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Updated: Jun 10, 2025

Influence of Hybrid Perovskite Fabrication Methods on Film Formation, Electronic Structure, and Solar Cell Performance
Published on: February 27, 2017
On the V OC loss in NiO-based inverted metal halide perovskite solar cells
Kousumi Mukherjee1, Denise Kreugel1, Nga Phung1
1Department of Applied Physics and Science Education, Eindhoven University of Technology P.O. Box 513 5600 MB Eindhoven The Netherlands k.mukherjee@tue.nl.
Abstract:
Recent reports have shown that nickel oxide (NiO) when adopted as a hole transport layer (HTL) in combination with organic layers, such as PTAA or self-assembled monolayers (SAMs), leads to a higher device yield for both single junction as well as tandem devices. Nevertheless, implementing NiO in devices without PTAA or SAM is seldom reported to lead to high-performance devices. In this work, we assess the effect of key NiO properties deemed relevant in literature, namely- resistivity and surface energy, on the device performance and systematically compare the NiO-based devices with those based on PTAA. To this purpose, (thermal) atomic layer deposited (ALD) NiO (NiOBu-MeAMD), Al-doped NiO (Al:NiOBu-MeAMD), and plasma-assisted ALD NiO (NiOMeCp) films, characterized by a wide range of resistivity, are investigated. Although Al:NiOBu-MeAMD (∼400 Ω cm) and NiOMeCp(∼80 Ωcm) films have a lower resistivity than NiOBu-MeAMD (∼10 kΩ cm), the Al:NiOBu-MeAMD and NiOMeCp-based devices are found to have a modest open circuit voltage (V OC) gain of ∼30 mV compared to NiOBu-MeAMD-based devices. Overall, the best-performing NiO-based devices (∼14.8% power conversion efficiency (PCE)) still lag behind the PTAA-based devices (∼17.5%), primarily due to a V OC loss of ∼100 mV. Further investigation based on light intensity analysis of the V OC and FF and the decrease in V OC compared to the quasi-Fermi level splitting (QFLS) indicates that the V OC is limited by trap-assisted recombination at the NiO/perovskite interface. Additionally, SCAPS simulations show that the presence of a high interfacial trap density leads to a V OC loss in NiO-based devices. Upon passivation of the NiO/perovskite interface with Me-4PACz, the V OC increases by 170-200 mV and is similar for NiOBu-MeAMD and Al:NiOBu-MeAMD, leading to the conclusion that there is no influence of the NiO resistivity on the V OC once interface passivation is realized. Finally, our work highlights the necessity of comparing NiO-based devices with state-of-the-art HTL-based devices to draw conclusion about the influence of specific material properties on device performance.
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