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Sub-nanosecond electromagnetic-micromagnetic dynamic simulations using the finite-difference time-domain method

机译:使用有限差分时域方法的亚纳秒电磁微磁动力学模拟

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摘要

This paper presents an efficient and simple approach of implementing the Landau-Lifshitz-Gilbert (LLG) equation of magnetisation motion within the Finite-difference Time-domain (FDTD) method. This combined electromagnetic-micromagnetic simulation technique is particularly important for modeling electromagnetic interaction with lossy magnetic material in the presence of current and magnetic sources, particularly at very high frequencies. The efficient implementation involves simple two-point spatial interpolations that are applicable to two and three-dimensional FDTD grids, and uses a stable iterative algorithm for the time integration of the LLG equation. A ferromagnetic resonance numerical experiment on a rectangular Permalloy prism excited through its cross-section by a non-uniform pulse field from a transmission line was carried out for the purpose of verifying the combined FDTD-LLG computations. The numerical results were in good agreement with linearised analytical solutions of the LLG equation for uniform and non-uniform precession modes. This paper also presents a brief investigation on the use of non-staggered FDTD grid schemes to model magnetic material using the LLG equation, and indicates that the classical FDTD staggered scheme offers simplicity in implementation and more accuracy for modeling wave interaction with lossy magnetic material than the non-staggered schemes based on Maxwell’s equations formulation.
机译:本文提出了一种在时域有限差分(FDTD)方法中实现磁化运动的Landau-Lifshitz-Gilbert(LLG)方程的有效且简单的方法。这种组合的电磁-微磁模拟技术对于在存在电流和磁源的情况下(特别是在非常高的频率下)建模与有损耗磁性材料的电磁相互作用特别重要。有效的实现方式包括适用于二维和三维FDTD网格的简单两点空间插值,并为LLG方程的时间积分使用稳定的迭代算法。为了验证组合的FDTD-LLG计算,对矩形坡莫合金棱镜进行了铁磁共振数值实验,该棱镜在其横截面中受到来自传输线的非均匀脉冲场的激励。数值结果与统一和非统一进动模式的LLG方程的线性化解析解非常吻合。本文还简要介绍了使用非交错FDTD网格方案通过LLG方程对磁性材料进行建模的过程,并指出经典的FDTD交错方案为实现与有损耗磁性材料的波相互作用建模提供了简便性,并且比基于麦克斯韦方程组的非交错方案。

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  • 作者

    Aziz, Mustafa M.;

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  • 年度 2013
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  • 原文格式 PDF
  • 正文语种 en
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