Circularly Polarized Dielectric Resonator Antenna Arrays with Fractal Cross-Slot-Coupled DRA Elements

Lin, Jia-Hong; Shen, Wen-Hui; Shi, Zhi-Dong; Zhong, Shun-Shi

doi:https://doi.org/10.1155/2017/8160768

International Journal of Antennas and Propagation

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Recent Advances in Array Antenna and Array Signal Processing for Radar

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Research Article | Open Access

Volume 2017 | Article ID 8160768 | https://doi.org/10.1155/2017/8160768

Circularly Polarized Dielectric Resonator Antenna Arrays with Fractal Cross-Slot-Coupled DRA Elements

Jia-Hong Lin,¹Wen-Hui Shen,¹Zhi-Dong Shi,¹and Shun-Shi Zhong¹

Academic Editor: Piotr Samczynski

Received04 Jul 2017

Revised28 Sept 2017

Accepted12 Oct 2017

Published14 Nov 2017

Abstract

In the design of circularly polarized (CP) dielectric resonator antenna (DRA) arrays, the regular-shaped DRAs with simple feeding configurations are mostly used as array elements to make the design procedure more efficient. However, such array element DRA usually achieves only about 6% axial ratio (AR) bandwidth. In this paper, a CP DRA element coupled by a fractal cross-slot which can radiate efficiently and excite the rectangular DRA simultaneously is considered. By adjusting the dimensions of the fractal cross-slot properly, the resonances of the fractal cross-slot and the dielectric resonator can be merged to obtain a wider AR bandwidth. Based on the proposed fractal cross-slot-coupled CP DRA element, two different CP DRA arrays are designed: a wideband CP DRA array and a low-sidelobe-level (SLL) CP DRA array. The designed DRA arrays are fabricated and measured, and structures and performances of the arrays are presented and discussed.

1. Introduction

Over the last decades, DRAs have become more and more popular because of their high radiation efficiency due to the absence of conductor as well as surface wave loss. On the other hand, DRAs can be fed by various feeding techniques, such as the microstrip line feed, the coaxial probe feed, the coplanar waveguide feed, and the aperture coupling feed.

Initial studies of DRAs were concentrated on linearly polarized (LP) designs. In 1985, Haneishi and Takazawa [1] designed the first CP DRA by truncating two opposite corners of a rectangular DRA, and since then many designs of CP DRAs have been proposed. Nowadays, most designs of CP DRA arrays are based on the sequential feeding technique which was proposed by Huang to generate the CP array with LP elements [2]. Moreover, three different kinds of microstrip feeding network for sequential feeding technique are studied in [3], and the hybrid ring feeding network shows a better performance than the parallel feeding network and the series one.

Except for the performance of feeding network, the performance of CP DRA array will also be affected by the array element. Several techniques have been proposed to enhance the axial ratio (AR) bandwidth of the single DRA, such as multiple-feed techniques [4–6], traveling wave excitation [7, 8], and novel DRA geometries [9–11]. However, such designs are not very suitable in the design of DRA array. The multiple-feed designs are complicated to implement because they need a complex feeding network. The lumped resistance in traveling wave excitation will cause a decrease in the radiation efficiency. And compared with the novel DRA geometries, regular-shaped DRAs can make the design procedure more efficient because their resonant frequencies can be predicted easily by the dielectric waveguide model (DWM) method [12].

For these reasons cited above, most designers prefer to use regular-shaped DRAs (e.g., rectangular, cylindrical, and elliptical DRAs) and simple feeding configurations (e.g., single microstrip feed and slot aperture feed) in the design of DRA array. Especially, to avoid the parasitic radiation from feeding network affecting the radiation pattern of the array, the slot aperture feed is mostly widely used. In [13], a cross-slot-coupled cylindrical DRA with 5.6% effective AR bandwidth (S₁₁ < −10 dB and AR < 3 dB) is used as the array element in the CP DRA array. In [3], the slot-coupled elliptical DRA with 5% effective AR bandwidth is used as the array element. It can be seen that such regular-shaped DRAs with simple feeding configurations usually suffer from a narrow effective AR bandwidth. To enhance the effective AR bandwidth of the array element, a structure of two-layered substrates is used in the design of a cross-slot-coupled rectangular DRA, and corresponding effective AR bandwidth of the array element is enhanced to about 9% [14].

