We consider in $ \mathbb R^3 $ the singularly perturbed Schrödinger-Poisson system
$ \begin{equation*} \begin{cases} - \varepsilon^2\Delta v+V(x)v+\phi(x)v = f(v)\\ - \Delta\phi = v^2 . \end{cases} \end{equation*} $
Using variational techniques, we construct solutions which concentrate around the saddle points of the external potential $ V $, as $ \varepsilon \rightarrow 0 $.
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