  We calculate the time dependence of the reflected entropy of two disconnected
regions after a global quench in $(1+1)$-dimensional conformal field theories
and in large temperature limit. For rational conformal field theories, we find
that the time evolution of the reflected entropy is the same as that of the
mutual information. We get the same result for holographic theories in the
limit where the separation between disconnected regions is much smaller than
their respective sizes. We discuss how this result is consistent with the
quasi-particle picture of Calabrese and Cardy \cite{calabrese-cardy}.
