Abstract
A dual-band dual-polarized omnidirectional antenna is investigated. The two bands are generated by a lower circular patch and an upper circular patch, respectively. A set of conductive vias and a coupled ring are utilized to widen the antenna bandwidth. Curved branches are introduced to contribute to circularly polarized radiation. A prototype was designed, fabricated and measured to demonstrate the performance of the antenna. Measured results show that an overlapped bandwidth of 15% from 2.22 to 2.58 GHz for both S11 ≤ −10 dB and axial ratio ≤3 dB is obtained in the low band, and an impedance bandwidth of 11.1% from 5.63 to 6.29 GHz is achieved in the high band. Measured peak gains are approximately 4.3 dBic and 5.4 dBi at two bands. Moreover, omnidirectional radiation patterns are also obtained within the operating band.
Introduction
Recently, circularly polarized (CP) omnidirectional antennas are of great interest since they can effectively reduce multipath effects, enhance the stability of wireless communication systems and provide a wide signal coverage. Therefore, a large number of efforts have been put into developing CP omnidirectional antennas [1–8]. In Ref. 1, by introducing shorting vias and vortex slots into a monopolar patch antenna, omnidirectional radiation patterns and wide axial ratio (AR) bandwidth were achieved. Based on dielectric resonator antennas, the designs presented in Refs. 2 and 3 could achieve AR bandwidths of 25.4 and 54.9%, respectively. However, the aforementioned designs all had profiles of more than 0.1λ0, which are not appropriate for space-limited applications. Patch antennas have advantages of low profile and simple structures, and are therefore suitable for designing CP omnidirectional antennas [4–8]. For instance, in Refs. 4–6, the antennas loaded with curved branches owned profiles of lower than 0.07λ0 and AR bandwidths of more than 14%. In Refs. 7 and 8, by cutting slits on radiating patches and ground planes, CP omnidirectional radiation performances were obtained and the antenna heights were only 0.028 and 0.026λ0, respectively.
With the blooming of wireless technologies, antennas with more than one operating band are becoming more and more necessary to satisfy various wireless standards. In Ref. 9, a dual-band CP omnidirectional antenna was proposed. By combining a dielectric resonator antenna and a patch antenna together, the design was able to realize AR bandwidths of 3.16 and 5.06% at two bands, separately. In Ref. 10, by utilizing a stacked-patch configuration, a dual-band frequency reconfigurable antenna was presented. In addition, based on artificial μ-negative transmission lines, a dual-band CP antenna was investigated in Ref. 11. As it is known, CP antennas are required for global positioning systems, satellite communications and linearly polarized antennas are needed for lots of other commercial applications. But few published designs are able to offer dual-band omnidirectional antennas with different polarization states in the two frequency bands. In Ref. 12, a dual-band dual-polarized antenna was proposed. Omnidirectional circular polarization is achieved in the low band and omnidirectional linear polarization is obtained in the high band. In Ref. 13, a dual-band antenna with different polarization and radiation properties over two bands for vehicular communications is presented. However, the AR bandwidth of the designs [12, 13] is too narrow to satisfy the modern wireless systems.
In this paper, a dual-band dual-polarized omnidirectional antenna is presented. The two bands are generated by two circular patches, separately. By adding a set of conductive vias and a coupled ring, the antenna bandwidths are enhanced significantly [14, 15]. Owing to the introduction of curved branches, a current loop can be formed to provide horizontally polarized field. Together with the vertically polarized field created by the lower circular patch, a CP omnidirectional radiation can be generated in the low band. To verify the design idea, a prototype was designed, fabricated and measured. Both simulated and measured results reveal that wide bandwidths, omnidirectional circular polarization and omnidirectional linear polarization can be achieved.
Antenna Geometry and Operating Principle
Antenna Geometry
Figure 1 shows the geometry of the proposed dual-band dual-polarized omnidirectional antenna and the detailed dimensions are listed in Table 1. As shown in Figure 1, the proposed antenna is mainly composed of an upper circular patch, an annular ring, a lower circular patch, a set of conductive vias, a ground plane, six curved branches and a coaxial probe. The upper circular patch is printed on the top of Substrate 1 (Taconic RF-30, thickness = 1 mm, εr = 3.0) and the annular ring is concentrically placed around the upper circular patch. The lower circular patch and the ground plane are printed on the top and bottom surfaces of Substrate 2 (Rogers 5,870, thickness = 3.175 mm, εr = 2.33). In order to excite two circular patches simultaneously to achieve a dual-band property, a clearance hole with a radius of 2.5 mm is etched in the center of the lower circular patch. In this way, the upper circular patch is directly fed by the inner conductor of the coaxial probe and the lower circular patch is fed by the coupling with the clearance hole. As a result, the design is able to operate at two bands. In addition, a set of N conductive vias (N = 15) are used to short the lower circular patch to the ground plane and six curved branches are loaded around the ground plane to contribute CP radiation in the low band.
FIGURE 1
TABLE 1
| Parameters | R1 | R2 | R3 | R4 | R5 |
|---|---|---|---|---|---|
| Values/mm | 17 | 17.3 | 29.3 | 48.3 | 0.7 |
| Parameters | Rg | Rs | L1 | L2 | a0 |
| Values/mm | 43.6 | 90 | 35.2 | 40.1 | 30.7 |
Dimensions of the proposed antenna.
