Triple Band-Notched UWB Planar Monopole Antenna Using Triple-Mode Resonator

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Progress In Electromagnetics Research C, Vol. 57, 117 125, 215 Triple Band-Notched UWB Planar Monopole Antenna Using Triple-Mode Resonator Huaxia Peng 1, 3, Yufeng Luo 1, 2, *, and Zhixin Shi 1 Abstract In this paper, a novel printed microstrip-fed monopole ultra-wideband (UWB) antenna with triple-notched bands using triple-mode stepped impedance resonator (SIR) is presented. The proposed triple-mode SIR is found to have the advantages of introducing triple-notched bands and providing higher degree of freedom to adjust the resonant frequencies. By coupling the triple-mode SIR beside the microstrip feedline, band-rejected filtering properties around the 5.2 GHz WLAN band, the 6.8 GHz RFID band, and the X-band satellite communication band, are generated. To validate the design concept, a novel compact UWB antenna with three notched bands is designed and measured. Results indicate that the proposed compact antenna not only retains triple band-rejections capability but also owns omni directional radiation patterns across nearly whole operating bandwidth for UWB communications. 1. INTRODUCTION Ultra-wideband (UWB) radio technology has attracted much attention since the US Federal Communications Commission (FCC) allocated a frequency range with a bandwidth of 7.5 GHz (3.1 1.6 GHz) for unlicensed radio applications. Many applications have been developed based on UWB technology such as short-range broadband communication, radar sensing, and body-area networking [1]. It is a well-known fact that planar monopole antennas present attractive features, such as simple structure, small size, low cost, stable radiation patterns, and constant gain over the entire operating band. Owing to these characteristics, planar monopoles are attractive for use in emerging UWB applications, and research activity is increasingly being focused on them [2 5]. However, the existing wireless networks such as IEEE 82.16 WiMAX system operating at 3.3 3.6 GHz, the wireless local area network (WLAN) for IEEE82.11a operating at 5.15 5.35 GHz/5.725 5.825 GHz, and 6.7 6.9 GHz RF identification (RFID) communication signals, X-band (7.9 8.2 GHz) satellite communication systems (XSCS) signals can interfere with UWB systems, thus compact UWB monopole antenna with multiple notched-bands are emergently required to reject these unwanted interfering signals [6 15]. To achieve desired band-notched performance, slots such as U-shaped, V-shaped, etc. are usually inserted on initial the UWB monopole antenna in [7, 8], however, only one notched band is created. In [9, 1], two notched bands can be introduced using defected ground structure (DGS), however, they are all based on multi-layer structure that would increase fabrication cost and hardly compatible with the existing microwave-integrated circuit. In [11, 12], two notched bands can also be obtained and these antenna structures are very simple and easy to fabricate, however, they use two or three single-mode resonators. Then, the spurious notched bands obtained by spurious resonances of the conventional resonance structures [13 15]. Received 7 April 215, Accepted 6 May 215, Scheduled 15 May 215 * Corresponding author: Yufeng Luo (eleyufengluo@163.com). 1 School of Mechanical and Electrical Engineering, Nanchang University, Nanchang 3331, China. 2 School of New Energy Science and Engineering, Xinyu Universiy, Xinyu 3384, China. 3 School of Electrical and Information Engineering, Hunan University of Technology (HUT), Zhuzhou 4127, China.

