Organic solar cell blends comprised of an electron donating polymer and electron accepting fullerene typically form upon solution casting a thin-film structure made up of a complex mixture of phases.These phases can vary greatly in: composition, order and thermodynamic stability; and they are dramatically influenced by the processing history. Understanding the processes that govern the formation of these phases and their subsequent effect on the efficiency of photo-generating and extracting charge carriers is of utmost importance to enable rational design and processing of these Organic photovoltaics (OPVs) have seen a rapid increase in performance over recent years, with certain polymer:fullerene blends now reaching efficiencies of more than 10%. This improvement has mainly been due to intense materials development efforts. Despite these activities, however, key understanding of various relevant aspects that dictate the structural and optoelectronics landscape of many OPV materials, is still lacking. For instance, it is still unclear why specic acceptors work well only in combination with certain donors. Moreover, thorough knowledge has not been established why small variations in the chemical structure of the active materials in certain cases can lead to signicant differences in device performance while in other scenarios essentially identical device characteristics are obtained.
2One reason for these differences that are observed in devices even for structurally very similar materials is that the manipulation of the chemical structure oen results in alteration of the energy levels, 1,3 which, in the case of the LUMO of the acceptor, should either promote charge dissociation or increase the open circuit voltage (V oc ) with a given donor. Chemical changes lead, however, also to a different miscibility of the two components,