# Planar Printed Shorted Monopole Antenna with Coupled Feed for LTE/WWAN Mobile Handset Applications

Authors: Do-Gu Kang; Youngje Sung
Journal: International Journal of Antennas and Propagation
 (2013)

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## Abstract

A shorted monopole antenna with coupled feed for LTE/WWAN mobile handset applications is described. The basic resonance of the shorted monopole combines with the resonance formed by the coupling between the coupling strip and the feeding pad to cover the LTE700, GSM850, and GSM900 bands. Both the feeding pad and the coupling strip operate with the shorting strip as a loop antenna. The resonance of the loop antenna and the harmonics of the shorted monopole combine to cover the GSM1800, GSM1900, UMTS, and LTE2300 bands. A stable and omnidirectional radiation pattern with reasonable gain has been observed over the operating bandwidth.


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## Body

## 1. Introduction

Technological advancements and the diversity of needs in wireless communication are leading to the development of antennas for smaller, lighter, and more multifunctional mobile handsets [1]. Consequently, planar monopoles [2–4] enabling pentaband WWAN (wireless wide area network) operation have been developed. The WWAN band covers the GSM850 (824–894 MHz), GSM900 (880–960 MHz), GSM1800 (1710–1880 MHz), GSM1900 (1850–1990 MHz), and UMTS (1920–2170 MHz) bands. These developed planar monopoles are, respectively, a monopole with coupled strips [2], a CPW-fed LI-shaped monopole [3], and a coupled-fed shorted monopole [4]. Recently, coupled-fed shorted monopoles covering not only the WWAN band but also the LTE band have been developed. The LTE band covers LTE700 (698–798 MHz), LTE2300 (2300–2400 MHz), and LTE2500 (2500–2690 MHz) [5, 6]. These monopoles operating in the WWAN/LTE bands are, respectively, a monopole with a tuning stub [5] and a monopole with a chip inductor-loaded shorted strip [6].In this paper, a shorted monopole antenna with coupled feed for LTE/WWAN bands is proposed. The base resonance of the shorted monopole combines with the resonance formed by the coupling between the feeding pad and the coupling strip to include the LTE700, GSM850, and GSM900 bands. The loop antenna is formed by both the coupled feed structure and the shorting strip. The loop resonance and a harmonic element combine to cover the GSM1800, GSM1900, UMTS, and LTE2300 bands. Therefore, the proposed structure covers the LTE700, LTE2300, GSM850, GSM900, GSM1800, GSM1900, and UMTS bands.


## 2. Antenna Geometry

Figure1 shows the proposed antenna which consists of a long radiator (AB), a coupling strip (BC), a feeding pad, and a shorting strip. l1 denotes the total length of the long radiator. l2 denotes the length of the part generating the coupled feed, and g denotes the gap between the feeding pad and the coupling strip; these are the two parameters that affect the coupled feed.  l3 denotes the length of the feeding pad. The antenna covers an area of 18×49 mm2 on the upper surface of an FR4 substrate with a 0.6 mm thick. The total area of the substrate is 118×49 mm2; the ground (GND) found on the lower surface of the substrate covers an area of 100×49 mm2.(a) 3D geometry of  the proposed antenna. (b) The antenna geometry as seen from above.
(a)
(b)


