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<front>
<journal-meta>
<journal-id journal-id-type="pmc">CSSE</journal-id>
<journal-id journal-id-type="nlm-ta">CSSE</journal-id>
<journal-id journal-id-type="publisher-id">CSSE</journal-id>
<journal-title-group>
<journal-title>Computer Systems Science &#x0026; Engineering</journal-title>
</journal-title-group>
<issn pub-type="ppub">0267-6192</issn>
<publisher>
<publisher-name>Tech Science Press</publisher-name>
<publisher-loc>USA</publisher-loc>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">23102</article-id>
<article-id pub-id-type="doi">10.32604/csse.2022.023102</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Article</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>A Compact Self-Isolated MIMO Antenna System for 5G Mobile Terminals</article-title><alt-title alt-title-type="left-running-head">A Compact Self-Isolated MIMO Antenna System for 5G Mobile Terminals</alt-title><alt-title alt-title-type="right-running-head">A Compact Self-Isolated MIMO Antenna System for 5G Mobile Terminals</alt-title>
</title-group>
<contrib-group content-type="authors">
<contrib id="author-1" contrib-type="author" corresp="yes">
<name name-style="western"><surname>Muhsin</surname><given-names>Muhannad Y.</given-names></name>
<xref ref-type="aff" rid="aff-1">1</xref><email>muhannad.y.muhsin@uotechnology.edu.iq</email>
</contrib>
<contrib id="author-2" contrib-type="author">
<name name-style="western"><surname>Salim</surname><given-names>Ali J.</given-names></name>
<xref ref-type="aff" rid="aff-2">2</xref>
</contrib>
<contrib id="author-3" contrib-type="author">
<name name-style="western"><surname>Ali</surname><given-names>Jawad K.</given-names></name>
<xref ref-type="aff" rid="aff-2">2</xref>
</contrib>
<aff id="aff-1"><label>1</label><institution>Microwave Research Group, Department of Electrical Engineering, University of Technology</institution>, <addr-line>Baghdad, 10001</addr-line>, <country>Iraq</country></aff>
<aff id="aff-2"><label>2</label><institution>Microwave Research Group, Department of Communication Engineering, University of Technology</institution>, <addr-line>Baghdad, 10001</addr-line>, <country>Iraq</country></aff>
</contrib-group><author-notes><corresp id="cor1">&#x002A;Corresponding Author: Muhannad Y. Muhsin. Email: <email>muhannad.y.muhsin@uotechnology.edu.iq</email></corresp></author-notes>
<pub-date pub-type="epub" date-type="pub" iso-8601-date="2022-01-18"><day>18</day>
<month>01</month>
<year>2022</year></pub-date>
<volume>42</volume>
<issue>3</issue>
<fpage>919</fpage>
<lpage>934</lpage>
<history>
<date date-type="received"><day>27</day><month>8</month><year>2021</year></date>
<date date-type="accepted"><day>28</day><month>9</month><year>2021</year></date>
</history>
<permissions>
<copyright-statement>&#x00A9; 2022 Muhsin, Salim and Ali</copyright-statement>
<copyright-year>2022</copyright-year>
<copyright-holder>Muhsin, Salim and Ali</copyright-holder>
<license xlink:href="https://creativecommons.org/licenses/by/4.0/">
<license-p>This work is licensed under a <ext-link ext-link-type="uri" xlink:type="simple" xlink:href="https://creativecommons.org/licenses/by/4.0/">Creative Commons Attribution 4.0 International License</ext-link>, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</license-p>
</license>
</permissions>
<self-uri content-type="pdf" xlink:href="TSP_CSSE_23102.pdf"></self-uri>
<abstract>
<p>A compact self-isolated Multi Input Multi Output (MIMO) antenna array is presented for 5G mobile phone devices. The proposed antenna system is operating at the 3.5 GHz band (3400&#x2013;3600 MHz) and consists of eight antenna elements placed along two side edges of a mobile device, which meets the current trend requirements of full-screen smartphone devices. Each antenna element is divided into two parts, a front part and back part. The front part consists of an I-shaped feeding line and a modified Hilbert fractal monopole antenna, whereas the back part is an L-shaped element shorted to the system ground by a 0.5 mm short stub. A desirable compactness can be obtained by utilizing the Hilbert space-filling property where the antenna element&#x2019;s overall planar size printed on the side-edge frame is just (9.57 mm &#x00D7; 5.99 mm). The proposed MIMO antenna system has been simulated, analyzed, fabricated and tested. Based on the self-isolated property, good isolation (better than 15 dB) is attained without employing additional decoupling elements and/or isolation techniques, which increases system complexity and reduces the antenna efficiency. The scattering parameters, antenna efficiencies, antenna gains, and antenna radiation characteristics are investigated to assess the proposed antenna performance. For evaluating the proposed antenna array system performance, the Envelope Correlation Coefficients (ECCs), Mean Effective Gains (MEGs) and channel capacity are calculated. Desirable antenna and MIMO performances are evaluated to confirm the suitability of the proposed MIMO antenna system for 5G mobile terminals.</p>
</abstract>
<kwd-group kwd-group-type="author">
<kwd>5G applications</kwd>
<kwd>compact antennas</kwd>
<kwd>isolation techniques</kwd>
<kwd>MIMO antennas</kwd>
<kwd>mobile terminals</kwd>
<kwd>self-isolated antennas</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="s1">
<label>1</label>
<title>Introduction</title>
<p>With increasing growth of wireless communication technologies, high data rates and intelligent services are being continuously demanded. Because of the advantages of large channel capacity, massive connection density and high spectral efficiency, the 5G wireless communication systems have attracted increasing attention in both academic and industrial fields [<xref ref-type="bibr" rid="ref-1">1</xref>]. One of the essential enabling technologies for the 5G communication systems is the Multiple Input Multiple Output (MIMO) technology. By utilizing the multipath property of the wireless communication environment, a MIMO system can improve the spectral efficiency and channel capacity without needing more bandwidth and/or transmitting power [<xref ref-type="bibr" rid="ref-2">2</xref>]. Whenever increasing MIMO system&#x2019;s antenna elements, larger channel capacity and more link reliability can be obtained. However, because of mobile devices&#x2019; limited space, the mutual coupling problem is becoming more pronounced with more penetration of antennas. The MIMO system&#x2019;s