In this paper, we consider the following Choquard equation involving the Kirchhoff type perturbation: \(\begin{aligned} -(a+b\int _{\mathbb {R}^{N}}|\nabla u|^{2}\textrm{d}x)\Delta u = \lambda u + (I_{\alpha }*|u|^{p})|u|^{p-2}u+\mu (I_{\alpha }*|u|^{q})|u|^{q-2}u \text{ in } \mathbb {R}^{N} \end{aligned}\) under the constraint \(\begin{aligned} \int _{\mathbb {R}^{N}}u^{2}\textrm{d}x=c^{2}, \end{aligned}\) where \(N\ge 3\) , \(a,b,c>0\) , \(\mu >0\) , \((N+\alpha )/N<q<(N+4+\alpha )/N<p<2^{*}_{\alpha }:=(N+\alpha )/(N-2)\) or \((N+4+\alpha )/N<q<p<2^{*}_{\alpha }\) , \(\mu >0\) and \(\lambda \in \mathbb {R}\) appears as a Lagrange multiplier. By developing a new perturbed Pohozaev constraint approach, we establish the existence of two normalized solutions for the above problem in the mixed critical case where \((N+\alpha )/N<q<(N+4+\alpha )/N<p<2^{*}_{\alpha }\) , and the existence of ground state solutions in the \(L^{2}\) –supercritical case where \((N+4+\alpha )/N<q<p<2^{*}_{\alpha }\) . Moreover, the asymptotic behavior for the normalized solutions was also explored.