mixture of electron donating and accepting materials-a bulk heterojunction (BHJ). Such interpenetrating donoracceptor mixtures form complicated multilength scale morphologies, often involving several phases such as ordered/ disordered donor, mixed donor-acceptor and ordered/disordered acceptor. The coexistence of neat and mixed donoracceptor domains is thought to be beneficial as it could provide an energy cascade [4,5] for charge separation, [6,7] followed by charge transport in the neat phases. However, the neat regions may be discontinuous, forcing charges to cross mixed domains multiple times during extraction. If the mixed regions are severely disordered or contain less than the percolation threshold of required material, charge transport is thought to deteriorate significantly, limiting device performance. [8] The effect of donor-acceptor mixing (or phase purity) on charge transport has been previously addressed using microstructural characterization, [9,10] steady-state, [11][12][13] and/or timeresolved [14][15][16] mobility measurements on BHJs with a varying donor-acceptor stoichiometry and/or processing conditions. Although such studies have revealed important trends, they remain mostly semiquantitative-the question of how pure the neat domains have to be and how detrimental domain discontinuities or donor-acceptor mixing are in relation to charge transport kinetics remains to a large extent unanswered. Not knowing which important charge transport features to optimize, limits the development of next generations of organic optoelectronic devices.Here, we address this by measuring photo-generated charge motion from the first hopping events (with sub-picosecond time resolution) to full extraction in complete solar cell devices based on coevaporated bulk heterojunctions of α-sexithiophene (α-6T) and buckminsterfullerene (C 60 ). We carefully vary the molar fraction of α-6T in C 60 from homogeneously diluted (<10% molar), to a point where α-6T begins to form isolated aggregates (>10%-25% molar) or is strongly aggregated (50% molar). We thus vary the distance between isolated α-6T sites and the level of disruption of the C 60 phase in a controlled manner-the α-6T:C 60 system may be viewed as a model for the mixed donor-acceptor phase in OPV. C 60 was chosen as the model acceptor since its use in organic electronics is In organic solar cells continuous donor and acceptor networks are considered necessary for charge extraction, whereas discontinuous neat phases and molecularly mixed donor-acceptor phases are generally regarded as detrimental. However, the impact of different levels of domain continuity, purity, and donor-acceptor mixing on charge transport remains only semiquantitatively described. Here, cosublimed donor-acceptor mixtures, where the distance between the donor sites is varied in a controlled manner from homogeneously diluted donor sites to a continuous donor network are studied. Using transient measurements, spanning from sub-picoseconds to microseconds photogenerated charge motion is measured i...