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81-Element single-layer reflectarray with double-ring phasing elements for wideband applications

机译:具有双环定相元件的81元件单层反射阵列,适用于宽带应用

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摘要

A microstrip reflectarray antenna utilizes a planar array of printed patch elements and a conventional prime or offset feed to form an alternative to the parabolic reflector [1]. It transforms the spherical wave of the feed into the planar wave by employing microstrip patch elements as radiators and phase shifters. Due to the use of planar technology, it offers a good balance between conventional reflector antennas and phased arrays. Because it uses many radiating elements it provides flexibility with respect to radiation pattern formation [2-4]. Its disadvantage is a limited operational bandwidth, which for the case of moderate gain is mainly due to a limited phase range and a high phase slope of the elements. In the wave transformation process, a full phasing range of 360° is desirable for unit cells containing patch elements. However, a variable size patch antenna developed on a single layer substrate offers a phasing range of about 300°. To overcome this problem, multilayer substrates including stacked variable-size patches for phasing the unit cells of a reflectarray have been devised to extend the phase range to multiples of 360°. The multi-layer approach with stacked patches not only extends the phase range but also reduces the slope of the phase curve as a function of patch dimensions [5-6]. However, the use of multi-layer substrates means that in practice layers of the reflectarray have to be manufactured separately and the assembly should leave no air gaps. This results in an elaborate and expensive manufacturing process. To overcome this problem, printed double-ring elements to form a single-layer reflectarray have been proposed. The double rings improve the phasing range of unit cells by utilizing multi-resonance behaviour. The extended range for unit cells containing double-ring elements has been demonstrated for the case of normal (TEM) wave incidence [7]. The assumption of normal incidence is less accurate for peripheral elements. Therefore in [8], TE and TM waves were considered to obtain an oblique incidence to obtain more accurate phasing characteristics of unit cells. © 2010 IEEE.
机译:微带反射阵列天线利用印刷的贴片元件的平面阵列和常规的主要或偏移馈电来形成抛物面反射器的替代方案[1]。它通过使用微带贴片元件作为辐射器和移相器,将进料的球面波转换为平面波。由于使用了平面技术,它在常规反射器天线和相控阵之间提供了良好的平衡。因为它使用许多辐射元件,所以它在辐射方向图的形成方面提供了灵活性[2-4]。其缺点是工作带宽有限,在中等增益的情况下,这主要是由于元件的有限相位范围和高相位斜率所致。在波变换过程中,对于包含贴片元件的晶胞,需要360°的完整相位范围。然而,在单层基板上开发的可变尺寸的贴片天线提供大约300°的相位范围。为了克服这个问题,已经设计出包括用于定相反射阵列的晶胞的堆叠的可变尺寸贴片的多层基板,以将相位范围扩展到360°的倍数。具有堆叠斑块的多层方法不仅扩展了相位范围,而且根据斑块尺寸减小了相位曲线的斜率[5-6]。但是,使用多层基板意味着实际上反射阵列的各层必须分别制造,并且组件应不留气隙。这导致复杂且昂贵的制造过程。为了克服这个问题,已经提出了形成单层反射阵列的印刷双环元件。双环通过利用多共振行为改善了晶胞的定相范围。对于正常(TEM)波入射情况,已经证明了含有双环元素的晶胞的扩展范围[7]。对于外围元素,垂直入射的假设不太准确。因此,在[8]中,TE和TM波被认为获得了斜入射,从而获得了更精确的晶胞相位特征。 ©2010 IEEE。

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