“…The ensemble N -representability problem is, in principle, solved, at least in the sense that a complete hierarchy of constraints on the 2RDM has been proposed. − In practical variational 2RDM (v2RDM) calculations, − ,,− however, one imposes only a subset of necessary N -representability conditions; such conditions usually include the two-particle (PQG) conditions or the partial three-particle conditions known as T1 and T2. , At the PQG level, in particular, large numbers of strongly correlated electrons can be efficiently treated; for example, a v2RDM-based calculation involving a (64e, 64o) active space can be completed in a matter of hours . While PQG-level calculations can give important insight into the qualitative properties of strongly correlated systems, the quantitative accuracy of such calculations can be poor, with the correlation energy often overestimated by as much as 20%, even in small systems near their equilibrium geometries .…”