118 Peng, Luo, and Shi In this communication, a novel compact printed UWB monopole with triple-notched bands based on triple-mode stepped impedance resonator (SIR) is presented. Firstly, the properties of the proposed triple-mode SIR are analyzed theoretically, which has three resonance frequencies and higher degree of adjusting freedom. The analyzed results reveal that triple band-stop performance can be obtained based on the triple-mode resonant property of the triple-mode SIR. Then, the triple notched-bands characteristic is achieved by putting the triple-mode SIR near by the feed line of the UWB antenna. Notice that the spurious notched-band of the triple-mode SIR is also far away from the UWB antenna work band. To validate the design concept, a novel planar ultra-wideband (UWB) antenna with triple sharply rejected notched bands respectively centered at frequencies of 5.2 GHz, 6.8 GHz and 8. GHz is designed and measured. The simulation and the measurement show that the antenna achieves an ultra wide bandwidth ranging from 2. GHz to 11. GHz and avoids the WLAN/RFID/XSCS interference. An omni directional pattern across the entire bandwidth in the H-Plane of the antenna is achieved. 2. UWB PLANAR MONOPOLE ANTENNA CONFIGURATION The geometry of the proposed UWB antenna triple-notched bands is shown in Figure 1. It can be seen that the antenna composed of a triple band-stop filter and a conventional planar circular monopole antenna. It is fabricated on Rogers 435B microwave substrate of thickness.58 mm and relatively permittivity 3.38. The band-stop filter (i.e., the triple notched-bands) is realized by coupling the triple-mode SIR to 5 Ω microstrip feed-lines. The design of triple-notched bands will be discussed in Section 3. The proposed planar UWB antenna has a circular patch with radius R 1 = 7.5 mm, which is fed by 5 Ω microstrip line of width w =1.1mm. In order to improve impedance matching performance, a rectangular slit is embedded in the ground plane, located under the microstrip feed line. The final optimized parameters of the planar UWB antenna are as follows: w 1 = 2 mm, w 2 =7.1mm, w 3 =1.8mm, l 1 = 38 mm, l 2 = 2 mm, l 3 =2.mm, r d =2.5mm, w gap =.1mm. l 2 R 1 r d w gap w 2 w 1 w w 3 l 3 l 1 Figure 1. Layout of the proposed UWB antenna with triple sharp notched-bands. 3. TRIPLE-MODE STEPPED IMPEDANCE RESONATOR UNIT ANALYSIS Figure 2(a) shows the geometry of the proposed triple-mode SIR. It consists of two half-wavelength SIRs and two short-circuited stubs on its center plane. Since the resonator is symmetrical to the T -T plane, the odd-even-mode method is implemented. For odd-mode excitation, the equivalent circuit is one quarter-wavelength resonator with one end grounded, as shown in Figure 2(b). From the resonance

L2, Z 1 /2 Progress In Electromagnetics Research C, Vol. 57, 215 119 L 1, Z 1 T L 2, Z 1 /2 L 3, Z 3 L 4, Z 4 T ' (a) Z ine L 1, Z 1 L3,Z3 Z ino (b) (c) L 1, Z 1 L 1, Z 1 Z ine2 Z ine1 L 2, Z 1 /2 L2, Z1 L 3, Z 3 (d) (e) Figure 2. (a) Configuration of the proposed novel triple-mode SIR. (b) Odd-mode equivalent circuit. (c) Even-mode equivalent circuit. (d) Path I of even-mode equivalent circuit. (e) Path II of even-mode equivalent circuit. T W s5 W s6 L s6 W gap W s3 L s4 L s5 W s2 L s2 L s3 Ws1 Input L s1 Ls2 Ouput T' (a) L 11 L 12 L 13 C 11 C 12 C 13 Figure 3. Geometry and equivalent circuit of the proposed coupled triple-mode SIR. (b)

12 Peng, Luo, and Shi condition of Y ino =, the odd-mode resonant frequency can be deduced as: c f ino = (1) 4L 1 εeff -1-1 S (db) 21-2 S (db) 21-2 -3 L s1=8.5 mm L s1=9. mm L s1 =9.5 mm -3 L s2 =.3 mm L s2 =.5 mm L s2 =.7 mm 2 3 4 5 6 7 8 9 1 (a) 2 3 4 5 6 7 8 9 1 (b) -1-1 S (db) 21-2 S (db) 21-2 -3 L s3 =2.4 mm L s3=2.7 mm L s3 =3. mm -3 L s4 =.5 mm L s4 =.7 mm L s4=.9 mm 2 3 4 5 6 7 8 9 1 (c) 2 3 4 5 6 7 8 9 1 (d) -1 S 21 (db) -2-3 L s5 =6.5 mm L s5 =6.8 mm L s5 =7.1 mm 2 3 4 5 6 7 8 9 1 Figure 4. Simulated S-parameters of the coupled triple-mode SIR for various dimensions: (a) L S1, (b) L S2,(c)L S3,(d)L S4,(e)L S5. (e)