performance is severely affected by the mutual coupling impact [<xref ref-type="bibr" rid="ref-3">3</xref>]. So, various techniques have been employed and provided reasonable solutions to solve this problem. One of these techniques includes the spatial diversity method [<xref ref-type="bibr" rid="ref-4">4</xref>&#x2013;<xref ref-type="bibr" rid="ref-6">6</xref>]. Good isolation can be obtained by this method but at the expense of decreasing the number of antennas, where the space variation between antennas is used as a key approach to achieve low mutual coupling. Isolation enhancement can be done with more compactness than the spatial diversity method by employing the polarization diversity method [<xref ref-type="bibr" rid="ref-7">7</xref>,<xref ref-type="bibr" rid="ref-8">8</xref>], and the pattern diversity method [<xref ref-type="bibr" rid="ref-9">9</xref>,<xref ref-type="bibr" rid="ref-10">10</xref>]. However the compact size and simple structure design of 5G mobile devices, which have high diversity performance capability with low ECCs, remains a highly requested aim for antenna engineers in designing MIMO antenna systems. Moreover, many other isolation techniques using external decoupling structures have been reported in the literature including parasitic structure [<xref ref-type="bibr" rid="ref-11">11</xref>,<xref ref-type="bibr" rid="ref-12">12</xref>], hybrid elements (neutralization line and parasitic element) [<xref ref-type="bibr" rid="ref-13">13</xref>], neutralization line [<xref ref-type="bibr" rid="ref-14">14</xref>,<xref ref-type="bibr" rid="ref-15">15</xref>], decoupling network [<xref ref-type="bibr" rid="ref-16">16</xref>,<xref ref-type="bibr" rid="ref-17">17</xref>], slot etching [<xref ref-type="bibr" rid="ref-18">18</xref>], hybrid decoupling like ground slot etching and meandered line parasitic element [<xref ref-type="bibr" rid="ref-19">19</xref>] or ground slot and neutralization line [<xref ref-type="bibr" rid="ref-20">20</xref>], and multimode decoupling technique [<xref ref-type="bibr" rid="ref-21">21</xref>]. Although these isolation techniques, which are based on additional decoupling structures, provide good isolation enhancement, the antenna efficiency might be reduced significantly. In other words, the isolation improvement is done at the expense of the antenna efficiency. For example, the antenna efficiency in [<xref ref-type="bibr" rid="ref-15">15</xref>] and [<xref ref-type="bibr" rid="ref-21">21</xref>] is affected notably, decreasing to 30% and 34%, respectively. Good isolation and antenna performance have been reported by utilizing the self-isolated technique [<xref ref-type="bibr" rid="ref-22">22</xref>]; however, the antenna element size is too large. In a self-isolated property, an antenna element operates as a radiated element as well as an isolation one at the same time. So, there will be no need for additional decoupling elements or/and isolation techniques. Nevertheless, a compact-size massive MIMO antenna system with good isolation and high efficiency for 5G mobile devices is still a challenge.</p>
<p>In this paper, a compact self-isolated eight-element antenna system that operates in the (3400&#x2013;3600 MHz) band is presented for future 5G MIMO mobile handsets. The main feature of this work is that it can effectively solve the isolation problem with keeping high antenna efficiency. Based on the self-isolated property, good isolation is obtained without utilizing decoupling elements and/or isolation techniques. In addition to that, a compact antenna size and simple structure is presented in the proposed system where the antenna element&#x2019;s overall planar size printed on the side-edge frame is just (9.57 mm &#x00D7; 5.99 mm). Furthermore, a high diversity performance with very low envelope correlation coefficients (ECCs) is attained, where a very good independence antenna&#x2019;s far-field radiation characteristics can be shown. Besides, good antenna and MIMO performances are achieved. The proposed antenna system was simulated and analyzed using the CST Microwave Studio software (version 2019). A prototype model of the proposed system was fabricated and its performance was measured. Reasonable agreement between the measured and simulated results has been obtained.</p>
</sec>
<sec id="s2">
<label>2</label>
<title>Proposed Antenna System</title>
<p>The proposed eight-element MIMO antenna system for 5G mobile phones is presented in <xref ref-type="fig" rid="fig-1">Fig. 1</xref>. The eight antenna elements of the proposed MIMO system are located over a mobile device&#x2019;s two long side edges. The main board size is (150 &#x00D7; 75) mm<sup>2</sup>. This is a typical size of a 5.5-inch phone device. A side edge frame of 7 mm height is selected for a slim smartphone device requirement. Both the system circuit board and the frame are designed by employing a double-sided FR4 substrate of 0.8 mm height. It has an approximate relative permittivity of 4.3 and a dielectric loss tangent of 0.02. At the bottom and the top of the main system board, two clearance areas are left for the current 4G antennas and other different antennas. The size of each clearance area is (8 &#x00D7; 75) mm<sup>2</sup>. As can be observed from <xref ref-type="fig" rid="fig-1">Fig. 1</xref>, the eight antenna elements are printed on the inner and outer surfaces of the two long side-edges of the frame substrate. They are located perpendicularly on the mobile device&#x2019;s main substrate, with each side having four antenna elements. All antennas have the same structure and dimensions. A 50 &#x03A9; SMA connector is employed for feeding antenna elements <italic>via</italic> holes from the backside of the main system ground. As illustrated in <xref ref-type="fig" rid="fig-1">Fig. 1</xref>, the distance between the front sides of the antennas which are printed on the inner frame surfaces is descried by <italic>D</italic>, and the distance between the back sides of the antenna elements is denoted by <italic>d</italic>, while the distance between the antenna feeding lines is indicated by <italic>DL</italic>. For example, <italic>D</italic>15 means the distance between the front sides of Ant1 and Ant5 and so on. In addition to that, the four antennas located at the mobile frame&#x2019;s corners are symbolized as Ant1, Ant2, Ant3 and Ant4, while the four antennas located at the middle of the mobile frame are denoted by Ant5, Ant6, Ant7 and Ant8. The following parameters are optimized for the proposed MIMO antenna system (<italic>D</italic>15 &#x003D; <italic>D</italic>47 &#x003D; <italic>D</italic>26 &#x003D; <italic>D</italic>38 &#x003D; 30.43 mm, <italic>D</italic>56 &#x003D; <italic>D</italic>78 &#x003D; 34.13 mm), (<italic>d</italic>15 &#x003D; <italic>d</italic>47 &#x003D; <italic>d</italic>26 &#x003D; <italic>d</italic>38 &#x003D; 33 mm, <italic>d</italic>56 &#x003D; <italic>d</italic>78 &#x003D; 39.27 mm), and (<italic>DL</italic>15 &#x003D; <italic>DL</italic>47 &#x003D; <italic>DL</italic>26 &#x003D; <italic>DL</italic>38 &#x003D; 39.62 mm, <italic>DL</italic>56 &#x003D; <italic>DL</italic>78 &#x003D; 34.13 mm). One can observe from the distance parameters the similarity of the frame long side-edges.</p>
