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A finite element scheme to study the nonlinear optical response of a. finite grating without and with defect

机译:一种研究无缺陷和有缺陷的有限光栅非线性光学响应的有限元方案

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We present a simple numerical scheme based on the finite element method (FEM) using transparent-influx boundary conditions to study the nonlinear optical response of a finite one-dimensional grating with Kerr medium. Restricting first to the linear case, we improve the standard FEM to get a fourth order accurate scheme maintaining a symmetric-tridiagonal structure of the finite element matrix. For the full nonlinear equation, we implement the improved FEM for the linear part and a standard FEM for the nonlinear part. The resulting nonlinear system of equations is solved using a weighted-averaged fixed-point iterative method combined with a continuation method. To illustrate the method, we study a periodic structure without and with defect and show that the method has no problem with large nonlinear effect. The method is also found to be able to show the optical bistability behavior of the ideal and the defect structure as a function of either the frequency or the intensity of the input light. The bistability of the ideal periodic structure can be obtained by tuning the frequency to a value close to the bottom or top linear band-edge while that of the defect structure can be produced using a frequency near the defect mode or near the bottom of the linear band-edge. The threshold value can be reduced by increasing the number of layer periods. We found that the threshold needed for the defect structure is much lower then that for a strictly periodic structure of the same length. References: 21
机译:我们提出了一种基于有限元法(FEM)的简单数值方案,利用透明-流入边界条件研究了有限一维光栅与Kerr介质的非线性光学响应。首先限制在线性情况下,我们改进了标准有限元,以获得一个四阶精确方案,保持有限元矩阵的对称三对角线结构。对于完整的非线性方程,我们为线性部分实现了改进的有限元,为非线性部分实现了标准有限元。所得非线性方程组采用加权平均定点迭代法和延续法求解。为了说明该方法,我们研究了无缺陷和有缺陷的周期性结构,并表明该方法在大非线性效应下没有问题。还发现该方法能够显示理想光和缺陷结构的光学双稳态行为作为输入光的频率或强度的函数。理想周期结构的双稳态可以通过将频率调谐到接近底部或顶部线性带边缘的值来获得,而缺陷结构的双稳态可以使用接近缺陷模式或线性带边缘底部的频率来产生。可以通过增加层周期数来减小阈值。我们发现,缺陷结构所需的阈值比相同长度的严格周期性结构要低得多。[参考文献: 21]

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