In this paper, a CP rectangular DRA element is designed using a relative permittivity ε_r = 8.9, which has an effective AR bandwidth of about 12% by introducing a fractal cross-slot on the ground plane under the resonator. The proposed DRA element has a simple structure without dual feeds or two-layered substrates, and the mutual coupling between two elements of the proposed structure is found to be small although the distance between the elements is relatively small. Based on the fractal cross-slot-coupled CP DRA element, a wideband CP DRA array and a low-sidelobe-level CP DRA array are designed and studied. The arrays are fabricated and their measured results are verified with the simulated one.

2. Design of the Array Element

2.1. Antenna Structure

The structure of the array element is shown in Figure 1. A Rogers RT/duroid 5880 (tm) substrate with relative permittivity ε_r = 2.2, dielectric loss tangent 0.0009, and thickness = 0.508 mm is used in the design, and the length and width of the substrate are both 50 mm. A ceramic cube with relative permittivity ε_r = 8.9, length = 9.8 mm, width = 9.8 mm, and height = 9.1 mm is mounted on the center of the ground plane, and beneath the ceramic cubic is a fractal cross-slot etched on the ground plane. The 50 Ω microstrip line on the bottom side of the substrate has a length of l_f1 + l_f2 and a width of w_f. As shown in Figure 1(a), l_f1 is the distance between the 50 Ω port and the center of the ceramic cubic, and l_f2 is the distance between the center of the ceramic cubic and the terminal of the 50 Ω microstrip line.

(a)

(b)

2.2. Effect of the Fractal Cross-Slot

Figure 1(b) shows the structures of the fractal cross-slot with iterations , 1, and 2. The fractal structure is developed from the ordinary cross-slot () which has lengths of l_s1, l_s2 (l_s2 = k_s × l_s1) and a width of w_s. In the iterative procedure, the width of the slot is constant, and the iterative angle and iterative length coefficient are φ and 0.5, respectively.

To explain the effect of the fractal structure, simulated S₁₁ and ARs of the array element with different values of and l_s1 are presented in Figure 2. According to the DWM method, the theoretical resonant frequencies of and modes in the proposed rectangular DRA are both 6.67 GHz. To obtain the CP radiation, these two modes should be excited simultaneously in the DRA. Of course, the practical resonant frequency in the DRA will also be affected by the feeding structure. Generally speaking, practical resonant frequencies of and modes will not be identical. As long as these two modes are excited at the adjacent frequency band, the effective CP radiation can be obtained. However, the AR bandwidth due to the resonances of the dielectric resonator is usually narrow. To enhance the AR bandwidth, dimensions of the cross-slot need to be adjusted suitably, so that the resonances of the cross-slot and the dielectric resonator can be merged to obtain a wider AR bandwidth, and then, the corresponding DRA will be a hybrid-radiation CP DRA.

(a)

(b)

However, when the ordinary cross-slot () is used, such hybrid-radiation CP DRA is difficult to be obtained. As shown in Figure 2, when and l_s1 = 7.9 mm, two resonant frequencies can be found in the S₁₁ curve. The lower resonant frequency (about 7.2 GHz) is due to the resonance of the DRA, and the higher one (about 8.6 GHz) is due to the resonance of the slot. In fact, the and modes in the DRA are not effectively excited here. According to the DWM method, the resonant frequency at 7.2 GHz is due to the mode in the DRA (the theoretical resonant frequency of mode is about 7.4 GHz). Besides the ineffective excitation of and modes, the resonant frequency of the slot is too far away from that of the DRA.

