Removing parametrized rays symplectically

preprint2020arXivOpen access

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,ω)(M,ω) be a symplectic manifold. Let [0,∞)×Q⊂R×Q[0,\infty)\times Q\subset\mathbb{R}\times Q be considered as parametrized rays [0,∞)[0,\infty) and let φ:[−1,∞)×Q→Mφ:[-1,\infty)\times Q\to M be an injective, proper, continuous map immersive on (−1,∞)×Q(-1,\infty)\times Q. If for the standard vector field ∂∂t\frac{\partial}{\partial t} on R\mathbb{R} and any further vector field νν tangent to (−1,∞)×Q(-1,\infty)\times Q the equation φ∗ω(∂∂t,ν)=0φ^*ω(\frac{\partial}{\partial t},ν)=0 holds then MM and M∖φ([0,∞)×Q)M\setminus φ([0,\infty)\times Q) are symplectomorphic.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.