The Floquet–Magnus and Fer Expansions: Application to Control the Spin Dynamics During the Phase Modulated Lee–Goldburg Radiation in Solid-State NMR

E. Mananga
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Abstract

Floquet–Magnus and Fer expansion (FE) schemes are used in nuclear magnetic resonance (NMR) for the calculation of effective Hamiltonians and propagators. This work focuses on applying the Floquet–Magnus and FE approaches to control the spin system evolution during the phase modulate Lee–Goldburg radiation experiment. Until now, the Frequency switched Lee–Goldburg and its variant called the Phase module Lee–Goldburg have been treated by only the average Hamiltonian theory and the bimodal Floquet approach. In this paper, we use the two developing expansion schemes in solid-state NMR for the calculation of the effective Hamiltonian and propagator during the spin dynamics. Our work unifies and generalizes existing results of the Floquet–Magnus and FEs and delivers illustrations of novel springs that boost previous applications that are based on the classical information. The generality of this work points to potential applications in problems related to solid-state NMR and theoretical developments of spectroscopy as well as interdisciplinary research areas whenever they include spin dynamics concepts.
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Floquet-Magnus和Fer展开:在固态核磁共振相位调制Lee-Goldburg辐射中控制自旋动力学的应用
在核磁共振(NMR)中,利用Floquet-Magnus和Fer展开(FE)格式计算有效哈密顿量和传播子。在相位调制Lee-Goldburg辐射实验中,应用Floquet-Magnus和有限元方法控制自旋系统的演化。到目前为止,频率开关Lee-Goldburg及其变体称为相位模块Lee-Goldburg仅用平均哈密顿理论和双峰Floquet方法来处理。在本文中,我们使用固体核磁共振的两种发展展开格式来计算自旋动力学中的有效哈密顿量和传播子。我们的工作统一并推广了Floquet-Magnus和FEs的现有结果,并提供了新颖弹簧的插图,从而促进了以前基于经典信息的应用。这项工作的通用性指出了与固态核磁共振和光谱学理论发展以及跨学科研究领域相关的问题的潜在应用,只要它们包括自旋动力学概念。
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审稿时长
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