isolated rays from a symplectic manifold result in a manifold symplectomorphic to the initial one. The same holds for higher dimensional parametrized rays under an additional condition. More precisely, let $(M,\\omega)$ be a symplectic manifold. Let $[0,\\infty)\\times Q\\subset\\mathbb{R}\\times Q$ be considered as parametrized rays $[0,\\infty)$ and let $\\varphi:[-1,\\infty)\\times Q\\to M$ be an injective, proper, continuous map immersive on $(-1,\\infty)\\times Q$. If for the standard vector field $\\frac{\\partial}{\\partial t}$ on $\\mathbb{R}$ and any further vector field $\\nu$ tangent to $(-1,\\infty)\\times Q$ the equation $\\varphi^*\\omega(\\frac{\\partial}{\\partial t},\\nu)=0$ holds then $M$ and $M\\setminus \\varphi([0,\\infty)\\times Q)$ are symplectomorphic.","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2020-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.4310/jsg.2022.v20.n2.a4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
Extracting isolated rays from a symplectic manifold result in a manifold symplectomorphic to the initial one. The same holds for higher dimensional parametrized rays under an additional condition. More precisely, let $(M,\omega)$ be a symplectic manifold. Let $[0,\infty)\times Q\subset\mathbb{R}\times Q$ be considered as parametrized rays $[0,\infty)$ and let $\varphi:[-1,\infty)\times Q\to M$ be an injective, proper, continuous map immersive on $(-1,\infty)\times Q$. If for the standard vector field $\frac{\partial}{\partial t}$ on $\mathbb{R}$ and any further vector field $\nu$ tangent to $(-1,\infty)\times Q$ the equation $\varphi^*\omega(\frac{\partial}{\partial t},\nu)=0$ holds then $M$ and $M\setminus \varphi([0,\infty)\times Q)$ are symplectomorphic.