Karim Maham M S, Ganose Alex M, Pieters Laura, Winnie Leung W W, Wade Jessica, Zhang Lina, Scanlon David O, Palgrave Robert G
Department of Chemistry, University College London, 20 Gordon Street, London WC1H 0AJ, United Kingdom.
Diamond House, Harwell Science and Innovation Campus, Diamond Light Source Ltd., Didcot, Oxfordshire OX11 0DE, United Kingdom.
Chem Mater. 2019 Nov 26;31(22):9430-9444. doi: 10.1021/acs.chemmater.9b03267. Epub 2019 Nov 5.
Mixed anion compounds in the vacancy ordered perovskite structure were synthesized and characterized experimentally and computationally with a focus on compounds where A = Cs. Pure anion CsSnX compounds were formed with X = Cl, Br, and I using a room temperature solution phase method. Mixed anion compounds were formed as solid solutions of CsSnCl and CsSnBr and a second series from CsSnBr and CsSnI. Single phase structures formed across the entirety of both composition series with no evidence of long-range anion ordering observed by diffraction. A distortion of the cubic ABX structure was identified in which the spacing of the BX octahedra changes to accommodate the A site cation without reduction of overall symmetry. Optical band gap values varied with anion composition between 4.89 eV in CsSnCl to 1.35 eV in CsSnI but proved highly nonlinear with changes in composition. In mixed halide compounds, it was found that lower energy optical transitions appeared that were not present in the pure halide compounds, and this was attributed to lowering of the local symmetry within the tin halide octahedra. The electronic structure was characterized by photoemission spectroscopy, and Raman spectroscopy revealed vibrational modes in the mixed halide compounds that could be assigned to particular mixed halide octahedra. This analysis was used to determine the distribution of octahedra types in mixed anion compounds, which was found to be consistent with a near-random distribution of halide anions throughout the structure, although some deviations from random halide distribution were noted in mixed iodide-bromide compounds, where the larger iodide anions preferentially adopted trans configurations.
合成了具有空位有序钙钛矿结构的混合阴离子化合物,并通过实验和计算对其进行了表征,重点研究了A = Cs的化合物。采用室温溶液相法制备了X = Cl、Br和I的纯阴离子CsSnX化合物。混合阴离子化合物由CsSnCl和CsSnBr形成固溶体,以及由CsSnBr和CsSnI形成的第二个系列。在两个组成系列的整个范围内均形成了单相结构,通过衍射未观察到长程阴离子有序的证据。确定了立方ABX结构的畸变,其中BX八面体的间距发生变化以容纳A位阳离子,而整体对称性未降低。光学带隙值随阴离子组成而变化,在CsSnCl中为4.89 eV,在CsSnI中为1.35 eV,但证明随组成变化具有高度非线性。在混合卤化物化合物中,发现出现了纯卤化物化合物中不存在的较低能量的光学跃迁,这归因于卤化锡八面体内局部对称性的降低。通过光电子能谱对电子结构进行了表征,拉曼光谱揭示了混合卤化物化合物中的振动模式,这些模式可归因于特定的混合卤化物八面体。该分析用于确定混合阴离子化合物中八面体类型的分布,发现其与整个结构中卤化物阴离子的近随机分布一致,尽管在混合碘化物 - 溴化物化合物中注意到与随机卤化物分布存在一些偏差,其中较大的碘化物阴离子优先采用反式构型。