<fig id="fig-1">
<label>Figure 1</label>
<caption>
<title>The proposed eight-element MIMO antenna system</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-1.png"/>
</fig>
<p><xref ref-type="fig" rid="fig-2">Fig. 2</xref> shows the perspective view of a single self-isolated compact antenna element. As seen from this figure, the antenna element can be divided into two parts, a front part and a back part. <xref ref-type="fig" rid="fig-3">Fig. 3</xref> depicts the detailed structure of the two parts. The front part of the antenna, as observed in <xref ref-type="fig" rid="fig-3">Fig. 3a</xref>, consists of an I-shaped feeding line and a modified Hilbert fractal monopole antenna. The second iteration of the Hilbert fractal geometry is considered and its modification is done by extending its long arm length. The symbol <italic>FL</italic> is used to describe the I-shaped feeding line which is fine-tuned for matching purposes. The long line length of the Hilbert&#x2019;s arm is represented by <italic>LL</italic> and the short one is described by <italic>LS</italic>. Very good antenna miniaturization is obtained by utilizing the Hilbert space-filling property, where the antenna element overall planar size is just (9.57 mm &#x00D7; 5.99 mm) which operates at the desired (3.4&#x2013;3.6) GHz band. Due to its small-size characteristic of 0.111 <inline-formula id="ieqn-1">
<mml:math id="mml-ieqn-1"><mml:mrow><mml:msub><mml:mi>&#x03BB;</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:math>
</inline-formula> &#x00D7; 0.069 <inline-formula id="ieqn-2">
<mml:math id="mml-ieqn-2"><mml:mrow><mml:msub><mml:mi>&#x03BB;</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:math>
</inline-formula> at 3.5 GHz and its printed design on the slim mobile frame, the proposed antenna element is appropriate for 5G massive MIMO antenna systems with slim and full-screen smartphone requirements. The smaller the antennas size the greater the distance between antennas. So, the probability of increasing the isolation between antennas is greater. The back part of the antenna element which serves as a virtual ground is demonstrated in <xref ref-type="fig" rid="fig-3">Fig. 3b</xref>. It has an L-shape which is shorted to the system ground by a 0.5 mm short stub directly under its vertical part. The length and width of the L-shape vertical stub are denoted by <italic>VL</italic> and <italic>VW</italic> respectively, while the horizontal stub dimensions are denoted by <italic>HL</italic> and <italic>HW</italic>, respectively. The coupling capacitance generated by the L-shaped shorted-stub is used to provide the desirable impedance matching. It is also employed to direct the antenna radiation for better diversity characteristics and radiation performance. For obtaining the desired antenna and MIMO performances of the proposed MIMO antenna system, the following parameters are optimized as follows: <italic>FL</italic> &#x003D; 9.97 mm, <italic>LL</italic> &#x003D; 7.70 mm, <italic>LS</italic> &#x003D; 2.25 mm, <italic>VL</italic> &#x003D; 5.84 mm, <italic>VW</italic> &#x003D; 1 mm, <italic>HL</italic> &#x003D; 6 mm, <italic>HW</italic> &#x003D; 0.8 mm.</p>

<fig id="fig-2">
<label>Figure 2</label>
<caption>
<title>Three-dimensional view of the single antenna element</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-2.png"/>
</fig>
<fig id="fig-3">
<label>Figure 3</label>
<caption>
<title>Single element front part (a) and back part (b)</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-3.png"/>
</fig>
<p>To further demonstrate the working principle of the proposed compact self-isolated antenna element, the effects of <italic>LL</italic> and <italic>VL</italic> on the input reflection coefficient have been demonstrated as depicted in <xref ref-type="fig" rid="fig-4">Figs. 4</xref> and <xref ref-type="fig" rid="fig-5">5</xref>, respectively. <xref ref-type="fig" rid="fig-6">Fig. 6</xref> illustrates the surface current distribution at 3.5 GHz. One can see from <xref ref-type="fig" rid="fig-4">Fig. 4</xref> that four values have been chosen for <italic>LL</italic>: 7.5 mm, 7.7 mm (the proposed one), 8 mm and 8.5 mm. As expected, the antenna resonance frequency shifts according to the antenna length. So in this case study, the antenna resonance frequency shifts to a lower value as the effective value of <italic>LL</italic> increases. As can be observed form <xref ref-type="fig" rid="fig-5">Fig. 5</xref> that four values have been introduced for the <italic>VL</italic> parameter which are 2.85 mm, 3.85 mm, 5.85 mm (the proposed one) and 6.85 mm. So the optimized <italic>VL</italic> parameter value, which is an effective parameter of the coupling capacitance generated by the virtual antenna ground, plays a vital role for obtaining a very good impedance matching. In addition to that, the virtual antenna ground (L-shaped shorted-stub) has been employed to direct the maximum antenna gain direction to a direction far away as much as possible from other antennas maximum gain directions. Thus, the isolation among antennas in the proposed MIMO system is improved. It is worth noting that these case studies have been taken on a single antenna (Ant1 alone) before extending the system to the proposed eight antenna elements which will be discussed in the next section. <xref ref-type="fig" rid="fig-6">Fig. 6a</xref> shows the surface current distribution of Ant1 front side. As depicted in this figure, the current mainly concentrates on the path (ABCDEFGH) and of course on the feeding line. The length of this current flowing path (the current direction is denoted by arrows) is about 22.85 mm, which is 0.26 <inline-formula id="ieqn-3">
