# A Dual-Band Printed End-Fire Antenna with DSPSL Feeding

Authors: Daofeng Ye; Yuanxin Li; Zhixi Liang; Yunliang Long
Journal: International Journal of Antennas and Propagation
 (2016)

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## Abstract

A novel dual-band printed end-fired antenna with double-sided parallel-strip line (DSPSL) feeding is presented. The DSPSL acts in wideband transition using balanced transmission. Two different modes of the parasitic patches allow the antenna to work in different bands. The printed antenna is designed as a quasi-Yagi structure to achieve directivity in the lower band, and the parallel rectangular patches serve as the parasitic director. These patches act as radiation patches with end-fire direction characteristics in the upper band. The measured bandwidths were 18.3% for the lower frequency band (2.28–2.74 GHz) and 12.6% for the upper frequency band (5.46–6.2 GHz).


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## Body

## 1. Introduction

Owing to excellent characteristics including a low profile, simple structure, and low cost, printed end-fire antenna has been widely studied and used in many applications. Microstrip-fed quasi-Yagi antenna [1] is a conventional printed antenna. To increase its bandwidth, it changes its transmission structure [2]. Another approach used a wideband quasi-Yagi antenna with a microstrip-to-slotline as its balun [3]. Another application used an I-shape resonator to obtain a gain enhancement of about 4–6 dB [4].Because of more diverse applications required for mobile wireless communication, some antennas for those devices require not only broad-band capabilities but the dual-band property. A conventional approach to achieve dual-band activity is using branch structure. In [5], the antenna with a simple branch structure allowed nonfixed base station backhaul in GSM communication. A printed antenna [6] for dual-band operations of L1-band Global Navigation Satellite System (GNSS) and S-band China Mobile Multimedia Broadcasting (CMMB) was realized by using a meandered driven dipole and a concave parabolic reflector, and an analogous dual-band quasi-Yagi Wi-Fi antenna was proposed in [7]. Another method was used for a proposed dual-band quasi-Yagi antenna [8] based on application of split ring resonators (SRRs) to provide dual-mode, but this device had a narrow bandwidth due to the limited transmission structure. The use of double-sided parallel-strip line (DSPSL) has potential to overcome this problem. Due to its balance structure, more freedom can be provided in the microwave circuit design. In the past, most studies of DSPSL focused on the microwave circuit design, such as the ultrawide band balun and the low-pass filter [9, 10]. Additional characterization and optimization of DSPSL have led to its wide application in the design of antenna performance [11, 12].In this paper, a new dual-band printed end-fired antenna is presented. The antenna is fed by DSPSL to achieve two operation bands. Two modes of this printed antenna allow function with dual-band characteristic. In different operating bands, the proposed antenna uses parallel rectangular patches either as a director element or as radiation patches, and the driver dipole alternatively acts as the radiation part or feeding part. The lower band (2.28–2.74 GHz) is centred at 2.4 GHz and its upper band (5.46–6.2 GHz) is centred at 5.8 GHz.


## 2. Antenna Design

Figure1 shows the layout of the proposed dual-band printed end-fired antenna. Each side of the antenna is symmetrical, with an arm of driver dipole, the DSPSL, a parallel rectangular patch, and a bent reflector. Figure 2 shows the top side of the proposed antenna. In order to operate in dual-band, the parallel rectangular patches are positioned on the top plane in place of the conventional parasitic dipole, allowing two independent modes, parasitic mode and radiation mode. The DSPSL acts as the feeding structure because it can provide balanced current at any frequency and broaden the bandwidth. Overall, the structure is simple. The reflector dipole is bent and its overall length is about twice the length of the driver dipole. The difference in the arms of the reflector allows changing the directivity of the two operating frequencies. The parameters of the proposed antenna are shown in Table 1.Table 1
Parameter of the proposed antenna.
Symbol
L
1
L
2
L
3
L
4
L
5
W
1
W
2
S
1
S
2
Size (mm)
25
35
20
25.35
17.6
2
5
0.5
1Figure 1
A dual-band printed end-fire antenna geometry.Figure 2
Dimensions of proposed dual-band printed end-fired antenna’s top side.All the patches, including the driver dipole, the parallel rectangular patches, the periodic offset DSPSL structure, and the bent reflectors, are printed on a Wangling Teflon woven glass fabric substrate with relative dielectric constant ofεr=2.65, the dielectric loss tangent of tan⁡θ=0.0015, and the thickness of h=0.8 mm. In the traditional design, the length of the driver dipole (2×L4) is approximately a half wavelength (λ/2) and about twice the length of the DSPSL (L1). To achieve a good match between the DSPSL and the driver, the widths of them are the same.


