Proceedings of Asia-Pacific Microwave Conference 2007 Modified Slotted Patch Electromagnetic Band Gap for Antenna Array Application 0. Ayopl, M.K.A Rahiml, T. Masril, M.N.A. Karim', M.Z.A. Abdul Aziz2 'Wireless Communication Centre, Faculty of Electrical Engineering, Universiti teknologi Malaysia, 813 10 Skudai Johore Baharu. 2Faculty of Electronic and Computer Engineering Universiti Teknikal Malaysia Melaka, 75450 Ayer Keroh, Melaka. Abstract- A modified slotted patch EBG structure has been investigated by measuring the forward transmission coefficient, S21. The thickness and dielectric constant of the substrate, the size and the gap of the elements in EBG structure has been modified and simulated to see the S21 value and followed by a discussion of the design and the evaluation of the structure itself. The simulation process was carried out using microwave office 2006 software. The 3 by 3 Modified Slotted patch EBG structures which has 11 mm x 11 mm elements size was fabricated using inexpensive Fire Retardant-4 (FR4) board, using wet etching techniques. The stimulated and measured S21 result shows the band gap of the structure, which are found to be between 2.24 GHz and 2.6 GHz at -20 dB. This structure is then incorporated into a 2 by 2 rectangular microstrip antenna array, operating at 2.4. The result shows that the radiation pattern improved with reducing side and back lobe with an extra gain of 1 dB compared with the antenna without the EBG structure. II. PARAMETRIC STUDY OF THE MODIFIED SLOTTED PATCH EBG STRUCTURE This paper is produced to study the characteristic of the Modified Slotted patch EBG structure. The parameters of the EBG structure such as size of the EBG lattice, the thickness of the substrate, the dielectric constant, and the gap between elements in EBG lattice are the parameters that will be investigated to determine the band gap frequency. The value of S21 has been measured to investigate the frequency band gap for the EBG structure. Figure 1 (a) shows the basic structure of the Modified Slotted patch EBG structure. Slotted patch EBG structure has been chosen due to the compact size and the ability of tuning the band gap frequency by adjusting the slot size. Keywords: Electromagnetic Band Gap (EBG), microstrip antenna array, slottedpatch, periodic structure I. INTRODUCTION Surface wave is the main problem in microstrip antenna design. This problem reduces the antenna's efficiency due to the large side and back radiation [1]. The front radiation is degrading, resulting from the enhancement of side and back radiation. The gain of the antenna is also reducing [2, 3]. To overcome this problem, the Electromagnetic Band Gap (EBG) structure has been created to suppress the propagation of the surface wave within the substrate [4]. This structure has become attractive in antenna application in recent years. Generally, the EBG structure can be realized by drilling a periodic pattern of holes in the substrate or by etching a periodic pattern of circles on the ground plane or by introducing a lattice of metallic pads connected to the ground with vias [5]. The EBG structure that has a lattice of metallic pads without using any vias has been created. The EBG structure should have a band gap frequency in the range of the operational frequency of the antenna. The frequency band gap of the EBG structure is investigated by measure the S21 value below -20 dB. This band gap of frequency is the result of the equivalent LC network in the EBG structure itself [6]. slot patch (a) (b) Figure 1: (a) One element of Modified slotted patch EBG structure and (b) the 3D view of Modified Slotted patch EBG structure A. The effect of the Element's Size on the EBG Structure The first parameter has been investigated is the effect of the size of elements in 3 by 3 Modified slotted patch EBG structure to the band gap frequency. The structure has been designed based on the Fire Retardant-4 (FR4) board which has relative permittivity 4.6, thickness 1.6 mm and 0.035 mm thickness of copper and ground plane. Figure 1 (b) shows the 1-4244-0749-4/07/$20.00 @2007 IEEE. Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 03:27 from IEEE Xplore. Restrictions apply. 