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Abstract

The scattering theory for the energy-critical wave equation on asymptotically flat spacetimes has, to date, been qualitative. While the qualitative scattering of solutions is well-understood, explicit bounds on the solution's global spacetime norms have been unavailable in this geometric setting. This paper establishes an explicit, exponential-type global bound on the Strichartz norm $\| u\|_{L^8_{t,x}}$ for solutions to the defocusing equation $\Box_g u=u^5$, where $\Box_g$ is the d'Alembertian associated with the perturbed metric. The bound depends on the solution's energy and an \textit{a priori} $\dot H^5 \times \dot H^4$ regularity bound on the solution. The proof develops a strategy that bypasses the need for vector-field commutators. It combines an interaction Morawetz estimate adapted to variable coefficients to control the solution's recent history with a dispersive analysis founded on integrated local energy decay to control the remote past. This strategy, in turn, necessitates the regularity and specific decay assumptions on the metric. As a result, this work upgrades the existing qualitative scattering theory to a fully quantitative statement, which provides a concrete measure of the global behavior of solutions in this geometric setting.