Bounded Solutions to an Energy Subcritical Non-linear Wave Equation on R^3

preprint2015arXivOpen access

Abstract

In this work we consider an energy subcritical semi-linear wave equation (3<p<53 < p < 5) ∂t2u−Δu=ϕ(x)∣u∣p−1u,(x,t)∈R3×R \partial_t^2 u - Δu = ϕ(x) |u|^{p-1} u, \qquad (x,t) \in {\mathbb R}^3 \times {\mathbb R} with initial data (u,ut)∣t=0=(u0,u1)∈H˙sp×H˙sp−1(R3)(u,u_t)|_{t=0} = (u_0,u_1)\in \dot{H}^{s_p} \times \dot{H}^{s_p-1}({\mathbb R}^3), where sp=3/2−2/(p−1)s_p = 3/2 - 2/(p-1) and the function ϕ:R3→[−1,1]ϕ: {\mathbb R}^3 \rightarrow [-1,1] is a radial continuous function with a limit at infinity. We prove that unless the elliptic equation −ΔW=ϕ(x)∣W∣p−1W-ΔW = ϕ(x) |W|^{p-1} W has a nonzero radial solution W∈C2(R3)∩H˙sp(R3)W \in C^2 ({\mathbb R}^3) \cap \dot{H}^{s_p} ({\mathbb R}^3), any radial solution uu with a finite uniform upper bound on the critical Sobolev norm ∥(u(⋅,t),∂tu(⋅,t))∥H˙sp×H˙sp(R3)\|(u(\cdot,t), \partial_t u(\cdot,t))\|_{\dot{H}^{s_p}\times \dot{H}^{s_p}({\mathbb R}^3)} for all tt in the maximal lifespan must be a global solution in time and scatter.

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