We investigate the normalized solutions of the following two-component Bose-Einstein condensates (BEC) system \begin{ equation}\left\{ \begin{ split} -\Delta u + (\lambda+P(x))u &= \alpha u^3 +\beta uv^2, && \text{ in } \mathbb{ R}^2,\\-\Delta v + (\lambda+Q(x))v &= \gamma v^3 +\beta u^2 v, && \text{ in } \mathbb{ R}^2, \end{ split} \right.\end{ equation} with $L^2$-constraint $$\int_{ \mathbb{ R}^2}(u^2+v^2)\,dx = 1.$$ For any $\alpha>0$, $\gamma > 0$ and $\ \beta \in (-\sqrt{ \alpha\gamma},0)\cup(0,\min \{ \alpha,\gamma\})\cup \left(\max \{ \alpha,\gamma\} , + \infty\right)$, we establish the existence of synchronized solutions concentrating on high-dimensional subsets of $\mathbb{ R}^2$ by employing a finite-dimensional reduction method combined with some local Pohozaev identities. More precisely, we construct vector radial solutions that concentrate on circles when $ \frac{ \alpha + \gamma - 2\beta}{ \alpha\gamma - \beta^2}$ tends to zero. Our results fill the blank in the system for high-dimensional concentrated normalized solutions.
Categories: math.AP