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)
Summary
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)
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