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多层石墨烯带中对称性破缺诱导的暗等离激元模式激发

Symmetry breaking induced excitations of dark plasmonic modes in multilayer graphene ribbons.

作者信息

Dai Y Y, Chen A, Xia Y Y, Han D Z, Liu X H, Shi L, Zi J

出版信息

Opt Express. 2016 Sep 5;24(18):20021-8. doi: 10.1364/OE.24.020021.

Abstract

Multilayer graphene can support multiple plasmon bands. If structured into graphene ribbons, they can support multiple localized plasmonic modes with interesting optical properties. However, not all such plasmonic modes can be excited directly due to the constrains of the structural symmetry. We show by numerical simulations that by breaking the symmetry all plasmonic modes can be excited. We discuss the general principles and properties of two-layer graphene ribbons and then extend to multilayer graphene ribbons. In multilayer graphene ribbons with different ribbon widths, a tunable broadband absorption can be attained due to the excitations of all plasmonic modes. Our results suggest that these symmetry-broken multilayer graphene ribbons could offer more degrees of freedom in designing photonic devices.

摘要

多层石墨烯可以支持多个等离激元带。如果将其构建成石墨烯带,它们可以支持具有有趣光学特性的多个局域等离激元模式。然而,由于结构对称性的限制,并非所有此类等离激元模式都能被直接激发。我们通过数值模拟表明,通过打破对称性,所有等离激元模式都可以被激发。我们讨论了双层石墨烯带的一般原理和特性,然后扩展到多层石墨烯带。在具有不同带宽度的多层石墨烯带中,由于所有等离激元模式的激发,可以实现可调谐的宽带吸收。我们的结果表明,这些对称性破缺的多层石墨烯带在光子器件设计中可以提供更多的自由度。

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