固体丙氨酸(多接触)交叉极化动力学和自旋晶格弛豫的解析描述

Jérôme Hirschinger, Jésus Raya
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引用次数: 1

摘要

本文利用经典和非经典耦合模型推导了量子主方程的精确和近似解析解,用于描述Hartmann-Hahn交叉极化(HHCP)和多重接触CP (MCCP)动力学。此外,Naito和McDowell最初得到的解析解[J]。化学。物理学报,84(1986)4181。用HHCP动力学第二阶段的振幅和HHCP/MCCP交叉时间表征了自旋扩散和T1ρ弛豫的不同状态。1H - 13c HHCP和MCCP动力学与(Lee-Goldburg) 1H T1ρ弛豫实验数据的分析提供了固体丙氨酸自旋动力学的一致图像,并解释了先前观察到的T1ρ和T1弛豫测量之间的明显差异。CH和CH3质子像预期的那样通过向NH3质子的自旋扩散而弛豫,但一般质子自旋温度的假设(其中弛豫的瓶颈在NH3位点)通常适用于T1弛豫,不适用于T1ρ弛豫。观察到一种扩散限制的情况,即核塞曼能量转移到晶格的速度比自旋扩散提供的速度快。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

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Analytical descriptions of (multiple-contact) cross-polarization dynamics and spin-lattice relaxation in solid alanine

In this work, several exact and approximate analytical solutions to the quantum master equation are derived using both classical and non-classical coupling models to describe the kinetics of Hartmann-Hahn cross-polarization (HHCP) and multiple-contact CP (MCCP). Moreover, the analytical solution originally obtained by Naito and McDowell [J. Chem. Phys. 84 (1986) 4181.] is shown to be incorrect and the different regimes of spin diffusion and T1ρ relaxation are characterized by the amplitude of the second stage of the HHCP dynamics and the HHCP/MCCP crossing time. The analysis of the 1H–13C HHCP and MCCP dynamics together with (Lee-Goldburg) 1H T1ρ relaxation experimental data provides a consistent picture of spin dynamics in solid alanine and explains the apparent discrepancies previously observed between T1ρ and T1 relaxation measurements. The CH and CH3 protons relax as expected via spin diffusion towards the NH3 protons but the assumption of common proton spin temperature, in which the bottleneck of relaxation is at the NH3 sites, generally valid for T1 relaxation breaks down for T1ρ relaxation. A diffusion-limited situation in which nuclear Zeeman energy is transferred to the lattice faster than can be supplied by spin diffusion is observed instead.

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