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An active transmitter antenna with beam scanning and beam shaping capability for 60GHz application

机译:具有光束扫描的有源发射器天线和60GHz应用的光束整形能力

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For 60GHz indoor communication systems [1], there is a remarkably large range of frequency allocated for unlicensed wireless telecommunications around 60 GHz (typically 59–66GHz). In Europe, the frequency ranges 62–63 GHz and 65–66 GHz are reserved for wideband mobile networks (Mobile Broadband System). In Japan, the 59–67 GHz band is reserved for wireless communications. In indoor operation, as the link between transmitter and receiver can be shadowed because of human body interposition for example, implementing beam-scanning antennas is needed to carry out high bite rate communications. Some solutions are conceivable to achieve beam-scanning antennas, for example phased arrays [2] but it does not allow for scanning the beam over a large angle and it induces losses due to phase shifters. It is the same limitation for switched antenna arrays based on a Butler matrix [3]. Homogeneous lenses may allow the obtention of a wide scan antenna [4] but bring about a problem of retro-diffusion from the lenses to the sources. Lüneburg lens avoids this problem because it presents a dielectric gradient index lens whose relative permittivity εT varies radially according to the law given by [5]. Moreover, this inhomogeneous lens offers the particularity to have infinity of focus points. So, it becomes possible to achieve a very wide scan antenna. Practically, inhomogeneous lens can be manufactured either from materials with varying effective dielectric permittivity [6] or by assembling a finite number of concentric homogeneous dielectric shells [7]. This kind of inhomogeneous spherical lens antenna has demonstrated off-axis performances by moving one source around the lens [8] and a beam shaping capability by associating several sources below the lens [9]. In this paper, we study a plate Luneburg lens to obtain a narrow beam (10°) for azimuth plane and a wide beam (70°) for elevation plane. First, a new mi- ed solution is chosen to manufacture the lens by using holes in a Teflon sheet (εT=2.04) and external foam crowns (εT=1.45 and εT=1.25). Secondly, the principle of the beam-scanning and beam-shaping antenna is matched by using one MMIC power amplifier behind each ridged source waveguide. Finally, a transmitter active reconfigurable antenna at 60 GHz is tested by measuring the received power and the radiation patterns for different configurations.
机译:对于60GHz室内通信系统[1],在60 GHz(通常为59-66GHz)的无牌无线电信中,分配了大量大量频率。在欧洲,频率范围为62-63 GHz和65-66 GHz为宽带移动网络(移动宽带系统)保留。在日本,59-67 GHz频段保留用于无线通信。在室内操作中,由于例如人体插入的发射器和接收器之间的链路可以被遮蔽,例如,需要实现光束扫描天线来执行高咬合速率通信。可以想到一些解决方案以实现光束扫描天线,例如相控阵列[2],但它不允许在大角度扫描光束,并且它引起相移引起的损耗。它是基于管道矩阵的切换天线阵列的相同限制[3]。均匀透镜可以允许基于宽扫描天线[4],但是从镜头到源的镜片中的复古扩散问题。 Lüneburg镜头避免了这个问题,因为它呈现了一种介电梯度索引镜头,其相对介电常数εt根据[5]给出的法律而径向变化。此外,这种不均匀镜头提供了具有焦点无限的特殊性。因此,可以实现非常宽的扫描天线。实际上,可以从具有不同有效介电常数[6]的材料的材料制造不均匀透镜,或者通过组装有限数量的同心均匀介电壳[7]。这种非均匀球形透镜天线通过在镜头[8]周围的一个源极和光束整形能力周围的一个源和光束整形能力[9]中通过围绕透镜[8]和光束整形能力进行了偏离性能。在本文中,我们研究了一个板莱氏透镜,以获得用于方位角平面的窄梁(10°),以及用于仰角的宽光束(70°)。首先,选择新的MI-ED解决方案以通过在Teflon板(εt= 2.04)和外部泡沫冠中的孔(εt= 1.45和= 1.25)中使用孔来制造镜头。其次,通过使用每个脊源波导后面的一个MMIC功率放大器匹配光束扫描和光束整形天线的原理。最后,通过测量用于不同配置的接收功率和辐射图案来测试60GHz的发射器有源可重新配置天线。

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