Research Article  Open Access
Wenjing Wu, Bo Yuan, Aiting Wu, "A QuadElement UWBMIMO Antenna with BandNotch and Reduced Mutual Coupling Based on EBG Structures", International Journal of Antennas and Propagation, vol. 2018, Article ID 8490740, 10 pages, 2018. https://doi.org/10.1155/2018/8490740
A QuadElement UWBMIMO Antenna with BandNotch and Reduced Mutual Coupling Based on EBG Structures
Abstract
A compact planar quadelement ultrawideband (UWB) antenna with a bandnotch and low coupling for multipleinput multipleoutput (MIMO) system is proposed in this paper. The antenna consists of four circular monopoles with modified defected ground plane and a periodic electromagnetic band gap (EBG) structures. The proposed EBG structures are modified from the traditional mushroomlike ones, comprised of patterns of grids on the top patch, the metallic ground plane, and several vias that connect the top and bottom plane. It is printed at the center of the dielectric substrate to lower electromagnetic coupling between the parallel elements. Besides, by etching four crescent ringshaped resonant slots on the radiators, a sharp bandnotched characteristic is achieved. From the experimental results, the −10 dB bandwidth of the antenna is extended covers from 3.0 to 16.2 GHz, with a sharp notched band at 4.6 GHz. And the isolation is greater than 17.5 dB between its elements, with a peak gain of 8.4 dB and a peak efficiency of 91.2%. Moreover, it has a compact size of at 3 GHz and could be a good candidate for portable devices.
1. Introduction
Since Federal Communications Commission (FCC) released the spectrum from 3.1 to 10.6 GHz for commercial applications [1], ultrawideband (UWB) technology has drawn considerable attention due to its merits of low complexity, lowpower consumptions, capability of high data rate, low interference, good timedomain resolution, and reduction of severe multipath effect [2]. Although UWB communication system makes use of huge frequency bands, the permitted power spectral density of the UWB signal is rather limited to avoid interference with other systems, such as the frequency band from 4400 to 4990 MHz, which is adopted in large capacity microwave relay trunk network. Multipleinputmultipleoutput (MIMO) technology enables the transmission of data over multiple channels and increases the channel capacity without additional power requirements; thus, it has been widely used in modern wireless communication system [3]. Furthermore, compact and planar antenna designs are of great demand since they are easier to integrate with wireless devices [4].
As a key technology for nextgeneration communication systems, MIMO technique can increase the capability and reliability without additional power or spectrum [5]. To achieve good performance and compact structure, good isolation between closelyspaced antennas is required for MIMO communication systems [6]. In [4], a compact quadelement wideband antenna with slotted ground plane is presented. By etching a modified slotted ground plane, the bandwidth is extended covers from 2 to 6 GHz with a compact size of at 2 GHz, but the isolation is only 14 dB between its elements. In [7], a wideband MIMO antenna with common elements suitable for WiFi and LTE wireless access point application is proposed. It consists of four microstrip feedlineprinted monopole antennas with common radiating element and a ringshaped ground plane; the impedance bandwidth is enhanced from 1.8 to 2.9 GHz by common element particular design. However, it only results in isolation of 15 dB in the operating frequency band. In [8], a fourelement MIMO patch antenna is designed for 2.45 GHz band operation. For the purpose of antenna miniaturization, it adopts complementary splitring resonator (CSRR) loading on its ground plane, which reduces the singleelement antenna size by 76%. But, the isolation of the antenna only achieves −10 dB. In [9], a dual element stacked patch antenna is designed for MIMO technology, it achieves a high isolation, and the minimum isolation reaches 31 dB mainly due to the orthogonal polarization modes of the two excited ports. Nevertheless, the relative operating frequency bandwidth is only 4.3% from 3.65 to 3.81 GHz and the overall dimension is at 3.65 GHz which is obviously large in miniaturization portable devices.
In this paper, a compact UWBMIMO antenna with a bandnotch and reduced mutual coupling is presented and fabricated. The initial design of a single element includes a circular monopole at the top layer of the dielectric substrate and a modified defected ground structure at the bottom layer to obtain an ultrawideband. Besides, a crescent ringshaped resonant slot is etched on the surface of the circular monopole to achieve a bandreject to inhibit the interference of large capacity microwave relay trunk network. The orthogonal placement of the elements can ensure the low coupling between the orthogonal element (e.g., 12 and 1–4) and a array electromagnetic band gap (EBG) structure can ensure high isolation between the parallel elements (e.g., 1–3 and 2–4). From the experimental results, the proposed antenna has ultrawideband covers from 3.0 to 16.2 GHz, the bandnotch centered at 4.6 GHz covers from 4.0 to 5.2 GHz, and good isolation of 17.5 dB between every two elements is achieved. Besides, radiation pattern, gain, efficiency, envelope correlation coefficient (ECC), total active reflection coefficient (TARC), mean effective gain (MEG), diversity gain (DG), and channel capacity loss (CCL) are measured and calculated.
