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间隙和分子运动的μ子自旋弛豫研究

Muon spin relaxation studies of interstitial and molecular motion.

作者信息

Cox S F

机构信息

ISIS Facility, Rutherford Appleton Laboratory, Chilton, Oxfordshire, UK.

出版信息

Solid State Nucl Magn Reson. 1998 Mar;11(1-2):103-21. doi: 10.1016/s0926-2040(97)00100-8.

DOI:10.1016/s0926-2040(97)00100-8
PMID:9650794
Abstract

The unusual methods of preparation and analysis of spin polarization in muSR spectroscopy, which exploit the unique properties of the positive muon, are introduced in this article. Following a summary overview of applications, particular attention is paid to the problem of spin-lattice relaxation for a muon experiencing a hyperfine interaction with a single unpaired electron. The specific cases considered are the interstitial diffusion of muonium--the 1-electron atom which may be considered as a light isotope of hydrogen-and the molecular dynamics of organic radicals labelled by muonium. Rate equations for the evolution of population in the hyperfine-coupled spin states are solved numerically for various relaxation mechanisms. The formalism is equally valid for conventional ESR studies of paramagnetic states but is pursued specifically to simulate T1-relaxation in muSR. The simulations are compared with literature data. Also treated is the case of intermittent hyperfine coupling, appropriate to electron capture and loss in semiconductors or soliton motion in polymers; for this, a Monte Carlo approach is used to simulate the muon response. (For low-dimensional motion, the relaxation function is not exponential, so that a unique value of T1 cannot be defined.) Finally, a proposal is made to implement muon-T1 measurements in the rotating frame; this is designed for the selective study of electronically diamagnetic muonium states (i.e., those without hyperfine coupling) in the presence of a paramagnetic muonium or radical fraction.

摘要

本文介绍了μSR光谱学中自旋极化的非常规制备和分析方法,这些方法利用了正μ子的独特性质。在对应用进行简要概述之后,特别关注了与单个未配对电子发生超精细相互作用的μ子的自旋 - 晶格弛豫问题。所考虑的具体情况是μ子素(可视为氢的轻同位素的单电子原子)的间隙扩散以及由μ子素标记的有机自由基的分子动力学。针对各种弛豫机制,数值求解了超精细耦合自旋态中粒子数演化的速率方程。该形式体系对于顺磁态的传统ESR研究同样有效,但专门用于模拟μSR中的T1弛豫。将模拟结果与文献数据进行了比较。还处理了间歇性超精细耦合的情况,这适用于半导体中的电子俘获和损失或聚合物中的孤子运动;为此,使用蒙特卡罗方法来模拟μ子响应。(对于低维运动,弛豫函数不是指数形式,因此无法定义唯一的T1值。)最后,提出了在旋转框架中进行μ子 - T1测量的建议;这旨在选择性研究在存在顺磁μ子素或自由基部分的情况下电子抗磁μ子素态(即那些没有超精细耦合的态)。

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