Recently, a strong debate has been pursued about the Newtonian limit (i.e. small velocity and weak field) of fourth order gravity models. According to some authors, the Newtonian limit of f(R)-gravity is equivalent to the one of Brans–Dicke gravity with ωBD=0, so that the PPN parameters of these models turn out to be ill-defined. In this Letter, we carefully discuss this point considering that
... [Show full abstract] fourth order gravity models are dynamically equivalent to the O'Hanlon Lagrangian. This is a special case of scalar–tensor gravity characterized only by self-interaction potential and that, in the Newtonian limit, this implies a non-standard behavior that cannot be compared with the usual PPN limit of General Relativity. The result turns out to be completely different from the one of Brans–Dicke theory and in particular suggests that it is misleading to consider the PPN parameters of this theory with ωBD=0 in order to characterize the homologous quantities of f(R)-gravity. Finally the solutions at Newtonian level, obtained in the Jordan frame for an f(R)-gravity, reinterpreted as a scalar–tensor theory, are linked to those in the Einstein frame.