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arXiv 2012.13519cond-mat.mes-hallphysics.optics
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通过声学石墨烯等离激元逼近单原子层场局域极限

Toward Monoatomic-Layer Field Confinement Limit via Acoustic Graphene Plasmons

In-Ho Lee, Tony Low, Luis Martín-Moreno, Phaedon Avouris, Sang-Hyun Oh

AI总结:

针对双层石墨烯远场激发下仅光学等离激元被主导激发的问题,提出用单/多纳米发射器选择性高效激发声学等离激元的策略,建立解析模型阐明发射器排布的作用,设计最优器件结构以逼近单原子层等离激元局域极限。

摘要:

双层石墨烯中的垂直等离激元耦合会产生两种杂化等离激元模式:光学等离激元和声学等离激元,二者在层间间隙处分别具有对称和反对称的电荷分布。然而,在大多数基于远场激发的实验中,双层石墨烯系统里只有光学等离激元被主导激发。本文提出了利用单个或多个纳米发射器选择性高效激发声学等离激元的策略。本文建立的解析模型阐明了发射器的位置和排布对所产生石墨烯等离激元对称性的作用。我们提出了一种最优器件结构,可实现双层石墨烯中声学等离激元的实验观测,进而逼近由单原子间隔层定义的等离激元局域终极水平——这是镜上石墨烯架构无法实现的。

英文摘要:

Vertical plasmonic coupling in double-layer graphene leads to two hybridized plasmonic modes: optical and acoustic plasmons with symmetric and anti-symmetric charge distributions across the interlayer gap, respectively. However, in most experiments based on far-field excitation, only the optical plasmons are dominantly excited in the double-layer graphene systems. Here, we propose strategies to selectively and efficiently excite acoustic plasmons with a single or multiple nano-emitters. The analytical model developed here elucidates the role of the position and arrangement of the emitters on the symmetry of the resulting graphene plasmons. We present an optimal device structure to enable experimental observation of acoustic plasmons in double-layer graphene toward the ultimate level of plasmonic confinement defined by a monoatomic spacer, which is inaccesible with a graphene-on-a-mirror architecture.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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