2. Proposed Antenna Configuration
The proposed antenna is fabricated on the lowcost FR4 substrate with a relative permittivity of 4.4, thickness of 1.6 mm, and loss tangent of 0.02. Electromagnetic simulator HFSS is used for calculating Sparameters, gain, efficiency, radiation pattern, ECC, TARC, MEG, DG, and CCL, while the dispersion characterization of surface waves propagating on the EBG structures is investigated by CST MWS.
2.1. SingleElement Antenna
The geometry of a single element of the four port antenna is shown in Figure 1. The evolution of the element to obtain an ultrawideband and a bandnotched at 4.6 GHz is shown in Figure 2. A printed circular monopole is adopted as the basic element for the antenna; from Figure 2, one can conclude that it radiates at 4.0 GHz and with a bandwidth of 1.46 GHz. The shape of the ground plane of the circular monopole radiator is a rectangle with dimensions of , as shown in Figure 2 (case I). To achieve an ultrawideband resonance, a big semicircle with radius of and two small semicircles with radius of are etched on the rectangle ground. The circular monopole radiator benefits from this defected ground structure which has an effect on impedance matching; thus, its simulated bandwidth is expanded covers from 3.3 to 18.0 GHz below −10 dB impedance bandwidth level, which is shown as case II in Figure 2. In order to inhibit the interference of large capacity microwave relay trunk network, a crescent ringshaped resonant structure is etched on the surface of the circular monopole antenna as shown in case III in Figure 2. The slot acts as a quarter (guided) wavelength parallel opencircuit transmission line that shorts the antenna at the frequency band from 4.0 to 5.2 GHz. The bandnotch characteristics at the frequency band are obtained by etching a crescent ringshaped resonant slot from the circular monopole of the antenna. The length of the slot is about at the center frequency of the notched band and can be calculated by the following formulas: where is the outer arc length of the etched slot that can be derived by trigonometric function of other geometric parameters as follows: , the geometric meanings of parameters , , and are illustrated in Figure 1(a), and and are in radian measurement; represents the inner arc length of the etched slot, its mathematical formula as follows: , , and are also illustrated in Figure 1(a), and is in radian measurement too; is the speed of the light; is the center frequency of the notched band; the value of relative permittivity is 4.4; is effective dielectric constant of the microstrip, and it is simplified from a formula for dielectric constant of the uniform medium. According to the center frequency of 4.6 GHz, the parameters of , , , and are calculated initially. Then, the parameters are optimized as = 5.7 mm, = 4.1 mm, = 0.7 mm, and = 4.0 mm by HFSS.
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2.2. Integration of a FourElement Antenna
By using the element proposed in the previous section, a simulated model of a quadelement UWBMIMO antenna is built as shown in Figure 3(a). Individual elements, occupying an area of , are placed rotationally and symmetrically in a square substrate with an interval of . As illustrated in Figure 4, the Sparameters between parallel element (i.e., 1–3 and 2–4) exhibit a suppressed isolation, overwhelmingly lower than 17.5 dB in the frequency band of 5.1 GHz–5.6 GHz and 7.3 GHz–9.1 GHz. However, the orthogonal arrangement of elements (i.e., 12 and 1–4) exhibits good isolation, which is mainly greater than 20 dB in the whole band. The orthogonal arrangement of elements in the antenna can ensure a good isolation between adjacent elements, which is due to the orthogonal polarization field produced in the elements and the mutual coupling is reduced. However, the parallel elements can produce the symmetrical electromagnetic field and the similar polarization; thus, the power will flow from antenna 1 to antenna 3 (antenna 2 to antenna 4) when they are excited, which leads to the high coupling between parallel elements. In Section 3, the EBG structures are proposed to inhibit the mutual coupling between the parallel elements.
