流动电子磁力中自旋涨落的动力学效应

S. Hirooka, M. Shimizu
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引用次数: 3

摘要

本文提出了一种在泛函积分形式和高斯近似下考虑电子铁磁体自旋涨落量子效应的方法。利用赫兹和克莱恩(1977)引入的近似方法和作者先前工作中获得的结果,他们获得了动态自旋磁化率。自旋涨落的动力学是通过局域自旋涨落的振幅来考虑的,局域自旋涨落是控制系统热力学和磁性能的最基本参数。简单的数值算例表明,与所谓静态近似的结果相比,自发磁化率和顺磁化率的温度依赖性有了显著的改善。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Dynamical effect of spin fluctuations in itinerant electron magnetism
The authors present a method which takes account of the quantum effect of spin fluctuations on itinerant electron ferromagnets in the functional integral formalism and in the gaussian approximation. Using a similar approximation to that introduced by Hertz and Klenin (1977) and the results obtained in the authors' previous work they obtain the dynamical spin susceptibility. Dynamics of spin fluctuations are taken into account through the amplitudes of the local spin fluctuations which are the most fundamental parameters dominating the thermodynamical and magnetic properties of the system. It is shown by simple numerical examples that a remarkable improvement is established for the temperature dependence of the spontaneous magnetisation and the paramagnetic susceptibility as compared with the results obtained in the so-called static approximation.
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