We solve the S=1/2 Kondo lattice model within the dynamical mean field theory. Detailed predictions are made for the dependence of the lattice Kondo resonance and the conduction electron spectral density on temperature and band filling, nc. Two low-energy scales are identified in the spectra: a renormalized hybridization pseudogap scale T*, which correlates with the single-ion Kondo scale, and a lattice Kondo scale T0≪T*, which acts as the Fermi-liquid coherence scale. The lattice Kondo resonance is split into a main branch, which is pinned at the Fermi level, and whose width is set by T0, and an upper branch at ω≈T*. The weight of the upper branch decreases rapidly away from nc=1 and vanishes for nc≲0.7 (however, the pseudogap in the conduction electron spectral density persists for all nc). On increasing temperature, we find that the lattice Kondo resonance vanishes on a temperature scale of order 10T0, the same scale over which the single-ion Kondo resonance vanishes in impurity model calculations. In contrast to impurity model calculations, however, we find that the position of the lattice Kondo resonance depends strongly on temperature. The results are used to make predictions on the temperature dependence of the low-energy photoemission spectrum of metallic heavy fermions and doped Kondo insulators. We compare our results for the photoemission spectra with available high-resolution measurements on YbInCu4 and YbAgCu4. The loss in intensity with increasing temperature, and the asymmetric lineshape of the low-energy spectra are well accounted for by our simplified S=1/2 Kondo lattice model.
