Analytical solutions of bound timelike geodesic orbits in effective-one-body frame
Chen Zhang, Wen-Biao Han
TL;DR
This paper develops analytical solutions for bound timelike geodesics in an extreme-mass-ratio binary within a deformed Kerr background used by the EOB framework. By employing Mino time $\lambda$ to decouple radial and polar motion and expressing the geodesics with Legendre elliptic integrals, it derives mass-ratio–corrected fundamental frequencies $\Omega_r$, $\Omega_\theta$, and $\Omega_\phi$ via Fourier expansions and constructs $t$-domain representations for gravitational-wave calculations. The work validates the analytical frequencies against numerical integrations, showing good agreement and substantial speedups, and demonstrates the practicality of using these results in the frequency-domain Teukolsky formalism for EMRI waveform generation. Overall, the results enable efficient EMRI waveform modeling with mass-ratio corrections within the EOB framework and set the stage for incorporating these analytical solutions into Teukolsky-based GW calculations.
Abstract
We derive the approximate analytical solutions of the bound timelike geodesic orbits in the effective-one-body (EOB) frame with extreme-mass ratio limit. The analytical solutions are expressed in terms of the elliptic integrals using Mino time $λ$ as the independent variable. Since Mino time decouples the $r$ and $θ$-motion, we also give explicit expressions for three orbital frequencies $Ω_r, ~Ω_θ, ~Ω_φ$ using the Fourier series expansion. With these analytical expressions at hand, we can perform Fourier expansions in Mino time $λ$ for any function expressed in terms of the coordinates $(r,θ,φ)$. In particular, the observer's time t is decomposed into Mino time $λ$, and the frequency-domain description is constructed from the $λ$-Fourier expansion and the expansion of t. These analytical expressions are quite simple to implement, and can be applicable for calculating gravitational waves (GWs) from extreme mass-ratio inspirals (EMRIs) with the frequency-domain Teukolsky equation.
