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Spin-Wave Resonances Affected by Skin-Effect in Conducting Magnetic Nanowire Arrays at Terahertz Frequencies

机译:受太赫兹频率的磁性纳米线阵列中的趋肤效应影响的自旋波共振。

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The properties of localized standing spin wave (SW) resonances are investigated numerically for a regular 2-D array of 10 nm diameter, 300 nm long metallic (iron) nanowires, magnetized at different orientations of the bias magnetic field ${mmb H}_{bf 0}$ with respect to the wire axis. At 30 THz the penetration depth of the electromagnetic (EM) waves can be close to the diameter of the nanowires, leading to interesting resonance effects as a result of the inhomogeneous $rf$ magnetization distribution across the nanowire diameter. The mathematical model considers the metallic character of the wires and the exchange interactions between the wires, when solving Maxwell equations simultaneously with the Landau-Lifshitz equation for the magnetization. The transmission coefficients $vert{rm T}_{21}vert$ of TEM waves through arrays with different wire radius were determined. There are well-defined extrema of $vert{rm T}_{21}vert$ at certain values of the bias magnetic field ${mmb H}_{bf 0}$, corresponding to ferromagnetic resonance (FMR) and antiresonance (FMAR) modes. The position of these maxima and minima does not depend on the orientation of ${bf H}_{bf 0}$, although $vert{rm T}_{21}vert$ is sensitive to the direction of ${mmb H}_{bf 0}$. The distribution of the $rf$ magnetization component across the nanowire is calculated for the second and low order exchange SW-n-n modes.
机译:对于直径为10 nm,长度为300 nm的金属(铁)纳米线的规则二维阵列,在偏置磁场$ {mmb H} _的不同方向上磁化,数值研究了局部驻旋波(SW)共振的特性。 {bf 0} $相对于线轴。在30 THz时,电磁波(EM)的穿透深度可能接近纳米线的直径,由于纳米线直径上$ rf $磁化分布不均匀,导致有趣的共振效应。当同时求解Maxwell方程和Landau-Lifshitz方程进行磁化时,该数学模型考虑了导线的金属特性以及导线之间的交换相互作用。确定通过具有不同线径的阵列的TEM波的透射系数$ vert {rm T} _ {21} vert $。在偏置磁场$ {mmb H} _ {bf 0} $的某些值处存在明确定义的极值$ vert {rm T} _ {21} vert $,对应于铁磁共振(FMR)和反共振(FMAR )模式。这些最大值和最小值的位置并不取决于$ {bf H} _ {bf 0} $的方向,尽管$ vert {rm T} _ {21} vert $对$ {mmb H}的方向敏感_ {bf 0} $。对于第二和低阶交换SW-n-n模式,计算了rf $磁化分量在纳米线上的分布。

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