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Based on the second kind of Green's identity,a boundary integral equation forarbitrary cross-section waveguide is transformed to a system of linear homogeneous algebraicequations by means of expansion of boundary bases and by using the eigenfunctions of a fictitiousregular boundary as weighting functions,which corresponds to less algebraic equations than BEMand simpler coefficients than the modified BEM.The numerical results for some typical metallicwaveguides are given by using the method of eigen-weighted boundary integral equation,and theyare accurate enough with fast convergence.  相似文献   
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本文采用横向谐振法和奇、偶激励法分析了平行耦合和对称弯曲耦合的沟槽型无辐射介质(GNRD)波导的耦合特性,并对实验样品进行了测试。理论计算结果和实验结果符合良好,为GNRD波导定向耦合器等元件的设计提供了理论依据。  相似文献   
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刘小勇  祝雷  冯一军 《中国物理 B》2016,25(3):34101-034101
We investigate the guiding modes of spoof surface plasmon polaritons(SPPs) on a symmetric ultra-thin plasmonic structure. From the analysis, we deduce the operating frequency region of the single-mode propagation. Based on this property, a spoof SPPs lowpass filter is then constituted in the microwave frequency. By introducing a transmission zero at the lower frequency band using a pair of stepped-impedance stubs, a wide passband filter is further realized. The proposed filter is fed by a transducer composed of a microstrip line with a flaring ground. The simulated results show that the presented filter has an extremely wide upper stopband in addition to excellent passband filtering characteristics such as low loss, wide band, and high square ratio. A prototype passband filter is also fabricated to validate the predicted performances.The proposed spoof-SPPs filter is believed to be very promising for other surface waveguide components in microwave and terahertz bands.  相似文献   
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本文选取本征函数作为权函数,由格林第二恒等式建立边界积分方程,并采用边界基形式得到线性齐次方程组。这种方法不仅降低了系数矩阵的维数,而且使其各项仍保持为简单一项,减少了计算量.本文提供了几种常见金属波导的例子,计算结果既收敛快、又足够准确。  相似文献   
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祝雷  吴世法  李亚琴 《激光杂志》2007,28(6):84-84,86
本文利用时域有限差分法(FDTD)模拟了在p极化平面波侧向照射下,扫描近场光学显微镜镀银膜四面锥形探针扫描直径30纳米银球"热点"处的电场增强因子及最佳条件.我们得出了膜厚和探针与银球之间间隙的最佳条件:间隙3纳米时最佳膜厚为20~50纳米,此时的场增强因子最强为70左右;膜厚30纳米时,间距1纳米增强因子最强为298.  相似文献   
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