To effectively excite the and modes and lower the resonant frequency of the slot, the simplest method is to increase the value of l_s1. By simulation, we found that the and modes can be most effectively excited when l_s1 = 12 mm. At this time, the resonant frequencies of the above two modes are about 6.4 GHz and 6.8 GHz, and resonant frequencies of two orthogonal modes in the slot can be lowered to 7.2 GHz and 7.9 GHz, as shown in Figure 2(a). In this situation, the corresponding CP bands of DRA and slot are found to be around 6.5 GHz and 7.5 GHz, respectively. However, according to Figure 2(b), we can find that these two CP bands are also too far away from each other to be merged.

Compared with the ordinary cross-slot, the fractal structure can lower the resonant frequency of the slot more efficiently. When the second iteration () is used, the resonant frequencies of and modes are also about 6.4 GHz and 6.8 GHz, but resonant frequencies of two orthogonal modes in the slot are further lowered to 7.0 GHz and 7.6 GHz. In this situation, CP bands of DRA and slot are found to be well merged, which can effectively enhance the AR bandwidth of the array element.

2.3. Simulated Results

In our design, the parameters of the array element are optimized by the FEM-based commercial software HFSS, and the final parameters of the array element are as follows: w_f = 1.52 mm, l_f1 = 25 mm, l_f2 = 4 mm, l_s1 = 9.7 mm, w_s = 0.4 mm, k_s = 0.57, and φ = 50°.

Figure 3 is the simulated AR and S₁₁ of the array element. The impedance bandwidth of the array element is 26.8% (from 6.12 to 8.01 GHz), and the 3 dB AR bandwidth is 11.9% (from 6.49 to 7.31 GHz). Compared with the results in [3, 13] and [14], the proposed array element coupled by the fractal cross-slot can achieve the widest effective AR bandwidth (11.9%, from 6.49 to 7.31 GHz).

Figure 4 is the simulated radiation patterns across the effective AR bandwidth. It can be seen that the radiation patterns are stable across the effective AR bandwidth. Moreover, the radiation pattern has no sidelobe in the upper half space at every frequency, and the maximum radiation happens at θ = 0° and φ = 0°, which can ensure the design of a low-sidelobe-level array. The left-hand circular polarization (LHCP) gain at 6.5 GHz, 6.75 GHz, 7.0 GHz, and 7.25 GHz are 7.16 dBi, 7.02 dBi, 6.61 dBi, and 6.33 dBi, respectively.

(a)

(b)

(c)

(d)

Since we are proposing the proposed fractal cross-slot coupled DRA for array applications, the mutual coupling between two array elements is studied. The positions of two DRAs in Figures 5(a) and 5(b)are roughly equal to that in a sequential feeding network and a series feeding network which will be used in our design, respectively. The simulated port mutual coupling is shown in Figure 6. The maximum mutual coupling between two elements is lower than −20 dB, which shows a good isolation between array elements.

(a)

(b)

3. Design of the Wideband CP DRA Array

3.1. Antenna Structure

The structure of the proposed 2 × 2 wideband CP DRA array is shown in Figure 7. The length l and width w of the substrate are 100 mm and 84 mm, respectively. In our design, the hybrid ring feeding network for sequential feeding technique is used, and details of the feeding network designs and analyses can be found in [3].

To get the best performance of the DRA array, parameters of the array are optimized by HFSS. In the design of the array element, the distance between the center of the DRA and the 50 Ω port is l_f1 = 25 mm. In fact, the value of l_f1 in the array element is decided by dimensions of the substrate. For the array element, a large enough substrate is needed to guarantee the performance of the DRA (mainly the radiation pattern and AR), which means that the value of l_f1 cannot be too small. But in the design of the array, the substrate is much larger than that in the array element, which can ensure the performance of the DRA array. In this situation, a smaller value of l_f1 can be selected to accelerate the simulation without degenerating the performance of the array.

Besides the value of l_f1, dimensions of the fractal cross-slot are also optimized in the design, and we find that value of w_s can affect the array more than other parameters.

3.2. Discussion of the Effect of w_s

Figure 8 shows the effect of w_s on AR of the DRA array. When w_s increases, the curve of AR is found to move to the higher frequency band, and the 3 dB AR bandwidth is enhanced due to a lower AR over the frequency band above 8 GHz. When w_s = 1.2 mm, the widest 3 dB AR bandwidth can be obtained. This is an interesting conclusion, which means that the value of w_s, which can lead the widest 3 dB AR bandwidth in the array, is very different from that in the array element.

