Nonstandard solutions for a perturbed nonlinear Schrödinger system with small coupling coefficients\protect\thanks{A perturbed nonlinear Schrödinger system

preprint2022arXivOpen access

Abstract

In this paper, we consider the following weakly coupled nonlinear Schrödinger system \begin{equation*} \left\{ \begin{array}{ll} -ε^{2}Δu_1 + V_1(x)u_1 = |u_1|^{2p - 2}u_1 + β|u_1|^{p - 2}|u_2|^pu_1, & x\in \mathbb{R}^N,\\ -ε^{2}Δu_2 + V_2(x)u_2 = |u_2|^{2p - 2}u_2 + β|u_2|^{p - 2}|u_1|^pu_2, & x\in \mathbb{R}^N, \end{array} \right. \end{equation*} where ε>0ε>0, β∈Rβ\in\mathbb{R} is a coupling constant, 2p∈(2,2∗)2p\in (2,2^*) with 2∗=2NN−22^* = \frac{2N}{N - 2} if N≥3N\geq 3 and +∞+\infty if N=1,2N = 1,2, V1V_1 and V2V_2 belong to C(RN,[0,∞))C(\mathbb{R}^N,[0,\infty)). When p≥2p\ge 2 and β>0β>0 is suitably small, we show that the problem has a family of nonstandard solutions {wε=(uε1,uε2):0<ε<ε0}\{w_ε = (u^1_ε,u^2_ε):0<ε<ε_{0}\} concentrating synchronously at the common local minimum of V1V_1 and V2V_2. All decay rates of Vi(i=1,2)V_i(i=1,2) are admissible and we can allow that β>0β>0 is close to 00 in this paper. Moreover, the location of concentration points is given by local Pohozaev identities. Our proofs are based on variational methods and the penalized technique.

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