Quasimodes and a Lower Bound on the Uniform Energy Decay Rate for Kerr-AdS Spacetimes
Gustav Holzegel, Jacques Smulevici
TL;DR
This work proves that quasimodes exist for the Klein–Gordon equation on Kerr–AdS exteriors, derived from a semiclassical nonlinear eigenproblem with semiclassical parameter $h=1/\sqrt{\ell(\ell+1)}$, and with exponentially small residuals. The axisymmetric reduction reduces the problem to a one-dimensional radial operator with a well-structured potential, enabling Weyl-law counting for bound states and Agmon-type exponential decay in the classically forbidden region. By cutting off these bound states, the authors construct quasimodes whose time evolution is nearly exact for times up to $t\sim e^{C\ell}$, and they show a positive limsup for a suitably defined energy functional, implying that uniform decay cannot occur faster than a logarithmic rate (matching previous upper bounds). The results sharpen the understanding of slow energy decay in Kerr–AdS spacetimes and connect to broader questions about universal minimal decay rates in black-hole geometries with AdS asymptotics. The methodology combines separation of variables, semiclassical spectral theory, Agmon estimates, and Duhamel-type arguments to establish sharp, frequency-resolved lower bounds on decay rates.
Abstract
We construct quasimodes for the Klein-Gordon equation on the black hole exterior of Kerr-Anti-de Sitter (Kerr-AdS) spacetimes. Such quasi-modes are associated with time-periodic approximate solutions of the Klein Gordon equation and provide natural candidates to probe the decay of solutions on these backgrounds. They are constructed as the solutions of a semi-classical non-linear eigenvalue problem arising after separation of variables, with the (inverse of the) angular momentum playing the role of the semi-classical parameter. Our construction results in exponentially small errors in the semi-classical parameter. This implies that general solutions to the Klein Gordon equation on Kerr-AdS cannot decay faster than logarithmically. The latter result completes previous work by the authors, where a logarithmic decay rate was established as an upper bound.
