  We employ dynamical mean field theory (DMFT) with a Quantum Monte Carlo (QMC)
atomic solver to investigate the finite temperature Mott transition in the
Hubbard model with the nearest neighbor hopping on a triangular lattice at
half-filling. We estimate the value of the critical interaction to be $U_c=12.0
\pm 0.5$ in units of the hopping amplitude $t$ through the evolution of the
magnetic moment, spectral function, internal energy and specific heat as the
interaction $U$ and temperature $T$ are varied. This work also presents a
comparison between DMFT and finite size determinant Quantum Monte Carlo (DQMC)
and a discussion of the advantages and limitations of both methods.
