Advances in Condensed Matter Physics
Volume 2017 (2017), Article ID 1279849, 8 pages
https://doi.org/10.1155/2017/1279849

Research Article

Design and Fabrication of a Novel Wideband DNG Metamaterial with the Absorber Application in Microwave X-Band

Ahmed Mahmood,1,2 Gölge Ögücü Yetkin,² and Cumali Sabah3,4

¹Department of Electrical Engineering, Salahaddin University, Erbil, Iraq
²Department of Electrical and Electronics Engineering, University of Gaziantep, 27310 Gaziantep, Turkey
³Department of Electrical and Electronics Engineering, Middle East Technical University-Northern Cyprus Campus (METU-NCC), Kalkanli, 99738 Guzelyurt, TRNC, Mersin 10, Turkey
⁴Kalkanli Technology Valley, Middle East Technical University-Northern Cyprus Campus (METU-NCC), Kalkanli, 99738 Guzelyurt, TRNC, Mersin 10, Turkey

Correspondence should be addressed to Gölge Ögücü Yetkin; golge.ogucu@gmail.com

Received 22 November 2016; Accepted 1 March 2017; Published 26 March 2017

Academic Editor: Gary Wysin

Copyright © 2017 Ahmed Mahmood 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 metamaterial, which exhibits a wideband double negative behavior in X-band, is proposed, designed, and investigated in this paper. The metamaterial is composed of modified S-shaped split-ring resonators (S-SRR). The periodic structure is designed and simulated using CST MWs. Next, the experiments are carried out, and it is shown that the simulation and the experimental results agree well and the designed structure has a wide bandwidth in X-band. An absorber application of this metamaterial is also provided, and the structure can be used as an absorber with absorption rate of over 80% for the polarization angles between 0° and 40°.

1. Introduction

Metamaterials are based on periodic or nonperiodic artificial engineered structures that exhibit unusual characteristic behaviors, like negative permeability and negative permittivity , simultaneously over a common resonance frequency band [1, 2]. From the first realization of the metamaterials by periodic wire and split-ring resonator (SRR) structures [3, 4], there are various modified shapes and geometries such as square, triangle, -, Ω-, L-, S-, and P-shaped resonators [5–11] utilized in the designs in order to meet certain specifications in the applications. These geometries can be set in one-, two- or three-dimensional arrangements to control the electromagnetic wave propagation behavior through the medium.

The wideband metamaterials in X-band have been designed in [10, 11]. S-shaped SRRs were printed on opposite side of the host material and transmitted power was provided to show the DNG characteristics of the designed configuration in [10]. The double P-shaped resonators in [11] were printed on single side unlike that in [10]. The -parameters were presented; however there were no possible metamaterial applications found.

In this paper, a novel wideband metamaterial comprising a modified S-shaped SRR is proposed for X-band frequencies. The entire periodic structure is placed on one side of the substrate, which simplifies the manufacturing process and can be considered as an advantage of the designed structure. The retrieved constitutive parameters and the -parameters obtained via simulations and experiments demonstrate that the proposed structure exhibits a wideband left-handed characteristic in X-band frequencies. An absorption application is selected and also studied for demonstration of the performance of the metamaterial. The structure can be used as an absorber with absorption rate of over 80% for the polarization angles between 0° and 40°.

2. Design and Simulation Conditions

A unit cell of the proposed structure is composed of a modified S-shaped SRR printed on the front side of a square substrate of a side length of 16 mm and thickness of 1.6 mm as shown in Figure 1(a). The two ends of the S-shaped SRR are elongated in such a way that they take the form of C-shaped SRRs. In the design, FR-4 Epoxy of permittivity and loss tangent is chosen as the substrate, and the copper of electrical conductivity  S/m with coating thickness of 0.017 mm is chosen for printing the SRRs. The simulations are carried out by using the commercial program CST Microwave Studio 2016. Figure 1(b) shows the parameters that represent the electric topology of a modified S-SRR unit cell with the inductors and capacitors. Explicit expressions for and can be found in [12–14].

