  Charmed (and bottom) hypernuclei are studied in the quark-meson coupling
(QMC) model. This completes systematic studies of charmed ($\Lambda_c^+,
\Sigma_c, \Xi_c$), and $\Lambda_b$ hypernuclei in the QMC model. Effects of the
Pauli blocking due to the underlying quark structure of baryons, and the
$\Sigma_c N - \Lambda_c N$ channel coupling are phenomenologically taken into
account at the hadronic level in the same way as those included for strange
hypernuclei. Our results suggest that the $\Sigma_c^{++}$ and $\Xi_c^+$
hypernuclei are very unlikely to be formed, while the $\Lambda_c^+$, $\Xi_c^0$
and $\Lambda_b$ hypernuclei are quite likely to be formed. For the $\Sigma_c^+$
hypernuclei, the formation probability is non-zero though small. A detailed
analysis is also made about the phenomenologically introduced Pauli blocking
and channel coupling effects for the $\Sigma_c^0$ hypernuclei.