## 3. Simulated and Measured Results

Figure2 shows the simulated and measured reflection coefficients for the proposed antenna and reference 1. The parameters for the proposed antenna were set to l1=78 mm, l2=16.5 mm, g=0.3 mm, and l3=21.5 mm. The prototype of the proposed antenna is based on the foregoing optimized parameters and is fabricated as shown in Figure 3. The simulation was carried out through HFSS. The simulated results were nearly identical to the measured results. The proposed antenna has four resonant frequencies (f1, f2, f3, and f4). The low band covers the LTE700, GSM850, and GSM900 bands, and the high band covers the GSM1800, GSM1900, UMTS, and LTE2300 bands. All the bands operated properly with a −6 dB bandwidth which is a widely used value for internal WWAN antennas in practical mobile phone application.Simulated and measured reflection coefficients for the proposed antenna and reference 1.
(a)
(b)Figure 3
Fabricated prototype of the proposed antenna.If the proposed antenna’s result is compared to reference 1′s (the proposed antenna with direct feed) result, the effect of the coupled feed can be observed. The matching characteristics of the base resonance were improved by the coupled feed that increases the electrical length. Therefore, the resonance frequency decreased. The resonance combined with the second resonance that was formed by the coupled feed. The two resonances form dual resonance. Therefore, the proposed antenna achieves a low wideband through the coupled feed.Figure4 shows the simulated reflection coefficients relative to the changes in the total length l1 of the long radiator. The base resonance f1 is formed by the long radiator’s length which was a resonance length of  λ/4 at f1 (0.69 GHz). Further, f3 decreased, which proves that f3 is a harmonic of f1. As l1 increased, the lower edge of the high band decreased from 1.8 to 1.71 GHz. Thus, the antenna covers the GSM1800 band. Therefore, considering the high band,  l1 was selected as 78 mm.Figure 4
Simulated reflection coefficients relative to changes in the total length of the long radiatorl1.Figure5 shows the simulated reflection coefficients relative to the changes in length l2 of the part generating the coupled feed l2. Because l2 affects the coupled feed, the resonance formed by the coupled feed was affected as l2 changed. The base resonance formed by the long radiator further combined with the resonance formed by the coupled feed as l2 increased. l2 was selected as 16.5 mm to allow the antenna to have low wideband characteristics.Figure 5
Simulated reflection coefficients relative to changes in the length of the part generating the coupled feedl2.Figure6 shows the simulated reflection coefficients relative to the changes in gap g between the feeding pad and the coupling strip. As g decreased, the matching of f2 improved in the state the matching between f1 and f2 improved. Thus, considering the low band, g was selected as 0.3 mm.Figure 6
Simulated reflection coefficients relative to changes in the gap between feeding pad and coupling stripg.Figure7 shows the surface current distribution simulated on the proposed antenna’s radiator and GND at f4=2.3 GHz. The red area indicates a strong field, whereas the blue area indicates a weak field. The maximum current is located at the beginning of the feeding pad, and the null of the current is located at the end. The coupled gap was electrically connected. The maximum current on the coupling strip generated the maximum current on the shorting strip’s end. The null is located between the maximum current on the shorting strip’s end and the maximum current on the shorting strip’s beginning. Through these findings, the path from the feeding pad to the coupled gap was combined with the path from the coupling strip to the shorting strip, which was the path of the loop operating at the λ resonant length. Therefore, f4 was the resonant frequency of the loop antenna.Figure 7
Surface current distribution simulated on the proposed antenna’s radiator and GND atf4=2.3 GHz.Figure8 shows the simulated reflection coefficients relative to the changes in length l3 of the feeding pad. As l3 increased, the matching characteristics between f1 and f2 improved with a decrease of f2. Because l3 affected the length of the coupled feed, its effect was analogous to the effect of l2 and g in the low band. Further, the matching characteristics between f3 and f4 improved with a decrease of f4. To take into consideration the effect of both the high band and low band, l3 was set to 21.5 mm. When a parameter study of l3 was compared with other parameter studies, it showed that f4 was relatively more transferred by l3. This is because l3 resides in the loop path.Figure 8
Simulated reflection coefficients relative to changes in the length of the feeding padl3.Figures9 and 10 show the simulated and measured 2D radiation patterns of the proposed antenna at f1=0.69 GHz, f2=0.9 GHz, f3=1.82 GHz, and f4=2.3 GHz. The radiation pattern was measured on the x-y, x-z, and y-z planes, on the basis of the direction of the antenna placement shown in Figure 1(a). The measured co-pols closely matched the simulated co-pols; the measured cross-pols were higher than the simulated cross-pols. The reason for this is that the GND was extended by the cabling used to measure the radiation pattern. Dipole-like radiation patterns with omnidirectional radiation in the azimuthal plane (x-y plane) are observed at two resonances of the low band in Figure 9. Conversely, more nulls and changes occurred in the radiation pattern observed for the two high band resonances in Figure 10. The obtained radiation patterns were analogous to the radiation patterns of WWAN mobile phone antennas [7, 8]. In addition, stable radiation patterns were obtained in both the low band and the high band. Figure 11 shows the measured average gain and efficiency of the proposed antenna. At the LTE700/GSM850/GSM900 band, the average gain varies from −4.8 to −3.6 dBi. At the GSM1800/GSM1900/UMTS band, it varies from −3.2 to −1.8 dBi, while it varies from −2.6 to −2.3 dBi at the LTE2300 band.Simulated and measured 2D radiation patterns of proposed antenna: (a)f1=0.69 GHz, (b) f2=0.9 GHz.
(a)
(b)Simulated and measured 2D radiation patterns of proposed antenna: (a)f3=1.82 GHz, (b) f2=2.3 GHz.
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(b)Figure 11
Measured average gain and efficiency of the proposed antenna.


## 4. Conclusions

In this work, a shorted monopole antenna with a coupled feed for LTE/WWAN mobile handset applications was proposed. The base resonance of the shorted monopole and the resonance formed by the coupled feed structure combine to form a low wideband. The coupled feed structure and the shorting strip generate the loop antenna. The loop resonance combines with the harmonic element, which forms a high wideband. Therefore, the proposed structure is suitable for seven-band mobile handset applications, covering the LTE700, GSM850, GSM900, GSM1800, GSM1900, UMTS, and LTE2300 bands. Good radiation characteristics for frequencies over the operating bands were observed.



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*Source: 151864-2013-01-22.xml*