Explain late-time QNM/tail amplitude comparability
Explain why amplitudes of quasi-normal modes and tail terms become comparable only at late times in BBH simulations—rather than shortly after merger—and determine whether this feature is tied to global boundary conditions such as the no-incoming-radiation condition at the horizon.
References
Open Issue 10 (OI-10) Why are the amplitudes comparable only at a late time such as \Sigma_0 rather than at earlier time \Sigma_1 soon after the merger? Is this feature also tied to a very global boundary condition such as `no incoming radiation' at $$?
Nonetheless, because we do not currently have a full description of spheroidal harmonics for general large complex \omega, within the window the large-arc contribution is not understood. In this work in Kerr we still operationally set the split time to be |r_|+|r'_| as the Schwarzschild limit, and we leave the discussion of the exact split time to future studies.
A complete characterization of the very-late-time evolution and its horizon-controlled asymptote will require a more comprehensive model and is left to future work.