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基于石墨烯的超表面中具有超强场局域化的拓扑保护表面等离激元模式。

Topologically protected plasmon mode with ultrastrong field localization in a graphene-based metasurface.

作者信息

Lu Yanxin, Chen Yihang

出版信息

Opt Express. 2021 Feb 15;29(4):6188-6198. doi: 10.1364/OE.418836.

DOI:10.1364/OE.418836
PMID:33726145
Abstract

Graphene plasmons, the electromagnetic waves coupled to charge excitations in a graphene sheet, have attracted great interest because of their intriguing properties, such as electrical tunability, long plasmon lifetime, and high degree of spatial confinement. They may enable the manufacture of novel optical devices with extremely high speed, low driving voltage, low power consumption and compact sizes. In this paper, we propose a graphene-based metasurface which can support a topologically protected graphene plasmon mode with the ability of ultrastrong field localization. We show that such a plasmonic metasurface, constructed by depositing a graphene sheet on a periodic silicon substrate, would exhibit different bandgap topological characteristics as the filling factor of the periodic substrate changes. By setting suitable Fermi levels of graphene at two different areas of the metasurface, topological interface plasmon modes can be excited, resulting in over 8 orders of magnitude enhancement of the plasmon intensity. The topologically protected plasmon mode is robust against the perturbation of the structural parameters, and its frequency can be tuned by adjusting the gate-voltage on the graphene sheet. This highly integrated platform could provide a pathway for low-power and actively controllable nonlinear optics.

摘要

石墨烯等离激元,即耦合到石墨烯片中电荷激发的电磁波,因其具有诸如电学可调性、较长的等离激元寿命和高度的空间限制等引人入胜的特性而备受关注。它们可能使制造具有极高速、低驱动电压、低功耗和紧凑尺寸的新型光学器件成为可能。在本文中,我们提出了一种基于石墨烯的超表面,它可以支持具有超强场局域化能力的拓扑保护石墨烯等离激元模式。我们表明,通过在周期性硅衬底上沉积石墨烯片构建的这种等离激元超表面,会随着周期性衬底的填充因子变化而展现出不同的带隙拓扑特性。通过在超表面的两个不同区域设置合适的石墨烯费米能级,可以激发拓扑界面等离激元模式,从而使等离激元强度增强超过8个数量级。拓扑保护的等离激元模式对结构参数的扰动具有鲁棒性,并且其频率可以通过调节石墨烯片上的栅极电压来调谐。这个高度集成的平台可为低功耗和主动可控的非线性光学提供一条途径。

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Opt Express. 2021 Feb 15;29(4):6188-6198. doi: 10.1364/OE.418836.
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