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1. Field of the Invention
The present disclosure relates to a dual polarization antenna structure with radome and design method thereof, which are particularly capable of increasing gain.
2. Description of Related Art Including Information Disclosed Under 37 CFR 1.97 and 37 CFR 1.98.
The front-end circuit antenna of a wireless communication system is an essential device, and its performance affects the signal quality of the system. Currently, an antenna array is used for increasing antenna gain. The antenna directionality and gain could be increased by increasing the number of the antenna devices. However, this technology would significantly increase the feeding network's signal loss, has complicated a design of the feeding network, and needs a large volume of the entire antenna apparatus. The gain of the antenna would not increase effectively; in addition, the maintenance of the base station would be complex and expensive, and the large antenna apparatus is not suitable for small base station applications.
Traditionally, the gain and directionality of the antenna are increased by using array antenna. The metal antenna radome made of meta-material, which is constructed by periodic meta/dielectric patterns, could be configured to achieve almost zero effective refraction near the antenna operation frequency, so as to increase the directionality or gain of the antenna. The metal antenna radome made of meta-material could increase the directionality or gain of the antenna, and decrease the beam-width of antenna radiation pattern, but such antenna radome could only increase the directionality or gain in a predefined signal direction and/or polarization; thus it could not be used for dual polarization antenna. In other words, the application of such technology is limited by the type of antenna. In addition, when the antenna radome using the related arts is used for single polarization antenna, the polarization directions of the antenna and the antenna radome have to be considered. If the polarization directions are not aligned, the increment of the directionality or gain would be decreased.
Therefore, the present disclosure proposes a dual polarization antenna radome with higher antenna gain and lower thicknesses of the antenna and antenna radome.
The disclosure provides a dual polarization antenna structure, antenna radome and the method thereof for increasing antenna gain and decreasing the height of the entire antenna structure.
An exemplary embodiment of the disclosure, a dual polarization antenna radome includes a plurality of dielectric substrates, wherein each of the plurality of dielectric substrates has a surface including a plurality of metal patterns arranged in the form of an array, and the metal patterns are substantially unchanged after rotating 90 degrees around an axis perpendicular to the dielectric substrate. Moreover, the obtained antenna performance is similar at both perpendicular directions according to the present disclosure.
Another exemplary embodiment of the disclosure, a dual polarization antenna structure includes an antenna and the above-mentioned antenna radome. The distance between the antenna and the antenna radome is less than or equal to 1/10th of the wavelength corresponding to the operation frequency.
Another exemplary embodiment of the disclosure, a method for constructing a dual polarization antenna structure includes the steps of analyzing refraction, transmission and impedance of metal patterns of an antenna radome; determining the metal patterns according to the analyses; and arranging the metal patterns in the form of an array on dielectric substrates of the antenna radome.
The present disclosure can be explained with the appended drawings to clearly disclose the technical characteristics of the present disclosure.
The antenna radome of the present disclosure, unlike that of the Fabry Perot design, is not limited by need of a grounding surface, and thus the application to a dipole antenna is exemplified below. The antenna 2 is a dipole antenna and includes two radiation conductors 17 on a substrate 13 and antenna feeding terminals 18 coupled to the radiation conductors 17. A dielectric substrate layer 4 is disposed on the antenna 2, and may be an air gap. The antenna radome 3 is disposed on the dielectric substrate layer 4 and includes a plurality of dielectric substrates 31, 32 and 33. There is a gap 341 between the dielectric substrate 31 and the dielectric substrate 32, and a gap 342 is formed between the dielectric layer 32 and the dielectric layer 33. The gaps 341 and 342 may be vacuums, or may include air or other dielectric materials. Each of the dielectric substrates 31, 32 and 33 is constituted of a plurality of array cell dielectric substrates 5, and the surface of the array cell dielectric substrate 5 includes metal pattern or metal totem 6. In an embodiment, the gap 341 or 342 has a preferred thickness of 1.6 mm. In a case of normalizing the wavelengths of a central frequency of 3.5 GHz, the size of the gap 341 or 342 is preferably 1.6/85 of the wavelength. The gap may be, but is not limited to, air or vacuum. The user could use proper materials as desired to obtain optimal dielectric constant, permeability and conductivity for achieving better antenna performance.
In general, the dielectric substrate layer 4 (which may be plural layers having different dielectric characteristic) is used for generating a distance between the antenna 2 and the antenna radome 3, and the user could adjust the distance for better antenna receiving and transmitting performance. In addition to air, the dielectric substrate layer 4 may be vacuum, FR4, SiO2Al2O3 etc. The material of the dielectric substrate layer 4 is not limited and could be selected as desired to configure for effective optimal dielectric constant, permeability and permittivity for better antenna performance. In this embodiment, the distance between the antenna 2 and the antenna radome 3 is 4 mm. In a case of normalizing the wavelengths of a central frequency of 3.5 GHz, the distance is preferably 4/85 of the wavelength or less than or equal to 1/10 of the wavelength. Likewise, the material or thickness of the dielectric substrate layer 4 is exemplified only, and the user could use different material and thickness for different operation frequency, so as to obtain better receiving and transmitting performance.
The metal pattern or metal totem 6 on the dielectric substrate 31, 32 or 33 is symmetrical along x and y directions. Therefore, the metal totem 6 is substantially unchanged after the dielectric substrate 31, 32 or 33 rotates around the axis perpendicular to the center of the dielectric substrate 31, 32 or 33 by 90 degrees. In other words, the surface of each of the dielectric substrate 31, 32 or 33 includes a plurality of metal totems 6 arranged in the form of an array, and the metal totems 6 are unchanged when the metal totems 6 rotate 90 degrees around an axis perpendicular to the dielectric substrate 31, 32 or 33. Accordingly, the antenna structure of the present disclosure has dual polarization characteristics.
In addition to the double crossed-I pattern shown in
The present disclosure also could be implemented in a patch antenna, and is exemplified below.
As shown in
In view of the above, both the dual polarization antenna structures 1 and 10 could increase the directionality and gain in two different polarization directions, so that they could be applied to dual polarization antenna to increase directionality and gain in two polarization directions. In the case of being applied to a single polarization antenna, it is not necessary to consider the alignment problem of the polarization direction of the single polarization antenna and the polarization direction of antenna radome for increasing gain. Therefore, the present disclosure could increase receiving and transmitting performance of the antenna significantly.
Given the above, the present disclosure proposes a dual polarization antenna radome constituted of metal patterns or totems, dielectric substrate layers and array cell dielectric substrates, which could increase directionality and gain thereof.
The above-described embodiments of the present disclosure are intended to be illustrative only. Numerous alternative embodiments may be devised by those skilled in the art without departing from the scope of the following claims.
Number | Date | Country | Kind |
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98106931 A | Mar 2009 | TW | national |
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Entry |
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Chinese Office Action issued on Aug. 8, 2012 for the Chinese counterpart application. |
English Translation of Chinese Office Action issued on Aug. 8, 2012 for the Chinese counterpart application. |
Ben A. Munk, “Frequency Selective Surfaces: Theory and Design”, A Wiley Interscience Publication, 2000, pp. 1, 14, 26-28, 35-37, 227-229, 240-255, 10/43, John Wiley & Sons, Inc., USA. |
Number | Date | Country | |
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20100225563 A1 | Sep 2010 | US |