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Eigenmodes analysis in two-dimensional random media

机译:二维随机媒体中的特征模

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Simplified method of eigenmodes simulation in random media based on numerical solution of the stationary wave equation for two-dimensional (2D) medium with a random distribution of dielectric permittivity is suggested. By means of discretization the wave equation can be reduced to the system of homogeneous linear equations that includes parameter α=(2πb/λ)~2, where b is the spacing between the nodes of discretization, λ - the wavelength. The values of α (and corresponding b/λ) were determined as eigenvalues of this system of linear equations. The relative field amplitudes in all discretization nodes i.e. eigenvectors were calculated with this α. 2D random medium was simulated by matrix whose elements randomly take on two different values. One of them corresponds to dielectric permittivity of the material particles, the other - to permittivity of the volumes between them. Under the assumption made, elements of such matrix represent material particles and spaces between them, quantity b - particles size. All calculations were made using MATLAB. Different variants of disordered (and ordered) media were examined. It was shown that localized modes exist only in disordered systems and in a limited range of ratio b/λ . The dependence of modes character on the value of filling ratio and dielectric permittivity is estimated. Some results for one- and three-dimensional media are represented.
机译:建议本征模式模拟的基础上用于与介电常数的随机分布的二维(2D)介质固定波动方程的数值解随机媒体的简化方法。通过离散化装置的波动方程可以减少到齐次线性方程的系统,其包括参数α=(2πb/λ)〜2,其中b为离散化,λ的节点之间的间距 - 波长。 α(和相应的B /λ)的值确定为这个系统的线性方程的特征值。在所有离散节点即本征向量的相对场幅度用这个计算α。 2D随机介质是由矩阵,其元素随机取两个不同的值模拟。他们中的一个对应于所述材料颗粒中,其他的介电常数 - 在它们之间的体积的介电常数。下作出的假设,例如矩阵的元素表示材料颗粒和在它们之间,QUANTITY B位 - 颗粒大小。所有的计算使用MATLAB制作。检查紊乱(及订购)介质的不同变体。结果表明,仅在无序系统和在比b /λ的有限范围存在局部模式。模式字符的上的填充比和介电常数的值的依赖性被估计。对于一维和三维媒体的一些结果表示。

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