# A Single-Point-Fed Wideband Circularly Polarized Rectangular Dielectric Resonator Antenna

Authors: Deqiang Yang; Meng Zou; Jin Pan
Journal: International Journal of Antennas and Propagation
 (2016)

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## Abstract

A single-point-fed circularly polarized (CP) rectangular dielectric resonator antenna (DRA) with wide CP bandwidth is presented. By usingTE111 and TE113 modes of the rectangular DRA, a wideband CP performance is achieved. The coupling slot of the antenna contains a resistor loaded monofilar-spiral-slot and four linear slots. Design concept of the proposed antenna is demonstrated by simulations, and parameter studies are carried out. Prototype of the proposed antenna was fabricated and measured. Good agreement between the simulation and measurement is obtained. The measured impedance bandwidth (|S11|<-10 dB) and 3 dB axial-ratio (AR) bandwidth are 51.4% (1.91–3.23 GHz) and 33.0% (2.15–3.00 GHz), respectively.


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## Body

## 1. Introduction

Dielectric resonator antenna (DRA) [1–4] is a good candidate for wireless service equipment due to its attractive characteristics such as small size, wide bandwidth, and high radiation efficiency.DRAs with circular polarization (CP) performance are more applicable for the wireless systems than the linearly polarized (LP) ones [5–9], because the CP wireless systems can support flexible orientation between the receiving and transmitting antennas. The published CP DRAs can be divided into two classes: single-point-fed [5–7] and dual-point-fed [8, 9] ones. Single-point-fed CP DRA is easy to implement, but its axial-ratio (AR) bandwidth is narrow. Dual-point-fed CP DRA has a wider AR bandwidth, but it needs a complicated power divider. Recently, several single-point-fed CP DRAs with wide 3 dB AR bandwidths have been reported. For example, a CP hollow rectangular DRA with wide AR bandwidth of 12.4% has been reported in [10]. In [11], simple inclined slot fed CP trapezoidal DRA with an AR bandwidth of as wide as 21.5% has been obtained. Single-point-fed wideband CP DRAs can also be realized by using novel feeding structures [12–14]. And in [15], a 3 dB AR bandwidth of 24.6% has been achieved by merging resonances of the DRA and coupling slot.In recent years, some CP DRAs with wideband [16, 17] and dual-band [18, 19] performances have been realized by taking advantages of the higher order modes of the DRAs. In this letter, a single-point-fed wideband CP rectangular DRA using higher order mode is investigated. The TE111 and TE113 modes of rectangular DRA are excited by microstrip line through a slot etched on ground plane to achieve wideband CP operation. Ansoft HFSS [20] was used to simulate the performances of the proposed DRA. Parametric studies have also been carried out to investigate the DRA. To verify the simulation, a prototype antenna was fabricated and measured. Reasonable agreement between the simulated and measured results was attained. The measured results show a wide 3 dB AR bandwidth of 33.0% and a wide impedance bandwidth (S11<-10 dB) of 51.4%.


## 2. Antenna Structure

Geometry of the single-point-fed wideband CP rectangular DRA is shown in Figure1. The rectangular DRA has dimensions of a = b = 22 mm and c = 40 mm, and it is manufactured from a ceramic material with permittivity of εr = 10. The substrate (εrs= 2.2) has a side length of lg = 50 mm and a thickness of t = 1 mm. The coupling slot etched on the ground plane consists of a monofilar-spiral-slot and four linear slots. The width of the slot is w = 1 mm. Main side lengths of the monofilar-spiral-slot are l3 = 6 mm, l4 = 6 mm, l5 = 7 mm, and l6 = 12 mm. Lengths of the slot arms located at 45° and 225° with respect to the x-axis are equal to l1. And the lengths of the other two slot arms located at 135° and 315° with respect to the x-axis are equal to l2. For the proposed DRA, the lengths of linear slots are l1 = 8.0 mm and l2 = 6.8 mm. A resistor with resistance of R = 62 Ω is placed at lr = 6 mm from the end of the slot. The 50 Ω microstrip line (wm = 3 mm, lm = 26 mm) is etched on the other side of substrate, and it is short-circuited to the ground plane at the end.Figure 1
Geometry of the proposed single-point-fed wideband CP rectangular DRA.Resonant frequencies ofTE111 and TE113 modes of the rectangular dielectric resonator (DR) can be calculated by using dielectric waveguide model (DWM) [21] or Ansoft HFSS. The calculated results of the DR in proposed antenna are shown in Table 1. Discrepancies between the two results are caused by error of the DWM.Table 1
Calculated resonant frequencies ofTE111 and TE113 modes of the proposed rectangular DR.
Computing method
T
E
111 mode
T
E
113 mode
DWM
2.42 GHz
3.03 GHz
Ansoft HFSS
2.52 GHz
3.08 GHz


