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BCC-Grid versus SC-Grid in the modeling of a sheet of graphene as a surface boundary condition in the context of ADE-FDTD

机译:BCC-Grid与SC-Grid在Ade-FDTD的上下文中为地表边界条件的图形模型

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Here, we model a thin layer of graphene located above a metal surface by means of a surface boundary condition in two different stencils, namely, a simple cubic grid (SC-Grid) and a body centered cubic grid (BCC-Grid). We extend the methodology described in the literature by taking into account the interband contribution of the graphene's conductivity in addition to the intraband contribution. The mathematical description of the presented developments is explained. Besides this, the metal in contact with the graphene sheet is considered as a dispersive medium; therefore, we deal with the problem by using the auxiliary differential equation finite-difference time-domain (ADE-FDTD) method. In this context, we compared the two stencils and demonstrated that BCC-Grid does not present discontinuities in the normal components of the electric and magnetic fields located on the graphene surface; in this respect, BCC-Grid is also more appropriate than the traditional Yee's cell for these type of applications.
机译:这里,我们通过两个不同的模板中的表面边界条件模拟位于金属表面上方的石墨烯层,即简单的立方网格(SC-Grid)和身体中心的立方网格(BCC-Grid)。除了内部贡献之外,我们通过考虑到石墨烯的电导率的基因带贡献来扩展文献中描述的方法。解释了所提出的发展的数学描述。除此之外,与石墨烯片接触的金属被认为是分散介质;因此,我们通过使用辅助微分方程有限差分时间域(ADE-FDTD)方法来处理问题。在这种情况下,我们比较了两个模板并证明了BCC-Grid在位于石墨烯表面上的电场和磁场的正常部件中不存在不连续性;在这方面,BCC-GRID也比传统的YEE的细胞更适合这些类型的应用。

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