Printer Friendly

Lowpass filter with wide stopband and sharp skirt using novel defected ground structure.

1. INTRODUCTION

A lowpass filter is commonly used in many microwave communication and radar systems to suppress harmonics and spurious frequencies. Therefore, wide stopband and sharp cutoff response are important factors in the design of the lowpass filter. Usually, the conventional method to implement lowpass filters is using stepped impedance structures and shunt stubs [1, 2]. The disadvantage of these structures is narrow stopband and poor cutoff response. Recently, numerous research works have been carried out to design high performance LPFs using defected ground structures (DGSs) [3-5]. In general, there are two effects of DGS; the bandgap effect, which stops wave propagating at the centre frequency of attenuation pole, and the slow-wave effect, which provides the size reduction of microwave circuits. A traditional DGS element uses a dumbbell-shaped pattern etched in the ground plane and can provide only one attenuation pole [6], which limits the bandwidth of the stopband and the cut off frequency responses. Although it can be overcome by cascading several DGS units in one-dimensional period pattern [7,8], the increased circuit size will become another problem. In order to realize simultaneously wide stopband and size minimization for the microstrip lowpass filter with DGS, a novel DGS unit that can offer dual attenuation poles is proposed. The proper control of these two attenuation poles can significantly suppress the spurious responses in the stopband with much smaller defected ground area. A microstrip lowpass filter prototype with a cutoff frequency of 3.2 GHz and wide stopband up to 30 GHz has been designed and experimentally characterized to demonstrate the proposed DGS usefulness.

2. DGS UNIT DESIGN

In this letter, a novel defected ground structure with two attenuation poles is provided. The position of the two attenuation poles can be adjusted independently, so a lowpass filter with ultra-wide stopband and sharp skirt can be realized by optimizing the parameters of the DGS.

Figure 1 shows the structure of a traditional DGS and the proposed DGSs. The dashed line outlines the microstrip line. The shape filled with grey color denotes the DGS pattern etched in the ground plane. From the schematic, one can notice that the only difference is that a pair of coupling stub is added in the aperture of the traditional DGS. The coupling length is [w.sub.4], the width of the coupling stub [w.sub.5], and the gap between two stubs [w.sub.6].

Two structures, both the traditional one and the one proposed in this letter, are simulated with a commercial EM simulation software IE3D. In simulation, the substrate used is Rogers RT6010 with relative permittivity 10.2 and thickness 1 mm. Associated parameters: [w.sub.1] = 1mm, [w.sub.2] = 4 mm, [w.sub.3] = 1.5 mm, [w.sub.4] = 2.8 mm, [w.sub.5] = 0.1mm, [w.sub.6] = 0.1mm, [l.sub.1] = 0.9 mm, [l.sub.2] = 2.9 mm. The simulated results are shown in Fig. 2.

Figure 2 shows the comparison of the frequency responses of traditional DGS unit and proposed DGS unit. It can be observed that the proposed DGS pattern has two attenuation poles while the traditional one has only one. The position of attenuation pole 2 of the novel DGS pattern located at 13 GHz, basically the same as the traditional DGS unit. Additionally, there is another attenuation pole located at about 10 GHz. Because of the existence of attenuation pole 1, a much sharper selectivity than the traditional DGS pattern can be achieved. By arranging the two attenuation poles properly, a lowpass filter with ultra-wideband stopband and sharp skirt could be implemented.

3. PARAMETRIC STUDY

During the parameter research, it is found that the positions of the two attenuation poles can be tuned independently by adjusting [w.sub.3] and [w.sub.4]. Fig. 3 shows the simulated [S.sub.21] with different values of [w.sub.3] and [w.sub.4]. Other parameters are the same as the ones given above.

From Fig. 3, it can be seen that when [w.sub.4] is fixed and [w.sub.3] increased, the second attenuation pole decreases from 17 GHz to 13.17 GHz while the first attenuation pole decreases from 10.27 GHz to 9.57 GHz. On the other hand, when [w.sub.3] is fixed and [w.sub.4] increased, the first attenuation pole decreases from 11.6 GHz to 9.275 GHz while the second attenuation pole increases from 12.725 GHz to 13.125 GHz. So we can conclude that the first attenuation pole is mainly controlled by [w.sub.4] and the second attenuation pole mainly controlled by [w.sub.3]. This independence will be beneficial for the filter design and tuning.

4. LOWPASS FILTER DESIGN

A lowpass filter with ultra-wide stopband and sharp skirt utilizing the proposed DGS pattern is designed, fabricated and measured.

In order to further suppress the harmonic responses, pairs of semi-lumped LC resonant stubs are added to improve the performance. The substrate used in the simulation and fabrication is Rogers RT5880 with relative permittivity 2.2 and thickness 0.508 mm. The parameters and photograph of the fabricated prototype is shown in Fig. 4. The simulated and measured results are depicted in Fig. 5.

