模式辐射可重构的超方向性单极子设计

M. M. Khouma, I. Dioum, A. Diallo, I. Diop, L. Sane, K. Diallo, S. Ouya
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摘要

本文对双单极子天线阵列的超指向性进行了全局研究。它主要基于乌兹科夫的理论,他定义了通过线性关联大量N个紧密间隔的散热器,在期望方向上以$N^{2}$的顺序获得高指向性的可能性。第一个研究是用特定的电流在大小和相位上激励单极子,以获得在期望方向上可重构的超指向性。其次,为了减少直至消除单极子之间的相互耦合,我们用&[1]激励单极子中的一个。然而,关于大量关联辐射体的最重要的工作是来自I.Uzkov[2],他在1946年指出了通过线性关联较大数量的N个紧密间隔的辐射元素来制造超指向性的可能性,即指向性为$N^{2}$的指向性。然后,他从下面定义的方程(1)和(2)中表明,当辐射元素被适当激发时,该指向性可以在期望的方向$(\theta ,\varphi )$上。单位电流和加载另一个阻抗由乌兹科夫的理论确定。利用仿真器Ansys HFSS计算单极子天线阵列的阻抗矩阵$H_{mn}$,然后利用电流激励系数$a_{{0} {n}}$确定阻抗$Z_{load}$。仿真结果表明,在两种情况下,在期望方向上的可重构指向性至少在$8 . 5 dB$左右,结果近似相似。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Monopole Design for Superdirectivity with Pattern Radiation Reconfigurable
This paper presents a global study for superdirectivity of an array of 2 monopoles antennas. It is principally based on Uzkov’s theory, who define the possibility to obtain a high directivity in order of $N^{2}$ in a desired direction by linearly associating a large number N of radiators closely spaced. A first study is made by exciting monopoles by specific currents excitation in magnitude and phase to obtain a superdirectivity reconfigurable in a desired direction. Secondly, to reduce until eliminate mutual coupling between monopoles, we excite one of monopole by a & [1]. However, the most significant works for a large number of associating radiators is from I.Uzkov [2], who states in 1946 the possibility to make a superdirectivity, meaning a directivity in order of $N^{2}$, by linearly associating a larger number N of closely spaced radiating elements. Then, he showed from equations (1) and (2) defined below that this directivity can be in a desired direction $(\theta ,\varphi )$ when radiating elements are properly excited. unit current and loaded the other one by an impedance determined from uzkov’s theory. Simulator Ansys HFSS is used to calculated impedance matrix $H_{mn}$ of monopoles antennas array and then currents excitation coefficients $a_{{0} {n}}$ used after to determine impedance $Z_{load}$. Simulations show approximately similar results in the 2 cases with a reconfigurable directivity a least in around of $8 . 5 dB$ in a desired direction.
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