Strong and tunable coupling between antiferromagnetic magnons and surface plasmons

H. Y. Yuan, Yaroslav M. Blanter, H. Q. Lin
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Abstract

Surface plasmons are the collective electron excitations in metallic systems and the associated electromagnetic wave usually has the transverse magnetic (TM) polarization. On the other hand, spin waves are the spin excitations perpendicular to the equilibrium magnetization and are usually circularly polarized in a ferromagnet. The direct coupling of these two modes is difficult due to the difficulty of matching electromagnetic boundary conditions at the interface of magnetic and non-magnetic materials. Here, we overcome this challenge by utilizing the linearly polarized spin waves in antiferromagnets (AFM) and show that a strong coupling between AFM magnons and surface plasmons can be realized in a hybrid 2D material/AFM structure, featuring a clear anticrossing spectrum at resonance. The coupling strength, characterized by the gap of anticrossing at resonance, can be tuned by electric gating on 2D materials and be probed by measuring the two reflection minima in the reflection spectrum. Further, as a potential application, we show that plasmonic modes can assist the coupling of two well-separated AFMs over several micrometers, featuring symmetric and antisymmetric hybrid modes. Our results may open a new platform to study antiferromagnetic spintronics and its interplay with plasmonic photonics.
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反铁磁磁子与表面质子之间的强可调耦合
表面等离子体是金属系统中电子的集体激发,相关电磁波通常具有横向磁(TM)极化。另一方面,自旋波是垂直于平衡磁化的自旋激发,在铁磁体中通常是圆极化的。由于磁性材料和非磁性材料界面的电磁边界条件难以匹配,这两种模式的直接耦合十分困难。在这里,我们利用反铁磁体(AFM)中的线性极化自旋波克服了这一难题,并证明在二维材料/AFM 混合结构中可以实现 AFM 磁子与表面等离子体之间的强耦合,其特点是共振时具有清晰的交叉谱。耦合强度以共振时的反交间隙为特征,可通过二维材料上的电门控进行调整,并通过测量反射谱中的两个反射极小值进行探测。此外,作为一种潜在的应用,我们还展示了plasmonic 模式可以帮助两个分离良好的原子力显微镜在几微米范围内耦合,具有对称和非对称混合模式的特点。我们的研究成果为研究反铁磁自旋电子学及其与等离子光子学的相互作用开辟了一个新平台。
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