Abstract

<h2>Summary</h2> Identification of electronic processes at buried interfaces of charge-selective contacts is crucial for photovoltaic and photocatalysis research. Here, transient surface photovoltage (SPV) is used to study the passivation of different hole-selective carbazole-based SAMs. It is shown that transient SPV and transient photoluminescence provide complementary information on charge transfer kinetics and trapping/de-trapping mechanisms, and that trap-assisted non-radiative recombination losses originate from electron trapping at the SAM-modified ITO/perovskite interface. The hole transfer rates and the density of interface electron traps, obtained by fitting SPV transients with a minimalistic kinetic model, depended strongly on the SAM's chemical structure, and densities of interface traps as low as 10<sup>9</sup> cm<sup>−2</sup>, on par with highly passivated c-Si surfaces, were reached for Me-4PACz, previously used in record perovskite/silicon tandem solar cells. The extracted hole transfer rate constants and interface trap densities correlated well with the corresponding fill factors and open-circuit voltages of high-efficiency solar cells.

Highlights

  • The passivation of contacts is decisive for achieving high solar energy conversion efficiencies of solar cells

  • The contact potential difference (CPD) spectrum was converted to the absolute work function (WF) using a freshly peeled highly oriented pyrolytic graphite (HOPG) reference sample (WFHOPG = 4.65 G 0.05 eV).[33]

  • In this work, hole-selective contact systems for halide perovskite (HaP) films based on Self-assembled monolayers (SAMs) bound to indium tin oxide (ITO) electrodes were studied by transient surface photovoltage (SPV)

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Summary

Introduction

The passivation of contacts is decisive for achieving high solar energy conversion efficiencies of solar cells. A model based only on rate equations is introduced and applied to the simulation and fitting of SPV transients in order to extract values for transfer rate constants and densities of electron traps at SAM-modified ITO/HaP interfaces.

Results
Conclusion

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