Removing parametrized rays symplectically

IF 0.6 3区 数学 Q3 MATHEMATICS Journal of Symplectic Geometry Pub Date : 2020-09-11 DOI:10.4310/jsg.2022.v20.n2.a4
B. Stratmann
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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.
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辛地去除参数化射线
从辛流形中提取孤立射线,得到的流形与初始流形的辛同构。在附加条件下,这同样适用于高维参数化射线。更准确地说,假设$(M,\omega)$是一个辛流形。将$[0,\infty)\times Q\subset\mathbb{R}\times Q$视为参数化射线$[0,\infty)$,并将$\varphi:[-1,\infty)\times Q\to M$视为沉浸在$(-1,\infty)\times Q$上的一个注入的、适当的、连续的地图。如果对于$\mathbb{R}$上的标准向量场$\frac{\partial}{\partial t}$和任何与$(-1,\infty)\times Q$相切的更远的向量场$\nu$,方程$\varphi^*\omega(\frac{\partial}{\partial t},\nu)=0$成立,那么$M$和$M\setminus \varphi([0,\infty)\times Q)$是辛形态的。
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来源期刊
CiteScore
1.30
自引率
0.00%
发文量
0
审稿时长
>12 weeks
期刊介绍: Publishes high quality papers on all aspects of symplectic geometry, with its deep roots in mathematics, going back to Huygens’ study of optics and to the Hamilton Jacobi formulation of mechanics. Nearly all branches of mathematics are treated, including many parts of dynamical systems, representation theory, combinatorics, packing problems, algebraic geometry, and differential topology.
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