3D view of the 3 by 3 Modified slotted EBG structure. Based on the above figure, a transmission line is placed on the second substrate. The second substrate which has thickness of 0.5 mm is placed on the Modified Slotted patch EBG structure which has thickness of 1.6 mm. The simulation has been done by transmitting a signal in a certain range of frequency through the transmission line. The result is shown in table 1 below. Table 1 shows the size of the element in Modified Slotted EBG structure and the band gap frequency respectively. TABLE 1: BAND GAP FREQUENCY FOR DIFFERENT SIZE ELEMENT. Patch size Slot size 5mmx5mm 6mmx6mm 7mmx7mm 8mmx8mm 9mmx9mm lOmmxlOmm llmmxllmm 2mmxO.5mm 2mmxlmm 2.5mmxlmm 3mmxlmm 3mmxlmm 4mmxlmm 5mmxlmm Band gap frequency (GHz) 3.74 -5.31 3.22 -4.47 2.97 -3.84 2.66 -3.69 2.46 -3.23 2.19 -2.96 1.98 -2.67 From table 2, the band gap frequency is reduced to a lower frequency when the dielectric constant of the substrate is increased. C. The Effect ofGap between Elements on the EBG Structure Figure 2 shows the structure of 3 by 3 Modified Slotted patch EBG structure. Generally, the gap between elements will introduce capacitance effect in overall EBG structure. The band gap frequency is measured for the different gap between elements. The simulated result is shown in figure 3. gap Figure 2: patch EBG m m structure -40~~ by 3 Modified Slotted ~ A 2D view of 3 ............. 0 Base on the table 1, the band gap frequency reduce to a lower frequency for a larger size of the elements in modified slotted EBG structure. To shift the band gap frequency to higher frequency, more capacitance is introduced means that the slot size should be increased. -10 -20 2~~~~~~~05mm 40 3 560 l mm 4 mm 5 mm -60 B. The Effect of Dielectric Constant on the EBG Structure Table 2 shows the characteristic of the Modified Slotted EBG structure base on the forward transmission coefficient, S21 when using the different value of dielectric constant. The simulation process is done on the structure like in figure 2. Referring to the figure 2, the EBG structure is designed on the 1.6 mm thick substrate. On the EBG structure, the 0.5 mm thick substrate is used to place the transmission line. A signal in a certain range of frequency is supplied through the transmission line. The result is presented in a table 2 below. TABLE 2: BAND GAP FREQUENCY FOR DIFFERENT DIELECTRIC CONSTANT Dielectric constant, 2 Band gap frequency, GHz 2.92 - 3.85 3 2.43 - 3.24 4.6 1.98 - 2.64 5 1.99 - 2.52 6 1.75 - 2.33 7 1.62 -2.15 8 1.53 - 2.02 9 1.43- 1.92 10 1.39- 1.81 0.5 1.0 1.5 2.0 2.5 3.0 Frequency, GHz 3.5 4.0 =L 4.5 Figure 3: The band gap frequency for different gap size. Figure 3 shows the band gap frequency for the different gap size. From the figure, the different gap sizes do not give much different to the characteristic of the band gap frequency. All the structure show the band gap frequency covers the frequency of interest at 2.4 GHz. D. The Effect of the Thickness in EBG Structure Referring to the figure 1 (b), the thickness of the second material on the EBG structure, h2 has been adjusted and simulated in different thickness of the substrate. The simulated result is presented in term of graph in figure 4. 1.4 1.6 1.8 2.0 2.2 2.4 2.6 Frequency (GHz) 2.8 3.0 32 Figure 4: The band gap frequency for different substrate thickness. Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 03:27 from IEEE Xplore. Restrictions apply. From figure 4, the thickness of the substrate on the EBG structure plays an important role to determine the band gap frequency of the EBG structure. The enhancement of the thickness of the second substrate on the EBG structure will reduce the range of the band gap frequency. It means that the EBG structure is only sufficient to the thicker antenna substrate. -1 -26 ioq -30 -vo -o0 -46 III. DEVELOPMENT OF THE MODIFIED SLOTTED PATCH EBG STRUCTURE The 3 by 3 Modified slotted patch EBG structure which a patch size of 11 mm x 11 mm has been selected to do the analysis in both simulation and fabrication. Before starting the fabrication process, the simulation process should prove that the structure can suppress the propagation of the surface wave in the band gap frequency. Figure 5 shows the simulated result for the forward transmission coefficient, S21 and the return loss, SI, respectively. 