mean that (undesired) geminate charge carrier recombination always competes with the (desired) charge carrier separation and therefore quantum effi ciencies are always moderate. The surprising experimental observations of exceptionally high quantum effi ciencies revealed that such a simplistic picture is insufficient to describe charge carrier separation in organic photovoltaics, and motivated a broad range of close physical investigations into this critical process aimed at developing an accurate mechanistic understanding of charge separation (that could be used to design high quantum effi ciency materials). In this manuscript we present a rich multidimensional set of transient absorption observations which provide detailed information (on the ps to µs timescale) about the behavior of mobile, separating charge carriers in the prototypical high quantum effi ciency poly[N-11′′-henicosanyl-2,7-carbaz olealt-5,5-(4′,7′-di-2-thienyl-2′,1′,3′-benzothiadiazole)] (PCDTBT): fullerene derivative blends. The measurements concurrently observe the relaxation of charge carriers within the disordered density of states (DOS), and the recombination of charge carriers at a sequence of different initial charge carrier concentrations. Understood through the lens of kinetic Monte Carlo calculations, these observations reveal how mobile charge carriers hop and relax, dissociating and re-associating potentially multiple times before extraction or recombination.The current literature regarding observations of charge carrier separation in organic bulk heterojunctions is in agreement with regards to the conclusion that charge carrier separation out of the geminate pairs occurs on the sub nanosecond timescale. A clear indication of the upper bound for the time within which charge carriers must separate was given by the precise measurement using an ultrafast pump-push-photocurrent technique of the lifetimes of geminate interfacial bound charge carrier pairs (also called interfacial charge-transfer state). [ 2 ] This work found that the lifetime for a geminate charge carrier pair which remained at the interface in relatively high quantum effi ciency blends (such as P3HT:PCBM) was in general on the order of 500 ps. Thus, charge carriers which separate must certainly achieve separation in less than 500 ps. Bakulin and coworkers in this work suggest that signifi cant charge carrier delocalization during the transient occupation of a higher lying interfacial geminate state (which would occur on the sub-picosecond timescale) is the crucial initial step towards separation. [ 2,3 ] This sub-nanosecond timescale for geminate charge pair separation is supported by a wide range The dynamics of charge carriers after their creation at, or near, an interface play a critical role in determining the effi ciency of organic solar cells as they dictate, via mechanisms that are not yet fully understood, the pathways for charge separation and recombination. Here, a combination of ultrafast transient spectroscopy and kinetic Monte Carlo simulations based on a...