JOURNAL OF TELECOMMUNICATIONS, VOLUME 10, ISSUE 2, SEPTEMBER 2011 14

A Novel Modified Monopole Antenna with a 5.5 GHz Notch Filter A. Siahcheshm and Y. Zehforoosh Abstract— This paper presents the results of a modified monopole antenna that exhibits 3-27 GHz performance. The proposed antenna consists of a triangular shaped radiating patch with notches. Also, the antenna’s truncated ground-plane incorporates a central notch. This modification significantly improves the antenna’s impedance bandwidth by 160% over an ultra-wideband frequency range from 3 to 27 GHz. The return-loss (S11) performance over this frequency range is simulated to be better than -10 dB. These characteristics make the proposed antenna an excellent candidate for numerous UWB applications and next generation communication systems. The key physical parameters affecting the antenna’s frequency characteristics have also been investigated in order to determine optimum antenna performance. The antenna’s simulated return-loss, and E-plane and H-plane radiation patterns show very good correlation with the requirements of UWB applications.

Index Terms— monopole antenna, UWB, notch filter, small antenna

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1 INTRODUCTION Ultra-wideband (UWB) technology has undergone many significant developments in recent years. However, there still remain many challenges in making this technology live up to its full potential. The work in this area has gained impetus with the Federal Communication Commission (FCC) permitting the marketing and operation of UWB products within the band 3.1 GHz to 10.6 GHz. This technology employs short duration pulses that result in very large or wideband transmission bandwidths. With appropriate technical standards, UWB devices can be operated using spectrum occupied by existing radio services without causing interference, thereby permitting scarce spectrum resources to be used more efficiently. However, this wireless communication technology still needs to be improved further to satisfy the insatiable demand for higher resolution and higher data rate requirements. One key component necessary to fulfill these requirements in UWB system is a planar antenna that is capable of providing a wide impedance bandwidth. The antenna needs to operate over the ultrawideband, as it is defined by the FCC. In addition, it needs to provide omni-directional radiation coverage over the entire UWB frequency range. Other aesthetic features sought from the antenna include being light weighted, small in size, and having a low profile. Several monopole configurations have been investigated for wideband applications thus for, which include the following structures: circular, square, elliptical, pentagonal, hexagonal etc. [1]–[6]. Among the proposed wideband antennas include the printed planar monopole antenna, which is a promising candidate for future appli-

cations due to its remarkably compact size, stable radiation characteristics and ease of construction. The triangular monopole antenna mounted above a ground-plane was first proposed in [7], and its impedance bandwidth is found to be dependent on the feeding gap and the antenna’s flare angle. A typical bandwidth of this antenna is approximately 30% [8]. Some variants of this type of antenna in an effort to increase its bandwidth have been studied, i.e. the tap monopole antenna [9], and the staircase bow-tie monopole antenna [10]. Although these techniques enhance the antenna’s bandwidth, the results show their bandwidth is limited to less than 100%. Another way which is proposed for increasing the impedance bandwidth of the triangular monopole is achieved by modifying its ground-plane [1]. Among the various planar monopole antennas of configurations, only a few triangular monopole antennas have been investigated for UWB applications [11, 12]. In this paper, we present a novel planar microstripfed triangular monopole antenna that exhibits 3-27 GHz. The design of the proposed structure is based on the antenna presented in [13], but has a smaller size and a significantly large operational frequency band. The triangular monopole antenna includes a notch function for 5.5 GHz. The antenna’s ground-plane is truncated and modified. This designed antenna operates over 3 to 27 GHz with S11 < -10 dB. Unlike other antennas reported in the literature to date, the proposed antenna displays a good omni-directional radiation pattern even at higher frequencies. The monopole antenna is analyzed using Ansoft’s High Frequency Simulator (HFSS) [14].

