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Faraday rotation due to excitation of magnetoplasmons in graphene microribbons

机译:石墨烯微带中的磁等离子体激发法拉第旋转

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摘要

A single graphene sheet, when subjected to a perpendicular static magnetic field, provides a Faraday rotation that, per atomic layer, greatly surpasses that of any other known material. In continuous graphene, Faraday rotation originates from the cyclotron resonance of massless carriers, which allows dynamical tuning through either external electrostatic or magneto-static setting. Furthermore, the rotation direction can be controlled by changing the sign of the carriers in graphene, which can be done by means of an external electric field. However, despite these tuning possibilities, the requirement of large magnetic fields hinders the application of the Faraday effect in real devices, especially for frequencies higher than a few terahertz. In this work we demonstrate that large Faraday rotation can be achieved in arrays of graphene microribbons, through the excitation of the magnetoplasmons of individual ribbons, at larger frequencies than those dictated by the cyclotron resonance. In this way, for a given magnetic field and chemical potential, structuring graphene periodically can produce large Faraday rotation at larger frequencies than what would occur in a continuous graphene sheet. Alternatively, at a given frequency, graphene ribbons produce large Faraday rotation at much smaller magnetic fields than in continuous graphene.
机译:单个石墨烯片在受到垂直静磁场的作用下,其法拉第旋转在每个原子层上都大大超过任何其他已知材料。在连续的石墨烯中,法拉第旋转源自无质量载流子的回旋共振,这允许通过外部静电或静磁设置进行动态调谐。此外,可以通过改变石墨烯中的载流子的符号来控制旋转方向,这可以借助于外部电场来完成。然而,尽管有这些调谐的可能性,但是大磁场的要求仍然阻碍了法拉第效应在实际设备中的应用,尤其是对于高于几太赫兹的频率。在这项工作中,我们证明了通过激发单个条带的磁等离子体激元,在比回旋加速器共振所要求的频率更大的频率下,可以在石墨烯微带阵列中实现大的法拉第旋转。这样,对于给定的磁场和化学势,与连续石墨烯片中发生的频率相比,周期性地构造石墨烯可以以更大的频率产生大的法拉第旋转。或者,在给定的频率下,石墨烯带在比连续石墨烯小得多的磁场下产生大的法拉第旋转。

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