A Compact Wideband Circularly Polarized Microstrip Slot Antenna with Parasitic Elements

Xia, Chenhui; Diao, Shuo; Yin, Wenting; Huang, Zhifang; Wang, Lei; Lei, Dengyun

doi:https://doi.org/10.1155/2021/5214891

International Journal of Antennas and Propagation

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Abstract Introduction Experimental Results Conclusion Data Availability Conflicts of Interest Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2021 | Article ID 5214891 | https://doi.org/10.1155/2021/5214891

A Compact Wideband Circularly Polarized Microstrip Slot Antenna with Parasitic Elements

Chenhui Xia,¹Shuo Diao,²Wenting Yin,³Zhifang Huang,⁴Lei Wang,²and Dengyun Lei²

Academic Editor: Paolo Burghignoli

Received27 Jul 2021

Revised22 Aug 2021

Accepted31 Aug 2021

Published28 Sept 2021

Abstract

A compact wideband circularly polarized (CP) microstrip slot antenna (MSA) with parasitic elements is designed in this letter. The CP MSA comprises a square-loop sequential-phase (SP) feeding configuration, four rotated rectangular patches, and four L-shaped slots embedded in the ground plane. The square-loop SP feeding structure comprises a square loop and an arc-shaped strip, which could provide a 270° phase difference. Four rotated rectangular patches are placed at the edge of the square-loop feeding configuration using a capacitively tightly coupled feeding method to stimulate the CP resonant mode. After selecting these elements and tuning proper dimensions, the broad operating bandwidths of 4.38–5.25 GHz (18%) for |S₁₁| <–10 dB and 4.65–5.31 GHz (13.2%) for AR <3 dB could be realized. Hence, the designed CP MSA has a potential application value in wireless communication.

1. Introduction

Because of the obvious merits, antenna arrays have been massively used in wireless communication systems. Compared with single-antenna units, antenna arrays have excellent characteristics in terms of wide bandwidth, high gain, and stable radiation patterns [1, 2]. Conversely, circular polarization (CP) antennas have obtained considerable attention in satellite and mobile communication [3, 4] because of their outstanding features of overcoming polarization misalignment and reducing multipath interference with respect to linear-polarization antennas. Thus, CP antenna arrays (CPAAs) have naturally been significantly studied because of their combination of the advantages of the two structures.

Thus far, several effective methods have been proposed for designing the CPAAs [5–10]. To compare and analyze these structures, the feeder network is essential in antenna array design. For example, two T-junction power dividers are joined as a sequential phase (SP) shifting feeding network in [5], two phase-shifted swaps and a 1 : 8 power divider are combined as stripline feeding network in [6], and Wilkinson power combiners and delay lines are used as a beamforming network in [7]. Among these feeding strategies, the SP feeding network is one of the potential candidates in the design of antenna arrays, which could excite a stable and SP difference to the port of the feedline. When the SP feeding network is introduced into the design of 2 × 2 CPAAs, the impedance bandwidth (IBW) and axial ratio (AR) bandwidth of CPAAs could be improved simultaneously. The SP feeding network could be categorized as follows: a series-parallel feeding structure [11, 12], aperture-coupled structure [9], coplanar waveguide-fed structure [13], and a square-loop rotated feed-network structure [14–22].

Additionally, based on the SP feed-network, the stacked technology is effective in CPAAs [21–25]. Round [21] and rectangular [22] patches as parasitic elements are stacked above the SP rotated feeding structure, which realize 6% and 28.1% of CP bandwidth, respectively. Although the stacked structure enhances the CP bandwidth, the profile of CPAAs is too high to meet the requirements of system integration.

This study develops a new scheme of the CP microstrip slot antenna (MSA) with 2 × 2 array and low-profile characteristics. The proposed CP MSA comprises a square-loop SP feed-network, four rotated rectangular patches, and four L-shaped slots embedded in the ground plane. The square-loop SP feed-network is composed of a square loop and an arc-shaped strip, which could provide a 270° phase difference. Four rotated rectangular patches are placed at the edge of the square-loop feeding configuration using a capacitively tightly coupled feeding method to stimulate a CP resonant mode. After selecting these elements and tuning proper dimensions, broad operating bandwidths of 4.38–5.25 GHz (18%) for |S₁₁| < −10 dB and 4.65–5.31 GHz (13.2%) for AR < 3 dB could be realized.

