Xue Xiu Zhong1, Wen Ming Zou1
1Department of Mathematical Sciences, Tsinghua University, Beijing, P. R. China
Tóm tắt
Consider the Schrödinger system
$\left\{ \begin{gathered}
- \Delta u + V_{1,n} u = \alpha Q_n (x)|u|^{\alpha - 2} u|v|^\beta , \hfill \\
- \Delta v + V_{2,n} v = \beta Q_n (x)|u|^\alpha |v|^{\beta - 2} v, \hfill \\
u,v \in H_0^1 (\Omega ), \hfill \\
\end{gathered} \right.$
where Ω ⊂ ℝ
N
, α, β > 1, α + β < 2* and the spectrum σ(−Δ + V
i,n
) ⊂ (0, + ∞), i = 1, 2; Q
n
is a bounded function and is positive in a region contained in Ω and negative outside. Moreover, the sets {Q
n
> 0} shrink to a point x
0 ∈ Ω as n → +∞. We obtain the concentration phenomenon. Precisely, we first show that the system has a nontrivial solution (u
n
, v
n
) corresponding to Q
n
, then we prove that the sequences (u
n
) and (v
n
) concentrate at x
0 with respect to the H
1-norm. Moreover, if the sets {Q
n
> 0} shrink to finite points and (u
n
, v
n
) is a ground state solution, then we must have that both u
n
and v
n
concentrate at exactly one of these points. Surprisingly, the concentration of u
n
and v
n
occurs at the same point. Hence, we generalize the results due to Ackermann and Szulkin [Arch. Rational Mech. Anal., 207, 1075–1089 (2013)].