Abstract

We study the Cauchy problem of the damped wave equation \begin{align*} \partial_{t}^2 u - \Delta u + \partial_t u = 0 \end{align*} and give sharp $L^p$-$L^q$ estimates of the solution for $1\le q \le p < \infty\ (p\neq 1)$ with derivative loss. This is an improvement of the so-called Matsumura estimates. Moreover, as its application, we consider the nonlinear problem with initial data in $(H^s\cap H_r^{\beta}) \times (H^{s-1} \cap L^r)$ with $r \in (1,2]$, $s\ge 0$, and $\beta = (n-1)|\frac{1}{2}-\frac{1}{r}|$, and prove the local and global existence of solutions. In particular, we prove the existence of the global solution with small initial data for the critical nonlinearity with the power $1+\frac{2r}{n}$, while it is known that the critical power $1+\frac{2}{n}$ belongs to the blow-up region when $r=1$. We also discuss the asymptotic behavior of the global solution in supercritical cases. Moreover, we present blow-up results in subcritical cases. We give estimates of lifespan and blow-up rates by an ODE argument.

Highlights

  • The damped wave equation∂t2u − ∆u + ∂tu = 0 is known as a model describing the wave propagation with friction, and studied for long years

  • To control the nonlinear term, we introduce an appropriate norm for the nonlinearity (see (38)), which is inspired by Hayashi, Kaikina and Naumkin [9]

  • In the supercritical case p > 1 + 2nr, we prove that the solution is approximated by that of the linear heat equation (4) with the initial data ε(u0 +u1)

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Summary

Introduction

We showed that if p > 1+ 2nr and if the initial data satisfy (u0, u1) ∈ (Hs,0 ∩H0,α)(Rn)× (Hs−1,0 ∩ H0,α)(Rn) with α > n( 1r − 12 ) and sufficiently small, the global solution uniquely exists In this setting, we cannot treat the critical case p = 1 + 2nr. In the supercritical case p > 1 + 2nr , we prove that the solution is approximated by that of the linear heat equation (4) with the initial data ε(u0 +u1) This extends the results by [29] to all space dimensions. For any δ > 0, there exist initial data (u0, u1) ∈ (Hs(Rn) ∩ Hrβ(Rn)) × (Hs−1(Rn) ∩ Lr(Rn)) and a constant ε2 = ε2(n, p, r, s, δ) > 0 such that for any ε ∈ (0, ε2], the lifespan of Hs-mild solutions defined by (14) is estimated as. Let d be the multiplier of D1, namely d(t, x) := F −1 χ (x)

Lp-Lq estimates for linear damped wave equation
Lp-Lq estimates for the derivative of the solution

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