时空扩展的唯一性和非唯一性结果

Pub Date : 2024-09-17 DOI:10.1093/imrn/rnae194
Jan Sbierski
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引用次数: 0

摘要

给定函数 $f:A \to\{mathbb{R}}^{n}$ 是定义在某个开放子集 $A \subseteq\{mathbb{R}}^{m}$ 上的具有一定正则性的函数,研究这个函数是否可以扩展到所有具有一定正则性的 ${mathbb{R}}^{m}$ 是一个经典的分析问题。如果扩展存在并且是连续的,那么在 $A$ 的闭合上它肯定是唯一确定的。在广义相对论中,洛伦兹流形而非 ${mathbb{R}}^{m}$ 上的函数也会出现类似的问题。然而众所周知,即使洛伦兹流形$(M,g)$的扩展是解析的,在边界上一般也会有各种选择。本文为全局双曲洛伦兹流形$(M,g)$的扩展建立了一个唯一性条件,重点关注低正则性:只要扩展至少是局部利普齐兹连续的,那么由不可扩展因果曲线$\gamma : [-1,0) \to M$锚定的任何两个扩展在$\gamma $在两个扩展中都有极限点的意义上都必须在边界上围绕这些极限点局部一致。我们还证明了这一点:只有荷尔德连续的锚定扩展一般不享有这个局部唯一性结果。
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Uniqueness and Non-Uniqueness Results for Spacetime Extensions
Given a function $f: A \to{\mathbb{R}}^{n}$ of a certain regularity defined on some open subset $A \subseteq{\mathbb{R}}^{m}$, it is a classical problem of analysis to investigate whether the function can be extended to all of ${\mathbb{R}}^{m}$ in a certain regularity class. If an extension exists and is continuous, then certainly it is uniquely determined on the closure of $A$. A similar problem arises in general relativity for Lorentzian manifolds instead of functions on ${\mathbb{R}}^{m}$. It is well-known, however, that even if the extension of a Lorentzian manifold $(M,g)$ is analytic, various choices are in general possible at the boundary. This paper establishes a uniqueness condition for extensions of globally hyperbolic Lorentzian manifolds $(M,g)$ with a focus on low regularities: any two extensions that are anchored by an inextendible causal curve $\gamma : [-1,0) \to M$ in the sense that $\gamma $ has limit points in both extensions must agree locally around those limit points on the boundary as long as the extensions are at least locally Lipschitz continuous. We also show that this is sharp: anchored extensions that are only Hölder continuous do in general not enjoy this local uniqueness result.
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