基于超材料结构的高增益圆波导阵列天线研究

L. Bin, Wu Bian, Liang Chang-hong
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引用次数: 7

摘要

提出了一种利用超材料结构提高圆波导阵列天线增益的新方法。采用数值模拟方法研究了具有超材料结构的超材料和高增益圆波导天线的电磁特性,并与传统圆波导天线进行了比较。仿真结果表明,该方法是有效的,超材料结构可以实现对辐射能量的聚集,从而提高了天线的增益,降低了旁瓣电平。Keywords-Metamaterial结构;圆波导天线阵列;本文提出了一种利用超材料结构设计的高增益圆波导阵列天线。采用数值方法研究了阵列天线的超材料结构特性和辐射特性。我们的研究表明,超材料结构可以实现有效的折射率接近于零并聚集辐射能量,与传统的阵列天线相比,具有超材料结构的阵列天线可以获得很大的天线增益提高。2本文研究的超材料是由周期为1 mm(在x轴和y轴方向上)的方形晶格铜网格组成的。栅格在z轴方向的间距为H mm,铜栅格的方孔边缘为(a-r)mm。超材料的结构如图1所示。
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A Study on High Gain Circular Waveguide Array Antenna Using Metamaterial Structure
A new method of improving the gain of circular waveguide array antenna using metamaterial structure is presented in this paper. The electromagnetic characteristics of metamaterial and high-gain circular waveguide antenna with the metamaterial structure are studied by using the numerical simulation method, which were also compared with those of the conventional circular waveguide antenna. The simulation results show that this method is effective and the metamaterial structure can realize congregating the radiation energy, so the gain of the antenna is increased and the side lobe level is decreased. Keywords-Metamaterial structure; Circular waveguide antenna arrays; High-gain In this paper, we present a new high gain circular waveguide array antenna design using metamaterials structure. The properties of metamaterial structure and the radiation characteristics of the array antennas are investigated by numerical method. Our studies demonstrate that the metamaterial structure can realize an effective refraction index which can be close to zero and congregate the radiation energy, and the array antenna with metamaterial structure can obtain a great improvement of the antenna gain, in comparison with the conventional array antenna. II. PRINCIPAL CHARACTERISTICS OF METAMATERIAL STRUCTURE The metamaterial,which is studied in this paper, is composed of copper grids with a square lattice and whose period is equal to a mm (in the x-axis and y-axis directions). The grids' spacing in the z-axis direction is H mm, and the edge of the square holes of the copper grids is (a-r)mm. the structure of the metamaterial is shown in figure 1.
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