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.
Authors
- Yuzheng Guo (ORCID: https://orcid.org/0000-0001-9224-3816)
- Xuewei Zhang (ORCID: https://orcid.org/0000-0001-9162-3681)
- Daping Chu (ORCID: https://orcid.org/0000-0001-9989-6238)
- John Robertson (ORCID: https://orcid.org/0000-0001-6558-528X)
- Xiaxia Cui
- Qidong Tai (ORCID: https://orcid.org/0000-0003-2199-2777)
Institutions
- Anhui University of Science and Technology (CN)
- University of Cambridge (GB)
- Wuhan University (CN)
- Swiss Federal Laboratories for Materials Science and Technology (CH)
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