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Generalized eigenproblem of hybrid matrix method for stable analysis of periodic multilayered bianisotropic media

机译:混合矩阵稳定分析周期性多层双行介质稳定分析的广义特征

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Electromagnetic wave propagation in periodic multilayered bianisotropic media has been a topic of considerable interest for many years. One of the celebrated techniques for analysis of such media is based on the combination of transfer matrix method and Floquet (Bloch) wave theory [1]. Once the transfer matrix for a unit cell has been determined through proper cascading, Floquet waves are found simply as its eigenvectors with the associated eigenvalues being the exponentials of Floquet wavenumbers. Despite being very useful, the transfer matrix method has been known to suffer from the inherent numerical instabilities [2], particularly when the layer thickness is large and/or the frequency is high. There have been various techniques proposed to alleviate the numerical problem including recursive transformation, eigen-, or Riccati-based admittance, impedance, and reflection or scattering matrix methods [2]-[5]. However, these techniques cannot be applied to find Floquet waves directly. The objective of this paper is to devise a stable method to determine the Floquet waves without appealing to the transfer matrix. The method is based on the solutions to a generalized eigenproblem of hybrid matrix, which is always stable for any thickness or frequency [6].
机译:周期性多层双行介质中的电磁波传播一直是多年来兴趣的主题。用于分析这种介质的庆祝技术之一是基于转移矩阵法和浮子(BLOCH)波理论的组合[1]。一旦通过适当的级联确定了单位电池的转移矩阵,发现浮子波只是其特征向量,其中相关的特征向量是浮子波数的指数。尽管非常有用,但已知传递矩阵方法遭受固有的数值不稳定性[2],特别是当层厚度大并且/或频率高时。已经提出了各种技术来缓解包括递归转化,特征或基于Riccati的进入,阻抗和反射或散射基质方法的数值问题[2] - [5]。然而,这些技术不能用于直接找到浮子波。本文的目的是设计稳定的方法来确定浮子波而不吸引转移矩阵。该方法基于混合矩阵的广义特征提名的解决方案,其对于任何厚度或频率始终是稳定的[6]。

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