4.8 Article

Impacts of the Electron Transport Layer Surface Reconstruction on the Buried Interface in Perovskite Optoelectronic Devices

Journal

JOURNAL OF PHYSICAL CHEMISTRY LETTERS
Volume 12, Issue 49, Pages 11834-11842

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.jpclett.1c03565

Keywords

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Funding

  1. National Key Research and Development Program of China [2018YFB2202900, 2021YFA0715600]
  2. National Natural Science Foundation of China [52192610, 61704131, 61804111]
  3. Joint Research Funds of Department of Science & Technology of Shaanxi Province
  4. Northwestern Polytechnical University [2020GXLH-Z-018]
  5. Fundamental Research Funds for the Central Universities
  6. Innovation Fund of Xidian University

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This study investigated the performance enhancement mechanism of the device after surface reconstruction by passivating different halogen groups at the ETL/perovskite interface using density functional theory combined with ab initio molecular dynamics. Halogen passivation stabilized the geometric structure of the perovskite surface, optimized surface reconstruction, and theoretically relieved the interface carrier recombination by balancing interfacial interaction. The findings have implications for the design of buried interface optimization in perovskite optoelectronic devices.
Using density functional theory combined with ab initio molecular dynamics, we comprehensively investigated the performance enhancement mechanism of the device after surface reconstruction by passivating different halogen groups (i.e., F or Cl) at the ETL/perovskite interface. We demonstrated that the halogen group at the ETL layer could stabilize the geometric structure of the perovskite surface by balancing the interfacial interaction, ionic migration, and lead iodide framework. Even though halogen passivation decreased and increased the interface charge transfer at the O- and SnO-terminated MAPbI(3)/SnO2 interfaces, respectively, halogen passivation optimized surface reconstruction and could theoretically relieve the interface carrier recombination according to the changes in conduction band offsets generated by halogen passivation. Furthermore, the interfacial carrier recombination of the MAPbI(3)/SnO2 interface was also connected to the interfacial gap states, which were smaller for O-terminated MAPbI(3)/SnO2 interfaces with halogen passivation-induced surface reconstruction but larger for the SnO-terminated cases. Hence, our findings have implications for the design of buried interface optimization in perovskite optoelectronic devices.

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