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2.3. Investigation of BandReject Gap Properties
As it is well known, EBG structures can suppress wave propagation in the space between the elements and produce a bandreject gap. Therefore, a periodic EBG structure is implemented to inhibit the mutual coupling between the parallel elements with the target frequency band of 5.1–5.6 GHz and 7.3–9.1 GHz. The EBG array structures, unit cell structure, geometrical parameters of the unit cell, and the parallel LC equivalent resonant circuit are shown in Figures 3(b)–3(e), respectively. The operation mechanism of this EBG structure can be explained by an equivalent LC resonant circuit: is the capacitance of air gap between adjacent EBG unit cells, is the capacitance of dielectric gap between top metallic patch and ground plane, and L represents the inductance of metallic vias. For an EBG structure with patch width , gap width , substrate thickness , and dielectric constant , the values of the inductor and the capacitors (i.e., and ) are determined by the following formulas [10]: where and S represents the crosssectional area of via hole, is the permeability of free space, and is the permittivity of free space. The initial parameters of the unit cell are calculated by (2), according to the frequency band of 5.1–5.6 GHz and 7.3–9.1 GHz. Then, dispersion diagram is drawn to further study the highimpedance surface of the EBG structures.
According to the initial parameters of the unit cell, dispersion characterization of surface waves propagating on the unit cell of EBG structures is investigated using finite integration technique (FIT) by CST MWS. The boundary conditions of side walls of the unit have to be considered periodic, and the boundaries at the top and the bottom of the model are defined as electric conductor, as illustrated in Figure 5(a). In order to cover the frequency band of 5.1–5.6 GHz and 7.3–9.1 GHz, the parameters of the unit cell are optimized as follows: = 1.75 mm, = 0.2 mm, = 3.9 mm, and = 0.1 mm. The numerically simulated dispersion diagram of the surface modes propagating in the EBG structure is conducted using CST eigenmode solver, as shown in Figure 5(b). A complete bandreject between the first mode (TM0 mode) and the second mode (TE1 mode) in the frequency band of 5.0–9.8 GHz can be observed., , and stand for symmetric points in the irreducible Brillouin zone. The branch represents with , the branch represents with , and the branch represents with [10–14]. Because of slowwave behavior of surface waves, dispersion curves are calculated only in the region under the light line, and the simulated frequency bandreject gap is from 5.0 to 9.8 GHz, as shown in Figure 5(b). Therefore, the isolation between the parallel elements has been enhanced from 17 dB to 20 dB within the bandreject gap of 5.1–5.6 GHz and 7.3–9.17 GHz when the EBG array structures placed at the center of the dielectric substrate, which could be observed in Figure 4(a).
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3. Measurement and Results
The proposed antenna is fabricated, as shown in Figure 6. Simulated and measured results of the quadelement UWBMIMO antenna system are discussed in this section. The measurements of the proposed antenna are implemented by using Rohde and Schwarz ZVM vector network analyzer.
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The simulated and measured Sparameters of the UWBMIMO antenna are shown in Figure 7. The measured Sparameter under −10 dB level is from 3.0 to 16.2 GHz with a bandwidth of 137.5%, which is less than the simulated one from 3.0 to 20.0 GHz. Deviation of curve occurs at highfrequency band between the measured result, and the simulated one is mainly due to the error of fabricating, welding, and testing. And reflection coefficient of the bandnotched antenna at 4.6 GHz is about −2.4 dB, which can inhibit the interference of large capacity microwave relay trunk network from 4.0 to 5.2 GHz. From the curves of Sparameters, it can be observed that the antenna system exhibits a measured minimum isolation of 17.5 dB between its elements throughout the operating band. A comparison between the proposed antenna and few other recently reported planar MIMO designs in terms of bandwidth, mutual coupling, and size is shown in Table 1, where is the largest freespace wavelength corresponding to the lowest operating frequency of the referenced antennas. It can be observed that the proposed planar MIMO antenna has an excellent bandwidth performance, a good inhibitory ability to rejected frequency band, and has a compact size.
Farfield patterns are obtained inside an anechoic chamber for antenna 1, while the other three elements are terminated with 50 impedances. Port 1 is measured due to the symmetrical of the proposed antenna, which leads to the same patterns when other ports are excited. Measured radiation patterns for xozplane, yozplane, and xoyplane at 3.5, 10.5, and 16.2 GHz are shown in Figure 8. It is observed that crosspolarization at some planes is quite high because of the orthogonal arrangement of the four elements, which leads to the orthogonal of the electrical field. Peak gain and efficiency measurements are also performed and are plotted in Figure 9. Gain measurements show a peak gain of 8.4 dB at 16 GHz, and a peak efficiency of 91.2% is obtained at 10 GHz.
