Does Excess Energy Assist Photogeneration in an Organic Low-Bandgap Solar Cell?

The field dependence of the photocurrent in a bilayer assembly is measured with the aim to clarify the role of excess photon energy in an organic solar cell comprising a polymeric donor and an acceptor. Upon optical excitation of the donor an electron is transferred to the acceptor forming a Coulomb...

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Veröffentlicht in:Advanced functional materials 2015-02, Vol.25 (8), p.1287-1295
Hauptverfasser: Hahn, Tobias, Geiger, Johannes, Blase, Xavier, Duchemin, Ivan, Niedzialek, Dorota, Tscheuschner, Steffen, Beljonne, David, Bässler, Heinz, Köhler, Anna
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Sprache:eng
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Zusammenfassung:The field dependence of the photocurrent in a bilayer assembly is measured with the aim to clarify the role of excess photon energy in an organic solar cell comprising a polymeric donor and an acceptor. Upon optical excitation of the donor an electron is transferred to the acceptor forming a Coulomb‐bound electron–hole pair. Since the subsequent escape is a field assisted process it follows that photogeneration saturates at higher electric fields, the saturation field being a measure of the separation of the electron–hole pair. Using the low bandgap polymers, PCDTBT and PCPDTBT, as donors and C60 as acceptor in a bilayer assembly it is found that the saturation field decreases when the photon energy is roughly 0.5 eV above the S1–S0 0–0 transition of the donor. This translates into an increase of the size of the electron‐hole‐pair up to about 13 nm which is close to the Coulomb capture radius. This increase correlates with the onset of higher electronic states that have a highly delocalized character, as confirmed by quantum‐chemical calculations. This demonstrates that accessing higher electronic states does favor photogeneration yet excess vibrational energy plays no role. Experiments on intrinsic photogeneration in donor photodiodes without acceptors support this reasoning. Exciton dissociation in bilayer solar cells is facilitated by exciting into higher‐lying, more delocalized excited states of the donor polymer. This is shown by measuring the field dependence of the photocurrent in PCDTBT/C60 cells and in PCPDTBT/C60 cells for different excitation energies and comparing this to the delocalization of the associated excited states as determined by quantum‐chemical calculations.
ISSN:1616-301X
1616-3028
DOI:10.1002/adfm.201403784