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Decoupling and recoupling using continuous-wave irradiation in magic-angle-spinning solid-state NMR: A unified description using bimodal Floquet theory

机译:魔术角旋转固态NMR中使用连续波辐射的去耦和重耦合:使用双峰Floquet理论的统一描述

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摘要

The application of two or more different time-dependent coherent perturbations with, in general, incommensurable frequencies occurs quite commonly in NMR experiments. Here we develop a unified description of the entire class of experiments using bimodal Floquet theory and van Vleck-Primas perturbation theory. This treatment leads to a time-independent effective Hamiltonian in Hilbert space and can be looked at as a generalization of average Hamiltonian theory to several incommensurate time dependencies. As a prototype experiment we treat the application of continuous-wave (cw) radio-frequency irradiation in combination with magic-angle sample spinning. Practically relevant examples of this type of experiments are heteronuclear spin decoupling and recoupling experiments using cw irradiation, e.g., rotary-resonance recoupling. Perturbations up to the third order must be taken into account to explain all experimentally observed resonance conditions. (C) 2005 American Institute of Physics.
机译:通常在NMR实验中通常会应用两个或更多个不同的时间相关的相干扰动,这些扰动通常具有不可估量的频率。在这里,我们使用双峰Floquet理论和van Vleck-Primas微扰理论对整个实验类别进行统一描述。这种处理导致希尔伯特空间中与时间无关的有效哈密顿量,并且可以看作是平均哈密顿量理论对几个不相称的时间依赖性的推广。作为原型实验,我们将连续波(cw)射频辐射与魔角样品旋转结合起来进行处理。这类实验的实际相关实例是使用连续辐射(例如旋转共振再耦合)的异核自旋解耦和再耦合实验。必须考虑到三阶扰动才能解释所有实验观察到的共振条件。 (C)2005美国物理研究所。

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