The Method of Potentials for the Frequency Spectrum of Non-Homogeneous Spherical Cavities

Z. Eremenko, Y. Tarasov, I. Volovichev
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引用次数: 1

Abstract

We develop a novel theoretical method for solving the Maxwell equations in cavity resonators with inhomogeneous and asymmetrical filling. The method relies on the transition from vector description of electromagnetic fields in the resonator to a description in terms of two scalar functions (Debye potentials) for which we derive the original control equations. The solution to these equations is carried out with the use of Green functions, for which we obtain the infinite set of coupled equations in the resonance mode representation. The equations, which contain operator-valued potentials, are solved unperturbatively, by applying the original method for resonance mode decoupling. The frequency spectrum of the resonator with central-layered dielectric infill, which is found based on the developed theory, is in good agreement with the spectrum obtained numerically directly from Maxwell equations. The analysis of the inter-frequency intervals in the spectrum reveals its gradual chaotization with breaking the resonator symmetry.
非均匀球腔频谱的位势法
提出了一种求解非均匀非对称填充腔谐振腔中麦克斯韦方程组的新理论方法。该方法依赖于从谐振腔中电磁场的矢量描述到两个标量函数(德拜势)的描述的转换,我们推导了原始控制方程。利用格林函数对这些方程进行了求解,得到了谐振模态表示下的无限组耦合方程。采用原始的共振模式解耦方法,对包含算子值势的方程进行了无摄动求解。根据所建立的理论,得到了具有中心层状介质填充的谐振腔的频谱,与直接由麦克斯韦方程数值计算得到的频谱符合得很好。对频谱的频间间隔分析表明,随着谐振腔对称性的破坏,频谱逐渐混沌化。
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