(a)

(b)

Figure 1: (a) The proposed unit cell with , , , , and . (b) Equivalent circuit model of proposed unit cell.

A unit cell of the proposed structure together with the ports applied in the simulations is shown in Figure 2. In the simulations, the unit cell is placed between two waveguide ports, which are perpendicular to the direction of the wave propagation, which is along negative -direction. To imitate the infinite structure, perfect electric boundary (PEB) conditions are set at the boundary surfaces perpendicular to the E-field while perfect magnetic boundary (PMB) conditions are at the boundary surfaces perpendicular to the H-field (see Figure 2). The frequency band is chosen as the X-band region (8–12 GHz).

Figure 2: The boundary conditions of the proposed unit cell used in the simulations.

3. Electric Field, Magnetic Field, and Surface Current Distributions

Basically, the nonhomogenous metamaterial structures provide a resonant RLC circuit behavior in some certain frequency bands. For the particular geometry in this paper, the modified S-shaped SRRs behave like inductors and the gaps as capacitors. To illustrate how the structure works when placed in an electromagnetic field region, the surface current distribution is presented in Figure 3 and the magnetic and electric field densities in Figure 4 at the operation frequency of 10.75 GHz, at which the structure behaves like a left-handed material. It can be observed from Figure 3 that the current is highly concentrated around the central wire and the copper shape structure. The magnetic field shows similar distribution as the current as shown in Figure 4(a), which supports that the resonance obtained is of magnetic type and the modified S-shaped elements are strongly coupled to this magnetic resonance. Moreover, a close examination of the current distribution in Figure 3 leads to the observation of some virtual gaps in addition to the actual gaps. These virtual gaps occur at current minimum points and this provides an additional capacitance-like response by being the voltage maxima points at the same time. The electric field is highly localized around these actual and virtual gaps as seen in Figure 4(b). The reason of high concentration around the actual gaps is the capacitive effect at these regions [13, 14].

Figure 3: The surface current distribution at 10.75 GHz.

(a)

(b)

Figure 4: (a) Magnetic field and (b) electric field distributions for the proposed unit cell at 10.75 GHz.

4. Simulated and Experimental Results

Before presenting the comparison of the simulated and the experimental results, it would be better to give some information about the experimental set-up. Experiment layout is prepared by placing the designed sample between two horn antennas, which are connected to a vector network analyzer (VNA) through coaxial cables as in Figure 5(a). By this way, the surface of the sample, which is shown in Figure 5(b), is guaranteed to be perpendicular to the direction of wave propagation. The metamaterial prototype is manufactured at in-house facilities using a circuit plotter with standard milling tool sets.

(a)

(b)

Figure 5: (a) Vector network analyzer, two horn antennas with coaxial cables. (b) Manufactured sample.

The incident electromagnetic wave propagates along negative -axis to excite the combined materials of the sample. The electric field vector and magnetic field vector are in the -axis and negative -axis, respectively (see Figure 2). For calibration purposes, a measurement is conducted without the sample. After that, the sample is placed between the two horn antennas and the -parameters are measured via VNA.

The simulated and the measured -parameter results, which are between 8 and 12 GHz, are presented in Figure 6. There are some small differences between the two types of obtained data, which may be due to the manufacture tolerances related to the dielectric dispersion and the etching process.

(a)

(b)

Figure 6: Simulated and measured -parameters: (a) the magnitude (dB) and (b) the phase (degrees).

The effective permittivity and permeability values are obtained from the -parameters given in Figure 6 by the use of the Nicolson-Ross-Weir (NRW) retrieval method [6, 15–17]. Using this method, the effective permittivity and permeability can be written as and , respectively, where is the propagation constant of free space. Here, , and the sign is chosen such that . Furthermore, , where , , and is the thickness of the slab. It clarifies that the integer has multiple choices, and it is not straightforward to assign the exact solution for the permittivity and permeability. To find the exact value of the integer , the group delay is calculated at each frequency, and then by taking the difference in phase of the data at adjacent frequency points and comparing it with the group delay caused with the assumed value of , the convergence on the correct value of is achieved. Thus, NRW method can be applied with justification.