Progress In Electromagnetics Research C, Vol. 57, 215 121 where f ino is the center frequency of the notch band, ε eff is the effective dielectric constant, and c is the light speed in free space. For even-mode excitation, the equivalent circuit is shown in Figure 2(c), which contains two resonant circuits: a quarter-wave-length resonator and a half-wavelength resonator, as shown in Figures 2(d) and (e). The even-mode resonant frequencies can be determined as follows: c f ine1 = 4(L 1 + L 2 + L 3 ) (2) ε eff f ine2 = c (2L 1 +2L 2 +2L 4 ) ε eff (3) where are Z 1 = Z 3 = Z 4 assumed for simplicity. The resonance frequencies can be determined by the electrical length. Compared with dual-mode resonator, the proposed structure can provide three resonant frequencies and higher degree of freedom in adjusting the locations of the resonant modes. The triple-mode SIR can result in triple band-stop performance when placed next to the microstrip line and it can be equivalent to three shunt-connected series resonance circuits, as shown in Figure 3. The triple-mode SIR can result in triple band-stop (i.e., the triple notched-bands) performance when placed (a) (b) (c) (d)

122 Peng, Luo, and Shi (e) (f) (g) Figure 5. Measured radiation pattern of the UWB planar monopole antenna: (a) 2.5 GHz, (b) 5. GHz, (c) 7.5 GHz, (d) 1. GHz, (e) 5.2 GHz, (f) 6.8 GHz, (g) 8. GHz. next to the microstrip line and it can be equivalent to three shunt-connected series resonance circuits. In this paper, the triple-mode SIR dimensions are selected as follows: w s1 =1.3 mm, w s2 =.3 mm, w s3 =.3 mm, w s5 =1.3 mm, l s1 =4.5 mm, l s2 =.5 mm, l s3 =1.45 mm, l s4 =.7 mm, l s5 =3.1 mm, l s6 =1.6 mm, r e =.1 mm. The frequency characteristics of the coupled triple-mode SIR with various dimensions are investigated by HFSS 11. to validate the multi-mode resonant property as shown in Figure 4. It can be seen that the frequency locations of the first and the second notched bands move down simultaneously as increase the dimensions of L s2 and L s4. And the frequency locations of the second and the third notched bands move down simultaneously as increase the dimensions of L s1. But only the first the notched band increases as decreases L s3 and the second notched band increases as decreases L s5. Therefore, by appropriately adjusting the resonator dimensions, triple notched bands can be achieved at desired frequencies.

Progress In Electromagnetics Research C, Vol. 57, 215 123 4. UWB ANTENNA WITH TRIPLE-NOTCHED BANDS Based on the triple band-stop characteristics previously described, a novel UWB planar monopole antenna with triple rejected notched bands is proposed and designed. All simulations have been carried out using Ansoft HFSS 11. simulation software based on the finite element method (FEM). The normalized radiation patterns in the E- (Phi = 18 deg) and s (Phi = 9 deg) are measured at 2.5 GHz, 5. GHz, 5.2 GHz, 6.8 GHz, 8. GHz, 7.5 GHz, and 1. GHz as in Figure 5. It can be found that the antenna has good omni directional radiation patterns in the (dotted). The radiation patterns in the (continuous) are in symmetry. Simulated and measured VSWR of the UWB antenna as shown in Figure 6 for comparison. We can notice that the UWB antenna possesses the impedance bandwidth from 2. GHz to 11. GHz for VSWR < 3 except in notched bands from 4.7 5.5 GHz, 6.7 7.1 GHz, and 7.6 8.3 GHz, respectively. The central frequencies of the notchedbands are about 5.2 GHz, 6.8 GHz, and 8. GHz, as well as the notch frequencies of the triple band-stop performance designed in Section 3. The notched-bands are very suitable to implement the rejection of 5.2 GHz wireless local area networks (WLAN) signal, 6.8 GHz RF identification (RFID) signal, and 8. GHz X-band satellite communication systems (XSCS) signal. Figure 7 shows the simulation of group delays in the UWB antenna with pulse response. The measured peak gain in the is given in Figure 8. The proposed antenna exhibits three significant antenna gain decreases at 5.2, 6.8, and VSWR 5 45 4 35 3 25 2 15 1 5 Simulation Measurement 2 3 4 5 6 7 8 9 1 11 Figure 6. Measurement and simulation of VSWR. Group delays 35 3 25 2 15 1 5-5 -1 2 3 4 5 6 7 8 9 1 11 Figure 7. Simulation of group delays in the UWB antenna with pulse response. 4 3 Gain (dbi) 2 1 2 4 6 8 1 Figure 8. Measured peak gain of the proposed UWB antenna with triple-notched.

