The existence of band gaps in Mott insulators such as perovskite oxides with partially filled 3d shells has been traditionally explained in terms of strong, dynamic inter-electronic repulsion codified by the on-site repulsion energy U in the Hubbard Hamiltonian. The success of the "DFT+U approach" where an empirical on-site potential term U is added to the exchange-and correlation Density Functional Theory (DFT) raised questions on whether U in DFT+U represents interelectronic correlation in the same way as it does in the Hubbard Hamiltonian, and if empiricism in selecting U can be avoided. Here we illustrate that ab-initio DFT without any U is able to predict gapping trends and structural symmetry breaking (octahedra rotations, Jahn-Teller modes, bond disproportionation) for all ABO3 3d perovskites from titanates to nickelates in both spin-ordered and spin disordered paramagnetic phases.We describe the paramagnetic phases as a supercell where individual sites can have different local environments thereby allowing DFT to develop finite moments on different sites as long as the total cell has zero moment. We use a recently developed exchange and correlation functional ("SCAN") that is sanctioned by the usual single-determinant, mean-field DFT paradigm with static correlations, but has a more precise rendering of self-interaction cancelation. Our results suggest that strong dynamic electronic correlations are not playing a universal role in gapping of 3d ABO3 Mott insulators, and opens the way for future applications of DFT for studying a plethora of complexity effects that depend on the existence of gaps, such as doping, defects, and band alignment in ABO3 oxides. ensuing localization. Within this framework, the experimental observations of a variety of different symmetry-breaking modes, such as those presented in Fig.1, or magnetic moments is not related to the gapping mechanism but can appear afterwards as an additional effect.Whereas Density Functional Theory (DFT) has been shown to be able to address numerous physical effects in such oxides, including ferroelectricity 10 , catalysis 11 and electrical battery voltage 12 , its use of a single Slater determinant and its mean-field treatment of electronelectron interactions (static correlations) has, according to numerous literature statements [13][14][15] , disqualified it for the study such "strongly correlated" oxides, requiring far more computationally costly dynamically correlated methodologies, such as Dynamical Mean Field Theory (DMFT). However, the DFT calculations in such demonstrations of failure 13-15 often used a nonspin polarized description and at times exchange correlation functionals that do not distinguish occupied from unoccupied orbitals (LDA or GGA functionals without U), and generally neglect sublattice displacements. For example, Ref. 14 demonstrated vanishing band gaps in LuNiO3, in contradiction with experiment, and Ref. 15 demonstrated failure to stabilize JT distortions in LaMnO3, again, in contradiction with both experiments and DMFT cal...