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• Amir Siahcheshm is with the Department of Electrical Engineering, Salmas branch, Islamic Azad University, Salmas, Iran. • Yashar Zehforoosh is with the Department of Electrical Engineering, Urmia branch, Islamic Azad University, Urmia, Iran. © 2011 JOT http://sites.google.com/site/journaloftelecommunications/

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2 ANTENNA STRUCTURE

3 RESULTS AND DISCUSSIONS

Fig. 1 shows the configuration of the proposed monopole antenna which consists of an inverted triangular structure whose base includes one square shaped notch, and an inverted U shaped notch. The ground-plane is truncated, as shown in Fig. 1, and envelops the feedline to the radiating triangular patch. The ground-plane includes a rectangular notch at its center for impedance matching. The proposed antenna is constructed from FR4 substrate with the thickness of 1.6 mm and relative dielectric constant of 4.4. The width of the microstrip feedline is fixed at 1.5 mm. The antenna’s dimensions are 35 mm × 30 mm (Ls × Ws). The dimensions of the notch (Lf × Wf) embedded in the ground-plane are important parameters in determining the sensitivity of the antenna’s impedance match. The proposed shape of the truncated ground-plane acts as an effective impedance matching network to realize an antenna with a very wide impedance bandwidth. This is because the truncation creates capacitive loading that neutralizes the inductive nature of the patch to produce nearly pure resistive impedance present at the antenna’s input [3]. The flare angle of the antenna also affects its impedance bandwidth. Here, the flare angle is set to be 90o. Also, as it will be shown in section 3, introducing U shaped slot on the radiating patch and carefully adjusting its dimensions result in filtering the 5.5 GHz WLAN bandwidth. The improvement in impedance match over the multi-octave bandwidth is attributed to the phenomenon of defected ground structure (DGS) with slots that create additional surface current paths in the antenna. Moreover, this ground-plane structure changes the inductive and capacitive nature of the input impedance, which in turn leads to change in bandwidth [15]. The proposed antenna is investigated by changing one parameter at a time, while fixing the others. To fully understand the behavior of the antenna’s structure and to determine the optimum parameters, the antenna was analyzed using Ansoft’s high-frequency structure simulator (HFSS). The optimum magnitudes of the physical parameters of the proposed antenna are shown in Fig. 1, which achieves a very wide impedance bandwidth from 3 to 27 GHz with S11< -10 dB.

Fig. 2 shows a comparison of the return-loss characteristics of a simple triangular monopole antenna by the same size as the proposed antenna. As shown, the simple triangular monopole antenna has a relatively narrow bandwidth [16]. As observed in Fig. 2, the successive modifications improve the bandwidth of the triangular monopole antenna. The inclusion of notches in the radiation patch and modifying the ground-plane has a significant effect on increasing its bandwidth.

Fig. 1. Configuration and parameters defining the proposed antenna.

-5

Return Loss (dB)

-10 -15 -20 -25 -30

proposed antenna simple monopole antenna

-35 -40

5

10

15

20

25

30

Frequency (GHz)

Fig. 2. Simulated return-loss performance of simple triangular monopole antenna and the proposed antenna.

The rectangular notch parameters Lm and Wm are parameters that have major effects on the antenna’s return-loss characteristics. By adjusting Lm and Wm, the electromagnetic coupling between the triangular patch and the ground-plane can be controlled. Fig. 3 shows the return-loss response for different values of Wm. It is observed that the impedance bandwidth is effectively improved over the lower frequencies as Wm is changed. It can be seen that the lower frequency of the impedance band is changed by increasing the gap, but the impedance match becomes even poorer for smaller values of Wm. Fig. 4 shows the return-loss plot for different values of Lm; this plot shows the sensitivity of the impedance match to this parameter. As indicated, the parameter Lm has an obvious effect on return-loss of the proposed antenna. -5 -10 -15

Return Loss (dB)

Wf = 2.6 mm Lf = 1.8 mm Ws= 30 mm Ls = 35 mm Lm = 5 mm Wm = 2.5 mm Lt = 11.5 mm Ln= 6.5 mm Wn = 3 mm Lp = 18.7 mm L b = 4.77 mm Rg = 16 mm Lk = 2 mm Lg = 8.5 mm

0

-20 -25 -30

Wm=3 mm -35

Wm=2.5 mm Wm=2 mm

-40

Wm=1.5 mm -45 -50 2

4

6

8

10

12

14

16

18

Frequency (GHz)

Fig. 3. Simulated return-loss characteristics of the proposed patch antenna with different values of Wm.

16

0

Return Loss (dB)

-10

-20

(a) (b) (c) (d) Fig. 6. Simulated current distributions for the proposed antenna at: (a) 3.1 GHz, (b) 4.9 GHz, (c) 6.7 GHz, and (d) 10 GHz.

