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The Energy of Charge‐Transfer States in Electron Donor–Acceptor Blends: Insight into the Energy Losses in Organic Solar Cells
965
Citations
69
References
2009
Year
Charge‐transfer StatesE CtEngineeringOrganic ElectronicsEnergy ConversionOrganic Solar CellCt EnergyExcitation Energy TransferPhotovoltaic DevicesChemistryEnergy E CtElectronic Excited StatePhotoelectrochemistryPhotovoltaicsEnergy LossesChemical EngineeringElectronic DevicesSolar Cell StructuresCharge SeparationCharge ExtractionPhotochemistryOrganic SemiconductorOrganic Solar CellsQuantum ChemistryElectrochemistryOrganic Charge-transfer CompoundNatural SciencesSolar CellsSolar Cell Materials
The authors propose a general experimental approach to determine the charge‑transfer energy (E_CT) in donor–acceptor blends using ground‑state absorption and electrochemical data. E_CT is calibrated against the photon energy of maximum CT luminescence to correct for a constant Coulombic term. They find that E_CT correlates linearly with Voc (eVoc = ECT – 0.5 eV), that photoinduced electron transfer occurs when Eg – ECT > 0.1 eV, that CT recombination to the triplet is possible when ECT – ET > 0.1 eV, and conclude that optimal blends require Voc ≈ Eg – 0.6 eV and ΔEST < 0.2 eV—conditions not yet met in conjugated materials.
Abstract Here, a general experimental method to determine the energy E CT of intermolecular charge‐transfer (CT) states in electron donor–acceptor (D–A) blends from ground state absorption and electrochemical measurements is proposed. This CT energy is calibrated against the photon energy of maximum CT luminescence from selected D–A blends to correct for a constant Coulombic term. It is shown that E CT correlates linearly with the open‐circuit voltage ( V oc ) of photovoltaic devices in D–A blends via eV oc = E CT − 0.5 eV. Using the CT energy, it is found that photoinduced electron transfer (PET) from the lowest singlet excited state (S 1 with energy E g ) in the blend to the CT state (S 1 → CT) occurs when E g − E CT > 0.1 eV. Additionally, it is shown that subsequent charge recombination from the CT state to the lowest triplet excited state ( E T ) of D or A (CT → T 1 ) can occur when E CT − E T > 0.1 eV. From these relations, it is concluded that in D–A blends optimized for photovoltaic action: i) the maximum attainable V oc is ultimately set by the optical band gap ( eV oc = E g − 0.6 eV) and ii) the singlet–triplet energy gap should be Δ E ST < 0.2 eV to prevent recombination to the triplet state. These favorable conditions have not yet been met in conjugated materials and set the stage for further developments in this area.
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