Operating Principle
As previously stated, by adding the annular ring and a set of conductive vias into the antenna structure, antenna bandwidths can be enhanced dramatically. The curved branches are used to contribute CP radiation. Therefore, in this part, principles of the annular ring, the conductive vias and the curved branches will be further discussed.
In this design, the annular ring is concentrically placed around the upper circular patch. In consequence, when the upper circular patch is fed, the annular ring can be excited simultaneously by energy coupling. By tuning the radius of the upper circular patch, the size of the annular ring and the distance between them, their resonant frequencies can be moved in proximity to each other. Hence, a wide impedance bandwidth can be obtained in the high band.
As illustrated in Ref. 15, a non-zero resonant frequency of TM01 mode can be created due to the loading of conductive vias. Together with the well-known TM02 mode generated by the lower circular patch, a wide impedance bandwidth can be realized then. The number, radius, and location of the conductive vias have effect on impedance matching of the antenna, and these parameters can be determined based on the design guideline given in Ref. 15.
As it is known, CP radiation requires two orthogonal electric fields with an equal amplitude and 90° phase difference. In this design, TMmn mode (m = 0, n = 1, 2) is generated by the vias-loaded lower circular patch, leading to vertically polarized electric field Eθ. And the introduction of curved branches can form a current loop around the ground plane, leading to horizontally polarized electric field Eφ. When these two orthogonal fields have an equal amplitude and a quadrature phase difference, CP radiation is achieved in the far field. Figure 2 gives the simulated current distribution on the lower circular patch and the ground plane at 2.4 GHz. It is seen that an equivalent vertical current formed by the circular patch and a current loop formed by the curved branch on the ground plane are excited simultaneously. Hence, circular polarization is achieved.
FIGURE 2
Results
To verify the proposed design, a fully functional prototype shown in Figure 3 was fabricated and measured. Ansys HFSS, a vector network analyzer and a near-field measurement system were used to obtain the simulated and measured results.
FIGURE 3
Simulated and measured S-parameters and axial ratios (ARs) of the proposed antenna are given in Figure 4. From the figure, it can be seen that the measured impedance bandwidths for S11 ≤ −10 dB are from 2.2 to 2.62 GHz in the low band and from 5.63 to 6.29 GHz in the high band, which agree well with the simulated results. The measured AR bandwidth for AR ≤ 3 dB is from 2.22 to 2.58 GHz. Therefore, the effective bandwidths of the proposed design are from 2.22 to 2.58 GHz and 5.63–6.29 GHz at two bands, respectively. Figure 5 shows the simulated and measured peak gains of the proposed antenna. The measured peak gains are approximately 4.3 dBic in the low band and 5.4 dBi in the high band. The discrepancies between the simulated and measured gains are mainly due to the fabrication tolerances and imperfect measurement system.
FIGURE 4
FIGURE 5
The simulated and measured radiation patterns in the azimuth plane (θ = 30°) and elevation plane (φ = 0°) at 2.35, 2.55 and 5.9 GHz are depicted in Figure 6. The measured radiation patterns are in well agreement with simulations. In the low band, omnidirectional radiation patterns can be observed and the left-hand (LH) CP fields are almost 15 dB stronger than the right-hand (RH) CP fields at θ = 30° and the whole azimuth plane, demonstrating LHCP radiation is achieved in the far field of the proposed design. In the high band, omnidirectional radiation patterns are also obtained and the cross-polarization levels are lower than −15 dB compared with the co-polarization counterpart in both planes. In consequence, a dual-band and dual-polarized antenna with well-controlled omnidirectional radiation patterns is realized in this design.
FIGURE 6
Conclusion
In this paper, a low-profile dual-band dual-polarized omnidirectional antenna has been proposed. A prototype was constructed and measured to demonstrate the antenna performance. The proposed antenna can achieve bandwidths of 15 and 11.1%, gains of approximately 4.3Â dBic and 5.4Â dBi at two bands, respectively. Besides, omnidirectional radiations with low cross-polarization levels can also be obtained. With these properties, the proposed antenna shows superiorities over the reported designs and is attractive for indoor communication systems.
Funding
This work was supported by the Key Research and Development Project of Guangdong Province (2020B0101080001) and the National Natural Science Foundation of China (62071308). (Corresponding author: LG).
Statements
Data availability statement
The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.
Author contributions
All authors listed have made a substantial, direct, and intellectual contribution to the work and approved it for publication.
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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Summary
Keywords
antenna, dual-band antenna, circularly polarized and linearly polarized, omnidirectional radiation, patch antenna
Citation
Gu H, Ge L and Zhang J (2020) A Dual-Band Dual-Polarized Omnidirectional Antenna. Front. Phys. 8:614911. doi: 10.3389/fphy.2020.614911
Received
07 October 2020
Accepted
20 November 2020
Published
15 December 2020
Volume
8 - 2020
Edited by
He Zhu, University of Technology Sydney, Australia
Reviewed by
Qiong-Sen Wu, Guangdong University of Technology, China
Fan Wu, Southeast University, China
Updates
Copyright
© 2020 Gu, Ge and Zhang.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Lei Ge, leige@szu.edu.cn
Present Address: College of Electronics and Information Technology, Shenzhen University, Shenzhen, China
This article was submitted to Radiation Detectors and Imaging, a section of the journal Frontiers in Physics
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