<mml:math id="mml-ieqn-3"><mml:mrow><mml:msub><mml:mi>&#x03BB;</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:math>
</inline-formula> (where <inline-formula id="ieqn-4">
<mml:math id="mml-ieqn-4"><mml:mrow><mml:msub><mml:mi>&#x03BB;</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:math>
</inline-formula> is the free space wavelength of 3.5 GHz). So this current path represents a 0.25 <inline-formula id="ieqn-5">
<mml:math id="mml-ieqn-5"><mml:mrow><mml:msub><mml:mi>&#x03BB;</mml:mi><mml:mn>0</mml:mn></mml:msub></mml:mrow></mml:math>
</inline-formula> monopole-like mode operating at 3.5 GHz resonance frequency. One can also see that the direction of the current flow is inverted at the IJ section and the current intensity is very weak, so the points M and N are considered as the current null points. The current intensity at the KL section is also weak, and point O is accounted as the current null point because of the capacitance in the IJ section (the lower section) which blocks the current flow at this point. <xref ref-type="fig" rid="fig-6">Fig. 6b</xref> illustrates the current distribution of the antenna virtual ground (L-shaped shorted-stub) with the main system&#x2019;s ground. As observed, the current intensity is mainly focused on the region confined under the antenna virtual ground at the main system&#x2019;s ground plane, which is the reason behind the self-isolated property of the proposed antenna element. The advantages of the proposed antenna structure with its self-isolated property in the proposed eight antenna elements will be discussed in the next section.</p>
<fig id="fig-4">
<label>Figure 4</label>
<caption>
<title>Simulated reflection coefficient as a function of LL</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-4.png"/>
</fig>
<fig id="fig-5">
<label>Figure 5</label>
<caption>
<title>Simulated reflection coefficient as a function of VL</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-5.png"/>
</fig>
<fig id="fig-6">
<label>Figure 6</label>
<caption>
<title>Simulated surface current distribution at 3.5 GHz. Antenna front side (a) and antenna back side with the main system ground (b)</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-6.png"/>
</fig>
</sec>
<sec id="s3">
<label>3</label>
<title>Results and Discussions</title>
<sec id="s3_1">
<label>3.1</label>
<title>Antenna Performance</title>
<p>The simulated results of the S-parameters for the proposed eight-element MIMO antenna system are sketched in <xref ref-type="fig" rid="fig-7">Fig. 7</xref>. As shown in <xref ref-type="fig" rid="fig-7">Fig. 7a</xref>, all the eight reflection coefficients of the antennas satisfy values less than &#x2013;10 dB (2:1 VSWR) over all the desired bandwidth (3.4&#x2013;3.6) GHz. This ensures a very good impedance matching. It can also be observed that there exists a very slight difference between the reflection coefficients of the eight antennas and that of the single antenna element (Ant1) presented in <xref ref-type="fig" rid="fig-4">Fig. 4</xref>. This gives an indication of an acceptable mutual coupling between antennas. Because of the antennas&#x2019; similarity in the structure and the distribution along the two side-edges frame, the simulation results are also similar. So, only the transmission coefficients of the single side-edge antennas (Ant1, Ant2, Ant5 and Ant6) are presented in <xref ref-type="fig" rid="fig-7">Fig. 7b</xref>. The transmission coefficients <italic>S</italic><sub>51</sub>, <italic>S</italic><sub>62</sub>, <italic>S</italic><sub>65</sub> are better than 12.2 dB, while <italic>S</italic><sub>21</sub>, <italic>S</italic><sub>61</sub>, <italic>S</italic><sub>52</sub> are better than 18 dB within the interested band. Therefore, good isolation is obtained without employing additional isolation elements and/or decoupling methods. To better explain the effectiveness of the proposed self-isolated antenna element in the proposed MIMO system&#x2019;s good isolation, the surface current distributions of the proposed antenna system at 3.5 GHz are illustrated in <xref ref-type="fig" rid="fig-8">Fig. 8</xref>. Two cases have been presented in this sketch where <xref ref-type="fig" rid="fig-8">Fig. 8a</xref> shows the case when Ant1 is excited and all other antennas are terminated with 50 &#x03A9;, while <xref ref-type="fig" rid="fig-8">Fig. 8b</xref> demonstrates the other case when Ant5 is excited and all other antennas are terminated with 50 &#x03A9;. As depicted in both figures, when either Ant1 or Ant5 is excited, the current intensity is concentrated in the region bounded inside the excited antenna area. This is the reason for good isolation of the proposed 8-element MIMO system. In this case, the desirable impedance matching and isolation are achieved without using matching circuits, additional isolation elements, and/or other decoupling methods which increases system complexity and reduces antenna efficiency. So, this is considered as the main advantage of the proposed MIMO antenna system.</p>
<fig id="fig-7">
<label>Figure 7</label>
<caption>
<title>Reflection coefficients (a) and transmission coefficients (b)</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-7.png"/>
</fig>
<fig id="fig-8">
<label>Figure 8</label>
<caption>
<title>Surface current distribution of the proposed antenna system at 3.5 GHz with Ant1 is excited and all other antenna elements terminated by 50 &#x03A9; (a) and Ant5 is excited and all other antenna elements terminated by 50 &#x03A9; (b)</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-8.png"/>
</fig>
<p>In addition to that, two cases have been studied to explain the effects of different array configurations. Due to the similarity, only the necessary S-parameters of a single side-edge are plotted in <xref ref-type="fig" rid="fig-9">Fig. 9</xref>. In case one, the distance (<italic>D</italic>15 &#x003D; <italic>D</italic>26 &#x003D; 10.43 mm) is taken between the adjacent antennas (Ant1 and Ant5, Ant2 and Ant6), whereas in case two, the distance (<italic>D</italic>15 &#x003D; <italic>D</italic>26 &#x003D; 15.43 mm) is chosen. As can be observed in <xref ref-type="fig" rid="fig-9">Figs. 9a</xref> and <xref ref-type="fig" rid="fig-9">9b</xref>, the reflection coefficients <italic>S</italic><sub>11</sub> and <italic>S</italic><sub>55</sub> do not change too much and are still satisfying the band of interest with acceptable impedance matching. The isolation (<italic>S</italic><sub>51</sub> in both cases) is reasonably reduced by decreasing the distance between antennas. However, the isolation is slightly reduced and is still at an acceptable value of more than 10 dB in both cases. This indicates the ability of the proposed self-isolated antenna structure in working well at different array element arrangements. So there is no need to use an impedance matching circuit or to re-optimize the antenna structure when an antenna moves from one location to another. This is one of the advantages of the proposed MIMO antenna system.</p>