To explain this problem more clearly, the effect of w_s on the AR of the array element is presented in Figure 9. It is true that the widest 3 dB AR bandwidth can be obtained when w_s = 0.4 mm. However, when w_s = 0.4 mm is used, AR of the array element will increase quickly with the increase of frequency. In this situation, the AR of the array element over the frequency band above 8 GHz is higher than 9 dB. When a larger value of w_s is used, the 3 dB AR bandwidth will deteriorate, but a lower AR can be found in the higher frequency band. When the value of w_s is larger than 1.0 mm, AR of the array element is basically lower than 9 dB from 6.0 to 8.5 GHz.

Through analyzing, we think that the above interesting phenomenon is due to the intrinsic characteristic of the sequential feeding network. As mentioned before, the sequential feeding technique can be used to generate CP array with LP elements, which means that the sequential feeding network can be used to lower the AR of the array element. For example, assume that AR of an array element at frequency f₀ is AR₀, if we use the sequential feeding technique to structure an array, the corresponding AR of the array at the same frequency f₀ should be lower than AR₀. So, if we want to obtain the widest 3 dB AR bandwidth in the DRA array, we can use another value of AR (AR′) as the design objective in the design of the array element, and AR′ should be higher than 3 dB.

Comparing the results in Figures 8 and 9, we can find that, considering the frequency band from 6.0 to 8.5 GHz, once the AR of the array element at a particular frequency (f₀) is not higher than 9 dB, the corresponding AR of the DRA array at the same frequency f₀ can be lowered to below 3 dB by the sequential feeding network. So, even though w_s = 0.4 mm can lead the widest 3 dB AR bandwidth in the array element, the larger value of w_s can lead a wider 9 dB AR bandwidth in the array element, which can finally lead a wider 3 dB AR bandwidth in the DRA array. Finally, we select w_s = 1.2 mm in our design, because in this situation, the widest 3 dB AR bandwidth can be obtained in the DRA array.

Of course, it must be point out that the above conclusion “once the AR of the array element at a particular frequency (f₀) is not higher than 9 dB, the corresponding AR of the DRA array at the same frequency f₀ can be lowered to below 3 dB” is not obtained by theoretical analysis or computation, but by the comparison of results in Figures 8 and 9. However, even though it is not a quantitative conclusion, we think that it is a correct qualitative conclusion, which can have a guiding significance in the design of antenna arrays.

3.3. Simulated and Measured Results

In our design, parameters of the DRA array are optimized by HFSS, and all optimized parameters of the array are shown in Table 1.

The proposed wideband CP DRA array is fabricated and measured, and the photo of the fabricated array is shown in Figure 10. To mount the dielectric resonator properly, two extra L-shaped slots are etched around the fractal cross-slot which can show an accurate position of the rectangular dielectric resonator, and by simulation, we ensure that such extra structure will not affect the performance of the array.

(a)

(b)

(c)

(d)

Figure 11 is the S₁₁ of the proposed DRA array. The simulated impedance bandwidth is 46.5% (from 5.54 to 8.90 GHz), and the measured one is 51.5% (from 5.52 to 9.35 GHz). According to Figure 11, the measured result has a wider impedance bandwidth than the simulated one due to a better impedance matching over the frequency band above 9.0 GHz.

The standard linearly polarized horn antennas are employed for radiation measurements. The simulated and measured boresight ARs of the array are shown in Figure 12. The simulated 3 dB AR bandwidth is 37.7% (from 5.84 to 8.55 GHz), and the measured one is 38.3% (from 6.06 to 8.93 GHz). A good agreement is obtained between the simulated and measured ARs, except for about 300 MHz shift between the simulated and measured results. The measured boresight LHCP gain of the array is also shown in Figure 12. Across most of the 3 dB AR bandwidth, the measured boresight LHCP gain is higher than 10 dBi (from 6.06 to 8.51 GHz), and a highest 12.17 dBi gain is found at 7.9 GHz.

