Existence and orbital stability of standing waves for nonlinear Schr\"odinger systems
By Tian-Xiang Gou, Louis Jeanjean. 2015
93 citations recorded by the source corpus.
In this paper we investigate the existence of solutions in $H^1(R^N) \times H^1(R^N)$ for nonlinear Schr\"odinger systems of the form \[ \left\{ \begin{aligned} -\Delta u_1 &= \lambda_1 u_1 + \mu_1 |u_1|^{p_1 -2}u_1 + r_1\beta |u_1|^{r_1-2}u_1|u_2|^{r_2}, \\ -\Delta u_2 &= \lambda_2 u_2 + \mu_2 |u_2|^{p_2 -2}u_2 + r_2 \beta |u_1|^{r_1}|u_2|^{r_2 -2}u_2, \end{aligned} \right. \] under the constraints \[\int_{R^N}|u_1|^2 \, dx = a_1>0,\quad \int_{R^N}|u_2|^2 \, dx = a_2>0. \] Here $ N \geq 1, \beta >0, \mu_i >0, r_i >1, 2 <p_i < 2 + \frac{4}{N}$ for $i=1,2$ and $ 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 $\lambda_1$ and $\lambda_2$ 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.
Subfields: Control and Systems Engineering, Mathematical Physics
View Paper: https://www.semanticscholar.org/paper/a61d8f91c4a970d4062a4811378b64f6957a5fce
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In Control and Systems Engineering
In Mathematical Physics
- Houwang Li
- Wenming Zou
- Thomas Bartsch
- Nicola Soave
- Louis Jeanjean
- Gianmaria Verzini
- R. Molle
- Xinfu Li
Citations in the corpus
- A natural constraint approach to normalized solutions of nonlinear Schr\"odinger equations and systems (2016, background): “11), and we mention that existence results under different assumptions on the data of the problem have been obtained in [8,9,21].”
- Existence and asymptotic behavior of normalized ground states for Sobolev critical Schrödinger systems (2022, methodology): “We refer the reader to [7, 26, 27, 28, 29, 30, 39, 40, 43] for scalar equations, [8, 9, 10, 11, 14, 21, 22, 31] for systems of two equations, [35] for systems of k equations.”