  We study the Choquard equation with a local perturbation \begin{equation*}
-\Delta u=\lambda u+(I_\alpha\ast|u|^p)|u|^{p-2}u+\mu|u|^{q-2}u,\ x\in
\mathbb{R}^{N} \end{equation*} having prescribed mass \begin{equation*}
\int_{\mathbb{R}^N}|u|^2dx=a^2. \end{equation*} For a $L^2$-critical or
$L^2$-supercritical perturbation $\mu|u|^{q-2}u$, we prove nonexistence,
existence and symmetry of normalized ground states, by using the mountain pass
lemma, the Poho\v{z}aev constraint method, the Schwartz symmetrization
rearrangements and some theories of polarizations. In particular, our results
cover the Hardy-Littlewood-Sobolev upper critical exponent case
$p=(N+\alpha)/(N-2)$. Our results are a nonlocal counterpart of the results in
\cite{{Li 2021-4},{Soave JFA},{Wei-Wu 2021}}.
