This work was mainly driven by the desire to explore, to what extentembedding some given geometry in a higher dimensional flat one is useful forunderstanding the causal structure of classical fields traveling in the former,in terms of that in the latter. We point out, in the 4D spatially flat FLRWuniverse, that the causal structure of transverse-traceless (TT) gravitationalwaves can be elucidated by first reducing the problem to a 2D Minkowski waveequation with a time dependent potential, where the relevant Green's functionis pure tail -- waves produced by a physical source propagate strictly withinthe null cone. By viewing this 2D world as embedded in a 4D one, the 2D Green'sfunction can also be seen to be sourced by a cylindrically symmetric scalarfield in 3D. From both the 2D wave equation as well as the 3D scalarperspective, we recover the exact solution of the 4D graviton tail, for thecase where the scale factor written in conformal time is a power law. There areno TT gravitational wave tails when the universe is radiation dominated becausethe background Ricci scalar is zero. In a matter dominated one, we estimate theamplitude of the tail to be suppressed relative to its null counterpart by boththe ratio of the duration of the source to the age of the universe $\eta_0$,and the ratio of the observer-source spatial distance (at the observer's time)to the same $\eta_0$. In a universe driven primarily by a cosmologicalconstant, the tail contribution to the background FLRW geometry after thesource has ceased, is the conformal factor $a^2$ times a spacetime-constantsymmetric matrix proportional to the spacetime volume integral of the TT partof the source's stress-energy-momentum tensor. In other words, massless spin-2gravitational waves exhibit a tail-induced memory effect in 4D de Sitterspacetime.
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机译:这项工作主要是由探索的欲望驱动的,在某种程度上,将某些给定的几何形状包含在高维平面中对于理解前者(就后者而言)传播的经典场的因果结构是有用的。我们指出,在4D空间平坦的FLRWuniverse中,可以通过首先将问题简化为具有时变势的二维Minkowski波方程来阐明横向无迹(TT)引力波的因果结构,其中相关格林函数是纯尾- -由物理源产生的波严格在零锥内传播。通过将2D世界视为嵌入4D场景中,还可以看到2D Green的功能来自3D中的圆柱对称标量场。从2D波动方程和3D标量透视图中,对于保形时间写的比例因子是幂定律的情况,我们可以恢复4D引力子尾部的精确解。由于背景Ricci标量为零,因此当宇宙受辐射主导时,没有TT引力波尾巴。在一个占主导地位的物质中,我们通过源的持续时间与宇宙年龄$ \ eta_0 $的比率以及观察者-源空间距离的比率来估计要被抑制的尾部相对于其零对应部分的振幅(在观察者的时间)到相同的$ \ eta_0 $。在主要由宇宙常数驱动的宇宙中,源停止后,尾部对背景FLRW几何的贡献是共形因子$ a ^ 2 $乘以时空常数矩阵,与源应力的TT部分的时空体积积分成比例-能量动量张量。换句话说,无质量的自旋2引力波在4D de Sitterspacetime中表现出尾巴诱发的记忆效应。
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