首页> 外文期刊>Journal of magnetism and magnetic materials >Influence of anisotropic dipolar interaction on the spin dynamics of Ni_(80)Fe_(20) nan°dot arrays arranged in honeycomb and octagonal lattices
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Influence of anisotropic dipolar interaction on the spin dynamics of Ni_(80)Fe_(20) nan°dot arrays arranged in honeycomb and octagonal lattices

机译:各向异性偶极相互作用对蜂窝状和八边形格子状Ni_(80)Fe_(20)纳米点阵列自旋动力学的影响

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Ultrafast spin dynamics in ferromagnetic nanodot arrays with dot diameter 100 nm and thickness 20 nm arranged in honeycomb and octagonal lattice symmetries are studied to explore the tunability of the collective magnetization dynamics. By varying the inter-dot separation between 30 nm and 300 nm drastic variation in the precessional dynamics from strongly collective to completely isolated regime has been observed by using all-optical time-resolved magneto-optical Kerr microscope. Micromagnetic simulation is exploited to gain insights about the resonant mode profiles and magnetic coupling between the nanodots. A significant spectral and spatial variation in the resonant mode with increasing dipolar interaction is demonstrated with increasing inter-dot separation. The spins driven by effective field inside single nanodots are prone to precess independently, generating two self-standing centre and edge modes in the array that are influenced by the relative orientation between the inter-dot coupling direction and bias magnetic field. The anisotropic behavior of dipolar field is rigorously investigated here. Splitting of the centre mode in case of octagonal lattice is experimentally observed here as a consequence of the anisotropic dipolar field between the nanodot pairs coupled horizontally and vertically, which is not found in the honeycomb lattice. In addition, proper understanding of the modification of dynamic mode profile by neighboring dipolar interaction built up here, is imperative for further control of the dynamic dipolar interaction and the corresponding collective excitation in magnonic crystals. The usage of nanodot lattices with complex basis structures can be advantageous for the designing of high density magnetic recording media, spin-wave filter and logic devices.
机译:研究了以蜂窝和八边形晶格对称排列的,直径为100 nm,厚度为20 nm的铁磁纳米点阵列的超快自旋动力学,以研究集体磁化动力学的可调性。通过在30 nm和300 nm之间改变点间距,通过使用全光时间分辨磁光Kerr显微镜观察到了进动动力学从强烈集体到完全孤立的剧烈变化。利用微磁仿真来获得有关谐振模式轮廓和纳米点之间的磁耦合的见解。随着点间间距的增加,随着偶极相互作用的增加,共振模式中的光谱和空间变化也明显。由单个纳米点内部的有效场驱动的自旋易于独立进动,从而在阵列中生成两个自立的中心模式和边缘模式,这些模式受点间耦合方向和偏置磁场之间的相对方向的影响。这里严格研究了偶极场的各向异性行为。由于在水平和垂直方向上耦合的纳米点对之间存在各向异性的偶极场,因此在实验中观察到八角形晶格时中心模式的分裂,这在蜂窝晶格中找不到。另外,正确理解由此处建立的相邻偶极相互作用引起的动态模式轮廓的改变,对于进一步控制动态偶极相互作用和强磁晶体中相应的集体激发是必不可少的。具有复杂基础结构的纳米点阵的使用对于设计高密度磁记录介质,自旋波滤波器和逻辑器件可能是有利的。

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