<fig id="fig-9">
<label>Figure 9</label>
<caption>
<title>Simulated S-parameters of different MIMO antenna array configurations. (a) Case one (b) Case two</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-9.png"/>
</fig>
<p><xref ref-type="fig" rid="fig-10">Fig. 10</xref> shows all the radiation and total antenna efficiencies, which are in the range (66%&#x2013;75%) and (56%&#x2013;66%), respectively along the working band. The proposed self-isolated MIMO antenna system does not incur additional losses of decoupling elements or/and isolation techniques which affect the antenna efficiency performance. Thus, desirable antenna efficiencies are obtained. <xref ref-type="fig" rid="fig-11">Fig. 11</xref> depicts the eight antennas&#x2019; gain of the proposed MIMO system along the operating band. As observed, the maximum gains of the four antennas located at the mobile frame&#x2019;s corners (Ant1, Ant2, Ant3 and Ant4) are about 4.07 dB, whereas the maximum gains of the four antennas located at the middle of the mobile frame (Ant5, Ant6, Ant7 and Ant8) are about 4.58 dB. So, they are appropriate for the 5G antenna requirement for mobile handsets. Three-dimensional and two-dimensional radiation patterns of all eight antennas at 3.5 GHz resonance frequency are displayed in <xref ref-type="fig" rid="fig-12">Figs. 12a</xref> and <xref ref-type="fig" rid="fig-12">12b</xref>, respectively. Radiation pattern of Ant1 is described by (a), Ant2 is indicated by (b) and so on. As observed, the maximum gains of the antennas are in different directions, thereby indicating a desirable pattern diversity feature. Furthermore, these radiation patterns completely cover all sides of the mobile device&#x2019;s mainboard, indicating a very good radiation coverage performance of the proposed antenna system.</p>
<fig id="fig-10">
<label>Figure 10</label>
<caption>
<title>Antenna efficiency</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-10.png"/>
</fig>
<fig id="fig-11">
<label>Figure 11</label>
<caption>
<title>Antenna gain</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-11.png"/>
</fig>
<fig id="fig-12">
<label>Figure 12</label>
<caption>
<title>Radiation patterns of all eight antennas at 3.5 GHz. (a) 3D (b) 2D</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-12.png"/>
</fig>
</sec>
<sec id="s3_2">
<label>3.2</label>
<title>MIMO Performance</title>
<p>In this subsection, important parameters are evaluated and discussed to assess the potential MIMO performance of the proposed antenna array. The correlation coefficient (&#x03C1;) indicates how much the multipath communication channels are correlated or isolated (<italic>i.e</italic>., a measure of the independency) [<xref ref-type="bibr" rid="ref-23">23</xref>]. This metric refers to the correlation between the antenna radiation patterns. The square of the correlation coefficient (<inline-formula id="ieqn-6">
<mml:math id="mml-ieqn-6"><mml:mrow><mml:msup><mml:mi>&#x03C1;</mml:mi><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:math>
</inline-formula>) is defined as the Envelope Correlation Coefficient (<inline-formula id="ieqn-7">
<mml:math id="mml-ieqn-7"><mml:mrow><mml:msub><mml:mi>&#x03C1;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula>). The ECC can be calculated based on the far-field radiation patterns by means of <xref ref-type="disp-formula" rid="eqn-1">Eq. (1)</xref> [<xref ref-type="bibr" rid="ref-24">24</xref>]:</p>
<p><disp-formula id="eqn-1"><label>(1)</label>
<mml:math id="mml-eqn-1" display="block"><mml:mspace width="thickmathspace" /><mml:mrow><mml:msub><mml:mi>&#x03C1;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mspace width="thickmathspace" /><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mrow><mml:mo>|</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mo>&#x222B;</mml:mo><mml:mspace width="negativethinmathspace" /><mml:mspace width="negativethinmathspace" /><mml:mspace width="negativethinmathspace" /><mml:mo>&#x222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>4</mml:mn><mml:mi>&#x03C0;</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mrow><mml:mover><mml:mi>F</mml:mi><mml:mo stretchy="false">&#x2192;</mml:mo></mml:mover></mml:mrow></mml:mrow><mml:mn>1</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>&#x2217;</mml:mo><mml:mspace width="thickmathspace" /><mml:mrow><mml:msub><mml:mrow><mml:mrow><mml:mover><mml:mi>F</mml:mi><mml:mo stretchy="false">&#x2192;</mml:mo></mml:mover></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mo>]</mml:mo></mml:mrow><mml:mspace width="thickmathspace" /><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x03A9;</mml:mi></mml:mrow><mml:mo>|</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mo>&#x222B;</mml:mo><mml:mspace width="negativethinmathspace" /><mml:mspace width="negativethinmathspace" /><mml:mspace width="negativethinmathspace" /><mml:mo>&#x222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>4</mml:mn><mml:mi>&#x03C0;</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mrow><mml:mo>|</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mrow><mml:mover><mml:mi>F</mml:mi><mml:mo stretchy="false">&#x2192;</mml:mo></mml:mover></mml:mrow></mml:mrow><mml:mn>1</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mo>|</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow><mml:mspace width="thickmathspace" /><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x03A9;</mml:mi><mml:mspace width="thickmathspace" /><mml:msub><mml:mrow><mml:mo>&#x222B;</mml:mo><mml:mspace width="negativethinmathspace" /><mml:mspace width="negativethinmathspace" /><mml:mspace width="negativethinmathspace" /><mml:mo>&#x222B;</mml:mo></mml:mrow><mml:mrow><mml:mn>4</mml:mn><mml:mi>&#x03C0;</mml:mi></mml:mrow></mml:msub><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mrow><mml:mo>|</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mrow><mml:mover><mml:mi>F</mml:mi><mml:mo stretchy="false">&#x2192;</mml:mo></mml:mover></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mo>|</mml:mo></mml:mrow></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow><mml:mspace width="thickmathspace" /><mml:mi>d</mml:mi><mml:mi mathvariant="normal">&#x03A9;</mml:mi></mml:mrow></mml:mfrac></mml:mrow></mml:mstyle></mml:math>
