Abstract

This paper is concerned with the asymptotic stability of degenerate stationary waves for viscous gases in the half space. We discuss the following two cases: (1) viscous conservation laws and (2) damped wave equations with nonlinear convection. In each case, we prove that the solution converges to the corresponding degenerate stationary wave at the rate t−α/4 as t → ∞, provided that the initial perturbation is in the weighted space \({L^2_\alpha=L^2({\mathbb R}_+;\,(1+x)^\alpha dx)}\) . This convergence rate t−α/4 is weaker than the one for the non-degenerate case and requires the restriction α α*(q) with another critical value α*(q). Our stability analysis is based on the space–time weighted energy method in which the spatial weight is chosen as a function of the degenerate stationary wave.

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