  Several observed states close to the $D\bar{D}^*$ and
$D^*_{(s)}\bar{D}^*_{(s)}$ thresholds, as the X(3872) and some XYZ particles
can be described in terms of a two-meson molecule. Furthermore, doubly charmed
states are also predicted. These new states are near the $D^*D^*$ and
$D^*D^*_s$ thresholds, % Therefore, if the previous XYZ are molecules, then,
there should be doubly charmed mesons with $J^P=1^+$ around the $D^*D^*$
threshold.
  %For this reason, it is important to evaluate observables related to them.
Because of the spin$=1$, they do not decay into $DD$. In this article we
compute decays to $DD^*$ and radiative decays of doubly charmed meson molecules
into $DD_{(s)}\gamma$. and have spin-parity $J^P=1^+$. Their natural decay
modes are $D_{(s)}D^*$, $DD_{(s)}\pi$ and $DD_{(s)}\gamma$ and
$D^*D_{(s)}\gamma$. We evaluate the widths of these states, named here as
$R_{cc}(3970)$ and $S_{cc}(4100)$, and obtain 44 MeV for the non-strangeness,
and 24 MeV for the doubly charm-strange state. Essentially, the decay modes are
$DD_{(s)}\pi$ and $DD_{(s)}\gamma$, being the $D\pi$ and $D\gamma$ emitted by
one of the $D^*$ meson which forms the molecule.