In this filter, two kinds of novel DGS unit with different dimensions are used, named type 1 and type 2. The parameters of type 1 are: [w.sub.2] = 8 mm, [w.sub.3] = 4.5 mm, [w.sub.4] = 2.4 mm, [w.sub.5] = 0.1mm, [w.sub.6] = 0.1mm, [l.sub.1] = 2.25 mm, [l.sub.2] = 5.9 mm. The parameters of type 2 are: [w.sub.2] = 9 mm, [w.sub.3] = 4.5 mm, [w.sub.4] = 4.4 mm, [w.sub.5] = 0.1 mm, [w.sub.6] = 0.1 mm, [l.sub.1] = 2.25 mm, [l.sub.2] = 5.9 mm. Other parameters are: [w.sub.7] = 0.2 mm, [w.sub.8] = 0.8 mm, [w.sub.9] = 0.2 mm, [w.sub.10] = 1.8 mm, [w.sub.11] = 1 mm, [w.sub.12] = 1 mm, [w.sub.13] = 1.5 mm, [w.sub.14] = 2 mm, [l.sub.a] = 67 mm, [w.sub.a] = 4.5 mm.

From Fig. 5, it is observed that the proposed DGS lowpass filter has a great harmonic suppression and selectivity performance. The fabricated filter has a<- 3dB cutoff frequency at 3.25 GHz, and suppression levels are greater than 30 dB from 3.75 to over 30 GHz. The square factor of BW3dB/BW30c;B is 0.87.

5. CONCLUSIONS

A novel DGS pattern with two attenuation poles is proposed in this letter. The novel DGS has two independently tunable attenuation poles. By finely adjusting the positions of the attenuation poles, wide stopband and sharp skirt characteristics can be achieved. In order to validate the proposed DGS pattern, a lowpass filter based on the new structure has been designed, fabricated and measured. This filter exhibits a sharp selectivity and a very wide stopband. The simulated results are in good agreement with the measured one.

ACKNOWLEDGMENT

This work was supported by the Fundamental Research Funds for the Central Universities.

REFERENCES

[1.] Matthaei, G. L., L. Young, and E. M. T. Jones, Microwave Filters, Impedance-matching Networks, and Coupling Structures, Artech House, Dedham, MA, 1980.

[2.] Makimoto, M. and S. Yamashita, Microwave Resonators and Filters for Wireless Communication: Theory, Design and Application, Springer, Berlin, 2001.

[3.] Ahn, D., J.-S. Park, C.-S. Kim, J. Kim, Y. Qian, and T. Itoh, "A design of the low-pass filter using the novel microstrip defected ground structure," IEEE Trans. on Microw. Theory and Tech., Vol. 49, No. 1, 86-93, 2001.

[4.] Song, K., Y. Z. Yin, et al., "Compact LPF with pair of coupling slots for wide stopband suppression," Electronics Letters, Vol. 46, No. 13, 922-924, 2010.

[5.] Taher, H., "High-performance low-pass filter using complementary square split ring resonators defected ground structure," IET Microwaves, Antennas & Propagation, Vol. 5, No. 7, 771-775, 2011.

[6.] Mandal, M. K. and S. Sanyal, "A novel defected ground structure for planar circuits," IEEE Microwave and Wireless Components Letters, Vol. 16, No. 2, 93-95, 2006.

[7.] Verma, A. K. and A. Kumar, "Synthesis of microstrip lowpass filter using defected ground structures," IET Microwaves, Antennas & Propagation, Vol. 5, No. 12, 1431-1439, 2011.

[8.] Kufa, M. and Z. Raida, "Lowpass filter with reduced fractal defected ground structure," Electronics Letters, Vol. 49, No. 3, 199-201, 2013.

Yang Li *, Hong-Chun Yang, and Shao-Qiu Xiao

School of Physical Electronics, University of Electronic Science and Technology of China, Chengdu 610054, China

Received 15 June 2013, Accepted 29 July 2013, Scheduled 31 July 2013

* Corresponding author: Yang Li (liyang8311@gmail.com).
COPYRIGHT 2013 Electromagnetics Academy
No portion of this article can be reproduced without the express written permission from the copyright holder.
Copyright 2013 Gale, Cengage Learning. All rights reserved.

Article Details
Printer friendly Cite/link Email Feedback
Author:Li, Yang; Yang, Hong-Chun; Xiao, Shao-Qiu
Publication:Progress In Electromagnetics Research Letters
Article Type:Report
Geographic Code:9CHIN
Date:Jun 1, 2013
Words:1454
Previous Article:A broadband circularly polarized antenna fed by horizontal L-shaped strip.
Next Article:Compact tunable dual-band bandpass filter based on substrate integrated waveguide and defected ground structure.
Topics:

Terms of use | Privacy policy | Copyright © 2019 Farlex, Inc. | Feedback | For webmasters