Frequency-domain calculation of the self force: the high-frequency problem and its resolution

TL;DR

This paper addresses the slow convergence issue in frequency-domain self-force calculations for eccentric orbits by proposing a method using homogeneous modes, leading to exponentially-fast convergence at the particle's location.

Contribution

It introduces a practical technique employing homogeneous modes to improve the convergence of frequency-domain self-force computations for eccentric orbits.

Findings

The new method achieves exponential convergence at the particle's location.

Application demonstrated with scalar charge in eccentric orbit around Schwarzschild black hole.

Potential applicability to gravitational self-force calculations using Teukolsky formalism.

Abstract

The mode-sum method provides a practical means for calculating the self force acting on a small particle orbiting a larger black hole. In this method, one first computes the spherical-harmonic $l$-mode contributions $F^{\mu}_l$ of the "full force" field $F^{\mu}$, evaluated at the particle's location, and then sums over $l$ subject to a certain regularization procedure. In the frequency-domain variant of this scheme the quantities $F^{\mu}_l$ are obtained by fully decomposing the particle's self field into Fourier-harmonic modes $l m \omega$, calculating the contribution of each such mode to $F^{\mu}_l$, and then summing over $\omega$ and $m$ for given $l$. This procedure has the advantage that one only encounters {\it ordinary} differential equations. However, for eccentric orbits, the sum over $\omega$ is found to converge badly at the particle's location. This problem (reminiscent of the familiar Gibbs phenomenon) results from the discontinuity of the time-domain $F^{\mu}_l$ field at the particle's worldline. Here we propose a simple and practical method to resolve this problem. The method utilizes the {\it homogeneous} modes $l m \omega$ of the self field to construct $F^{\mu}_l$ (rather than the inhomogeneous modes, as in the standard method), which guarantees an exponentially-fast convergence to the correct value of $F^{\mu}_l$, even at the particle's location. We illustrate the application of the method with the example of the monopole scalar-field perturbation from a scalar charge in an eccentric orbit around a Schwarzschild black hole. Our method, however, should be applicable to a wider range of problems, including the calculation of the gravitational self-force using either Teukolsky's formalism, or a direct integration of the metric perturbation equations.