The Methods for Generating Radiation Null in Filtering Antennas

Lei Wang, Kai Xu, Jin Shi
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Abstract

Filtering antennas have been achieved more attention for the advantages of reducing the requirement of the filter in wireless communication systems. The radiation nulls of filtering antenna can further improve the frequency selectivity and decrease the mutual coupling between the closely placed antennas operating at different frequencies so that the placement distance of the antennas can be decreased. Therefore, various methods for generating radiation null have been investigated. One is to use cross-coupling or electromagnetic hybrid coupling of filtering theory. The other is to generate transmission zero by feed structure, which is a radiation null for the whole antenna. The last one is to achieve the radiation null by the radiator structure, which will produce a field that cancels each other out. In this paper, two filtering antennas with radiation nulls are reviewed to introduce the methods for radiation nulls. One is the dual-polarized filtering patch antenna fed by substrate integrated cavity (SIC). The second-order filtering response is achieved by using one SIC resonator and one slotted square patch while the radiation nulls can be produced by connecting the coupled lines with feeding lines in parallel. The other is a circular dense dielectric (DD) patch antenna realized by stacking an upper DD patch on the lower DD patch. The two reflection zeros are achieved because the dual DD patches are both operating at TM11 mode. The two radiation nulls near the lower band-edge are produced by the opposite E-field distribution inside the upper DD patch and the quarter-wavelength open-circuit stub, while the two radiation nulls near the upper band-edge are produced by the opposite E-field distribution inside the lower DD patch and the opposite E-field distribution at the edges of the two DD patches. The performances of the two designs are given.
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滤波天线中产生辐射零值的方法
在无线通信系统中,滤波天线以其降低对滤波器要求的优点而受到越来越多的关注。滤波天线的辐射零线可以进一步提高频率选择性,减少在不同频率工作的紧密放置的天线之间的相互耦合,从而减小天线的放置距离。因此,研究了各种产生辐射零的方法。一种是采用交叉耦合或电磁混合耦合的滤波理论。另一种是通过馈电结构产生传输零,这是整个天线的辐射零。最后一种是通过散热器结构来实现辐射零,它会产生一个相互抵消的场。本文综述了两种带辐射零点的滤波天线,介绍了处理辐射零点的方法。一种是衬底集成腔(SIC)馈电的双极化滤波贴片天线。采用一个SIC谐振腔和一个开槽方形贴片实现了二阶滤波响应,而将耦合线与馈线并联可以产生辐射零点。另一种是圆形密集介电(DD)贴片天线,其原理是将上贴片叠加在下贴片上。实现两个反射零是因为两个DD补丁都在TM11模式下运行。下带边缘附近的两个辐射零是由上DD贴片和四分之一波长开路短段内部相反的e场分布产生的,而上带边缘附近的两个辐射零是由下DD贴片内部相反的e场分布和两个DD贴片边缘相反的e场分布产生的。给出了两种设计方案的性能。
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