  This paper explores the energy scales of the doped Anderson lattice model
using dynamical mean-field theory (DMFT), using a continuous-time Quantum Monte
Carlo (CTQMC) impurity solver. We show that the low temperature properties of
the lattice can not be scaled using the single ion local Kondo temperature
$T_K$ but instead are governed by a doping-dependent coherence temperature $T*$
which can be used to scale the temperature dependence of the spectral function,
transport properties, and entropy. At half filling $T*$ closely approximates
the single ion $T_K$, but as the filling $n_c$ is reduced to zero, $T*$ also
vanishes. The coherence temperature $T*$ is shown to play a role of effective
impurity Kondo temperature in the lattice model, and physical observables show
significant evolution at $T*$. In the DMFT framework, we showed that the
hybridization strength of the effective impurity model is qualitatively
affected by the doping level, and determines $T*$ in the lattice model.
