Spin-wave contributions to nuclear magnetic relaxation in magnetic metals

V. Irkhin, M. Katsnelson
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引用次数: 9

Abstract

Abstract:The longitudinal and transverse nuclear magnetic relaxation rates 1/T1(T) and 1/T2(T) are calculated for three- and two-dimensional (3D and 2D) metallic ferro- and antiferromagnets (FM and AFM) with localized magnetic moments in the spin-wave temperature region. The contribution of the one-magnon decay processes is strongly enhanced in comparison with the standard T-linear Korringa term, especially for the FM case. For the 3D AFM case this contribution diverges logarithmically, the divergence being cut at the magnon gap ω due to magnetic anisotropy, and for the 2D AFM case as ω-1. The electron-magnon scattering processes yield T2ln(T/ω) and T2/ω1/2-terms in 1/T1 for the 3D AFM and 2D FM cases, respectively. The two-magnon (“Raman”) contributions are investigated and demonstrated to be large in the 2D FM case. Peculiarities of the isotropic 2D limit (where the correlation length is very large) are analyzed.
自旋波对磁性金属核磁弛豫的贡献
摘要:计算了三维和二维(3D和2D)金属铁磁体和反铁磁体(FM和AFM)的纵向和横向核磁弛豫率1/T1(T)和1/T2(T)。与标准t -线性Korringa项相比,单磁振子衰变过程的贡献大大增强,特别是在FM情况下。对于三维原子力显微镜,这一贡献呈对数发散,由于磁各向异性,发散在磁振子间隙ω处被切断,对于二维原子力显微镜,发散为ω-1。三维AFM和二维FM的电子-磁振子散射过程在1/T1下分别产生T2ln(T/ω)和T2/ω1/2项。研究了二维调频情况下的双磁振子(“拉曼”)贡献,并证明其很大。分析了各向同性二维极限(其中相关长度非常大)的特性。
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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