Figure 7 presents the simulated and the experimental results for the real parts of the effective permittivity and permeability together with the real part of the refractive index of the structure. As can be observed, the results compare well, and the structure has negative real parts in the frequency bands ~8–10.45 GHz and ~10.65–11.75 GHz for the permittivity and in the frequency band ~8.5–12 GHz for the permeability. Thus the proposed structure exhibits a wideband metamaterial behavior.

(a)

(b)

(c)

Figure 7: The simulated and experimental results for the real parts of (a) permittivity, (b) permeability, and (c) refractive index.

5. Absorber Application

To investigate the performance of the proposed S-shaped SRR, the absorption characteristics of the structure are studied both experimentally and through simulations. The absorption of a material is function of frequency and can be formulated by , where and represent the reflection and the transmission characteristics, respectively [18]. In order to maximize the absorption, both the reflection and the transmission can be minimized at the resonance frequency. In this study, a copper layer on the backside of the substrate material is added, so that the absorption expression is reduced to , and it almost depends only on reflection now [18–20].

Figure 8(a) shows the VNA and the experiment alignment setting. After the calibration test without the testing sample, horn antenna is used to illuminate the sample in the X-band frequency regime, which is connected with VNA by a coaxial cable. As can be seen in Figure 8(b), the measurement results show good agreement with the simulation results. A maximum in the absorption ratio is about 99.99% at 8.94 GHz experimentally. Both the experimental and the simulation results suggest that the proposed structure can be used for perfect absorption applications. Note that the discrepancies between the experimental and simulation data are imputed to fabrication tolerances and dielectric dispersion of the substrate. The misalignment during the experiment may also be considered as another source of error.

(a)

(b)

Figure 8: (a) Absorption experiment setting. (b) Simulated and measured results of reflection and absorption ratio.

Furthermore, the -parameter and the absorption characteristics are simulated for different polarization angles in 8.75–9.05 GHz frequency band. In Figure 9, is presented for normal and oblique incidences. It is observed that reflection achieves its lowest value in normal incidence case and the resonance occurs around 8.912 GHz. As the polarization varies from normal to oblique incidence, the reflection also varies and a stable frequency response can be obtained for when .

(a)

(b)

Figure 9: Frequency response of for different polarization angles: (a) and varies and (b) varies and .

In Figure 10, the absorption characteristics are provided in the frequency band of 8.75–9.05 GHz for the polarization angle between and . It can be deduced that the proposed metamaterial can be used as a narrow band, 175 MHz perfect absorber with absorption over 90% in 8.825–9.0 GHz. At the resonance frequency around 8.912 GHz, is 0.0039. Correspondingly, the absorption rate is 99.99% at the resonance and the device can be used as a perfect absorber at the mentioned frequency.

(a)

(b)

Figure 10: Absorption for different polarization angles: (a) varies and and (b) and .

6. Conclusion

In this work, a modified S-shape ring resonator in periodic arrangement is introduced and investigated both numerically and experimentally. Based on the experiment results obtained, it has been demonstrated that the proposed structure exhibits wideband DNG characteristics in the frequency band of interest. In other words, the experimented novel metamaterial is well designed and successfully operates around the resonance frequency to provide simultaneously double negative permittivity and permeability in X-band. Additionally, simple fabrication of this novel metamaterial is another design advantage.

An absorber application has also been studied and measured. The measurement results show good agreement with the simulation results. Additionally, the simulated results for -parameters and the absorption rate are obtained at different polarization angles. It has been shown that high absorption can be achieved for oblique incidences up to 40° and with absorption peak more than 90% between 8.825 and 9 GHz. A perfect absorber can be obtained at the resonance frequency around 8.912 GHz.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

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