In this paper, we investigate how nonlocal correlations affect, selectively,
the physics of correlated electrons over different energy scales, from the
Fermi level to the band-edges. This goal is achieved by applying a diagrammatic
extension of dynamical mean field theory (DMFT), the dynamical vertex
approximation (DΓA), to study several spectral and thermodynamic
properties of the unfrustrated Hubbard model in two and three dimensions.
Specifically, we focus first on the low-energy regime by computing the
electronic scattering rate and the quasiparticle mass renormalization for
decreasing temperatures at a fixed interaction strength. This way, we obtain a
precise characterization of the several steps, through which the Fermi-liquid
physics is progressively destroyed by nonlocal correlations. Our study is then
extended to a broader energy range, by analyzing the temperature behavior of
the kinetic and potential energy, as well as of the corresponding energy
distribution functions. Our findings allow us to identify a smooth, but
definite evolution of the nature of nonlocal correlations by increasing
interaction: They either increase or decrease the kinetic energy w.r.t. DMFT
depending on the interaction strength being weak or strong, respectively. This
reflects the corresponding evolution of the ground state from a nesting-driven
(Slater) to a superexchange-driven (Heisenberg) antiferromagnet (AF), whose
fingerprints are, thus, recognizable in the spatial correlations of the
paramagnetic phase. Finally, a critical analysis of our numerical results of
the potential energy at the largest interaction allows us to identify possible
procedures to improve the ladder-based algorithms adopted in the dynamical
vertex approximation.Comment: 33 pages, 15 figure