  The reduced dynamics of the system $S$, interacting with the environment $E$,
is not given by a linear map, in general. However, if it is given by a linear
map, then this map is also Hermitian. In order that the reduced dynamics of the
system is given by a linear Hermitian map, there must be some restrictions on
the set of possible initial states of the system-environment or on the possible
unitary evolutions of the whole $SE$. In this paper, adding an ancillary
reference space $R$, we assign to each convex set of possible initial states of
the system-environment $\mathcal{S}$, for which the reduced dynamics is
Hermitian, a tripartite state $\omega_{RSE}$, which we call it the reference
state, such that the set $\mathcal{S}$ is given as the steered states from the
reference state $\omega_{RSE}$,. The set of possible initial states of the
system is also given as the steered set from a bipartite reference state
$\omega_{RS}$. The relation between these two reference states is as
$\omega_{RSE}=id_{R}\otimes \Lambda_{S}(\omega_{RS})$, where $id_{R}$ is the
identity map on $R$ and $\Lambda_{S}$ is a Hermitian assignment map, from $S$
to $SE$. As an important consequence of introducing the reference state
$\omega_{RSE}$, we generalize the result of [F. Buscemi, Phys. Rev. Lett. 113,
140502 (2014)]: We show that, for a $U$-consistent subspace, the reduced
dynamics of the system is completely positive, for arbitrary unitary evolution
of the whole system-environment $U$, if and only if the reference state
$\omega_{RSE}$ is a Markov state. In addition, we show that the evolution of
the set of system-environment (system) states is determined by the evolution of
the reference state $\omega_{RSE}$ ($\omega_{RS}$).
