From Polynomial Stability to Periodic Well-posedness in Partially Dissipative Systems

TL;DR

This paper links polynomial stability of semigroups to periodic well-posedness in complex systems, providing explicit conditions for forcing functions in models like fluid-structure interactions.

Contribution

It characterizes the dense set of forcings ensuring periodic well-posedness under polynomial stability using resolvent bounds and Fourier analysis.

Findings

Polynomial stability implies explicit forcing conditions for well-posedness.

Resolvant bounds translate into loss of derivatives on forcing functions.

Applicable to models like heat-wave interactions and thermoelastic systems.

Abstract

The study of resonances (and well-posedness) for complex systems under time-periodic loading is of broad interest in application. The work of Galdi et al.~(2014) connects asymptotic stability of solutions to an unforced Cauchy problem to solvability of the time-periodic forced problem. Uniform stability of the solution semigroup gives periodic well-posedness for all forces in the natural mild forcing class, whereas strong stability yields only existence of a dense set of forcings for which resonance can be excluded. We address an intermediate regime for polynomial (also: rational or semiuniform) stability. Working with a Fourier decomposition in Hilbert space, we demonstrate that polynomial stability of the semigroup yields an explicit characterization of the dense forcing set on which periodic well-posedness holds. More precisely, resolvent bounds translate directly into certain losses of time derivatives on the forcing required to ensure well-posedness. Our result is motivated by partially dissipative models -- including the famous heat-wave interaction problem idealizing fluid-structure interactions, as well as some thermoelastic, viscoelastic, and weakly damped hyperbolic systems -- for which polynomial decay is the natural regime.