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Does Excess Energy Assist Photogeneration in an Organic Low‐Bandgap Solar Cell?
Author(s) -
Hahn Tobias,
Geiger Johannes,
Blase Xavier,
Duchemin Ivan,
Niedzialek Dorota,
Tscheuschner Steffen,
Beljonne David,
Bässler Heinz,
Köhler Anna
Publication year - 2015
Publication title -
advanced functional materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 6.069
H-Index - 322
eISSN - 1616-3028
pISSN - 1616-301X
DOI - 10.1002/adfm.201403784
Subject(s) - delocalized electron , photocurrent , organic solar cell , band gap , acceptor , materials science , solar cell , electron , molecular physics , multiple exciton generation , chemical physics , atomic physics , chemistry , optoelectronics , condensed matter physics , physics , polymer , quantum mechanics , composite material , organic chemistry
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 C 60 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 S 1 – S 0 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.