124 Peng, Luo, and Shi 8. GHz; this is indicative of the effect of the notched bands. The deviations of the measurements from the simulations are expected mainly due to the reflections from the connectors and the finite substrate. The overall size is about 38 2 mm 2. 5. CONCLUSIONS In this work, a high-performance UWB planar monopole antenna, with triple highly rejected notchedbands, has been successfully implemented and investigated. The triple notched-bands can be easily tuned to the desirable frequency location by controlling the parameters of the proposed triple-mode SIR. The proposed antenna covers the frequency range for the UWB systems, between 2. GHz and 11. GHz, with a rejection band around WLAN, RFID, and XSCS. The introduced triple-mode SIR is simple and flexible for blocking undesired narrow band radio signals appeared in UWB band. Using the advantage of small real estate, outstanding performance can be realised for broadband antennas, which are now widely demanded in UWB applications. The measured results show good performance in terms of the reflection coefficient, antenna gain and radiation patterns. To summarise, the proposed planar monopole antenna is very useful for modern UWB wireless communication systems owing to its marked properties of simple topology, compact size, and excellent performance. ACKNOWLEDGMENT This work was supported by the National Natural Science Foundation of China under Grant Nos. 5116433 and 5136536, the Jiangxi province ground plan of science and technology for insitution of higher education No. KJLD125, the Jiangxi province Science and technology supporting project No. 2123BBE5116, the Jiangxi province Natural Science Foundation of China under Grant No. 2132BAB2621, Scientific Research Fund of Jiangxi province Nos. 12747 and 11739 and 12748,, and the Hunan Province Nature Science Foundation of China under Grant No. 14JJ2118. REFERENCES 1. Revision of Part 15 of the Commission s Rules Regarding Ultra-wideband Transmission Systems, First Note and Order Federal Communications Commission, ET-Docket 98 153, 22. 2. Naghshvarian-Jahromi, M., Novel wideband planar fractal monopole antenna, IEEE Trans. Antennas Propag., Vol. 56, No. 12, 3844 3849, 28. 3. Naser-Moghadasi, M., H. Rousta, and B. S. Virdee, Compact UWB planar monopole antenna, IEEE Antennas Wirel. Propag. Lett., Vol. 8, 1382 1385, 29. 4. Mazinani, S. M. and H. R. Hassani, A novel broadband plate-loaded planar monopole antenna, IEEE Antennas Wirel. Propag. Lett., Vol. 8, 1123 1126, 29. 5. Sun, M., Y. P. Zhang, and Y. Lu, Miniaturization of planar monopole antenna for ultra-wideband radios, IEEE Trans. Antennas Propag., Vol. 58, No. 7, 242 242, 21. 6. Zhao, J.-D., J.-P. Wang, G. Zhang, and J.-L. Lin, Compact UWB bandpass filter with dual notched bands using E-shaped resonator, IEEE Microw. Wirel. Compon. Lett., Vol. 23, No. 12, 638 64, 213. 7. Lee, W.-S., D.-Z. Kim, K.-J. Kim, and J.-W. Yu, Wideband planar monopole antennas with dual band-notched characteristics, IEEE Trans. Microwave Theory Tech., Vol. 54, 28 286, 26. 8. Chung, K., J. Kim, and J. Choi, Wideband microstrip-fed monopole antenna having frequency band-notch function, IEEE Microwave Wireless Compon. Lett., Vol. 15, 766 768, 25. 9. Kim, Y. and D. H. Kwon, CPW-fed planar ultra wideband antenna having a frequency band notch functions, Electron. Lett., Vol. 4, 43 45, 24. 1. Yin, K. and J. P. Xu, Compact ultra-wideband antenna with dual bandstop characteristic, Electron. Lett., Vol. 44, 453 454, 28. 11. Bi, D.-H., Z.-Y. Yu, S.-G. Mo, and X.-C. Yin, Two new ultra-wideband antennas with 3.4/5.5 GHz dual band-notched characteristics, Microwave Opt. Tech. Nol. Lett., Vol. 51, 2942 2945, 29.

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