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Revealing Local Dynamics of the Protonic Conductor CsH(PO3H) by Solid-State NMR Spectroscopy and First-Principles Calculations

机译:通过固态NMR光谱和第一原理计算揭示质子导体CSH(PO3H)的局部动力学

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© 2017 American Chemical Society. A joint study incorporating multinuclear solid-state NMR spectroscopy and first-principles calculations has been performed to investigate the local structure and dynamics of the protonic conductor CsH(PO 3 H) in the paraelectric phase. The existence of the superprotonic phase ( > 137 °C) is clearly confirmed by NMR, in good agreement with the literature. The variable-temperature 1 H, 2 H, and 31 P NMR data further reveal a distribution of motional correlation times, with isotropic rotation of the phosphite ion being observed below the superprotonic phase transition for a small but gradually increasing subset of anions. This isotropic rotation is associated with fast local protonic motion, with the distribution of correlation times being tentatively assigned to internal defects or surface adsorbed H 2 O. The phosphite ion dynamics of the majority slower subset of phosphite ions is quantified through analysis of variable-temperature 17 O spectra recorded from 34 to 150 °C, by considering a model for the pseudo C 3 rotation of the phosphite ion around the P-H bond axis below the phase transformation. An extracted activation energy of 0.24 ± 0.08 eV (23 ± 8 kJ mol -1 ) for this model was obtained, much lower than that reported from proton conductivity measurements, implying that no strong correlation exists between long-range protonic motion and C 3 rotations of the phosphite. We conclude that proton conduction in CsH(PO 3 H) in the paraelectric phase is governed by the activation energy for exchange between donor and acceptor oxygen sites, rotation of the phosphite units, and the lack of isotropic rotation of the phosphite ion. Surprisingly, coalescence of 17 O NMR resonances, as would be expected for rapid isotropic reorientations of all phosphite groups, is not observed above the transition. Potential reasons for this are discussed.
机译:©2017美国化学学会。掺入多核固态NMR光谱和第一原理计算的联合研究已经进行在顺电相,调查质子导体的CsH(PO 3 H)的局部结构和动力学。通过NMR,与文献吻合良好,清楚地证实了超级化相(> 137℃)的存在。可变温度1 H,2 H和31 P NMR数据进一步揭示了运动相关时间的分布,具有低于超声波相变的磷矿离子的各向同性旋转,用于小但逐渐增加阴离子的阴影。这种各向同性旋转与快速局部质子运动相关联,随着初步缺陷或表面吸附的H 2 O的相关时间分布。通过分析可变温度来定量大多数磷矿离子子集的亚磷酸离子动力学通过考虑亚磷矿离子围绕相变下的pH键合轴围绕pH键合轴的伪C 3旋转的模型,记录34至150°C的17 o光谱。获得该模型的0.24±0.08eV(23±8 kJ mol -1)的提取的活化能量,远低于质子电导率测量值,这意味着在远程质子运动和C 3旋转之间不存在强烈相关性亚磷矿。我们的结论在顺电相在csh(PO 3 H),该质子传导由活化能为供体和受体位点的氧,亚磷酸酯单元的旋转,并且缺乏亚磷酸根离子的各向同性旋转之间交换控制。令人惊讶的是,在过渡之上,未观察到17 O NMR共振的聚结,如将用于所有亚磷酸盐基团的快速各向同性重新定位。讨论了潜在原因。

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