The simulated and measured radiation patterns with vertical and horizontal polarization at 6.5 GHz, 7.5 GHz, and 8.5 GHz in x-z plane are shown in Figure 13. Over the lower frequency band, the patterns are stable, and symmetric radiation can be found in the broadside directions. Moreover, good agreements are obtained between the simulated and measured results at 6.5 GHz and 7.5 GHz. When frequency increases to 8.5 GHz, about 5° beam tilt can be found in the measured pattern. Compared with the simulated result, a higher gain can also be found at 8.5 GHz, as well as a higher back-lobe level.

(a)

(b)

(c)

3.4. Comparisons

Table 2 gives the comparisons of the proposed DRA array to other reported wideband CP DRA arrays. It can be seen that the proposed DRA array in this paper can provide a wider effective AR bandwidth than others. It is necessary to point out that the sequential feeding technique and the corresponding hybrid ring feeding network are all used in [3, 14], and this design. So, we can ensure that it is the structure of fractal cross-slot and the careful parameter optimization that provide a wider effective AR bandwidth in our design.

4. Design of the Low-Sidelobe-Level CP DRA Array

In recent years, more and more attentions have been paid to the design of low-sidelobe-level DRA arrays. In [15], low-sidelobe-level DRA array fed by dielectric insular image guide (DIIG) is investigated. In [16], slot windows and reflector are used in the design of DRA array. In [17], DRA array with parasitic DRA elements is proposed. However, it seems that most of the designs mentioned in this paper are either on generating circular polarization or suppressing the SLL of DRA array, but not both.

In this paper, a low-sidelobe-level CP DRA array is also designed based on the proposed fractal cross-slot-coupled array element, which can be another verification of the proposed DRA element.

4.1. Antenna Structure

Figure 14 shows the structure of the designed 1 × 6 low-sidelobe-level CP DRA array. In this design, we rotate all slots to 90° to generate the right-handed circularly polarized (RHCP) radiation. Six ceramic cubes are mounted on a substrate with length L = 206 mm and width W = 59 mm. The proposed DRA array is designed to operate at 7.0 GHz with a −20 dB SLL. To achieve such goal, a Chebyshev amplitude distribution and the corresponding series feeding network are used. To achieve a −20 dB SLL, the current ratios of the 6-element Chebyshev array is I₁ : I₂ : I₃ = 1 : 0.777 : 0.551. Details of series feeding network designs and analyses can be found in [18].

When the series feeding network is used, we need to adjust the input impedance of the array element to get 50 Ω input impedance in the sum port of the DRA array. In our design, the required input impedance of the array element is 190 Ω. To reduce the discontinuity of the width of the microstrip line in the feeding network, two λ/4 lines are used for impedance conversion in our design. Firstly, the 70 Ω microstrip line is used between the array element and series feeding network, which can convert the input impedance of the array element to 98 Ω. Thus, the input impedance in the sum port becomes 25.85 Ω. So, another 36 Ω microstrip line is used to get the 50 Ω input impedance in the sum port.

The parameters of the DRA array are optimized by HFSS, and the final results are shown in Table 3. Different from the sequential feeding network, the series feeding network has no effect on AR, so it can be found that the optimized value of w_s in Table 3 is close to the optimized value in array element.

4.2. Simulated and Measured Results

The proposed DRA array is fabricated and measured, and a photo of the array is shown in Figure 15.

(a)

(b)

(c)

Figures 16 and 17 show the S₁₁, AR, and boresight RHCP gain of the array. The simulated and measured impedance bandwidths of the array are 18.1% (from 6.38 to 7.65 GHz) and 33.1% (from 6.07 to 8.48 GHz), respectively. The simulated 3 dB AR bandwidth is 13.9% (from 6.51 to 7.48 GHz), and the measured one is 12.4% (from 6.58 to 7.45 GHz). Due to a better impedance matching over the frequency band from 7.8 to 8.5 GHz, the measured impedance is much wider than the simulated one. However, it is obvious that the real performance of DRA array will be subject to the measured 3 dB AR bandwidth, which is 1.5% narrower than the simulated AR bandwidth. Across the measured 3 dB AR bandwidth, the boresight RHCP gain of the array is about 12.5 dBi, except a lowest measured RHCP gain around 7.1 GHz (about 10.0 dBi), and the highest measured RHCP gain is 13.43 dBi at 7.4 GHz.

