We characterize and compare blended and bilayered heterojunctions of polymer photovoltaic devices using poly͓oxa-1,4-phenylene-1,2-͑1-cyano͒-ethenylene-2,5-dioctyloxy-1,4-phenylene-1,2-͑2-cyano͒-ethenylene-1,4-phenylene͔ ͑CN-ether-PPV͒ and poly͓2,5-dimethoxy-1,4-phenylene-1,2-ethenylene-2-methoxy-5-͑2-ethylhexyloxy͒-1,4-phenylene-1,2-ethenylene͔ ͑M3EH-PPV͒ as electron-and hole-transporting polymers, respectively. We find that both blended and bilayered structures have substantially improved current densities ͑Ͼ3 mA/ cm 2 ͒ and power efficiencies ͑ϳ1% under white light͒ over neat films. Improved exciton dissociation at multiple interfaces and reduced recombination due to energy and charge transfers increases the charge-carrier collection in both types of heterojunction devices, but low electron mobilities in the polymers lead to low fill factors and reduced quantum efficiency ͑ϳ20% ͒ that limit the power efficiency. Time-resolved photoluminescence reveals that for blended structures both the hole and electron-transporting polymers undergo efficient quenching with the exciton decay being dominated by the existence of two fast decay channels of 0.12 and 0.78 ns that are assigned to interspecies charge transfer and account for the increased short-circuit current observed. For layers, these components are not as prevalent. This result indicates that greater exciton generation at the dissociating interface and more efficient charge collection in the thin layers is primarily responsible for the improved short-circuit current, a conclusion that is further supported by numerical simulations of the exciton generation rate and charge collection. We also report evidence for an intermediate exciplex state in both types of structures with the greatest yield for blends with 50 wt % of CN-ether-PPV. Overall, the improved performance is due to different processes in the two structures; efficient bulk exciton quenching and charge transfer in blends and enhanced exciton generation and charge collection in layers. The optimization of each photovoltaic heterostructured device relies on this understanding of the mechanisms by which each material architecture achieves high power efficiencies.

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