Some Results on the Scattering Theory for Nonlinear Schrödinger Equations in Weighted L2L^{2} Space

preprint2011arXivOpen access

Abstract

We investigate the scattering theory for the nonlinear Schrödinger equation i∂tu+Δu+λ∣u∣αu=0i \partial_{t}u+ Δu+λ|u|^αu=0 in Σ=H1(Rd)∩L2(∣x∣2;dx)Σ=H^{1}(\mathbb{R}^{d})\cap L^{2}(|x|^{2};dx). We show that scattering states u±u^{\pm} exist in ΣΣ when αd<α<4d−2α_{d}<α<\frac{4}{d-2}, d≥3d\geq3, λ∈Rλ\in \mathbb{R} with certain smallness assumption on the initial data u0u_{0}, and when α(d)≤α<4d−2α(d)\leq α< \frac{4}{d-2}(α∈[α(d),∞)α\in [α(d), \infty), if d=1,2d=1,2), λ>0λ>0 under suitable conditions on u0u_{0}, where αdα_{d}, α(d)α(d) are the positive root of the polynomial dx2+dx−4dx^{2}+dx-4 and dx2+(d−2)x−4dx^{2}+(d-2)x-4 respectively. Specially, when λ>0λ>0, we obtain the existence of u±u^{\pm} in ΣΣ for u0u_{0} below a mass-energy threshold M[u0]σE[u0]<λ−2τM[Q]σE[Q]M[u_{0}]^σE[u_{0}]<λ^{-2τ}M[Q]^σE[Q] and satisfying an mass-gradient bound ∥u0∥L2σ∥∇u0∥L2<λ−τ∥Q∥L2σ∥∇Q∥L2\|u_{0}\|_{L^{2}}^σ\|\nabla u_{0}\|_{L^{2}}<λ^{-τ}\|Q\|_{L^{2}}^σ\|\nabla Q\|_{L^{2}} with 4d<α<4d−2\frac{4}{d}<α<\frac{4}{d-2}(α∈(4d,∞)α\in (\frac{4}{d}, \infty), if d=1,2d=1,2), and also for oscillating data at critical power α=α(d)α=α(d), where σ=4−(d−2)ααd−4σ=\frac{4-(d-2)α}{αd-4}, τ=2αd−4τ=\frac{2}{αd-4} and QQ is the ground state. We also study the convergence of u(t)u(t) to the free solution eitΔu±e^{itΔ}u^{\pm} in ΣΣ, where u±u^{\pm} is the scattering state at ±∞\pm\infty respectively.

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