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Self-defect-passivation by Br-enrichment in FA-doped Cs(1−x)FA(x)PbBr(3) quantum dots: towards high-performance quantum dot light-emitting diodes
Halide vacancy defect is one of the major origins of non-radiative recombination in the lead halide perovskite light emitting devices (LEDs). Hence the defect passivation is highly demanded for the high-performance perovskite LEDs. Here, we demonstrated that FA doping led to the enrichment of Br in...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7479606/ https://www.ncbi.nlm.nih.gov/pubmed/32901051 http://dx.doi.org/10.1038/s41598-020-71666-8 |
Sumario: | Halide vacancy defect is one of the major origins of non-radiative recombination in the lead halide perovskite light emitting devices (LEDs). Hence the defect passivation is highly demanded for the high-performance perovskite LEDs. Here, we demonstrated that FA doping led to the enrichment of Br in Cs(1−x)FA(x)PbBr(3) QDs. Due to the defect passivation by the enriched Br, the trap density in Cs(1−x)FA(x)PbBr(3) significantly decreased after FA doping, and which improved the optical properties of Cs(1−x)FA(x)PbBr(3) QDs and their QD-LEDs. PLQY of Cs(1–x)FA(x)PbBr(3) QDs increased from 76.8% (x = 0) to 85.1% (x = 0.04), and L(max) and CE(max) of Cs(1–x)FA(x)PbBr(3) QD-LEDs were improved from L(max) = 2880 cd m(−2) and CE(max) = 1.98 cd A(−1) (x = 0) to L(max) = 5200 cd m(−2) and CE(max) = 3.87 cd A(−1) (x = 0.04). Cs(1–x)FA(x)PbBr(3) QD-LED device structure was optimized by using PVK as a HTL and ZnO modified with b-PEI as an ETL. The energy band diagram of Cs(1–x)FA(x)PbBr(3) QD-LEDs deduced by UPS analyses. |
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