Analytical high-order post-Newtonian expansions for extreme mass ratio binaries
Chris Kavanagh, Adrian C. Ottewill, Barry Wardell
TL;DR
This work develops analytic high-order post-Newtonian expansions for gauge-invariant quantities in extreme mass ratio binaries by leveraging the MST functional-series method in the Regge-Wheeler framework. It combines exact low-$ ext{l}$ solutions with a large-$ ext{l}$ PN template to construct the metric perturbation for a particle on a circular Schwarzschild orbit and applies mode-sum regularization to extract Detweiler-Whiting regular fields, yielding PN expansions up to $y^{15.5}$ (with higher terms available online) for redshift, spin-precession, and tidal invariants. The results are cross-validated against previous PN/self-force work and are readily applicable to obtaining the high-PN expansion of the EOB radial potential $a(y)$, enabling enhanced waveform modeling. The authors also discuss extensions to Kerr spacetimes and to higher-order multipoles, highlighting the broader impact on precision gravitational-wave predictions and the PN/self-force correspondence. Overall, the paper provides a robust analytic framework for very high-order PN analyses of gauge-invariant quantities in EMR binaries, with clear pathways to Kerr generalizations and additional invariants.
Abstract
We present analytic computations of gauge invariant quantities for a point mass in a circular orbit around a Schwarzschild black hole, giving results up to 15.5 post-Newtonian order in this paper and up to 21.5 post-Newtonian order in an online repository. Our calculation is based on the functional series method of Mano, Suzuki and Takasugi (MST) and a recent series of results by Bini and Damour. We develop an optimised method for generating post-Newtonian expansions of the MST series, enabling significantly faster computations. We also clarify the structure of the expansions for large values of $\ell$, and in doing so develop an efficient new method for generating the MST renormalised angular momentum, $ν$.