</disp-formula></p>
<p>where &#x2126; defines the solid angle, <inline-formula id="ieqn-8">
<mml:math id="mml-ieqn-8"><mml:mover><mml:mrow><mml:mrow><mml:msub><mml:mi>F</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow><mml:mspace width="thickmathspace" /></mml:mrow><mml:mo>&#x2192;</mml:mo></mml:mover><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi mathvariant="normal">&#x0398;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:math>
</inline-formula> indicates the three dimensional far field radiation pattern and the asterisk sign (&#x002A;) refers to the Hermitian product. In addition to that, the ECC can be obtained simply in terms of the S-parameters from <xref ref-type="disp-formula" rid="eqn-2">Eq. (2)</xref> as indicated in [<xref ref-type="bibr" rid="ref-25">25</xref>]:</p>
<p><disp-formula id="eqn-2"><label>(2)</label>
<mml:math id="mml-eqn-2" display="block"><mml:mrow><mml:mo>|</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>&#x03C1;</mml:mi><mml:mi>e</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi><mml:mo>,</mml:mo><mml:mi>N</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow><mml:mo>|</mml:mo></mml:mrow><mml:mo>=</mml:mo><mml:mspace width="thickmathspace" /><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:mrow><mml:mo>|</mml:mo><mml:mrow><mml:msubsup><mml:mrow><mml:mo movablelimits="false">&#x2211;</mml:mo></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:msubsup><mml:mo>&#x2061;</mml:mo><mml:msubsup><mml:mi>S</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow><mml:mo>|</mml:mo></mml:mrow></mml:mrow><mml:mrow><mml:msqrt><mml:mrow><mml:mo>|</mml:mo><mml:mrow><mml:msub><mml:mrow><mml:mo movablelimits="false">&#x220F;</mml:mo></mml:mrow><mml:mrow><mml:mi>k</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mo>=</mml:mo><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>j</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:msub><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>[</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mo>&#x2212;</mml:mo><mml:mspace width="thickmathspace" /><mml:msubsup><mml:mrow><mml:mo movablelimits="false">&#x2211;</mml:mo></mml:mrow><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>N</mml:mi></mml:msubsup><mml:mo>&#x2061;</mml:mo><mml:msubsup><mml:mi>S</mml:mi><mml:mrow><mml:mi>i</mml:mi><mml:mo>,</mml:mo><mml:mi>n</mml:mi></mml:mrow><mml:mo>&#x2217;</mml:mo></mml:msubsup><mml:mrow><mml:msub><mml:mi>S</mml:mi><mml:mrow><mml:mi>n</mml:mi><mml:mo>,</mml:mo><mml:mi>k</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:mrow><mml:mo>]</mml:mo></mml:mrow></mml:mrow><mml:mo>|</mml:mo></mml:mrow></mml:msqrt></mml:mrow></mml:mfrac></mml:mrow><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /></mml:mstyle></mml:math>
</disp-formula></p>
<p>In this formula, N is the number of antennas and the antenna elements are expressed as <italic>i</italic> and <italic>j</italic>, respectively. For acceptable MIMO performance, the values of ECCs between the MIMO antennas should be less than 0.5. The smaller the ECCs, the better the MIMO system diversity performance is. The ECCs between the antennas in the proposed eight elements MIMO system are plotted in <xref ref-type="fig" rid="fig-13">Fig. 13</xref>, which are calculated based on the E-filed radiation patterns of <xref ref-type="disp-formula" rid="eqn-1">Eq. (1)</xref> under the hypothesis of uniform propagation channel with balanced polarization. Due to the similarity of the results, only antennas of the single side-edge frame are presented. As observed, the ECCs are all less than 0.02 in the desired band, which are far less from the accepted criteria (ECC &#x003C; 0.5). So the proposed MIMO antenna system has a capability of a high diversity performance. Based on the small ECCs values, high diversity gain performance of the proposed MIMO antenna system is attained which is better than 9.9 dB in the desired band.</p>
<p>The Mean Effective Gain (MEG) is considered as one of the effective performance metrics for MIMO antenna systems. It can be well-defined as the ratio between the mean received power of the antenna to the total mean incident power when the antenna is moved over a random mobile environment route. MEG can be obtained from <xref ref-type="disp-formula" rid="eqn-3">Eq. (3)</xref> below [<xref ref-type="bibr" rid="ref-26">26</xref>]:</p>
<p><disp-formula id="eqn-3"><label>(3)</label>
<mml:math id="mml-eqn-3" display="block"><mml:mi>M</mml:mi><mml:mi>E</mml:mi><mml:mi>G</mml:mi><mml:mo>=</mml:mo><mml:mspace width="thickmathspace" /><mml:msubsup><mml:mrow><mml:mo>&#x222B;</mml:mo></mml:mrow><mml:mn>0</mml:mn><mml:mrow><mml:mn>2</mml:mn><mml:mi>&#x03C0;</mml:mi></mml:mrow></mml:msubsup><mml:mo>&#x2061;</mml:mo><mml:msubsup><mml:mrow><mml:mo>&#x222B;</mml:mo></mml:mrow><mml:mn>0</mml:mn><mml:mi>&#x03C0;</mml:mi></mml:msubsup><mml:mo>&#x2061;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mspace width="thickmathspace" /><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mrow><mml:mi>X</mml:mi><mml:mi>P</mml:mi><mml:mi>R</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi>X</mml:mi><mml:mi>P</mml:mi><mml:mi>R</mml:mi></mml:mrow></mml:mfrac></mml:mrow><mml:mspace width="thickmathspace" /><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>&#x03B8;</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>&#x03B8;</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:mspace width="thickmathspace" /><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mn>1</mml:mn><mml:mrow><mml:mn>1</mml:mn><mml:mo>+</mml:mo><mml:mi>X</mml:mi><mml:mi>P</mml:mi><mml:mi>R</mml:mi></mml:mrow></mml:mfrac></mml:mrow><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>&#x03C6;</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>&#x03C6;</mml:mi></mml:msub></mml:mrow><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mi>&#x03B8;</mml:mi><mml:mo>,</mml:mo><mml:mi>&#x03C6;</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mstyle></mml:mstyle><mml:mo>)</mml:mo></mml:mrow><mml:mspace width="thickmathspace" /><mml:mo stretchy="false">(</mml:mo><mml:mi>sin</mml:mi><mml:mo>&#x2061;</mml:mo><mml:mi>&#x03B8;</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mspace width="thickmathspace" /><mml:mi>d</mml:mi><mml:mi>&#x03B8;</mml:mi><mml:mspace width="thickmathspace" /><mml:mi>d</mml:mi><mml:mi>&#x03C6;</mml:mi><mml:mspace width="thickmathspace" /><mml:mspace width="thickmathspace" /></mml:math>
