  We investigate the three-baryon system with charm +1 in a simple model.
  Charmed lambda $\Lambda_{c}$ is assumed to orbit an unperturbed deuteron in a
charmed lambda-deuteron potential based on a separable charmed lambda-nucleon
potential from chiral effective field theory techniques extrapolations of
lattice QCD data for the $\Lambda_{c}N$ $^{1}S_{0}$ and $^{3}S_{1}$ partial
waves.
  We have estimated the strength and the range of the $\Lambda_{c}$d potential.
  Also, the $\Lambda_{c}$ particle momentum distribution in
$_{\Lambda_{c}}^{3}H$ is presented and compared by $\Lambda$ particle in
$_{\Lambda}^{3}H$. It is found that there is no bound $_{\Lambda_{c}}^{3}H$
state by solving eigenvalue condition equation.
