Electromagnetic TE- and TM-waves propagation in a plane waveguide covered with graphene characterized by nonlinear conductivity

Yury G. Smirnov, S. Tikhov
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Abstract

Background. Guiding properties of waveguiding structures with graphene are of great importance for various applications and have been studied in many papers. In all such studies, graphene was characterized, as a rule, by linear surface conductivity. However, if the intensity of an electromagnetic wave is large enough, the interaction of graphene with the electromagnetic wave becomes nonlinear; in this case, it is more correct to describe graphene by nonlinear conductivity. Aim. This work is aimed at studying the influence of cubic nonlinearity of graphene, corresponding to the so-called self-action effects (not affecting the frequency of the incident wave), on the propagation of TE- and TM-polarized waves in the structure, which is a plain dielectric layer covered on one side by graphene. Methods. In this study, the guiding properties of the waveguide are studied using primarily an analytical approach. Thus, from Maxwell’s equations, material equations and boundary conditions, a couple of dispersion equations for TE-and TM-polarized waves is derived and then its solvability is studied. In addition, some numerical experiments are carried out in the study. Results. The dispersion equations of the studied waveguiding structure for TE- and TM-polarized waves are derived in explicit form. Studying analytically obtained equations, conditions for waveguide parameters are found, providing the existence of a given number of waveguide modes. In addition, some numerical results are obtained in the paper, which give an idea of the influence of nonlinear effects on the electromagnetic waves propagating in the structure. Conclusion. The results obtained in this paper reveal two effects related to the cubic nonlinearity of graphene. Firstly, in a plain dielectric layer with graphene coating in the strong nonlinear regime TE-waves with longer wavelength and TM-waves with shorter wavelength propagate compared to electromagnetic waves that propagate in the same structure in the linear regime. Secondly, the strong cubic nonlinearity leads to a greater localization of the electromagnetic wave within the waveguiding structure.
以非线性传导性为特征的石墨烯平面波导中的电磁 TE 波和 TM 波传播
背景。石墨烯波导结构的导波特性对各种应用都非常重要,已有许多论文对此进行了研究。在所有这些研究中,石墨烯通常以线性表面导电性为特征。然而,如果电磁波的强度足够大,石墨烯与电磁波的相互作用就会变成非线性;在这种情况下,用非线性导电性来描述石墨烯更为正确。目的。这项工作旨在研究石墨烯的立方非线性(相当于所谓的自作用效应(不影响入射波的频率))对 TE 极化波和 TM 极化波在石墨烯单面覆盖的普通介电层结构中传播的影响。研究方法本研究主要采用分析方法研究波导的导向特性。因此,根据麦克斯韦方程、材料方程和边界条件,推导出一对 TE 和 TM 偏振波的频散方程,然后研究其可解性。此外,研究还进行了一些数值实验。研究结果所研究波导结构的 TE 偏振和 TM 偏振波色散方程是以显式形式推导出来的。通过研究分析得到的方程,找到了波导参数的条件,从而确保存在一定数量的波导模式。此外,文中还得出了一些数值结果,从而了解了非线性效应对在该结构中传播的电磁波的影响。结论本文获得的结果揭示了与石墨烯立方非线性有关的两种效应。首先,在带有石墨烯涂层的普通电介质层中,在强非线性状态下,与线性状态下在相同结构中传播的电磁波相比,TE 波的波长更长,TM 波的波长更短。其次,强立方非线性导致电磁波在波导结构内更加局部化。
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