Figures 18 and 19 are the normalized radiation patterns of the array. It is necessary to point out that all data in Figures 18 and 19 are based on the total gain of the DRA array. As mentioned above, two standard linearly polarized horn antennas are employed for radiation measurements, so the measured results of radiation pattern consist of two parts: the vertical polarized gain G_V and the horizontal polarized gain G_H, and the corresponding total gain can be computed by

Figure 18 shows the normalized radiation patterns of the array at 7.0 GHz. The simulated SLL in x-z plane (φ = 0°) is about −21 dB, which is lower than our design target. Of course, we think that such result is derived from the errors in simulation. The measured SLL at 7.0 GHz is −18.72 dB, which is very close to the design target.

As shown in Figure 19, the frequency band over which SLL < −15 dB is found to be from 6.67 to 7.37 GHz, which is 9.97%. As mentioned above, over such frequency band (SLL < −15 dB), S₁₁ < −10 dB and AR < 3 dB can also be satisfied. The lowest measured SLL of −19.23 dB happens at 6.94 GHz.

4.3. Comparisons

Because no reported results of low-sidelobe-level CP DRA arrays are found, we present the comparisons of the proposed array to other reported low-sidelobe-level and wideband DRA arrays (LP arrays) in recent years in Table 4. The proposed low-sidelobe-level CP DRA array shows a wider impedance bandwidth than other designs (except [16], in which the slot windows and reflector are used), and the minor difference between the expected SLL and the obtained SLL can show a successful suppression of sidelobe. Of course, compared to our design, higher antenna gain can be found in others. We think the cause of that is the difference in element number. Through the abovementioned comparisons, we believe that our design can be considered as a good design of low-sidelobe-level and wideband DRA array. On this basis, an extra 3 dB AR bandwidth of 12.4% can be obtained in our design. Compared with the purely LP arrays, we think that the proposed low-sidelobe-level DRA array with CP characteristic is more attractive and valuable.

5. Conclusion

Based on the proposed fractal cross-slot-coupled CP DRA, designs of a wideband CP DRA array and a low-sidelobe-level DRA array are proposed in this paper. Effective AR bandwidth of the proposed wideband CP DRA array is 38.3% (from 6.06 to 8.93 GHz), and 12.17 dBi peak gain is obtained. The proposed low-sidelobe-level CP DRA array has an effective AR bandwidth of 12.4% (from 6.58 to 7.45 GHz), and a 9.97% (from 6.67 to 7.37 GHz) for −15 dB SLL bandwidth is obtained. The results of our work show that the proposed fractal cross-slot-coupled DRA element, which has a simple structure without dual feeds or two-layered substrates, is quite suitable for the design of DRA arrays.

Conflicts of Interest

The authors declare that there are no competing interests regarding the publication of this paper.

Acknowledgments

This work was supported by the Natural Science Foundation of China under Grant no. 61171031.

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Copyright © 2017 Jia-Hong Lin 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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International Journal of Antennas and Propagation

Recent Advances in Array Antenna and Array Signal Processing for Radar

Circularly Polarized Dielectric Resonator Antenna Arrays with Fractal Cross-Slot-Coupled DRA Elements

Abstract

1. Introduction

2. Design of the Array Element

2.1. Antenna Structure

2.2. Effect of the Fractal Cross-Slot

2.3. Simulated Results

3. Design of the Wideband CP DRA Array

3.1. Antenna Structure

3.2. Discussion of the Effect of ws

3.3. Simulated and Measured Results

3.4. Comparisons

4. Design of the Low-Sidelobe-Level CP DRA Array

4.1. Antenna Structure

4.2. Simulated and Measured Results

4.3. Comparisons

5. Conclusion

Conflicts of Interest

Acknowledgments

References

Copyright

3.2. Discussion of the Effect of w_s