In this paper, we consider the multiplicity of solutions to the following Choquard equation \(\begin{aligned} -\varepsilon ^2\Delta u+V(x)u=\lambda u+\varepsilon ^{-\alpha }(I_\alpha *[h( x)|u|^p])h(x)|u|^{p-2}u\quad \text{ in } {\mathbb {R}}^{N}, \end{aligned}\) with a prescribed mass \(\begin{aligned} \int _{{\mathbb {R}}^N}|u|^2dx=a\varepsilon ^N, \end{aligned}\) where \(N\ge 1\) , \(a,\varepsilon >0\) , \(\alpha \in (0,N)\) , \(\frac{N+\alpha }{N}<p<\frac{N+\alpha +2}{N}\) , \(I_\alpha \) is the Riesz potential, \(\lambda \in {\mathbb {R}}\) appears as an unknown Lagrange multiplier, \(h: {\mathbb {R}}^{N} \rightarrow [0,\infty )\) is a bounded and continuous function and the potential V is a continuous function. Under some assumptions on V, we show that when \(\varepsilon \) is small enough the numbers of normalized ground states are at least the numbers of global maximum points of h.