氘交叉极化魔角旋转

D. Marks , N. Zumbulyadis , S. Vega
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引用次数: 18

摘要

本文提出了一个理论模型,描述了一个自旋系统(1)上的交叉极化魔角自旋(CPMAS)核磁共振实验,该自旋系统由一组i = 12的非丰自旋和一个s = 1的稀有自旋组成。用Floquet理论描述了魔角自旋实验过程中的自旋演化。该模型是最近引入的用于描述s (12)INspin系统的CPMAS的形式主义的扩展。首先,给出了2h CPMAS对部分氘化二甲基砜和丙二酸的实验结果。监测了2h自由感应衰变信号的旋转回波强度,并绘制了混合时间内施加在氘核和质子上的射频场强度差的函数图。然后给出了s = 1自旋系统的Floquet描述,以便引入CPMAS NMR的Floquet模型。定义了旋转四极自旋的Floquet哈密顿量,讨论了旋转坐标系中自旋锁定与Floquet空间中的自旋锁定的区别。随后描述了在CPMAS实验中这些(1)in系统的自旋演化。推导了这些实验的修正Hartmann-Hahn条件,并给出了计算交叉极化s-自旋信号强度的方法。讨论仅限于具有相对较小的四极相互作用的自旋为1的原子核,并针对2h CPMAS。研究了四极频率为40 kHz和120 kHz的粉末样品的s -自旋信号强度与哈特曼-哈恩条件不匹配的关系。
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Deuterium Cross-Polarization Magic-Angle Spinning

In this publication a theoretical model is presented that describes cross-polarization magic-angle spinning (CPMAS) NMR experiments on a spin systemS(1)IN, consisting of a set ofNabundant homonuclear spins withI= 12 coupled to a single rare spin withS= 1. The spin evolution during this magic-angle spinning experiment is described using Floquet theory. The model is an extension of the formalism that was recently introduced to describe CPMAS ofS(12)INspin systems. First, experimental results of2H CPMAS experiments on partially deuterated dimethyl sulfone and malonic acid are shown. The rotational-echo intensities of the2H free-induction-decay signals were monitored and plotted as a function of the difference between the intensities of the RF fields applied on the deuterons and the protons during the mixing time. Then the Floquet description of a spin system withS= 1 is presented in order to enable the introduction of the Floquet model for CPMAS NMR. The Floquet Hamiltonian of the rotating quadrupolar spin is defined and the difference between spin locking in the rotating frame and in Floquet space is discussed. This is followed by a description of the spin evolution of theS(1)INsystem during CPMAS experiments. The modified Hartmann–Hahn conditions for these experiments are derived and a methodology for calculating the cross-polarization S-spin signal intensities is demonstrated. The discussion is restricted to spin-1 nuclei with relatively small quadrupole interactions and is directed toward2H CPMAS. S-spin signal intensities as a function of mismatched Hartmann–Hahn conditions are evaluated for powder samples with quadrupolar frequencies of 40 and 120 kHz.

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