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Uphill and downhill charge generation from charge transfer to charge separated states in organic solar cells.

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Abstract

It is common knowledge that molecular energy level offsets of a type II heterojunction formed at the donor-acceptor interface are considered to be the driving force for photoinduced charge transfer in organic solar cells. Usually, these offsets – present between molecular energy levels of the donor and acceptor – are obtained via cyclic voltammetry (CV) measurements of organic semiconductors cast in a film or dissolved in solution. Simply transferring such determined energy levels from solution or film of single materials to blend films may be obviously limited and not be possible in full generality. Herein, we report various cases of material combinations in which novel non-fullerene acceptors did not yield successful charge transfer, although energy levels obtained by CV on constituting single materials indicate a type II heterojunction. Whilst the integer charge transfer (ICT) model provides one explanation for a relative rise of molecular energy levels of acceptors, further details and other cases have not been studied so far in great detail. By applying energy-resolved electrochemical impedance spectroscopy (ER-EIS) on several donor-acceptor combinations, a Fano-like resonance feature associated with a distinctive molecular energy level of the acceptor as well as various relative molecular energy level shifts of different kinds could be observed. By analyzing ER-EIS and absorption spectra, not only the exciton binding energy within single materials could be determined, but also the commonly unknown binding energy of the CT state with regard to the joint density of states (jDOS) of the effective semiconductor. The latter is defined by transitions between the highest occupied molecular orbitals (HOMO) of the donor and the lowest unoccupied molecular orbitals (LUMO) of the acceptor. Using this technique among others, we identified cases in which charge generation may occur eitherviauphill or by downhill processes between the charge transfer exciton and the electronic gap of the effective semiconductor. Exceptionally high CT-exciton binding energies and thus low charge generation yields were obtained for a case in which the donor and acceptor yielded a too intimate blend morphology, indicating π-π stacking as a potential cause for unfavorable molecular energy level alignment.

Beteiligte Universitäten/Institutionen: Laboratory of Organic and Macromolecular Chemistry (IOMC), Friedrich Schiller University Jena, Humboldtstr. 10, Jena, D-07743, Germany; Center for Energy and Environmental Chemistry Jena (CEEC Jena), Friedrich Schiller University Jena, Philosophenweg 7a, Jena, D-07743, Germany; King Abdullah University of Science and Technology (KAUST), KAUST Solar Center (KSC), Physical Sciences and Engineering Division (PSE), Material Science and Engineering Program (MSE), Thuwal, 23955-6900, Saudi Arabia; Institute of Physics, Slovak Academy of Sciences, Dúbravská cesta 9, Bratislava, 845 11, Slovakia; Centre for Advanced Material Application, Slovak Academy of Sciences, Dúbravská cesta 9, Bratislava, 845 11, Slovakia; Faculty of Electrical Engineering and Information Technology, Slovak University of Technology, Bratislava, 812 19, Slovakia; Institute of Physics, Technische Universität Chemnitz, Chemnitz, 09126, Germany; Experimental Physics VI, Julius Maximilian University of Würzburg, Würzburg, 97074, Germany; Department of Chemistry, University of Calgary, 731 Campus Place N.W., Canada; Production Technology Group, Technische Universität Ilmenau, Gustav-Kirchhoff-Platz 2, Ilmenau, Germany; Institute for Micro and Nanotechnologies, Technische Universität Ilmenau, Gustav-Kirchhoff-Str.7, Ilmenau, D-98693, Germany; Peter Debye Institute for Soft Matter Physics, Universität Leipzig, Leipzig, 04103, Germany; Department of Physics and Astronomy, University of Sheffield, Sheffield, S102TN, United Kingdom; Linz Institute for Organic Solar Cells (LIOS), Johannes Kepler University Linz, Altenbergerstr. 69, Linz, 4040, Austria; Institute of Polymer Chemistry, Johannes Kepler University Linz, Altenbergerstr. 69, Linz, 4040, Austria; Institute of Polymeric Materials and Testing, Johannes Kepler University, Altenbergerstr. 69, Linz, 4040, Austria