剩余的二极极线宽度在魔法角度旋转的质子固态NMR中.
Matías Chávez1, Thomas Wiegand1, Alexander A Malär1
1Physical Chemistry, ETH Zürich, Vladimir-Prelog-Weg 2, 8093 Zürich, Switzerland.
Magnetic resonance (Gottingen, Germany)
|October 31, 2023
概括
固态NMR中的魔法角旋转会导致由于二极相互作用而导致残余线的扩大. 在高旋转频率时,二阶条数占主导地位,影响线宽和位置.
科学领域:
- 固态核磁共振 (NMR) 光谱学
- 量子力学和旋转动力学的量子力学.
背景情况:
- 魔法角旋转 (MAS) 对于在固态NMR中平均化异型相互作用至关重要.
- 在合自旋系统中的同核二极相互作用会导致由于非通通的哈密尔顿人而导致残余线的扩大.
研究的目的:
- 在MAS下分析合质子自旋系统中的剩余线宽.
- 调查二阶和高阶术语对光谱线形状和位置的影响.
主要方法:
- 使用Floquet理论对有效的哈密尔顿数到第三阶的理论计算.
- 对于小自旋系统,与数值获得的有效哈密尔顿数进行比较.
- 对模型物质中质子光谱的实验数据的分析.
主要成果:
- 第二阶项在旋转频率>75 kHz时主导剩余线宽,显示出特定的依赖性.
- 化学转移截断部分模仿了线宽上的第三阶效应.
- 二级贡献导致线条扩大和重心转移.
结论:
- 第二阶二极相互作用是剩余线扩大和高MAS频率的移动的主要原因.
- 了解这些效应对于在固态NMR中准确的光谱解释至关重要.
- 实验观察与二次哈密尔顿效应的理论预测一致.
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