Power-conversion efficiencies of organic heterojunction solar cells can be increased by using semiconducting donor-acceptor materials with complementary absorption spectra extending to the near-infrared region. Here, we used continuous wave fluorescence and absorption, as well as nanosecond transient absorption spectroscopy to study the initial charge transfer step for blends of a donor poly(p-phenylenevinylene) derivative and low-band gap cyanine dyes serving as electron acceptors. Electron transfer is the dominant relaxation process after photoexcitation of the donor. Hole transfer after cyanine photoexcitation occurs with an efficiency close to unity up to dye concentrations of B30 wt%. Cyanines present an efficient self-quenching mechanism of their fluorescence, and for higher dye loadings in the blend, or pure cyanine films, this process effectively reduces the hole transfer. Comparison between dye emission in an inert polystyrene matrix and the donor matrix allowed us to separate the influence of self-quenching and charge transfer mechanisms. Favorable photovoltaic bilayer performance, including high open-circuit voltages of B1 V confirmed the results from optical experiments. The characteristics of solar cells using different dyes also highlighted the need for balanced adjustment of the energy levels and their offsets at the heterojunction when using low-bandgap materials, and accentuated important effects of interface interactions and solid-state packing on charge generation and transport.
IntroductionThe potential of cheap photovoltaics is fueling the interest in organic semiconductors. [1][2][3][4] State-of-the-art devices are made from a combination of electron-donor and electron-acceptor (D-A) materials, sandwiched between metallic electrodes. 5 Photoexcitation of either of the two components leads to an exciton that can dissociate into free charge carriers at the D-A interface. 6 After charge separation, electrons and holes are transported via drift and diffusion processes to the electrodes, where they are collected, giving rise to an electric current. 2 Device efficiency is determined by the short-circuit current (J sc ), the open-circuit voltage (V oc ), and the fill factor (FF) via Z = (J sc V oc FF)/P, where P is the incident optical power. The FF is a measure of the ability to transport and extract charges when the applied voltage approaches V oc ; J sc is determined by the fraction of absorbed photons from the incident sunlight as well as by the ability to create charges via exciton dissociation at the D-A interface. Consensus has now been reached that V oc correlates with the energy difference (E D ) between the highest occupied molecular orbital (HOMO) of the donor and the lowest unoccupied molecular orbital (LUMO) of the acceptor. [7][8][9] It follows that both J sc and V oc depend on the donor and acceptor energy levels and their offsets at the heterojunction (for illustration, see Fig. 1c). A high V oc requires a high E D . However, this implies that the HOMO-HOMO (E HH ) and LUMO-LUMO (E...