2. Antenna Design

2.1. Antenna Configuration

Figure 1 shows the entire structure and detailed geometry of the proposed CP MSA with SP feeding characteristics. The proposed CP MSA comprised four rectangular patches with dimensions (L1 × L2 and L3 × L4), four L-shaped slots with dimensions (D4 × D5 × D6), a square-loop SP feed-network, which includes a square-loop with inner and outer side length (D2 × D3), and an arc-shaped strip with different radius (R1 × R2). The square-loop feeding structure and rectangular patches are printed at the top of a substrate (Rogers 5880, εr₁ = 2.2, H1 = 1.524 mm, and tanδ = 0.0009), whereas the L-slots are etched at the bottom of the substrate. A high frequency full-wave simulator is used to tune the dimensions of the proposed CP MSA, and the optimized sizes are listed as follows: L = 55.4 mm, W = 55.4 mm, L1 = 18 mm, L2 = 19.2 mm, L3 = 3 mm, L4 = 2.9 mm, D1 = 2.6 mm, D2 = 9.2 mm, D3 = 13.2 mm, D4 = 19.9 mm, D5 = 25.1 mm, D6 = 2.6 mm, R1 = 1.6 mm, R2 = 3.8 mm, and H1 = 1.524 mm.

2.2. Antenna Mechanism

To reveal the operated mechanism of the proposed CP MSA, Figure 2(a) shows four evolutionary models (Ant. I to Ant. IV). The models depict a step-by-step design process, and for comparison, Figures 2(b) and 2(c) show the corresponding |S₁₁| and AR values. Note that the square-loop SP structure could excite the fundamental mode (TM₁₁), and the corresponding resonance-frequency point (f₁₁) can be tuned by using the average circumference of the square loop, and the formula is as follows [17]:where ε_r represents the dielectric constant of the substrate, c represents the speed of light, and D2 and D3 represent the square-loop side-lengths. When the length of the arc-shaped strip is a quarter of the waveguide wavelength, the 90°phase difference could be obtained, which is a necessary condition for exciting CP resonant modes. Instead of using the traditional placement method that places four rectangular/square patches at the edge of the square loop [16, 17, 22], we chose to place four rotated rectangular patches at the corners of the square loop (Ant. I) through proximity coupling. As shown in Figure 2, Ant. I with four rotated rectangular patches has two AR resonant points, with AR values being less than 3 dB. This is because the square-loop SP structure could provide a stable continuous phase (0°, 90°, 180°, and 270°). When four L-shaped strips are separately connected with the square-loop, Ant. I has poor return-loss and AR values. To improve the CP bandwidth of Ant. II, the L-shaped strips and rectangular patches are introduced into Ant. III. The 3 dB ARBW and −10 dB IBW of Ant. III could be improved. However, the CP performance of Ant. III is not as good as that of Ant. I, meaning that the four L-shaped strips do not increase the bandwidth. Furthermore, when the L-shaped strip as a parasitic slot is etched into the ground plane, the ARBW and IBW of Ant. IV could be increased. Regarding performance improvement, the introduction of L-shaped slots could generate a new current flow path and extend the previous current path, which deviates the AR resonance points. Finally, the proposed antenna could realize a wide −10 dB IBW of 19.8% (5.64, 5.08–6.2 GHz) and a 3 dB ARBW of 17.5% (5.5, 5.02–5.98 GHz). Furthermore, Table 1 presents a comparison with previously published CP antennas to demonstrate our design’s superior performance. From the table, although the CPBW and peak gain of the proposed antenna is not as good as some referenced antennas in Table 1, the proposed antenna features a new design and low profile, which is the greatest contribution of the proposed antenna.

