Fernandes Arantxa, Moran Robert F, McKay David, Griffiths Ben L, Herlihy Anna, Whittle Karl R, Dawson Daniel M, Ashbrook Sharon E
School of Chemistry, EaStCHEM and Centre of Magnetic Resonance, University of St Andrews, St Andrews, UK.
School of Engineering, University of Liverpool, Liverpool, UK.
Magn Reson Chem. 2021 Sep;59(9-10):961-974. doi: 10.1002/mrc.5140. Epub 2021 Feb 15.
Characterising the local structures (e.g., the cation distribution) of mixed-metal ceramics by NMR spectroscopy is often challenging owing to the unfavourable properties (low γ, large quadrupole moment and/or low abundance) of many metal nuclei. O is an attractive option owing to the prevalence of oxygen within ceramics. The moderate γ and small quadrupole moment of O mean that the greatest barrier to accessing the information available from this nucleus is isotopic enrichment. We explore the challenges of ensuring uniform isotopic enrichment with O (g) for the pyrochlore solid solutions, Y Sn Ti O , La Sn Zr O and La Sn Hf O , demonstrating that high enrichment temperatures (900 °C for 12 hr) are required. In addition, for sites with very high symmetry (such as the tetrahedral OY4 and OLa4 sites with C ≈ 0 present here), we demonstrate that quantitative O NMR spectra require correction for the differing contributions from the centreband of the satellite transitions, which can be as high as a factor of ~3.89. It is common to use first-principles calculations to aid in interpreting NMR spectra of disordered solids. Here, we use an ensemble modelling approach to ensure that all possible cation arrangements are modelled in the minimum possible number of calculations. By combining uniform isotopic enrichment, quantitative NMR spectroscopy and a comprehensive computational approach, we are able to show that the cation distribution in Y Sn Ti O is essentially random, whereas in La Sn Zr O and La Sn Hf O , OLa2SnZr and OLa2SnHf sites are slightly energetically disfavoured, leading to a weak preference for clustering of like cations.
通过核磁共振光谱法表征混合金属陶瓷的局部结构(例如阳离子分布)通常具有挑战性,这是因为许多金属核具有不利的性质(低γ值、大的四极矩和/或低丰度)。由于氧在陶瓷中普遍存在,因此用氧进行表征是一个有吸引力的选择。氧的γ值适中且四极矩小,这意味着获取该原子核可用信息的最大障碍是同位素富集。我们探讨了确保用(^{17})O(g)对烧绿石固溶体Y(_2)Sn(_2)Ti(_2)O(_7)、La(_2)Sn(_2)Zr(_2)O(_7)和La(_2)Sn(_2)Hf(_2)O(7)进行均匀同位素富集的挑战,证明需要高温富集(900℃,12小时)。此外,对于具有非常高对称性的位点(例如这里存在的具有(C{4v}\approx0)的四面体OY4和OLa4位点),我们证明定量(^{17})O核磁共振谱需要对卫星跃迁中心带的不同贡献进行校正,其差异可能高达约3.89倍。使用第一性原理计算来辅助解释无序固体的核磁共振谱是很常见的。在这里,我们使用一种系综建模方法,以确保在尽可能少的计算中对所有可能的阳离子排列进行建模。通过结合均匀同位素富集、定量核磁共振光谱和全面的计算方法,我们能够表明Y(_2)Sn(_2)Ti(_2)O(_7)中的阳离子分布基本上是随机的,而在La(_2)Sn(_2)Zr(_2)O(_7)和La(_2)Sn(_2)Hf(_2)O(_7)中,OLa2SnZr和OLa2SnHf位点在能量上略有不利,导致同类阳离子聚类的微弱偏好。