English

Existence and orbital stability of standing waves for nonlinear Schr\"odinger systems

Analysis of PDEs 2016-03-01 v2

Abstract

In this paper we investigate the existence of solutions in H1(RN)×H1(RN)H^1(R^N) \times H^1(R^N) for nonlinear Schr\"odinger systems of the form {Δu1=λ1u1+μ1u1p12u1+r1βu1r12u1u2r2,Δu2=λ2u2+μ2u2p22u2+r2βu1r1u2r22u2, \left\{ \begin{aligned} -\Delta u_1 &= \lambda_1 u_1 + \mu_1 |u_1|^{p_1 -2}u_1 + r_1\beta |u_1|^{r_1-2}u_1|u_2|^{r_2}, \\ -\Delta u_2 &= \lambda_2 u_2 + \mu_2 |u_2|^{p_2 -2}u_2 + r_2 \beta |u_1|^{r_1}|u_2|^{r_2 -2}u_2, \end{aligned} \right. under the constraints RNu12dx=a1>0,RNu22dx=a2>0.\int_{R^N}|u_1|^2 \, dx = a_1>0,\quad \int_{R^N}|u_2|^2 \, dx = a_2>0. Here N1,β>0,μi>0,ri>1,2<pi<2+4N N \geq 1, \beta >0, \mu_i >0, r_i >1, 2 <p_i < 2 + \frac{4}{N} for i=1,2i=1,2 and r1+r2<2+4N r_1 + r_2 < 2 + \frac{4}{N}. This problem is motivated by the search of standing waves for an evolution problem appearing in several physical models. Our solutions are obtained as constrained global minimizers of an associated functional. Note that in the system λ1\lambda_1 and λ2\lambda_2 are unknown and will correspond to the Lagrange multipliers. Our main result is the precompactness of the minimizing sequences, up to translation, and as a consequence we obtain the orbital stability of the standing waves associated to the set of minimizers.

Keywords

Cite

@article{arxiv.1512.08952,
  title  = {Existence and orbital stability of standing waves for nonlinear Schr\"odinger systems},
  author = {Tianxiang Gou and Louis Jeanjean},
  journal= {arXiv preprint arXiv:1512.08952},
  year   = {2016}
}