COMPACT MICROSTRIP ANTENNA BASED ON FRACTAL METASURFACE WITH LOW RADAR CROSS SECTION AND WIDE BANDWIDTH Evelyn Bustos (992), Pamela Guerrero (924), Jhonny Asqui (935) evelyn.bustos@espoch.edu.ec pamela.guerrero@espoch.edu.ec silvio.asqui@espoch.edu Escuela de Ingenierı́a en Electrónica Telecomunicaciones y Redes - FIE - ESPOCH Riobamba - Ecuador Abstract.- The compact antenna with wide bandwidth is important. In this paper, we have studied the microstrip slot antenna for wireless application based on the fractal structure which has covered 2.6–4.1 GHz (85 % bandwidth). The circular slot antenna with four rectangular slots is considered and then six dual rings are added to the antenna. Finally, for improving the matching a disk is placed in the central part of the slot. The fractal model has been considered for low RCS, for improving the bandwidth, for amending the matching of the antenna by controlling the current distribution and it is modified for C-band application. controlling the antenna surface current distribution.[4] Furthermore, as mentioned the fractal method is developed as a conventional method for RCS reduction while the fractal shapes are known as self-similar shapes, and are usually found in galaxies, cloud boundaries, mountain ranges, coastlines, snowflakes, trees, and leaves and fractal method have been examined for various applications like antenna and the absorbers based on metamaterial . Recently, the fractal shapes are more attractive to reflect-array and monopole antenna to reduce the RCS. The microstrip circular slot antenna with a straight feed line is selected as our basic structure. We have investigated that we can obtain wider bandwidth with a great enhancement only by adding rectangular slot and the dual ring structure[5]. Finally, the circular disk is located in the central part of the slot for improving the matching of the antenna and the fractal technique is used to reduce the radar cross section. These aforementioned references have been presented to improve the problem of the bandwidth. Fractal shapes have the interesting self-similarity property. Briefly speaking, self-similarity can be described as the replication of the geometry of the structure at a different scale within the same structure. Thus, the self-similarity of fractal structure results in a multiband or wideband behavior. At the same time, fractal shapes can be used to design the antenna and FSS for reducing the sizes of them[6]. Although the dual-band or multi-band FSS can be achieved based on the different geometry lengths, the bandwidth is still limited. To resolve this problem, the wideband FSS and high-order FSS are developed for a good performance. Traditionally, a wideband or multipole FSS can be obtained by cascading the multifirst-order FSSs with the quarter wavelength interval between each other[7]. I. INTRODUCTION The microstrip antenna is a conventional kind of antenna for radar application which it is used for various applications such as communication system, medical application, mobile services and radar systems in missile .In addition, the radar cross section (RCS) of the antenna is known as an important factor for some of these applications. The radar cross section (RCS) is noticed for stealth application by coating the surface of an aircraft[1] . Exactly, the RCS is a parameter for measuring of the object detection and the low RCS means that an object can find hard by radar systems. Consequently, it is attractive for stealth application . On the other hand, nowadays antennas with low RCS have been noticed while the fractal technique is one of the main methods for this goal[2] . Moreover, the ultrawideband antenna with low RCS has been considered such Vivaldi antenna , the monopole antenna with small ground [3]. The patch antenna is more considered for various microwave applications or for reducing the RCS. The loads have been combined by Yagi antenna and patch feed for decreasing of the RCS . Moreover, the metasurface and frequency selective surface recently have been studied for low radar cross section and circular polarization application, simultaneously based on II.PROPOSED ANTENNA The microstrip slot antenna has been developed based on feed coupling with the ground layer. The various shapes of the slot antenna like rectangular and circular formation have been studied during the past decades [8]. Moreover, the metamaterial or other 1 structures have been considered for different qualifications such as circular polarization or wider bandwidt [9]. Fig. 1 shows the antenna designing step from a simple slot to the final antenna. The geometry of the antenna is presented in Fig. 2(a) and (b) for the ground layer and the feed line, respectively, where the feed line is connected to a 50 ohm SMA connector. As shown here, the main