Towards a covariant framework for post-Newtonian expansions for radiative sources

Hartong, Jelle, Musaeus, Jørgen
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Abstract

We consider the classic problem of a compact fluid source that behaves non-relativistically and that radiates gravitational waves. The problem consists of determining the metric close to the source as well as far away from it. The non-relativistic nature of the source leads to a separation of scales resulting in an overlap region where both the $1/c$ and (multipolar) $G$-expansions are valid. Standard approaches to this problem (the Blanchet--Damour and the DIRE approach) use the harmonic gauge. We define a `post-Newtonian' class of gauges that admit a Newtonian regime in inertial coordinates. In this paper we set up a formalism to solve for the metric for any post-Newtonian gauge choice. Our methods are based on previous work on the covariant theory of non-relativistic gravity (a $1/c$-expansion of general relativity that uses post-Newton-Cartan variables). At the order of interest in the $1/c$ and $G$-expansions we split the variables into two sets: transverse and longitudinal. We show that for the transverse variables the problem can be reduced to inverting Laplacian and d'Alembertian operators on their respective domains subject to appropriate boundary conditions. The latter are regularity in the interior and asymptotic flatness with a Sommerfeld no-incoming radiation condition imposed at past null infinity. The longitudinal variables follow from the gauge choice. The full solution is then obtained by the method of matched asymptotic expansion. We show that our methods reproduce existing results in harmonic gauge to 2.5PN order.
辐射源后牛顿展开的协变框架
我们考虑一个经典问题的致密流体源的行为,非相对论性和辐射引力波。这个问题包括确定离源近和离源远的度量。源的非相对论性导致尺度分离,导致重叠区域,其中$1/c$和(多极)$G$-展开都有效。解决这个问题的标准方法(Blanchet- Damour和DIRE方法)使用谐波测量。我们定义了一个“后牛顿”的量规类,它在惯性坐标系中承认牛顿制度。在本文中,我们建立了求解任何后牛顿规范选择的度规的形式化方法。我们的方法是基于之前关于非相对论引力协变理论的工作(广义相对论的1/c -扩展,使用后牛顿-卡坦变量)。按照$1/c$和$G$展开的兴趣顺序,我们将变量分成两组:横向和纵向。我们证明,对于横向变量,问题可以简化为在适当的边界条件下,在各自的区域上的拉普拉斯算子和达朗伯算子的逆变换。后者是内部正则性和在过去零无穷远处施加无入射辐射条件下的渐近平坦性。纵向变量来源于量规的选择。然后用匹配渐近展开的方法得到了问题的全解。我们证明了我们的方法将现有的结果在谐波测量中再现到2.5PN阶。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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