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A Numerical Study of Electromagnetic Waves in Periodic Waveguides

机译:周期波导中电磁波的数值研究

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Here are considered time-harmonic electromagnetic waves in a quadratic waveguide consisting of a periodic dielectric core enclosed by conducting walls. The permittivity function may be smooth or have jumps. The electromagnetic field is given by a magnetic vector potential in Lorenz gauge, and defined on a Floquet cell. The Helmholtz operator is approximated by a Chebyshev collocation, Fourier-Galerkin method. Laurent's rule and the inverse rule are employed for the representation of Fourier coefficients of products of functions. The computations yield, for known wavenumbers, values of the first few eigenfrequencies of the field. In general, the dispersion curves exhibit band gaps. Field patterns are identified as transverse electric, TE, transverse magnetic, TM, or hybrid modes. Maxwell's equations are fulfilled. A few trivial solutions appear when the permittivity varies in the guiding direction and across it. The results of the present method are consistent with exact results and with those obtained by a low-order finite element software. The present method is more efficient than the low-order finite element method.
机译:在这里,二次波导管中的时间谐波电磁波被认为是由被导电壁包围的周期性介电芯组成的。介电常数函数可以是平滑的或具有跳跃。电磁场由Lorenz量规中的磁矢量势给出,并在Floquet单元上定义。 Helmholtz算符通过Chebyshev搭配Fourier-Galerkin方法近似。劳伦特法则和逆法则用于表示函数乘积的傅立叶系数。对于已知的波数,该计算得出该场的前几个本征频率的值。通常,色散曲线表现出带隙。场模式被标识为横向电,TE,横向磁,TM或混合模式。麦克斯韦方程组成立。当介电常数沿引导方向和整个引导方向变化时,会出现一些简单的解决方案。本方法的结果与精确结果以及通过低阶有限元软件获得的结果一致。本方法比低阶有限元方法更有效。

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