International Journal of Antennas and Propagation

Volume 2012 (2012), Article ID 513829, 6 pages

doi:10.1155/2012/513829

Research Article

Band-Notched Ultrawide Band Planar Inverted-F Antenna

H. T. Chattha,¹ M. K. Ishfaq,² Y. Saleem,³ Y. Huang,⁴ and S. J. Boyes⁴

¹Department of Electrical Engineering, University of Engineering and Technology Lahore, Faisalabad Campus, Faisalabad, Pakistan

²Department of Electrical Engineering, GC University, Faisalabad, Pakistan

³Department of Computer Science and Engineering, University of Engineering and Technology Lahore, Pakistan

⁴Department of Electrical Engineering and Electronics, University of Liverpool, Liverpool L69 3GJ, UK

Received 25 February 2012; Accepted 9 April 2012

Academic Editor: Minh-Chau Huynh

Copyright © 2012 H. T. Chattha 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.

Abstract.

A novel ultrawide band planar inverted-F antenna with band-notched characteristics is presented in this paper. The planar inverted-F antenna uses two parasitic elements to enhance the bandwidth to cover the ultrawide band. The band-notched feature is added by inserting a W-shaped slot on the top radiating element of the antenna with a band rejection from 5.08 to 6 GHz (measured). Both the measured and simulated results are obtained to draw the conclusions.

1. Introduction

A considerable amount of research has been conducted for developing the ultrawide band (UWB) antennas for its characteristics such as high data rate, being low power, and having wide bandwidths, and simple hardware structure in many real world applications. In 2002, Federal Communications Commission (FCC) of USA allocated a bandwidth from 3.1 GHz to 10.6 GHz to ultrawide band [1]. This band also covers the bands of the previously present wireless networks with standards such as IEEE 802. 11a in USA (5.15–5.35 GHz, 5.725–5.825 GHz), HIPERLAN/2 in Europe (5.15–5.35 GHz, 5.47–5.725 GHz), and Microwave Access (WiMAX) system (5.25–5.825 GHz) [2, 3]. To avoid the interference between these UWB systems and the nearby communication systems such as wireless (WLAN), there is a need to employ some form of filter. In order to save the space and cost and reduce the complexity of the UWB system, this filter should ideally be integrated into the radiating element of the antenna. To tackle this issue, many printed type of antennas with band-notched characteristics have been presented [2–10]. All these antennas have almost omnidirectional radiation patterns; however, some UWB applications require antennas with comparatively higher directivity.

The planar inverted-F antenna (PIFA) is now widely used in mobile and portable radio applications due to its simple design, lightweight, low cost, conformal nature, reliable performance, and attractive radiation pattern [11–14]. The PIFA has higher directivity as compared to the planar monopole antennas which makes it more suitable for certain UWB applications [15]. PIFA was previously known as an antenna having narrow-band characteristics and a reasonable research is already done to enhance its impedance bandwidth [16–18]. Feik et al. have shown in [19] that the fractional impedance bandwidth up to about 25% can be obtained by having different shapes of feed plates. Recently, some UWB PIFA antennas are introduced [20, 21] and one band-notched UWB PIFA is introduced using a spiral slot [22] on the feed plate. However, the UWB PIFAs presented in the [21, 22] have height  mm which is relatively high and also it has two PIFA antennas (one on each edge of the ground plane) to cover the whole UWB band which makes it very difficult to integrate with other PCB components. This paper presents a single-element band-notched UWB PIFA for height  mm by introducing a W-shaped slot on the top radiating plate.

2. Antenna Configurations

The structure of the designed PIFA as shown in Figure 1 has a radiating top plate with dimensions of width and length and and are width and length of the ground plane. The dimensions of the shorting and feeding plates are and , respectively, having a horizontal distance of between them and is the height of the antenna having air in the space between the top plate and the substrate. The distance of the parasitic element having a shape of an inverted-L from the feeding plate is . This parasitic element has a thickness of . The horizontal extension of this element is having a thickness of . Second parasitic element rectangular in shape is inserted at the upper edge of the ground plane at a distance from the shorting plate. The width of this element is . The heights of both the parasitic elements are the same and is equal to having a vertical distance of between the elements and the radiating plate. The W-shaped slot on the top plate is inserted at a distance from the side edge and at a distance of from the upper edge of the top plate. The W-shaped slot is shown separately in Figure 1 to highlight its dimensions. The thickness of the slot is 0.5 mm. The feeding to the PIFA is provided by a coaxial cable with an SMA connector as shown in Figure 2.

