Abstract:The scheduled launch of the LISA Mission in the next decade has called attention to the gravitational self-force problem. Despite an extensive body of theoretical work, long-time numerical computations of gravitational waves from extreme-massratio-inspirals remain challenging. This work proposes a class of numerical evolution schemes suitable to this problem based on Hermite integration. Their most important feature is time-reversal symmetry and unconditional stability, which enables these methods to preserve … Show more
“…The application of the framework in black-hole perturbation theory has reached a mature stage, and it has established itself as an essential method in the study of wave propagation on a fixed background. Initially, the works focused on the development of numerical codes for time evolutions, benchmarked by the study of the late time decay of several fields propagating in black-hole spacetimes [31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48]. In this context, the hyperboloidal foliations also offer the correct tool for rigourous mathematical statements about the perturbations' late time decay and black-hole dynamical stability [49][50][51][52][53].…”
This work offers a didactical introduction to the calculations and geometrical properties of a static, spherically symmetric spacetime foliated by hyperboloidal time surfaces. We discuss the various degrees of freedom involved, namely the height function, responsible for introducing the hyperboloidal time coordinate, and a radial compactification function. A central outcome is the expression of the Trautman–Bondi mass in terms of the hyperboloidal metric functions. Moreover, we apply this formalism to a class of wave equations commonly used in black-hole perturbation theory. Additionally, we provide a comprehensive derivation of the hyperboloidal minimal gauge, introducing two alternative approaches within this conceptual framework: the in-out and out-in strategies. Specifically, we demonstrate that the height function in the in-out strategy follows from the well-known tortoise coordinate by changing the sign of the terms that become singular at future null infinity. Similarly, for the out-in strategy, a sign change also occurs in the tortoise coordinate’s regular terms. We apply the methodology to the following spacetimes: Singularity-approaching slices in Schwarzschild, higher-dimensional black holes, black hole with matter halo, and Reissner–Nordström–de Sitter. From this heuristic study, we conjecture that the out-in strategy is best adapted for black hole geometries that account for environmental or effective quantum effects.
This article is part of a discussion meeting issue ‘At the interface of asymptotics, conformal methods and analysis in general relativity’.
“…The application of the framework in black-hole perturbation theory has reached a mature stage, and it has established itself as an essential method in the study of wave propagation on a fixed background. Initially, the works focused on the development of numerical codes for time evolutions, benchmarked by the study of the late time decay of several fields propagating in black-hole spacetimes [31][32][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48]. In this context, the hyperboloidal foliations also offer the correct tool for rigourous mathematical statements about the perturbations' late time decay and black-hole dynamical stability [49][50][51][52][53].…”
This work offers a didactical introduction to the calculations and geometrical properties of a static, spherically symmetric spacetime foliated by hyperboloidal time surfaces. We discuss the various degrees of freedom involved, namely the height function, responsible for introducing the hyperboloidal time coordinate, and a radial compactification function. A central outcome is the expression of the Trautman–Bondi mass in terms of the hyperboloidal metric functions. Moreover, we apply this formalism to a class of wave equations commonly used in black-hole perturbation theory. Additionally, we provide a comprehensive derivation of the hyperboloidal minimal gauge, introducing two alternative approaches within this conceptual framework: the in-out and out-in strategies. Specifically, we demonstrate that the height function in the in-out strategy follows from the well-known tortoise coordinate by changing the sign of the terms that become singular at future null infinity. Similarly, for the out-in strategy, a sign change also occurs in the tortoise coordinate’s regular terms. We apply the methodology to the following spacetimes: Singularity-approaching slices in Schwarzschild, higher-dimensional black holes, black hole with matter halo, and Reissner–Nordström–de Sitter. From this heuristic study, we conjecture that the out-in strategy is best adapted for black hole geometries that account for environmental or effective quantum effects.
This article is part of a discussion meeting issue ‘At the interface of asymptotics, conformal methods and analysis in general relativity’.
“…Most of this progress in waveform modeling has been driven by calculations in the Fourier domain [2-7, 9, 10]. While there has been continued progress in time-domain calculations [11][12][13][14], and while it is possible to construct practical surrogate models [15] from a bank of time-domain waveforms, most development has been on Fourier methods that leverage the disparate time scales in small-mass-ratio binaries: the fast orbital time scale ∼ M and the slow time scale ∼ M/ε over which the system evolves. This separation of scales allows one to divide waveform generation into two steps: an expensive offline step in which one solves Fourier-domain field equa-tions on a grid of slowly evolving parameter values (e.g., eccentricity, semi-latus rectum, the mass and spin of the primary black hole, etc.…”
Second-order gravitational self-force theory has recently led to the breakthrough calculation of "first post-adiabatic" (1PA) compact-binary waveforms [Phys. Rev. Lett. 130, 241402 (2023)]. The computations underlying those waveforms depend on a method of solving the perturbative second-order Einstein equation on a Schwarzschild background in the Fourier domain. In this paper we present that method, which involves dividing the domain into several regions. Different regions utilize different time slicings and allow for the use of "punctures" to tame sources and enforce physical boundary conditions. We demonstrate the method for Lorenz-gauge and Teukolsky equations in the relatively simple case of calculating parametric derivatives ("slow time derivatives") of first-order fields, which are an essential input at second order.
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