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In Situ Growth Mechanism for High‐Quality Hybrid Perovskite Single‐Crystal Thin Films with High Area to Thickness Ratio: Looking for the Sweet Spot

The development of in situ growth methods for the fabrication of high‐quality perovskite single‐crystal thin films (SCTFs) directly on hole‐transport layers (HTLs) to boost the performance of optoelectronic devices is critically important. However, the fabrication of large‐area high‐quality SCTFs wi...

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Detalles Bibliográficos
Autores principales: Tang, Xiaobing, Wang, Zhaojin, Wu, Dan, Wu, Zhenghui, Ren, Zhenwei, Li, Ruxue, Liu, Pai, Mei, Guanding, Sun, Jiayun, Yu, Jiahao, Zheng, Fankai, Choy, Wallace C. H., Chen, Rui, Sun, Xiao Wei, Yang, Fuqian, Wang, Kai
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9069385/
https://www.ncbi.nlm.nih.gov/pubmed/35261191
http://dx.doi.org/10.1002/advs.202104788
Descripción
Sumario:The development of in situ growth methods for the fabrication of high‐quality perovskite single‐crystal thin films (SCTFs) directly on hole‐transport layers (HTLs) to boost the performance of optoelectronic devices is critically important. However, the fabrication of large‐area high‐quality SCTFs with thin thickness still remains a significant challenge due to the elusive growth mechanism of this process. In this work, the influence of three key factors on in situ growth of high‐quality large‐size MAPbBr(3) SCTFs on HTLs is investigated. An optimal “sweet spot” is determined: low interface energy between the precursor solution and substrate, a slow heating rate, and a moderate precursor solution concentration. As a result, the as‐obtained perovskite SCTFs with a thickness of 540 nm achieve a record area to thickness ratio of 1.94 × 10(4) mm, a record X‐ray diffraction peak full width at half maximum of 0.017°, and an ultralong carrier lifetime of 1552 ns. These characteristics enable the as‐obtained perovskite SCTFs to exhibit a record carrier mobility of 141 cm(2) V(−1) s(−1) and good long‐term structural stability over 360 days.