Reconstruction of black hole metric perturbations from Weyl curvature: II. The Regge–Wheeler gauge

Reconstruction of black hole metric perturbations from Weyl curvature: II. The Regge–Wheeler gauge
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从韦尔曲率重建黑洞度量扰动:II。

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发表时间:
2002
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通讯作者:
C. Lousto
C. Lousto
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作者:
C. Lousto

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旋转黑洞的微扰理论用外尔纯量ψ4和ψ0来描述,它们都满足Teukolsky的复主波方程,自旋s = 2,分别代表出射和入射辐射。我们明确地构造出这些Weyl标量在Regge-Wheeler规范在非旋转极限的度量扰动。我们用纽曼-彭罗斯语言提出了克尔背景下雷吉-惠勒规范的推广,并讨论了建立旋转黑洞扰动时空的方法。我们还提供了双向的波形之间的关系,定义在度量和曲率的方法在时域中,也被称为(逆)Wavrasekhar变换,广义包括物质。
Perturbation theory of rotating black holes is described in terms of the Weyl scalars ψ4 and ψ0, each satisfying Teukolsky's complex master wave equation with spin s = ∓2, and respectively representing outgoing and ingoing radiation. We explicitly construct the metric perturbations out of these Weyl scalars in the Regge–Wheeler gauge in the non-rotating limit. We propose a generalization of the Regge–Wheeler gauge for a Kerr background in Newman–Penrose language and discuss the approach for building up the perturbed spacetime of a rotating black hole. We also provide two-way relationships between waveforms defined in the metric and curvature approaches in the time domain, also known as (inverse) Chandrasekhar transformations, generalized to include matter.