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

机译:具有60 GHz应用的波束扫描和波束成形功能的有源发射机天线

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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的室内通信系统[1],在60 GHz(通常为59-66GHz)左右的频率范围内,分配给未经许可的无线电信的频率范围非常大。在欧洲,频率范围62-63 GHz和65-66 GHz保留给宽带移动网络(移动宽带系统)。在日本,59-67 GHz频带保留用于无线通信。在室内操作中,由于发射机和接收机之间的链接可能由于例如人体插入而被遮蔽,因此需要使用波束扫描天线来执行高比特率通信。可以想到一些解决方案来实现波束扫描天线,例如相控阵[2],但它不允许在大角度上扫描波束,并且由于移相器而引起损耗。对于基于Butler矩阵的开关天线阵列来说,这是同样的局限性[3]。均质的透镜可能允许获得较宽的扫描天线[4],但会带来从透镜到光源的向后扩散问题。 Lüneburg透镜避免了这个问题,因为它提供了一种介电梯度折射率透镜,其相对介电常数εT根据[5]给出的定律径向变化。而且,这种不均匀的透镜提供了具有无限焦点的特殊性。因此,可以实现非常宽的扫描天线。实际上,不均匀透镜可以由具有不同有效介电常数的材料制成[6],也可以通过组装有限数量的同心均匀介电壳[7]来制造。这种不均匀的球面透镜天线通过在透镜[8]上移动一个光源而表现出离轴性能,并且通过在透镜[9]下方关联多个光源而具有波束成形能力。在本文中,我们研究了一种平板型Luneburg透镜,它在方位角平面上获得窄光束(10°),在仰角平面上获得宽光束(70°)。首先,通过使用特氟龙板中的孔(εT= 2.04)和外部泡沫凸度(εT= 1.45和εT= 1.25),选择一种新的解决方案来制造镜片。其次,通过在每个脊状源波导后面使用一个MMIC功率放大器来匹配波束扫描和波束成形天线的原理。最后,通过测量不同配置的接收功率和辐射方向图来测试60 GHz发射机有源可重配置天线。

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