  Closed shell charmed hypernuclei $^5_{\Lambda_c}$Li, $^{17}_{\Lambda_c}$F,
$^{41}_{\Lambda_c}$Sc, $^{57}_{\Lambda_c}$Cu, $^{133}_{\Lambda_c}$Sb and
$^{209}_{\Lambda_c}$Bi are calculated within Hartree-Fock approach by using
three different force sets derived from microscopic Brueckner-Hartree-Fock
calculations of $\Lambda$ hypernuclei. Ground state properties (binding
energies, $\Lambda_c$ separation energies, $\Lambda_c$ single particle energies
and $\Lambda_c$ densities) of charmed nuclei are examined. Due to the Coulomb
repulsion between protons and the $\Lambda_c$ baryon, charmed hypernuclei are
most bound for $16\leq$A$\leq 41$, where $^{17}_{\Lambda_c}$F can be considered
as an excellent candidate to measure charmed hypernuclei. The competition
between the attractive nucleon-$\Lambda_c$ interaction and the Coulomb
repulsion is discussed, and we compare $\Lambda$ and $\Lambda_c$ hypernuclei
properties.
