Hamilton outlines the proof that the reduced holonomy group does not expand under Ricci flow in theorem 4.1 of "The Formation of Singularities in the Ricci Flow." The argument uses a maximum principle applied to the curvature operator. Kotschwar's "Ricci Flow and the Holonomy Group" shows that the reduced holonomy group is preserved in backwards time as well. Consequently, the reduced holonomy is exactly preserved by Ricci flow.
An alternative argument applies in the particular case of an initially Kahler manifold evolving by Ricci flow. Namely, the associated 2-form $\omega_t = g_t(J \cdot, \cdot)$ satisfies
$$\frac{\partial}{\partial t} d \omega_t = d \rho_t, \quad d\omega_0 = 0, \text{ and} \quad d\rho_0 = 0,$$
where $\rho = Ric(J \cdot, \cdot)$ is the Ricci form.
With a suitable uniqueness result on solutions to this differential equation, one can then conclude that $d\omega_t = 0$ for all $t \in (0, T)$. That is, $(M, g_t, J, \omega_t)$ is Kahler for all $t \in (0, T)$.