Figure 1: PIFA geometry.

Figure 2: The built PIFA with SMA connector.

3. Results

The optimization of the entire antenna parameters is performed through parametric study in high frequency structure simulator (HFSS) in order to get the maximum impedance bandwidth and feed is provided at the upper edge of the ground plane. The optimized values of all the parameters are found as follows:  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm,  mm, and  mm.

The simulated and experimental results of the reflection coefficient are shown in Figure 3. It is evident that the bandwidth achieved by these techniques of inserting parasitic elements for  dB is extremely broad from about 3.4 to 11.2 GHz. The lower frequency and first resonance is controlled by the main structure of PIFA, whereas the insertion of inverted-L-shaped parasitic element creates a second resonance at 6.5 GHz, and the presence of rectangular-shaped parasitic element produces a third resonance around 10.7 GHz (simulated). Due to the insertion of W-shaped slot, band-notched characteristics are introduced with a band rejection from 5.08 to 6 GHz (measured). The simulated and measured results are generally in good agreement. Their differences are mainly due to the cables and connectors which are not being involved in the simulations but exist in the measurements and the manufacturing tolerance in getting the accurate parameters in the manual fabrication of this antenna. Figure 4 shows the simulated and measured peak gain of the band-notched PIFA as a function of frequency in GHz. A sharp decrease in peak gain is observed in the notched frequency band centered at around 5.3 GHz (measured) which confirms that this antenna provides a good level of rejection to signals at frequencies within the notched band. The impedance of this PIFA versus the frequency in GHz is shown in Figure 5 to get a better understanding of this antenna.

Figure 3: Ref. coefficients (dB) versus frequency (GHz).

Figure 4: Simulated peak gain (dB) versus frequency (GHz).

Figure 5: Impedances versus frequency (GHz).

The simulated 3D radiation pattern (polar plot) of the band-notched PIFA at 7.5 GHz is shown in Figure 6 and the measured 2D radiation patterns of this antenna are shown in Figure 7. Figure 8 shows the simulated time-domain response of the PIFA to an input pulse which affirms the suitability of the PIFA for UWB applications.

Figure 6: Simulated 3D radiation pattern of PIFA at 7.5 GHz.

(a)

(b)

Figure 7: (a) 2D rad. pattern with total gain in dB for elevation plane (Φ = 0°) for diff. frequencies, (b) 2D rad. pattern with total gain in dB for azimuth plane (θ = 90°) for different frequencies.

Figure 8: The time domain response of PIFA.

4. Parametric Study

The parameters of the W-shaped slot are varied to observe its effects on the band-notched characteristics of the PIFA antenna. The distance from the side edge of the top plate is varied from 1 mm to 10 mm while all other parameters are held constant. Figure 9 shows the variation of versus the frequency in GHz which makes it obvious that position of the W-slot on the top plate does not significantly affects the notched band of the PIFA but significantly affects the performance of PIFA over the UWB band.

Figure 9: Simulated (dB) for values of versus frequency (GHz).

Similarly the length of the outer legs of the W-shaped slot is varied from 5 mm to 7 mm to observe its effects. Figure 10 shows that varying the length changes the band which is notched by the insertion of W-shaped slot whereas it does not significantly affect the performance of the PIFA over the UWB band. Therefore, we can vary the length to change the band to be notched. In the similar way, the length of the inner legs of the W-shaped slot is also varied from 2 mm to 6 mm to observe its effects on the performance of the W-shaped slot and on the overall performance of the PIFA. It is obvious as shown in Figure 11 that the length is very critical parameter to decide which band is exactly to be notched. Varying the length also varies the performance of the PIFA over the UWB band. Therefore, an appropriate and optimized value of is required to get the exact band to be notched by the W-shaped slot and also to achieve the reflection coefficient below −10 dB over the UWB band.

Figure 10: Simulated (dB) for values of versus frequency (GHz).

Figure 11: Simulated (dB) for values of versus frequency (GHz).

5. Conclusions

A band-notched UWB PIFA antenna is presented in this paper. It has been shown that a very wide bandwidth is achieved which almost covers the whole UWB band from 3.4 to 11.2 GHz and a band rejection from 5.08 to 6 GHz is achieved by inserting a W-shaped slot on the top plate.

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