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Synthesis of highly confined surface plasmon modes with doped graphene sheets in the midinfrared and terahertz frequencies

机译:在中红外和太赫兹频率下用掺杂的石墨烯片合成高度受限的表面等离子体激元模式

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We investigate through analytic calculations the surface plasmon dispersion relation for monolayer graphene sheets and a separated parallel pair of graphene monolayers. An approximate form for the dispersion relation for the monolayer case was derived, which was shown to be highly accurate and offers intuition to the properties of the supported plasmon mode. For parallel graphene pairs separated by small gaps, the dispersion relation of the surface plasmon splits into two branches, one with a symmetric and the other with an antisymmetric magnetic field across the gap. For the symmetric (magnetic field) branch, the confinement may be improved at reduced absorption loss over a wide spectrum, unlike conventional surface plasmon modes supported on metallic surfaces that are subjected to the tradeoff between loss and confinement. This symmetric mode becomes strongly suppressed for very small separations, however. On the other hand, its antisymmetric counterpart exhibits reduced absorption loss for very small separations or long wavelengths, serving as a complement to the symmetric branch. Our results suggest that graphene plasmon structures could be promising for waveguiding and sensing applications in the midinfrared and terahertz frequencies.
机译:我们通过分析计算研究了单层石墨烯片和分离的平行石墨烯单层对的表面等离子体扩散关系。得出了单层情况下色散关系的近似形式,该形式被证明是非常准确的,并为所支持的等离激元模式的性质提供了直觉。对于由小间隙分开的平行石墨烯对,表面等离激元的色散关系分为两个分支,一个分支具有对称的磁场,另一个分支具有反对称的磁场。对于对称(磁场)分支,可以在宽的光谱范围内以减小的吸收损失来改善限制,这与在损失和限制之间进行权衡的金属表面上支撑的常规表面等离激元模式不同。但是,对于非常小的间距,此对称模式将受到强烈抑制。另一方面,它的反对称对应物在非常小的间隔或长波长处表现出降低的吸收损耗,可作为对称分支的补充。我们的结果表明,石墨烯等离激元结构在中红外和太赫兹频率的波导和传感应用中可能很有希望。

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