Relatively non-degenerate integrated decay estimates on subextremal Kerr de Sitter
Georgios Mavrogiannis
TL;DR
The paper proves a relatively non-degenerate integrated decay estimate for solutions to the Klein–Gordon equation on subextremal Kerr–de Sitter spacetimes, under a mode stability assumption on Carter’s radial ODE. The authors introduce a frequency-dependent pseudodifferential commutator \(\mathcal{G}\), regularized to \(\widetilde{\mathcal{G}}\) to enable Coifman–Meyer type estimates, and combine it with a subextremal Morawetz bound to control a bulk term that degenerates at trapped sets in a controlled way. The main result shows that axisymmetric data yield unconditional decay (and exponential convergence to a constant), while in the general non-axisymmetric case the decay follows from (MS) and the new commutation framework, with the very slowly rotating regime included. This work advances stability results in Kerr–de Sitter by blending spectral (Fourier) analysis with modern pseudodifferential commutators, paving the way for nonlinear stability results on such backgrounds.
Abstract
We study the Klein--Gordon equation $\Boxψ-μ^2_{\textit{KG}}ψ=0$ on subextremal Kerr de Sitter black hole backgrounds with parameters $(a,M,l)$, where $l^2=\frac{3}Λ$. We prove a "relatively non degenerate integrated" decay estimate assuming an appropriate mode stability statement for real frequency solutions of Carter's radial ode. Our results, in particular, apply unconditionally in the very slowly rotating case $|a|\ll M,l$, and in the case where $ψ$ is axisymmetric. Exponential decay for $ψ$ to a constant is a consequence of this estimate. To prove our result, we introduce a novel pseudodifferential commutation operator $\mathcal{G}$ that generalizes our previous purely physical space commutation \cite{mavrogiannis} and we use it in conjunction with the Morawetz estimate of our companion \cite{mavrogiannis4}. This pseudodifferential operator is defined using Fourier decomposition with respect to time frequencies $ω$ and azimuthal frequencies $m$, but does not require Carter's full separation.
