Long time dynamics for the focusing nonlinear Schrödinger equation with exponential nonlinearities

preprint2020arXivOpen access

Abstract

In this paper, we study the focusing nonlinear Schrödinger equation with exponential nonlinearities i∂tu+Δu=−(e4π∣u∣2−1−4πμ∣u∣2)u,u(0)=u0∈H1,(t,x)∈R×R2, i \partial_t u + Δu = - \left(e^{4π|u|^2} - 1 - 4πμ|u|^2 \right) u, \quad u(0) = u_0 \in H^1, \quad (t,x) \in \mathbb{R} \times \mathbb{R}^2, where μ∈{0,1}μ\in \{0, 1\}. By using variational arguments, we first derive invariant sets where the global existence and finite time blow-up occur. In particular, we obtain sharp thresholds for global existence and finite time blow-up. In the case μ=1μ=1, by adapting a recent argument of Arora-Dodson-Murphy \cite{ADM}, we study the long time dynamics of global solutions. It turns out that either there exist tn→+∞t_n\rightarrow +\infty and Rn→∞R_n \rightarrow \infty such that u(tn)u(t_n) vanishes inside B(0,Rn)B(0,R_n) for all n≥1n\geq 1 or the solution scatters in H1H^1.

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