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Abstract
A critical bottleneck for improving the performance of organic solar cells (OSC) is minimising non-radiative losses in the interfacial charge-transfer (CT) state via the formation of hybrid energetic states. This requires small energetic offsets often detrimental for high external quantum efficiency (EQE). Here, we obtain OSC with both non-radiative voltage losses (0.24 V) and photocurrent losses (EQE > 80%) simultaneously minimised. The interfacial CT states separate into free carriers with ≈40-ps time constant. We combine device and spectroscopic data to model the thermodynamics of charge separation and extraction, revealing that the relatively high performance of the devices arises from an optimal adjustment of the CT state energy, which determines how the available overall driving force is efficiently used to maximize both exciton splitting and charge separation. The model proposed is universal for donor:acceptor (D:A) with low driving forces and predicts which D:A will benefit from a morphology optimization for highly efficient OSC.
Understanding the mechanism of non-radiative losses in organic photovoltaics is crucial to improve the performance further. Here, the authors use combined device and spectroscopic data to reveal universal model to maximise exciton splitting and charge separation by adjusting the energy of charge transfer state.
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1 Imperial College London, Department of Chemistry and Centre for Plastic Electronics, London, UK (GRID:grid.7445.2) (ISNI:0000 0001 2113 8111); Institute of Materials for Electronics and Energy Technology (I-MEET), Friedrich Alexander-University Erlangen-Nuremberg, Erlangen, Germany (GRID:grid.5330.5) (ISNI:0000 0001 2107 3311)
2 IFN-CNR, Dipartimento di Fisica, Milano, Italy (GRID:grid.472645.6)
3 Friedrich Alexander-University Erlangen-Nuremberg, Department of Chemistry and Pharmacy, Erlangen, Germany (GRID:grid.5330.5) (ISNI:0000 0001 2107 3311)
4 IFN-CNR, Dipartimento di Fisica, Milano, Italy (GRID:grid.472645.6); Kyoto Institute of Technology, Department of Chemistry and Materials Technology, Kyoto, Japan (GRID:grid.419025.b) (ISNI:0000 0001 0723 4764)
5 Institute of Materials for Electronics and Energy Technology (I-MEET), Friedrich Alexander-University Erlangen-Nuremberg, Erlangen, Germany (GRID:grid.5330.5) (ISNI:0000 0001 2107 3311)
6 Institut für Physik und Astronomie Physik weicher Materie University of Potsdam, Potsdam, Germany (GRID:grid.11348.3f) (ISNI:0000 0001 0942 1117)
7 University of Oxford, Department of Chemistry, Chemistry Research Laboratory, Oxford, UK (GRID:grid.4991.5) (ISNI:0000 0004 1936 8948)
8 Advent Technologies SA, Patras, Greece (GRID:grid.4991.5); National Hellenic Research Foundation, Athens, Greece (GRID:grid.22459.38) (ISNI:0000 0001 2232 6894)
9 Advent Technologies SA, Patras, Greece (GRID:grid.22459.38); Institute of Chemical Biology, National Hellenic Research Foundation, Athens, Greece (GRID:grid.22459.38) (ISNI:0000 0001 2232 6894)
10 King Abdullah University of Science and Technology (KAUST), Division of Physical Sciences and Engineering (PSE), KAUST Solar Center (KSC), Thuwal, Saudi Arabia (GRID:grid.45672.32) (ISNI:0000 0001 1926 5090)
11 University of Oxford, Department of Chemistry, Chemistry Research Laboratory, Oxford, UK (GRID:grid.4991.5) (ISNI:0000 0004 1936 8948); King Abdullah University of Science and Technology (KAUST), Division of Physical Sciences and Engineering (PSE), KAUST Solar Center (KSC), Thuwal, Saudi Arabia (GRID:grid.45672.32) (ISNI:0000 0001 1926 5090)
12 Institute of Materials for Electronics and Energy Technology (I-MEET), Friedrich Alexander-University Erlangen-Nuremberg, Erlangen, Germany (GRID:grid.5330.5) (ISNI:0000 0001 2107 3311); Bavarian Center for Applied Energy Research (ZAE Bayern), Erlangen, Germany (GRID:grid.432437.5) (ISNI:0000 0000 9653 6862); Helmholtz-Institute Erlangen-Nürnberg (HI ERN), Erlangen, Germany (GRID:grid.461896.4)