The envelope correlation coefficients (ECC), diversity gain (DG), and total active reflection coefficient (TARC) are computed for evaluating the diversity performance of the proposed quadelement MIMO antenna. ECC quantifies the correlation between the branch signals received by different elements, and a lower ECC signifies higher pattern diversity. The envelope correlation coefficient of the fourantenna system can be given by [15] where XPR is the ratio of crosspolarization power, which is defined as ( are the vertical component strength of the electric field and the horizontal component strength of the electric field, resp.). are the complex envelops of component of farfield radiation patterns, respectively, when the th port is excited and the other ports are terminated with 50 impedance. are the probability distributions of the power incident on the antenna in the polarizations, respectively. The angle is defined by in elevation and in azimuth. ECC is below 0.3 in the working frequency band from 3.0 to 16.5 GHz as shown in Figure 10, and that could ensure the favorable diversity gain (DG) presented in Table 2. TARC is the square root of the sum of all incident powers at the ports minus radiated power and then divided by the sum of all incident powers at the ports of an Nport antenna. TARC can be computed by the following formula, given by [8] where and are the incident signals and reflected signals, respectively, is the antenna’s scattering matrix, is the excitation vector, and represents the scattered vector. Formula (5) can be written as

According to the fourport MIMO antenna system, TARC is a parameter that refers to the coupling of the ports, and its value is between 0 and 1, where 0 means all incident power is radiated, but 1 means all incident power is reflected. TARC curves for the proposed MIMO antenna with different phase combinations between the four elements are described in decibels in Figure 11. The excited port 1 is kept at , while the other ports (i.e., ports 2, 3, and 4) are excited with different phases. For example, if the legend reads (), it means that the excited phase of antenna 2 is at shift with antenna 1, antenna 3 is at shift, and antenna 4 is consistent with antenna 1. As evident from the figures, the simulated TARC curves have an agreement with the curve at some phases shift (e.g., , , and ) of the excited ports, where more incident power is radiated.
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To quantify the average received signal strength for each element, mean effective gains (MEGs) are calculated as the ratio of mean received power to the mean incident power. The MEG of the antenna can be calculated using its twodimensional gain pattern, which is given by [8] as where is the crosspolarization discrimination (XPD) of the incident field, and are the power gain patterns. The MEG of the proposed antenna is tabulated in Table 2. An XPD of 0 dB corresponds to outdoor applications and an XPD of 6 dB corresponds to indoor applications. As evident from the Table, the antenna has a good MEG performance as deviations between the MEGs of the various elements are both less than 3 dB.
Theoretically, the channel capacity can be improved by increasing the number of antennas of the MIMO system. However, the uncorrelated Rayleigh fading will result in channel capacity loss (CCL) of the MIMO system. The capacity loss () of the fourelement MIMO antenna can be evaluated by using the equation as follows [16, 17]: where is the receiving antenna correlation matrix that is given by , and , for = 1, 2, 3, or 4. The simulated and measured capacity losses of the proposed MIMO antenna are shown in Figure 12; it can be seen that the simulated capacity loss is less than 0.4bits/s/Hz in the operating frequency band except for the frequency band of 3.0 GHz–5.7 GHz and 7.0 GHz–8.3 GHz. Observed from Figure 4 and Figure 9, the isolation of parallel element is 2 to 4.5 dB lower in the band of 3.0 GHz–3.8 GHz and 1 to 3 dB lower in the band of 5.1 GHz–5.7 GHz than the standard isolation of 22 dB, the radiation efficiency in the band of 3.8 GHz–5.1 GHz is probably 1% to 52.8% lower than lowest 78.2% efficiency in other operating frequency band, and the isolations of orthogonal element and parallel element in 7.0 GHz–8.3 GHz are about 0.2 dB to 2 dB and 0.1 dB to 3 dB lower than the standard isolation of 22 dB, respectively. In addition, the measured one can also be analyzed in the same way. Therefore, the higher isolation and radiation efficiency will induce lower channel capacity loss.
4. Conclusion
In this paper, a compact planar quadelement UWBMIMO antenna with bandnotch and reduced mutual coupling based on EBG structures is presented. The antenna is fabricated on a FR4 substrate and occupies a total size of 60 × 60 × 1.6 mm^{3}. The antenna system exhibits good impedance matching across the −10 dB operating bandwidth. By etching four crescent ringshaped resonant slots on the radiators, a sharp bandnotched characteristic is achieved at 4.6 GHz. Low mutual coupling is achieved by orthogonal placement of the elements and loading EBG structures. The radiation efficiency, ECC, TARC, MEG, DG, and CCL have been calculated to evaluate the diversity performance of the proposed MIMO antenna. In short, the quadelement UWBMIMO antenna with band rejection and high isolation has an application value in modern wireless communication systems.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
This work was supported by the NSFC under Contract 61501153.
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Copyright
Copyright © 2018 Wenjing Wu 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.