Normalized bound states for the nonlinear Schrodinger equation in bounded domains

preprint2016arXivOpen access

Abstract

Given ρ>0ρ>0, we study the elliptic problem find (U,λ)∈H01(Ω)×R such that {−ΔU+λU=∣U∣p−1U∫ΩU2 dx=ρ, \text{find } (U,λ)\in H^1_0(Ω)\times \mathbb{R} \text{ such that } \begin{cases} -ΔU+λU=|U|^{p-1}U \int_Ω U^2\, dx=ρ, \end{cases} where Ω⊂RNΩ\subset\mathbb{R}^N is a bounded domain and p>1p>1 is Sobolev-subcritical, searching for conditions (about ρρ, NN and pp) for the existence of solutions. By the Gagliardo-Nirenberg inequality it follows that, when pp is L2L^2-subcritical, i.e. 1<p≤1+4/N1<p\leq1+4/N, the problem admits solution for every ρ>0ρ>0. In the L2L^2-critical and supercritical case, i.e. when 1+4/N≤p<2∗−11+4/N \leq p < 2^*-1, we show that, for any k∈Nk\in\mathbb{N}, the problem admits solutions having Morse index bounded above by kk only if ρρ is sufficiently small. Next we provide existence results for certain ranges of ρρ, which can be estimated in terms of the Dirichlet eigenvalues of −Δ-Δ in H01(Ω)H^1_0(Ω), extending to general domains and to changing sign solutions some results obtained in [Noris, Tavares, Verzini, Analysis & PDE, 2014] for positive solutions in the ball.

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