Advanced Functional Materials · 2007 · 299 citations · 23 references
Natural SciencesMaterials EngineeringMaterials ScienceElectronic MaterialsPolymer ChemistryPolymer MaterialsConducting PolymersConductive PolymersOrganic SemiconductorsPhotovoltaic DevicesPhotovoltaic MaterialsSolar CellsElectron-hole RecombinationFill FactorOperating ConditionsOrganic Photovoltaic CellsOrganic PhotovoltaicsOrganic Solar CellsPhotocurrent GenerationVoltage
The study investigates the photogeneration mechanism in MDMO‑PPV:PCNEPV all‑polymer solar cell blends. The photocurrent is strongly voltage‑dependent because low carrier mobilities, dielectric constant, and polymer intermixing limit exciton dissociation, leading to a low fill factor, reduced photocurrent, and increased recombination losses, with Langevin recombination dominating at one sun.
Abstract The photogeneration mechanism in blends of poly[2‐methoxy‐5‐(3′,7′‐dimethyloctyloxy)‐1,4 ‐ phenylene vinylene] (MDMO‐PPV) and poly[oxa‐1,4‐phenylene‐(1‐cyano‐1,2‐vinylene)‐(2‐methoxy‐5‐(3′,7′‐dimethyloctyloxy)‐1,4‐phenylene)‐1,2‐(2‐cyanovinylene)‐1,4‐phenylene] (PCNEPV) is investigated. The photocurrent in the MDMO‐PPV:PCNEPV blends is strongly dependent on the applied voltage as a result of a low dissociation efficiency of the bound electron–hole pairs. The dissociation efficiency is limited by low carrier mobilities, low dielectric constant, and the strong intermixing of the polymers, leading to a low fill factor and a reduced photocurrent at operating conditions. Additionally, electrons trapped in the PCNEPV phase recombine with the mobile holes in the MDMO‐PPV phase at the interface between the two polymers, thereby affecting the open‐circuit voltage and increasing the recombination losses. At an intensity of one sun, Langevin recombination of mobile carriers dominates over trap‐assisted recombination.
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