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首页> 外文期刊>Physica, B. Condensed Matter >Magnon spectrum of a symmetric-spin nanocontact on a ferromagnetic ultrathin film
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Magnon spectrum of a symmetric-spin nanocontact on a ferromagnetic ultrathin film

机译:铁磁超薄膜上对称自旋纳米接触的磁能谱

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A theoretical model is presented for the study of the magnetic properties and the coherent magnon transport via monatomic chains in ultrathin magnetic films. In particular, we studied a finite number of monatomic chains joining two slabs of ferromagnetic material. Each slab consists of five atomic layers of a cubic lattice with magnetically ordered spins coupled by the Heisenberg exchange. The system is supported on a non-magnetic substrate and otherwise considered free from magnetic interactions. The spin dynamics of the ultrathin film is studied by the matching method. The individual and the total magnon transmissions of the ultrathin ferromagnetic film, scattering coherently at the nanojunction zone, and the localized spin states in the boundary domain are calculated and analyzed. The interatomic magnetic exchange is varied on the boundary domain specifically for three cases of magnetic exchange to investigate the consequences of magnetic softening and hardening for the calculated properties. Numerical results show characteristic interference effects between the incident spinwaves and the localized spin states of the nanocontact. The calculated properties are presented for arbitrary incidence of the magnons on the boundary, for all accessible frequencies in the propagating bands, and for the interatomic magnetic exchange of the magnetic film. The localized magnon branches created by the nanocontact domain are observed in the Brillouin zone.
机译:提出了一种理论模型,用于研究超薄磁性膜中单原子链的磁性和相干磁振子的传输。特别是,我们研究了有限数量的连接两个铁磁材料平板的单原子链。每个平板都由立方晶格的五个原子层组成,这些原子层的磁有序自旋通过海森堡交换耦合。该系统被支撑在非磁性衬底上,否则被认为没有磁性相互作用。通过匹配法研究了超薄膜的自旋动力学。计算并分析了超薄铁磁薄膜的单个和全部磁振子传输,它们在纳米结区相干地散射,并在边界域中局限了自旋态。原子间磁交换在边界域上发生变化,特别是针对三种情况的磁交换,以研究磁软化和硬化对计算所得特性的影响。数值结果表明入射自旋波与纳米接触的局部自旋态之间的特征干涉效应。给出了计算得出的特性,用于边界上的强子的任意入射,传播带中所有可及的频率以及磁性膜的原子间磁性交换。在布里渊区观察到了由纳米接触域产生的局部磁振子分支。

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