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甲基卤化铅钙钛矿中甲基铵阳离子动力学:固态核磁共振视角

Methylammonium Cation Dynamics in Methylammonium Lead Halide Perovskites: A Solid-State NMR Perspective.

作者信息

Bernard Guy M, Wasylishen Roderick E, Ratcliffe Christopher I, Terskikh Victor, Wu Qichao, Buriak Jillian M, Hauger Tate

机构信息

Gunning-Lemieux Chemistry Centre, University of Alberta , 11227 Saskatchewan Drive NW, Edmonton, Alberta, Canada T6G 2G2.

National Research Council Canada , 100 Sussex Drive, Ottawa, Ontario, Canada K1A 0R6.

出版信息

J Phys Chem A. 2018 Feb 15;122(6):1560-1573. doi: 10.1021/acs.jpca.7b11558. Epub 2018 Feb 2.

Abstract

In light of the intense recent interest in the methylammonium lead halides, CHNHPbX (X = Cl, Br, and I) as sensitizers for photovoltaic cells, the dynamics of the methylammonium (MA) cation in these perovskite salts has been reinvestigated as a function of temperature via H, N, and Pb NMR spectroscopy. In the cubic phase of all three salts, the MA cation undergoes pseudoisotropic tumbling (picosecond time scale). For example, the correlation time, τ, for the C-N axis of the iodide salt is 0.85 ± 0.30 ps at 330 K. The dynamics of the MA cation are essentially continuous across the cubic ↔ tetragonal phase transition; however, H and N NMR line shapes indicate that subtle ordering of the MA cation occurs in the tetragonal phase. The temperature dependence of the cation ordering is rationalized using a six-site model, with two equivalent sites along the c-axis and four equivalent sites either perpendicular or approximately perpendicular to this axis. As the cubic ↔ tetragonal phase transition temperature is approached, the six sites are nearly equally populated. Below the tetragonal ↔ orthorhombic phase transition, H NMR line shapes indicate that the C-N axis is essentially frozen.

摘要

鉴于近期人们对作为光伏电池敏化剂的卤化甲基铵铅(CH₃NH₃PbX,X = Cl、Br和I)兴趣浓厚,通过氢、氮和铅核磁共振光谱,重新研究了这些钙钛矿盐中甲基铵(MA)阳离子的动力学随温度的变化。在所有三种盐的立方相中,MA阳离子进行准各向同性翻滚(皮秒时间尺度)。例如,碘化物盐的C-N轴的相关时间τ在330K时为0.85±0.30皮秒。MA阳离子的动力学在立方相↔四方相转变过程中基本连续;然而,氢和氮核磁共振线形表明,MA阳离子在四方相中发生了细微的有序排列。使用六位点模型合理化了阳离子有序排列的温度依赖性,其中沿着c轴有两个等效位点,垂直或近似垂直于该轴有四个等效位点。随着接近立方相↔四方相转变温度,六个位点的占据情况几乎相同。在四方相↔正交相转变温度以下,氢核磁共振线形表明C-N轴基本冻结。

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