TY - JOUR
T1 - On the VOC loss in NiO-based inverted metal halide perovskite solar cells
AU - Mukherjee, Kousumi
AU - Kreugel, Denise
AU - Phung, Nga
AU - van Helvoirt, Cristian A.A.
AU - Zardetto, V.
AU - Creatore, M.
PY - 2024/11/7
Y1 - 2024/11/7
N2 - 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 (VOC) 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 VOC loss of ∼100 mV. Further investigation based on light intensity analysis of the VOC and FF and the decrease in VOC compared to the quasi-Fermi level splitting (QFLS) indicates that the VOC 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 VOC loss in NiO-based devices. Upon passivation of the NiO/perovskite interface with Me-4PACz, the VOC 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 VOC 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.
AB - 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 (VOC) 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 VOC loss of ∼100 mV. Further investigation based on light intensity analysis of the VOC and FF and the decrease in VOC compared to the quasi-Fermi level splitting (QFLS) indicates that the VOC 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 VOC loss in NiO-based devices. Upon passivation of the NiO/perovskite interface with Me-4PACz, the VOC 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 VOC 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.
UR - https://www.scopus.com/pages/publications/85206480782
U2 - 10.1039/D4MA00873A
DO - 10.1039/D4MA00873A
M3 - Article
C2 - 39415776
SN - 2633-5409
VL - 5
SP - 8652
EP - 8664
JO - Materials Advances
JF - Materials Advances
IS - 21
ER -