Divergence of infinite-variance nonradial solutions to the 3d NLS equation

preprint2010arXivOpen access

Abstract

We consider solutions u(t)u(t) to the 3d NLS equation i∂tu+Δu+∣u∣2u=0i\partial_t u + Δu + |u|^2u=0 such that ∥xu(t)∥L2=∞\|xu(t)\|_{L^2} = \infty and u(t)u(t) is nonradial. Denoting by M[u]M[u] and E[u]E[u], the mass and energy, respectively, of a solution uu, and by Q(x)Q(x) the ground state solution to −Q+ΔQ+∣Q∣2Q=0-Q+ΔQ+|Q|^2Q=0, we prove the following: if M[u]E[u]<M[Q]E[Q]M[u]E[u]<M[Q]E[Q] and ∥u0∥L2∥∇u0∥L2>∥Q∥L2∥∇Q∥L2\|u_0\|_{L^2}\|\nabla u_0\|_{L^2}>\|Q\|_{L^2}\|\nabla Q\|_{L^2}, then either u(t)u(t) blows-up in finite positive time or u(t)u(t) exists globally for all positive time and there exists a sequence of times tn→+∞t_n\to +\infty such that ∥∇u(tn)∥L2→∞\|\nabla u(t_n)\|_{L^2} \to \infty. Similar statements hold for negative time.

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