Decay of large solutions around shocks to multi-D viscous conservation law with strictly convex flux
Moon-Jin Kang, HyeonSeop Oh
TL;DR
This work addresses quantitative stability and decay for large perturbations of planar viscous shocks in multi-D scalar viscous conservation laws with strictly convex flux. It develops an $a$-contraction with shifts framework in the setting $\Omega = \mathbb{R} \times \mathbb{T}^2$, constructing a weight function and a dynamical shift to obtain contraction of the relative entropy and, under an $L^1$-integrable perturbation, a decay rate of $t^{-1/4}$ in $L^2$ toward the planar shock. The analysis hinges on a two-region decomposition of perturbations, Taylor expansions near the shock, and a novel multi-dimensional nonlinear Poincaré-type inequality with constraints to control cubic nonlinearities, together with precise truncation and comparison arguments. The results yield a quantitative description of convergence to planar shocks under large perturbations and establish uniform bounds on the shift, providing a significant step in the understanding of multi-D shock stability for viscous conservation laws with a single entropy.
Abstract
We consider a planar viscous shock for a scalar viscous conservation law with a strictly convex flux in multi-dimensional setting, where the transversal direction is periodic. We first show the contraction property for any solutions evolving from a large bounded initial perturbation in $L^2$ of the viscous shock. The contraction holds up to a dynamical shift, and it is measured by a weighted relative entropy. This result for the contraction extends the existing result in 1D \cite{Kang19} to the multi-dimensional case. As a consequence, if the large bounded initial $L^2$-perturbation is also in $L^1$, then the large perturbation decays of rate $t^{-1/4}$ in $L^2$, up to a dynamical shift that is uniformly bounded in time. This is the first result for the quantitative estimate converging to a planar shock under large perturbations.