slot is made in the circular shape with 4 small rectangular slots which they are rotated 45. Then, the six dual ring structures are added to the antenna as parasitic loads and finally, a disk is placed at the center for matching. provided wider bandwidth and lower RCS. In addition, the RCS is improved at the resonance frequency and the antenna gain is more than the similar research with high efficiency. Exactly, this antenna has a compact size in comparison with the other suggested model because we have combined the metasurface layer inside of the ground layer. The total size of the antenna is 40x40 mm2. It is designed on FR4 with the thickness of 1.6 mm as a low cost substrate with the permittivity of 4.3 and loss tangent of 0.02. The antenna all dimensions are a = 40 mm, b = 3.65 mm, c = 4 mm, d0 = 27 mm, d1 = 7.8 mm, d2 = 5.8 mm, d3 = 5.2 mm, w = 3 mm and l = 20 mm. Apparently, we have compounded a metasurface to the conventional microstrip slot antenna which is Figure 1: The four steps in antenna design from slot antenna to slot antenna with the fractal ring. Figure 2: The antenna’s geometry (a) the ground layer with parasitic elements, (b) the feed line geometry. III.SIMULATION OF ANTENNA Fig.4 . The simulated tool is using Ansoft Designer Fig.3. Besides, in the simulator program can obtain several graphic as the radiation pattern , impedance should in this case have zero imaginary part, and 50 in the real The result indicates that the bandwidth is about part, which results are shown in Fig.5. 1.5Ghz,from 2,6 to 4.1GHz.which results are shown in 2 The antenna radiation pattern for Phi = 0 and Phi = polarization. Fig.6 shows the antenna 2D radiation 90 at 3.1 GHz and slot is known for their bi-directional pattern for simulation and experimental. radiation pattern in Phi = 0 and Omnidirectional pattern in phi = 90 where the antenna shows low cross Figure 3: Simulation of antenna in ansoft designer Figure 4: The result indicates that the bandwidth 3 Figure 5: Diagram real and imaginary impedance. We can see the diagram where the imaginary part is aproximately zero at 3.1 GHz. Figure 6: Radiation Pattern IV. IMPLEMENTATION AND RESULTS rect results, the antenna was deployed in FR4, taking into account the design measures within the simulation, Fig.7. presents the final structure. Once the simulation was done and to obtain cor- 4 Figure 7: Top and bottom side The results were obtained using the signal genera- distance and obtained the following gain value of 49dB tor, which is connected to the antenna and a spectrum at the operating frequency of 3.1GHz.Therefore, it is analyzer where the receiver and transmitter are shown considered that the antenna works correctly. in Fig.8. The antenna was located at a considerable Figure 8: Measured results In addition, gain values in dB were taken at frequencies from 2.43 Ghz to 3.8 Ghz.The data obtained are shown in Fig.9.This graphic indicates that there are frequencies with higher and lower gain in which the antenna, you can also work. Through the use of Mat- lab, was obtained from the graph of the frequency with respect to the gain of the antenna.The figure previous indicates that relationship, having some similarity with that generated in the simulation in Ansoft Designer. 5 Figure 9: Frequency vs. Gain The measurement of the antenna was made by varying the theta and phi angles, this variation indicates the radiation that the antenna, in Fig.10 these data are observed with respect to the phi angle. Figure 10: Radiation phi angle V. CONCLUSION of a high precision especially if it works with high frequencies where the length of the antenna is going to be specified in Micrometers. The length of the antenna is inversely proportional to the frequency of operation that is why the order of the Ghz the antenna has a more short structure. The equipment used for the testing and analysis of our antennas were a Spectrum Master of the High Performance Handheld Spectrum Analyzer and a signal generator which to be working in perfect condition give us an analysis with low level of error. After implementing the transmitting and receiving antenna, it was obtained as a result that the frequency of operation with which the antenna worked is 1.4 GHz compared to the frequency of 1.5 Ghz with which work was done in simulations. Concluding that the frequency of operation had a phase shift of 0.1 Ghz. In addition to achieving an antenna sufficiently efficient it can be seen that the materials with which they were manufactured are of low monetary cost but 6 VI. RECOMMENDATION with reduced radar cross section. Prog Electromagn Res 2009;96:299–308. To obtain a correct gain of the antennas, the equipment must be configured correctly, in the different op[5] W. S. Chen and K. Y. 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