0 ...... I -30 -40 S21 Si i -50 -60 -70 1.4 1.6 1.6 2.0 2.2 2.4 2.6 Frequency (GHz) easuremert 2.8 3.0 3.2 Figure 7: The simulated and measured result for 3 by 3 Modified Slotted patch EBG structure Figure 7 shows the simulated and measured result for 3 by 3 Modified Slotted patch EBG structure which has 11 mm x 11 mm element's size. From the above graph, the band gap frequency is narrower than the simulated result. The measured result shows that the band gap frequency extend from 2.24 GHz up to 2.6 GHz, but it still covers the frequency of interest at 2.4 GHz. t -20 co m IV. IMPLEMENTATION OF THE MODIFIED SLOTTED PATCH EBG STRUCTURE IN 2 BY 2 MICROSTRIP ANTENNA ARRAY. .. -10 q- -70 I 1.4 1.6 1.8 2.0 2.2 2.4 2.6 Frequency (GHz) 2.8 3.0 i 3.2 The 11 mm x 11 mm patch size has been implemented to the 2 by 2 microstrip antenna array to see the effect of the EBG structure on the performance of the microstrip antenna array. Figure 8 shows the 2 by 2 microstrip antenna array with and without Modified slotted patch EBG structure. Figure 5: The simulated result for SI, and S21 From the graph, the Modified slotted patch EBG structure has a band gap frequency measured at S21 at -20 dB and below is from 1.98 GHz to 2.67 GHz. At this band gap frequency, the value of SI, is almost near to 0 dB indicates that the signal in the frequency band gap cannot propagate on the EBG surface. This Modified slotted patch EBG structure has been fabricated and measured to see the performance. Figure 6 shows the 3 by 3 Slotted Patch EBG structures that has been fabricated and measured. The performance of this EBG structure is shown in figure 7. Figure 8: A 2 by 2 microstrip array antenna with and without the Modified Slotted patch EBG structure. Figure 6: The 3 by 3 Modified Slotted Patch EBG structure Figure 9 shows the measured E-co polarization for 2 by 2 microstrip antenna array as shown in figure 8. From the figure, the maximum power received is -22 dBm for the antenna without modified slotted patch EBG structure. By surrounding the same antenna with modified slotted patch EBG structure, the power received is -21 dBm. The 1 dB increment is noticed. The side and back radiation for the 2 by 2 microstrip antenna array with EBG structure is reduced. Figure 10 shows the comparison of measured H-Co polarization for 2 by 2 microstrip antenna array with and Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 03:27 from IEEE Xplore. Restrictions apply. without Modified Slotted patch EBG structure at a frequency of 2.4 GHz. From the figure, the maximum power received is 23 dBm for the antenna without slotted patch EBG structure. The power received increase to -22 dBm for the antenna with slotted patch EBG structure. The side lobe and back lobe for the 2 by 2 microstrip array antenna with EBG structure is reduced. 330~ P-.60 .k \.i V. CONCLUSION The characteristic of the Modified Slotted patch EBG structure has been presented. The EBG structure is depending on the types of material used which has certain dielectric constant, the thickness of the substrate, the gap between elements and the different size of elements in EBG structure. Next, the integration of the Modified Slotted patch EBG structure with the microstrip antenna array has improved the performance of the antenna. The radiation patterns of the antenna with modified slotted EBG structure in term of the side and back radiation are better compared to the microstrip antenna array without modified slotted patch EBG structure. By using the EBG structure, the surface wave effect is reduced, resulting to the improvement of the antenna performance. 90 -30 -20 270 -20 -30 -40 240 The authors would like to thanks the Ministry of Science, Technology and Innovation (MOSTI) of Malaysia for supporting this works. Sg120 .X -30 -30 210 - ACKNOWLEDGEMENTS 2 1 without EBG vs degree -with EBG vs d~eyee 1 150 REFERENCES Figure 9: Measured E-Co polarization for 2 by 2 microstrip antenna array [1] [2] [3] 300, 270 -20 V -30 -30 240 60 -20 [4] 90 120 -30 210 -twthout EBO vs degree 150 [5] [6] F. Yang, and Y. 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Simon Tse, Paul Young, John Batchelor, " EBG Ground Plane Combines the Periodic Metalized Elements and the Perforated Dielectric Effects for Enhance Performance," Proceedings of the 2006 Antennas & Propagation Conference, Burleigh Court Conference Centre, Li Yang, Mingyan Fan, and Zhenghe Feng, .A Spiral Electromagnetic Bandgap(EBG) structure and is Application in Microstrip Antenna Arrays,. IEEE Asia-Pacific Conf Proc., Microwave Conf., Proc., Vol. 3, pp. 4, Dec. 2005. -I-withEBvs de3e Figure 10: Measured H-Co polarization for 2 by 2 microstrip antenna array Authorized licensed use limited to: UNIVERSITY TEKNOLOGI MALAYSIA. Downloaded on December 23, 2008 at 03:27 from IEEE Xplore. Restrictions apply.
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