## 3. Results

To verify the design, the proposed single-point-fed wideband CP rectangular DRA was fabricated and measured. Photographs of the fabricated antenna are shown in Figure2. To avoid air gap between the DR and ground plane, the resistor is soldered at the bottom of the substrate by two via holes. Simulated and measured reflection coefficients of the proposed antenna are shown in Figure 3. Measured impedance bandwidth (S11<-10 dB) is 51.4% (1.91–3.23 GHz), and it agrees well with the simulated one. With reference to Figure 3, there are four resonant frequencies found at 2.24 GHz, 2.44 GHz, 2.84 GHz, and 3.16 GHz across the measured impedance bandwidth. The first couple of resonant frequencies are due to the TE111 modes, and the second couple of resonant frequencies are caused by the TE113 modes.Figure 2
Photographs of the fabricated antenna.Figure 3
Simulated and measured reflection coefficients of the proposed single-point-fed wideband CP rectangular DRA.Figure4 shows the simulated and measured broadside ARs of the proposed antenna. The simulated and measured 3 dB AR bandwidth are 31.2% (2.19–3.00 GHz) and 33.0% (2.15–3.00 GHz), respectively. From Figure 4, two simulated minimum AR values of 1.7 dB and 0.9 dB are obtained at 2.42 GHz and 2.90 GHz, respectively. SimulatedH-fields in the proposed DRA at 2.42 GHz and 2.90 GHz are shown in Figures 5(a) and 5(b).H-field distributions demonstrate that the TE111 mode is excited at 2.42 GHz and the TE113 mode is excited at 2.90 GHz. Figure 6 shows the simulated and measured patterns of the proposed single-point-fed wideband CP rectangular DRA. The radiation patterns of proposed antenna are broadside as expected, because both of the TE111 and TE113 are broadside modes. And the antenna is RHCP in broadside direction across the CP bandwidth. Figure 7 shows the simulated and measured RHCP gains of the proposed DRA. The measured peak RHCP gain is 6.8 dBi at 2.70 GHz. And the measured result shows an average RHCP gain of 5.4 dBi across the 3 dB AR bandwidth.Figure 4
Simulated and measured axial ratios of the proposed single-point-fed wideband CP rectangular DRA.Figure 5
H-fields in the proposed single-point-fed wideband CP rectangular DRA. (a) H-fields at 2.42 GHz. (b) H-fields at 2.90 GHz.
(a)
(b)Figure 6
Simulated and measured radiation patterns of the proposed single-point-fed wideband CP rectangular DRA. (a) 2.3 GHz. (b) 2.7 GHz.
(a)
(b)Figure 7
Simulated and measured RHCP gains of the proposed single-point-fed wideband CP rectangular DRA.


