High-quality bulk hybrid perovskite single crystals within minutes by inverse temperature crystallization
By M. Saidaminov, A. Abdelhady, B. Murali, E. Alarousu, Victor M. Burlakov, W. Peng, I. Dursun, Lingfei Wang, Yao He, Giacomo Maculan and 4 more. Nature Communications, 2015
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Single crystals of methylammonium lead trihalide perovskites (MAPbX3; MA=CH3NH3+, X=Br− or I−) have shown remarkably low trap density and charge transport properties; however, growth of such high-quality semiconductors is a time-consuming process. Here we present a rapid crystal growth process to obtain MAPbX3 single crystals, an order of magnitude faster than previous reports. The process is based on our observation of the substantial decrease of MAPbX3 solubility, in certain solvents, at elevated temperatures. The crystals can be both size- and shape-controlled by manipulating the different crystallization parameters. Despite the rapidity of the method, the grown crystals exhibit transport properties and trap densities comparable to the highest quality MAPbX3 reported to date. The phenomenon of inverse or retrograde solubility and its correlated inverse temperature crystallization strategy present a major step forward for advancing the field on perovskite crystallization. Hybrid perovskites are a promising class of materials for photovoltaic applications. Here, addressing the need for high-quality hybrid perovskite materials, the authors achieve the rapid growth of hybrid perovskite single crystals of high quality by inverse temperature crystallization.
Subfields: Electrical and Electronic Engineering, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/f589139750008c380b866c72a0e7f2b56c669ef7
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Citations in the corpus
- Large polarons in lead halide perovskites (2017, background): “5 scaling lawpredicted fromacoustic phonon scattering in nonpolar semiconductors (52), analysis based on this mechanism yields charge carrier mobilities of the order of 10(3) cm(2) V s (53–56), which is one order of magnitude higher than the experimental values (5, 6, 8, 23, 49, 50).”
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