</disp-formula></p>
<p>where the cross-polarization power ratio is denoted as XPR, and <inline-formula id="ieqn-9">
<mml:math id="mml-ieqn-9"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi>&#x03C6;</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> and <inline-formula id="ieqn-10">
<mml:math id="mml-ieqn-10"><mml:mrow><mml:msub><mml:mi>P</mml:mi><mml:mi mathvariant="normal">&#x0398;</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> indicate the phi and theta components of the normalized angular power density functions of the incoming plane waves, while <inline-formula id="ieqn-11">
<mml:math id="mml-ieqn-11"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi mathvariant="normal">&#x0398;</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> and <inline-formula id="ieqn-12">
<mml:math id="mml-ieqn-12"><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>&#x03C6;</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> are the antenna gain components. It is worth noting that for good MIMO antenna system diversity performance and system power balance, the MEGs of the MIMO antennas should satisfy the required criteria of (<inline-formula id="ieqn-13">
<mml:math id="mml-ieqn-13"><mml:mi>M</mml:mi><mml:mi>E</mml:mi><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> &#x2245; <inline-formula id="ieqn-14">
<mml:math id="mml-ieqn-14"><mml:mi>M</mml:mi><mml:mi>E</mml:mi><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula>) [<xref ref-type="bibr" rid="ref-10">10</xref>,<xref ref-type="bibr" rid="ref-27">27</xref>], where <inline-formula id="ieqn-15">
<mml:math id="mml-ieqn-15"><mml:mi>M</mml:mi><mml:mi>E</mml:mi><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>i</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> and<inline-formula id="ieqn-16">
<mml:math id="mml-ieqn-16"><mml:mspace width="thickmathspace" /><mml:mi>M</mml:mi><mml:mi>E</mml:mi><mml:mrow><mml:msub><mml:mi>G</mml:mi><mml:mi>j</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> are the mean effective gains of the <italic>i</italic> and <italic>j</italic> antennas, respectively. <xref ref-type="fig" rid="fig-14">Fig. 14</xref> depicts the MEGs for all eight antennas of the proposed MIMO system, which are taken under the assumption of uniform distribution for the azimuth direction and Gaussian distribution for the elevation direction of the angular power density function. It can be seen that the MEGs for all antennas are stable along the operating band. Furthermore, the MEGs nearly satisfy the equality condition of the antenna elements in the designed MIMO system.</p>
<fig id="fig-13">
<label>Figure 13</label>
<caption>
<title>ECCs of the proposed system</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-13.png"/>
</fig>
<fig id="fig-14">
<label>Figure 14</label>
<caption>
<title>MEGs of the proposed eight antennas</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-14.png"/>
</fig>
<p>Another significant parameter used to evaluate the multiplexing performance of the proposed MIMO antenna system is the channel capacity (CC), indicating the maximum data rate that can be achieved. It can be computed by <xref ref-type="disp-formula" rid="eqn-4">Eq. (4)</xref> [<xref ref-type="bibr" rid="ref-28">28</xref>]:</p>
<p><disp-formula id="eqn-4"><label>(4)</label>
<mml:math id="mml-eqn-4" display="block"><mml:mi>C</mml:mi><mml:mi>C</mml:mi><mml:mo>=</mml:mo><mml:mspace width="thickmathspace" /><mml:mi>l</mml:mi><mml:mi>o</mml:mi><mml:mrow><mml:msub><mml:mi>g</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:mrow><mml:mspace width="thickmathspace" /><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:mrow><mml:mo>+</mml:mo><mml:mspace width="thickmathspace" /><mml:mstyle displaystyle="true" scriptlevel="0"><mml:mrow><mml:mfrac><mml:mi>P</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:mrow></mml:mfrac></mml:mrow><mml:mspace width="thickmathspace" /><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>R</mml:mi></mml:msub></mml:mrow><mml:mspace width="thickmathspace" /><mml:mi>H</mml:mi><mml:mrow><mml:msup><mml:mi>H</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msup></mml:mrow><mml:mspace width="thickmathspace" /><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:mrow></mml:mstyle></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:math>
</disp-formula></p>
<p>CC is the channel capacity of the MIMO system in bits/s/Hz, <inline-formula id="ieqn-17">
<mml:math id="mml-ieqn-17"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> and <inline-formula id="ieqn-18">
<mml:math id="mml-ieqn-18"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>R</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> are the covariance matrices of the transmitted and received antennas, while <italic>N</italic> and <italic>P</italic> are the noise power and signal power, respectively. The sign (&#x2217;) indicates the complex conjugate transpose operation, <italic>H</italic> is the random channel matrix (independent and identically distributed (i.i.d) Gaussian imaginary and real parts) and <inline-formula id="ieqn-19">
<mml:math id="mml-ieqn-19"><mml:mrow><mml:msup><mml:mi>H</mml:mi><mml:mo>&#x2217;</mml:mo></mml:msup></mml:mrow><mml:mspace width="thickmathspace" /></mml:math>
</inline-formula> its transpose, <inline-formula id="ieqn-20">
<mml:math id="mml-ieqn-20"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>t</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> and <inline-formula id="ieqn-21">
<mml:math id="mml-ieqn-21"><mml:mrow><mml:msub><mml:mi>N</mml:mi><mml:mi>r</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> are the number of antennas at the transmitter and receiver ends respectively, and <inline-formula id="ieqn-22">
<mml:math id="mml-ieqn-22"><mml:mrow><mml:msub><mml:mi>I</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>r</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>
</inline-formula> is an <italic>N &#x00D7; N</italic> unity matrix. This study aims to focus only on the effects in the user terminal so that <inline-formula id="ieqn-23">
<mml:math id="mml-ieqn-23"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>T</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mi>I</mml:mi></mml:math>
