The propagation of (massless) scalar, electromagnetic and gravitational waves on fixed Schwarzschild background spacetime is described by the general time-dependent Regge-Wheeler equation. We transform this wave equation to usual Schwarzschild, Eddington-Finkelstein, Painleve-Gullstrand and Kruskal-Szekeres coordinates. In the first three cases, but not in the last one, it is possible to separate a harmonic time-dependence. Then the resulting radial equations belong to the class of confluent Heun equations, i.e., we can identify one irregular and two regular singularities. Using the generalized Riemann scheme we collect properties of all the singular points and construct analytic (local) solutions in terms of the standard confluent Heun function HeunC, Frobenius and asymptotic Thome series. We study the Eddington-Finkelstein case in detail and obtain a solution that is regular at the black hole horizon. This solution satisfies causal boundary conditions, i.e., it describes purely ingoing radiation at $r=2M$. To construct solutions on the entire open interval $r \, \in \; ]0,\infty[ \,$, we give an analytic continuation of local solutions around the horizon. Black hole scattering and quasi-normal modes are briefly considered as possible applications and we use semi-analytically calculated graybody factors together with the Damour-Ruffini method to reconstruct the power spectrum of Hawking radiation emitted by the black hole.
In this paper we construct the Fermi coordinates along any arbitrary line in simple analytical way without use the orthogonal frames and their parallel transport. In this manner we extend the Eddington approach to the construction of the Fermi metric in terms of the Riemann tensor. In the second part of the present article we show how the proposed approach works practically by applying it for deriving the Fermi coordinates for the static observer in the Schwarzschild spacetime.
Trumpet geometries play an important role in numerical simulations of black hole spacetimes, which are usually performed under the assumption of asymptotic flatness. Our Universe is not asymptotically flat, however, which has motivated numerical studies of black holes in asymptotically de Sitter spacetimes. We derive analytical expressions for trumpet geometries in Schwarzschild-de Sitter spacetimes by first generalizing the static maximal trumpet slicing of the Schwarzschild spacetime to static constant mean curvature trumpet slicings of Schwarzschild-de Sitter spacetimes. We then switch to a…
The Kottler spacetime in isotropic coordinates is known where the metric is time-dependent. In this paper, the Kottler spacetime is given in isotropic static coordinates (i.e., the metric components are time-independent). The metric is found in terms of the Jacobian elliptic functions through coordinate transformations from the Schwarzschild-(anti-)de Sitter metric. In canonical coordinates, it is known that the unparameterized spatially projected null geodesics of the Kottler and Schwarzschild spacetimes coincide. We show that in isotropic static coordinates, the refractive indices of Kottler…
Schwarzschild-de Sitter Metric and Inertial Beltrami Coordinates
在考虑坐标条件下，得到了具有宇宙学常数$Λ$的爱因斯坦场方程的Schwarzschild-Beltrami-deSitter（S-BdS）度规解.本文对de Sitter不变狭义相对论（dS-SR）和de Sitter广义相对论（dS-GR，或GR with a $Λ$）作了简要的评述。Beltrami度规$B_{μν}$为dS时空提供了惯性参考系。通过对1918年以来文献中的Schwarzschild-de Sitter（S-dS）度规$g_{μν}^{(M)}$的考察，发现已有的S-dS度规$g_{μν}^{(M)}$描述的是引力和惯性力的混合效应，而不是dS-GR中“太阳质量”$g_{μν}^{(M)}|_{M\rightarrow 0}=B_{μν}$引起的纯引力效应。这样，我们找到了dS-GR的S-BdS解，写在惯性Beltrami坐标中。这是S-dS度量的一种新形式。讨论了它的物理意义和可能的应用。
In this report, we discuss the dynamics of photons in a five-dimensional Schwarzschild black hole. We find that the corresponding Eddington-Finkelstein-like coordinate admits two time-coordinate singularities for a particular condition. This condition is due to the existence of a non-zero angular momentum related to the extra spatial dimension. By introducing a new Regge-Wheeler tortoise coordinate, both singularities can be removed from the Eddington-Finkelstein-like coordinate. It is identified that the additional singularity is related to the photon sphere in a hyperplane, and we analyze it…
The Construction and Application of Penrose Diagrams, with a Focus on the Maximally Analytically Extended Schwarzschild Spacetime
Argelander Institute for Astronomy - University of Bonn（波恩大学阿尔兰德天文研究所）；Lichtenberg Group for History and Philosophy of Physics - Faculty of Philosophy, University of Bonn（波恩大学哲学学院利希滕贝格物理历史与哲学研究组）
Matching Radial Geodesics in Two Schwarzschild Spacetimes (e.g. Black-to-White Hole Transition) or Schwarzschild and de Sitter Spacetimes (e.g. Interior of a Non-singular Black Hole)
Coordinate Independence of the Schwarzschild Black Hole Accretion Vlasov Gas Model
College of Mathematics and Physics, Hunan University of Arts and Sciences（常德学院数学与物理学院）；Hunan Province Key Laboratory Integration of Photoelectric Information Integration and Optical Manufacturing Technology（湖南省光电信息集成与光学制造技术重点实验室）；Center for Astrophysics, Guangzhou University（广州大学天体物理中心）
Action-angle coordinates are a tool commonly used in celestial mechanics to systematically parametrize and store general solutions of the equations of motion of astrophysical bodies. I perturbatively construct action-angle coordinates for bound test particle motion in static, spherically symmetric space-times using a post-circular expansion. Then I specialise the expressions to the motion in the gravitational fields of Schwarzschild black holes and give explicit formulas for the Hamiltonian to the 10th power in the radial action (20th power in eccentricity), and the transformation to angle coo…
