Band Alignment and Interfacial Stability of Co<sub>3</sub>O<sub>4</sub> vs NiO as a Hole Transport Layer with FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> Perovskite

The unstable cubic phase of halide perovskites (ABX<sub>3</sub>) and the poor interfacial quality between their absorbing layer and the hole transport layer (HTL) cause the long-term instability of halide perovskite solar cells (PSCs). To stabilize the intrinsic cubic perovskite structure, mixing CH<sub>3</sub>NH<sup>+</sup> (MA<sup>+</sup>) and CH(NH<sub>2</sub>)<sup>+</sup> (FA<sup>+</sup>) large organic ions at the A site is frequently used. Although NiO offers better stability than organic HTLs, such as poly(triaryl-amine) (PTAA), the stability of NiO-based PSCs still remains an issue, primarily due to the formation of interfacial Ni vacancies at the NiO/perovskite interface. In this theoretical study, by analyzing Co<sub>3</sub>O<sub>4</sub>/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> and NiO/perovskite interfaces, we show that Co<sub>3</sub>O<sub>4</sub> offers greater benefits as an HTL material than NiO for three main reasons. First, Co<sub>3</sub>O<sub>4</sub>/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> shows a type II band alignment with a small valence band offset (0.13 eV), whereas NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> interfaces give type I band alignments. Second, Co<sub>3</sub>O<sub>4</sub>/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> interfaces show higher adhesion energy (1.48 J/m<sup>2</sup>) than NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> interfaces, indicating enhanced interfacial stability. Third, the formation of interfacial Co vacancies in NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> presents greater difficulty due to their higher formation energy of 1.75 eV compared to the Ni vacancies in NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub>, suggesting better stability under environmental conditions. FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> also shows higher adhesion energies with Co<sub>3</sub>O<sub>4</sub> or NiO than those for MAPbI<sub>3</sub>. Therefore, we suggest that the combination of Co<sub>3</sub>O<sub>4</sub> as the HTL and FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> as the light-absorbing layer holds great potential for achieving PSCs with long-term stability.

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Publication Details

Journal
ACS Applied Materials & Interfaces
Published
2025-04-08
DOI
https://doi.org/10.1021/acsami.4c20008
Citations
6
Primary Topic
Perovskite Materials and Applications
Type
article
Field-Weighted Citation Impact
4.38
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article

Band Alignment and Interfacial Stability of Co3O4 vs NiO as a Hole Transport Layer with FA0.4MA0.6PbI3 Perovskite

Yuzheng Guo, Xuewei Zhang, Daping Chu, John Robertson et al.
6 citations
ACS Applied Materials & Interfaces
Perovskite Materials and Applications
4.38
article

Band Alignment and Interfacial Stability of Co3O4 vs NiO as a Hole Transport Layer with FA0.4MA0.6PbI3 Perovskite

Yuzheng Guo, Xuewei Zhang, Daping Chu, John Robertson, Xiaxia Cui, Qidong Tai
article en
6 citations

Abstract

The unstable cubic phase of halide perovskites (ABX<sub>3</sub>) and the poor interfacial quality between their absorbing layer and the hole transport layer (HTL) cause the long-term instability of halide perovskite solar cells (PSCs). To stabilize the intrinsic cubic perovskite structure, mixing CH<sub>3</sub>NH<sup>+</sup> (MA<sup>+</sup>) and CH(NH<sub>2</sub>)<sup>+</sup> (FA<sup>+</sup>) large organic ions at the A site is frequently used. Although NiO offers better stability than organic HTLs, such as poly(triaryl-amine) (PTAA), the stability of NiO-based PSCs still remains an issue, primarily due to the formation of interfacial Ni vacancies at the NiO/perovskite interface. In this theoretical study, by analyzing Co<sub>3</sub>O<sub>4</sub>/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> and NiO/perovskite interfaces, we show that Co<sub>3</sub>O<sub>4</sub> offers greater benefits as an HTL material than NiO for three main reasons. First, Co<sub>3</sub>O<sub>4</sub>/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> shows a type II band alignment with a small valence band offset (0.13 eV), whereas NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> interfaces give type I band alignments. Second, Co<sub>3</sub>O<sub>4</sub>/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> interfaces show higher adhesion energy (1.48 J/m<sup>2</sup>) than NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> interfaces, indicating enhanced interfacial stability. Third, the formation of interfacial Co vacancies in NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> presents greater difficulty due to their higher formation energy of 1.75 eV compared to the Ni vacancies in NiO/FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub>, suggesting better stability under environmental conditions. FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> also shows higher adhesion energies with Co<sub>3</sub>O<sub>4</sub> or NiO than those for MAPbI<sub>3</sub>. Therefore, we suggest that the combination of Co<sub>3</sub>O<sub>4</sub> as the HTL and FA<sub>0.4</sub>MA<sub>0.6</sub>PbI<sub>3</sub> as the light-absorbing layer holds great potential for achieving PSCs with long-term stability.

ACS Applied Materials & InterfacesVol. 17(16)
Anhui University of Science and Technology (CN), University of Cambridge (GB), Wuhan University (CN), Swiss Federal Laboratories for Materials Science and Technology (CH)
Openalex Percentile: Top 6%
Perovskite Materials and Applications
4.38
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