-30

Lm=5 mm -40

Lm=4.5 mm Lm=4 mm Lm=3.5 mm

-50

-60 2

4

6

8

10

12

14

16

18

Frequency (GHz)

Fig. 4. Simulated return-loss characteristics of the proposed patch antenna with different values of Lm.

The proposed antenna’s far-field radiation patterns are simulated in the two principle planes, y-z plane for the E-field and x-z plane for the H-field. Fig. 7 shows that the radiation pattern plots at several different frequencies are stable. It is noticed that the E-field pattern is omnidirectional at lower frequencies and is near omnidirectional at higher frequencies.

In this study, in order to filter the WLAN frequency bandwidth and reduce the electromagnetic interference between UWB and WLAN systems, a U shaped slot is embedded on the radiating patch of the proposed antenna, as depicted in Fig. 1. Fig. 5 shows the return-loss response for several values of Ln. These graphs indicate the effect of adding a U shaped slot on the patch. This phenomenon occurs because the slot acts as current perturbation on the radiating patch. 10

Return Loss (dB)

0

-10

-20

Ln=7 mm -30

Ln=6.5 mm Ln=6 mm Ln=5.5 mm

-40

Ln=5 mm Ln=4.5 mm -50 2

4

6

8

10

12

14

16

18

Frequency (GHz)

Fig. 5. Simulated return-loss characteristics of the proposed patch antenna with different values of Ln.

The spectrum of the antenna in Fig. 2 shows many resonances. These resonances correspond to the different modes of field distribution. Fig. 6 shows the simulated current distribution at the frequencies of 3.1 GHz, 4.9 GHz, 6.7GHz, and 10 GHz. Fig. 6(b) and (c) show a strong current distribution located around the top notch in the radiating patch, as well as the current flow directed towards the corners of patch. This indicates that the modifications in the truncated ground-plane excite resonance modes at a higher frequency, which effectively extend the antenna’s bandwidth, and also embedding a U shaped notch acts as a filtering function by affecting the current distribution.

Fig. 7. Simulated Radiation patterns of the proposed antenna, Eplane (solid line) and H-plane (dotted line).

4 CONCLUSION In this paper, a modified triangular monopole compact planar antenna is proposed which exhibits multioctave bandwidth performance and completely satisfies the requirements for UWB applications. The results show that the impedance bandwidth of the proposed antenna is significantly improved with modification on the radiating patch. The proposed antenna exhibits an impedance bandwidth of 160% over a very wide frequency range from 3 to 27 GHz with return-loss better than -10 dB. Also, results show good radiation patterns within the UWB frequency range.

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ACKNOWLEDGMENT Special thanks are extended to the Islamic Azad University of Salmas, since this paper is prepared due to the research project done for the above mentioned university, and also we appreciate all the facilities and financial support they provided us to do the research.

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Amir Siahcheshm was born in Urmia, WA, Iran in 1981. He received the B.Sc. Degree in communication engineering from Islamic Azad University of Urmia, Iran (2003) and M.Sc. degree (with honors) from Urmia University, Iran in communication engineering (2007). Previously, he was teaching at Islamic Azad University of Urmia and Sama Technical and Vocational Institution affiliated by Islamic Azad University of Urmia. At the meantime, he has been teaching at several other public and non-governmental universities, located in Urmia, Iran. He was a research assistant at the Club of Young Researchers, affiliated by Islamic Azad University of Salmas, Iran. And also, since 2008, he has been accepted as a member of the Society of the Talented People in Iran (BMN). Currently, he is a lecturer at Islamic Azad University of Salmas, Iran. His research interests include microstrip antennas, wireless systems, microwave devices and optimization methods in electromagnetics. Yashar Zehforoosh was born in Urmia, Iran in 1981. He received his M.Sc. degree from Urmia University in 2007 in telecommunication engineering fields and waves. Currently, he is working through his PhD degree in science and research branch of Islamic Azad University, Tehran, Iran. Meanwhile, he is a faculty of electrical engineering department of Urmia branch in Islamic Azad University, Urmia, Iran from 2009. His research interests include broadband antennas, electromagnetic structures and UWB systems.

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