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Abstract The interfaces between absorber and transport layers are shown to be critical for perovskite device performance. However, quantitative characterization of interface recombination has so far proven to be highly challenging in working perovskite solar cells. Here, methylammonium lead halide (CH 3 NH 3 PbI 3 ) perovskite solar cells are studied based on a range of different hole‐transport layers, namely, an inorganic hole‐transport layer CuO x , an organic hole‐transport layer poly(triarylamine) (PTAA), and a bilayer of CuO x /PTAA. The cells are completed by a 6,6‐phenyl‐C 61 ‐butyric acid methyl ester (PCBM)/bathocuproine/Ag electron contact. Energy levels are characterized using photoelectron spectroscopy and recombination dynamics by combining steady‐state photoluminescence and transient photoluminescence with numerical simulations. While the PTAA‐based devices hardly show any interface recombination losses and open‐circuit voltages >1.2 V, substantial losses are observed for the samples with a direct CuO x /perovskite interface. These losses are assigned to a combination of energetic misalignment at the CuO x /perovskite interface coupled with increased interface recombination velocities at the perovskite/PCBM interface.
Haddad et al. (Sun,) studied this question.