Abstract

In this paper, we consider the following nonlinear coupled elliptic systems with continuous potentials: $$\left\{ \begin{gathered} - {\varepsilon ^2}\Delta u + \left( {1 + \delta P\left( x \right)} \right)u = {\mu _1}{u^3} + \beta u{v^2}in\Omega , \hfill \\ - {\varepsilon ^2}\Delta v + \left( {1 + \delta Q\left( x \right)} \right)u = {\mu _2}{u^3} + \beta {u^2}vin\Omega , \hfill \\ u > 0,v > 0in\Omega , \hfill \\ \frac{{\partial u}}{{\partial v}} = \frac{{\partial u}}{{\partial v}} = 0on\partial \Omega , \hfill \\ \end{gathered} \right.$$ where Ω is a smooth bounded domain in R N for N = 2, 3, δ, e, μ1 and μ2 are positive parameters, β ∈ R, P(x) and Q(x) are two smooth potentials defined on Ω, the closure of Ω. Due to Liapunov-Schmidt reduction method, we prove that (Ae) has at least O(1/(e|lne|) N ) synchronized and O(1/(e|lne|)2N) segregated vector solutions for e and δ small enough and some β ∈ R. Moreover, for each m ∈ (0,N) there exist synchronized and segregated vector solutions for (Ae) with energies in the order of eN-m. Our results extend the result of Lin et al. (2007) from the Lin-Ni-Takagi problem to the nonlinear Schr¨odinger elliptic systems with continuous potentials.

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