(a)

(b)

(c)

2.3. Surface Current Analysis

To understand the underlying CP working principle, Figure 3 depicts the simulated surface current distributions of the proposed CP MSA with vector characteristics. The correspondingly continuous phases of 0° and 90° are also marked in Figure 3. Observed that the surface currents are orthogonal in 0° and 90°, which is a necessary condition for exciting CP, the surface current is mainly distributed on the rectangular patch, with a small amount of distribution on edge of the L-shaped slot, whether at low frequency (4.7 GHz) or high frequency (5.2 GHz). Note that the surface currents on the rectangular patch and L-shaped slot with different phases (0° and 90°) are orthogonal. The total surface current of the proposed CP MSA is the vector sum of the surface currents on the edge of L-shaped slots and rectangular patches. As shown in Figure 3, the total surface currents could rotate counterclockwise with varying phases (0° and 90°) at AR resonance points (4.7 and 5.2 GHz). Thus, the proposed CP MSA radiates right-hand CP waves in the +z direction. Additionally, according to the above analysis, we can conclude that the etched L-shaped slots introduce a new current flow path and make the ground plane participate in the radiation. Furthermore, the CP bandwidth of the proposed CP MSA can be improved.

(a)

(b)

3. Experimental Results

In this section, a simulated model of the proposed CP MSA was printed and tested to verify the rationality of the design. The |S₁₁| values are tested by a vector network analyzer (VNA), while the AR, gain, and radiation pattern values are tested by the Satimo Starlab System. For comparison, Figures 4 and 5 depict the correspondingly simulated and measured results. Note that the measured 3 dB ARBW and −10 dB IBW are 13.2% (4.98, 4.65–5.31 GHz) and 18.0% (4.815, 4.38–5.25 GHz), whereas the simulated results are 13.7% (4.95, 4.61–5.29 GHz) and 17.6% (4.88, 4.45–5.31 GHz), respectively. Based on the simulated and measured results, the measured and simulated CP bandwidths are 12.1% (4.95, 4.65–5.25 GHz) and 13.7% (4.95, 4.61–5.29 GHz). The simulated gains and radiation efficiencies and measurement environment photograph of antenna are shown in Figures 4(c) and 4(d), respectively. The measured gains are smaller than the simulated gains at the entire frequency band due to the measurement errors. The simulated and measured peak gains are 10.2 and 9.1 dBi, and the simulated radiation efficiencies are greater than 90% within the CPBW. Additionally, Figure 5 depicts the normalized radiation patterns at 4.7, 5.0, and 5.2 GHz. The figure shows the simulated and measured left-hand CP waves are less than the right-hand CP parts by at least 20 dB in the yoz- and xoz-plane, which reveals that the proposed CP MSA could radiate right-hand CP waves. Because of the error in manufacturing and measured environment, minor differences between the tested and simulated values could be found.

(a)

(b)

(c)

(d)

(a)

(b)

(c)

4. Conclusion

In this study, a compact wideband CP MSA with parasitic elements is designed. The proposed CP MSA consists of a square-loop SP feed network, four rotated rectangular patches, and four L-shaped slots embedded in the ground plane. The square-loop SP feed network is composed of a square loop and an arc-shaped strip, which could provide a 270° phase difference. Four rotated rectangular patches are placed at the edge of the square-loop feeding configuration using a capacitively tightly coupled feeding method to stimulate a CP resonant. The bandwidth of CP MSA could be improved by combining CP modes produced by parasitic elements. After selecting these elements and tuning proper dimensions, the broad operating bandwidths of 4.38–5.25 GHz (18%) for |S₁₁| < −10 dB and 4.65–5.31 GHz (13.2%) for AR < 3 dB could be realized. Hence, the proposed CP MSA has a potential application value in wireless communication.

Data Availability

The data used to support the findings of this study are available from the corresponding author upon request.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Acknowledgments

The research was funded by Guangzhou Basic and Applied Basic Research Foundation (no. 202102020883).

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Copyright

Copyright © 2021 Chenhui Xia et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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