## 3. Antenna Analysis

Due to the opposite current direction in DSPSL, the transmission structure has no electromagnetic wave radiation and, compared with the antenna presented in [8], the current directions of the double arms of the dipole are the same to ensure end-fire direction without offset. The characteristic impendence of DSPSL is calculated with the modified ratio of the patch’s width to the thickness of the substrate in [11]; that is,(1)Z0=120πεeffW+1.393+0.667ln⁡W+1.444,where εeff is the effective dielectric constant of the substrate. The suitable expression of εeff is(2)εeff=εr+12+εr-1211+10/W,where εr is the relative dielectric constant of the substrate. W is the modified ratio. For the nonoffset DSPSL,(3)W=Th-1,where T is the width of the patch and h is the thickness of the substrate in the DSPSL.According to (2), the characteristic impendence of this DSPSL is about 50 Ω. The bandwidth is wider compared to the conventional printed quasi-Yagi antenna because of its balanced transmission structure.TheE-field magnitudes of two operating frequency are shown in Figure 3, and they are obviously different. This difference results from two different modes of the parallel rectangular patches, a director mode and a radiation mode. In Figure 3(a), the proposed antenna is a traditional quasi-Yagi antenna, and the electric field distributed in the dipole is apparently stronger than the rectangular patch at 2.4 GHz. The radiation of the antenna is mostly generated by the driver dipole and the parallel rectangular patches operate in parasitic mode to act as a conventional parasitic director element, identical to the mechanism of the traditional print quasi-Yagi antenna.Figure 3
E-field magnitude of the antenna at (a) 2.4 GHz and (b) 5.8 GHz.
(a)
(b)When antenna resonates at 5.8 GHz in Figure3(b), the power mainly radiates out from the parallel rectangular patches. The E-field magnitude of the edge of rectangular patches as well as the part of the dipole that is located below the rectangular patches is stronger. The driver dipole has an alternative mode of operation in this operation band and acts in feeding, not as radiation parts. In this condition, the dipole of the antenna forces a time-varying magnetic field in the axial direction of the rectangular patches, thus forcing the parallel rectangular patches to resonate at 5.8 GHz. This reveals that the parallel rectangular patches are in radiation mode and behave like a radiation source at high frequency.In this situation, two frequencies are generated independently of each other. The frequencies are easily controlled by changing the length of the dipole and the patches, the length of the dipole is approximately a half wavelength of the lower frequency, and the patches have the same length of about half the wavelength of the upper frequency. TheS-parameter (S11) of the antennas with different lengths of the dipole and the patches are shown in Figure 4 and they can work separately in the GMS band and GNSS band.Figure 4
The simulatedS11 with different lengths of the dipole and the patches.


## 4. Measured Result

A dual-band printed end-fire antenna was fabricated and is shown in Figure5. The S11 results of the proposed antenna were measured and are shown in Figure 6. The proposed antenna works at two bands: a low operating frequency of 2.4 GHz with 18.3% bandwidth which is provided from 2.28 GHz to 2.74 GHz and an upper operating frequency of 5.8 GHz that is generated by the radiation mode of the parallel rectangular patches, with a bandwidth of about 12.6%.Figure 5
Fabricated dual-band printed end-fired antenna.
(a)
Top layer
(b)
Bottom layerFigure 6
Measured and simulatedS11 for the antenna.The far-field radiation patterns are measured and shown in Figure7. End-fire radiation patterns were detected in thex-y and thex-z planes at two frequencies. The main lobe of the antenna points to the +x direction. Figure 8 shows the gains and efficiencies of the dual-bands. In different bands, the peak gain of the proposed antenna was about 5.2 dB. The measured total efficiency was 83%~95% from 2.2 GHz to 2.8 GHz and 84%~98% from 5.4 GHz to 6.3 GHz.Figure 7
Measured radiation pattern of the antenna in (a)x-y plane and (b)x-z plane.
(a)
(b)Figure 8
Gain and efficiency of (a) lower operating band and (b) upper operating band.
(a)
(b)


## 5. Conclusion

A dual-band printed end-fired antenna with DSPSL feeding is presented. The proposed antenna has dual-band capacity resulting from substitution of the conventional director of the linear parasitic element with parallel rectangular patches. The application of the DSPSL easily simplifies the transmission structure. This antenna has a simple structure and will be useful in the applications of personal communication systems, such as Wi-Fi system.



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*Source: 9845392-2016-05-26.xml*