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Free electromagnetic radiation from the graphene monolayer with spatially modulated conductivity in THz range

机译:来自石墨烯单层的自由电磁辐射,具有在THz范围内进行空间调制的电导率

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摘要

An infinite graphene layer is known to support graphene surface plasmon polariton (GSP) confined at the interface between the two dielectric half-spaces. In the case of finite width graphene stripe, the termination of the graphene layer acts both as a scattering source and as a "mirror", thus producing Fabry-Perot (FP)-type resonance. These resonant wavelengths in the presence of free-standing graphene stripe are investigated using the homogeneous convolution-type integral equation approach. The capabilities of the suggested numerical method are illustrated with the results for the transmission spectrum of TM electromagnetic waves travelling in the direction perpendicular to the graphene stripe. Special attention is paid to the case of spatially modulated conductivity of the graphene monolayer, and thus the feasibility of controlling the GSP response.
机译:已知无限大的石墨烯层支持限制在两个介电半空间之间的界面处的石墨烯表面等离振子极化(GSP)。在有限宽度的石墨烯条的情况下,石墨烯层的末端既充当散射源又充当“镜”,从而产生法布里-珀罗(FP)型共振。使用齐次卷积型积分方程方法研究了存在独立石墨烯条纹的情况下的这些共振波长。通过沿垂直于石墨烯条的方向传播的TM电磁波的透射光谱结果,说明了所建议的数值方法的功能。要特别注意石墨烯单层的空间调制电导率的情况,因此要注意控制GSP响应的可行性。

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