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Ferromagnet/Superconductor Hybrid Magnonic Metamaterials

机译:铁磁体/超导体混合磁超材料

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摘要

In this work, a class of metamaterials is proposed on the basis of ferromagnet/superconductor hybridization for applications in magnonics. These metamaterials comprise of a ferromagnetic magnon medium that is coupled inductively to a superconducting periodic microstructure. Spectroscopy of magnetization dynamics in such hybrid evidences formation of areas in the medium with alternating dispersions for spin wave propagation, which is the basic requirement for the development of metamaterials known as magnonic crystals. The spectrum allows for derivation of the impact of the superconducting structure on the dispersion: it takes place due to a diamagnetic response of superconductors on the external and stray magnetic fields. In addition, the spectrum displays a dependence on the superconducting critical state of the structure: the Meissner and the mixed states of a type II superconductor are distinguished. This dependence hints toward nonlinear response of hybrid metamaterials on the magnetic field. Investigation of the spin wave dispersion in hybrid metamaterials shows formation of allowed and forbidden bands for spin wave propagation. The band structures are governed by the geometry of spin wave propagation: in the backward volume geometry the band structure is conventional, while in the surface geometry the band structure is nonreciprocal and is formed by indirect band gaps.
机译:在这项工作中,在铁磁体/超导体混合的基础上提出了一类超材料,用于超磁材料。这些超材料包含铁磁磁振子介质,该介质被感应耦合至超导周期性微结构。在这种混合体中的磁化动力学的光谱学证明了在介质中形成具有交替分散体的区域以进​​行自旋波传播,这是开发称为镁铁晶体的超材料的基本要求。该频谱可以推导超导结构对分散体的影响:它是由于超导体对外部磁场和杂散磁场的反磁响应而发生的。此外,光谱还显示出对结构超导临界状态的依赖性:区分了迈斯纳(Meissner)和II型超导体的混合态。这种依赖性暗示了混合超材料对磁场的非线性响应。对混合超材料中自旋波色散的研究表明,形成了自旋波传播的允许带和禁止带。能带结构受自旋波传播的几何形状支配:在后向体积几何中,能带结构是常规的,而在表面几何形状中,能带结构是不可逆的,并且是由间接能带隙形成的。

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