“…Even the best approximations of its key ingredient, the exchange-correlation (XC) energy functional, cannot describe strong electron correlations, like those of the cuprates, and cannot exactly cancel the so-called self-interaction, a property which the exact functional should satisfy. On top of that, they fail to recover long-range van der Waals interactions, 4 are not completely safe for the description of the hydrogen bond, 5 and have intrinsic problems with situations of near degeneracy (when two sets of Kohn-Sham orbitals have very close energies); 6,7,8 more generally, the "chemical accuracy" has not yet been reached. To overcome the latter group of problems, there has been a growing interest in "mixed schemes" which combine the DFT with other approximate methods by splitting the coulombic electron-electron interaction 1/r = v ee (r) into a short-range (SR) and a long-range (LR) part (see e.g.…”