## 4. Parametric Studies

Effects of the resistor on antenna performances are investigated by HFSS simulations. Simulated AR of the proposed DRA without resistor loading is shown in Figure4. The DRA without resistor has a 3 dB AR bandwidth of 6.1% (2.72–2.89 GHz). And the 3 dB AR bandwidth of the loaded one is about 5.0 times of the unloaded one. Simulated reflection coefficient of the unloaded one is shown in Figure 3. The resistor has a small effect on the reflection coefficient of the proposed antenna. Simulated total efficiencies of the proposed DRA with and without resistor loading are shown in Figure 8. The efficiency of the loaded one is smaller than the unloaded one because of the loss introduced by the resistor. The minimum efficiency and average efficiency of the loaded one across the CP bandwidth are 0.62 and 0.89, respectively. Figure 9 shows the simulated RHCP and LHCP gains of the proposed DRA with and without resistor loading. From Figure 9, the LHCP component drops a lot when the antenna is loaded, and the resistor has a small effect on the RHCP component of the proposed antenna.Figure 8
Simulated total efficiencies of the proposed DRA with and without resistor loading.Figure 9
Simulated gains of the proposed DRA with and without resistor loading. (a) RHCP gains. (b) LHCP gains.
(a)
(b)To explain the effect of resistor on antenna performance, the electric fieldEs→ in the slot is studied. Figure 10 shows the simulated Es→ at f = 2.4 GHz and f = 2.9 GHz in different time steps for the antenna without resistor loading. Es→ is strong at the position of the resistor for f = 2.4 GHz, while it is weak at the position of the resistor for f = 2.9 GHz. This means that some power will be dissipated in the resistor at 2.4 GHz and very little power will be lost in the resistor at 2.9 GHz when the antenna is loaded, and that is why the resistor has effect on only lower band of the antenna. Moreover, it can be seen that the equivalent magnetic current (Ms→=Es→×Z^) in the monofilar-spiral-slot at 2.4 GHz is in a travelling waveform. The resistor, which acts as a resistive termination for the monofilar-spiral-slot, can improve travelling wave performance of the equivalent magnetic current and thus the CP performance at the lower band.Figure 10
SimulatedEs→ in the slot. (T=1/f).The AR and total efficiency for different values ofR are shown in Figure 11. With reference to the figure, the widest CP bandwidth is obtained at R = 60 Ω. And the total efficiency remains almost unchanged when R increases from 20 Ω to 100 Ω.Figure 11
AR and total efficiency and for different values ofR.Effects of the location of resistor on antenna performances have also been studied. The 3 dB AR bandwidth as function oflr is shown in Figure 12, and it can be observed that CP bandwidth of the proposed antenna increases with the increase of lr. Minimum total efficiency and average total efficiency across the 3 dB AR bandwidth versus lr are also exhibited in Figure 12. From Figure 12, both of the minimum and average total efficiency decrease with the increase of lr. Proper value of lr can be decided based on Figure 12 and the special design objectives.Figure 12
Effects oflr on AR and total efficiency of the proposed antenna.Comparison between the proposed antenna and some of the recently published single-point-fed CP DRAs is listed in Table2. It is seen that the proposed antenna has a wide bandwidth and reasonable antenna efficiency.Table 2
Comparison between the proposed antenna and other published single-point-fed CP DRAs.
DRA shape
ε
r
3 dB AR bandwidth
Impedance bandwidth
Average total efficiency
Reference
Hollow rectangular
9.4
12.4%
32.5%
—
[10]
Trapezoidal
9.4
21.5%
33.5%
90%
[11]
Rectangular
9.2
14.0%
19.0%
98%
[12]
Rectangular
12
18.7%
53.5%
75%
[13]
Rectangular
12
25.5%
—
82%
[14]
Rectangular
10
33.0%
51.4%
89%
Proposed


## 5. Conclusion

A single-point-fed wideband CP rectangular DRA has been proposed and discussed in this letter. The design concept is based on utilizing the fundamentalTE111 and high order TE113 modes of rectangular DRA. Proposed design concept has been certified by HFSS simulation. And parametric studies have been carried out to investigate effects of the resistor on antenna performances. A prototype antenna was designed and fabricated. The measured 3 dB AR bandwidth and impedance bandwidth (S11<-10 dB) are as wide as 33.0% and 51.4%, respectively.



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*Source: 8210781-2016-01-17.xml*