</inline-formula> (uncorrelated lossless transmitting antennas), where <italic>I</italic> is the identity matrix. To associate the effects of the proposed MIMO antennas in this model which are simulated by MATLAB software, the <inline-formula id="ieqn-24">
<mml:math id="mml-ieqn-24"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>R</mml:mi></mml:msub></mml:mrow></mml:math>
</inline-formula> is computed from <xref ref-type="disp-formula" rid="eqn-5">Eq. (5)</xref>:</p>
<p><disp-formula id="eqn-5"><label>(5)</label>
<mml:math id="mml-eqn-5" display="block"><mml:mrow><mml:msub><mml:mi>C</mml:mi><mml:mi>R</mml:mi></mml:msub></mml:mrow><mml:mo>=</mml:mo><mml:mi>I</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mspace width="thickmathspace" /><mml:mrow><mml:msup><mml:mi>S</mml:mi><mml:mi>H</mml:mi></mml:msup></mml:mrow><mml:mi>S</mml:mi></mml:math>
</disp-formula></p>
<p>where <italic>S</italic> is the S-parameters matrix of the proposed MIMO antenna system which are obtained from the CST&#x2019;s simulated results. As it can be seen in <xref ref-type="fig" rid="fig-15">Fig. 15</xref>, the channel capacities of the proposed eight-element MIMO system are computed for different values of the Signal to Noise Ratio (SNR) based on Rayleigh fading channel environment model.</p>
<fig id="fig-15">
<label>Figure 15</label>
<caption>
<title>Simulated channel capacities of the proposed 8-element MIMO system</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-15.png"/>
</fig>
</sec>
</sec>
<sec id="s4">
<label>4</label>
<title>MIMO Antenna System Prototype and Measurement Results</title>
<p>The proposed 8-element MIMO smartphone antenna was fabricated and experimentally tested. The assembled prototype model is depicted in <xref ref-type="fig" rid="fig-16">Fig. 16</xref>. Through the measurement process, each antenna under test (AUT) is connected to the vector network analyzer (VNA) and other antenna elements are connected to 50 &#x03A9; matched terminal loads (MTL). Due to the similarity and for the brevity, only the necessary simulated and measured S-parameters have been plotted in <xref ref-type="fig" rid="fig-17">Figs. 17a</xref> and <xref ref-type="fig" rid="fig-17">17b</xref>, respectively. As observed, acceptable impedance matching and good isolation performance (better than 15 dB) are obtained by the proposed MIMO antenna system. The measured and simulated results are in good agreement. However, there are some deviations between them which may be due to fabrication tolerances, soldering effects, and/or measurement errors.</p>
<fig id="fig-16">
<label>Figure 16</label>
<caption>
<title>Fabricated prototype model of the proposed antenna (a) Perspective view (b) Back view</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-16.png"/>
</fig>
<fig id="fig-17">
<label>Figure 17</label>
<caption>
<title>Measured and simulated S-parameters (a) Reflection coefficients (b) Transmission coefficients</title></caption>
<graphic mimetype="image" mime-subtype="png" xlink:href="CSSE_23102-fig-17.png"/>
</fig>
<p><xref ref-type="table" rid="table-1">Tab. 1</xref>, presents a summary for the performance comparison of the proposed eight-element MIMO antenna system with some other recent MIMO antenna systems reported for the 5G mobile phone devices. Compared with other MIMO antenna systems, the proposed one has got a smaller size and lower ECC. Good system isolation and eight antenna total efficiencies are obtained by adopting the self-isolation property where there is no additional antenna efficiency loss by other decoupling elements and/or isolation techniques. So it can be seen from the <xref ref-type="table" rid="table-1">Tab. 1</xref>, that the proposed eight-element MIMO system is able to provide a massive MIMO system with a very comparable antenna and MIMO performance.</p>
<table-wrap id="table-1"><label>Table 1</label>
<caption>
<title>Performance comparison with other recent works</title></caption>
<table><colgroup>
<col/>
<col/>
<col/>
<col/>
<col/>
<col/>
<col/>
<col/>
<col/>
</colgroup>
<thead>
<tr>
<th style="background:#FFFFFF;">Ref.</th>
<th style="background:#FFFFFF;">Bandwidth (GHz)</th>
<th style="background:#FFFFFF;">Total Efficiency (%)</th>
<th style="background:#FFFFFF;">Isolation<break/>(dB)</th>
<th style="background:#FFFFFF;">ECC</th>
<th style="background:#FFFFFF;">Overall System Size (mm<sup>2</sup>)</th>
<th style="background:#FFFFFF;">Antenna<break/>Element Size<break/>(mm &#x00D7; mm)</th>
<th style="background:#FFFFFF;">MIMO Order</th>
<th style="background:#FFFFFF;">Isolation<break/>Technique</th>
</tr>
</thead>
<tbody>
<tr>
<td>[<xref ref-type="bibr" rid="ref-9">9</xref>]</td>
<td>(3.3&#x2013;3.6) (&#x2013;6 dB)</td>
<td>(44&#x2013;53)</td>
<td>&#x003E;15</td>
<td>&#x003C;0.15</td>
<td>(40 &#x00D7; 100)</td>
<td>(14 &#x00D7; 44.7)</td>
<td>8 &#x00D7; 8</td>
<td>Pattern diversity</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-20">20</xref>]</td>
<td>(3.3&#x2013;3.6) (&#x2013;6 dB)</td>
<td>(45&#x2013;60)</td>
<td>&#x003E;15</td>
<td>&#x003C;0.15</td>
<td>(40 &#x00D7; 124)</td>
<td>(12.5 &#x00D7; 4.9)</td>
<td>8 &#x00D7; 8</td>
<td>Ground slot etching and Neutralization line</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-27">27</xref>]</td>
<td>(3.4&#x2013;3.6) (&#x2013;10)</td>
<td>&#x003E;40</td>
<td>&#x003E;10</td>
<td>&#x003C;0.1</td>
<td>(75 &#x00D7; 150)</td>
<td>(7 &#x00D7; 10)</td>
<td>8 &#x00D7; 8</td>
<td>Self-isolated</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-29">29</xref>]</td>
<td>(3.3&#x2013;5) (&#x2013;10 dB)</td>
<td>&#x003E;46</td>
<td>&#x003E;14.5</td>
<td>&#x003C;0.1</td>
<td>(75 &#x00D7; 150)</td>
<td>(22 &#x00D7; 6)</td>
<td>8 &#x00D7; 8</td>
<td>Self-isolated</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-30">30</xref>]</td>
<td>(2.55&#x2013;2.65) (&#x2013;10 dB)</td>
<td>(48&#x2013;58)</td>
<td>&#x003E;13</td>
<td>&#x003C;0.2</td>
<td>(68 &#x00D7; 136)</td>
<td>(18.6 &#x00D7; 18.6)</td>
<td>8 &#x00D7; 8</td>
<td>Polarization diversity</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-31">31</xref>]</td>
<td>(3.3&#x2013;3.6) (&#x2013;6 dB)</td>
<td>(42&#x2013;75)</td>
<td>&#x003E;13</td>
<td>&#x003C;0.15</td>
<td>(75 &#x00D7; 155)</td>
<td>(28.8 &#x00D7; 1)</td>
<td>8 &#x00D7; 8</td>
<td>Balanced mode excitation</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-32">32</xref>]</td>
<td>2.55&#x2013;2.65 (&#x2013;10 dB)</td>
<td>(48&#x2013;63)</td>
<td>&#x003E;12.5</td>
<td>&#x003C;0.15</td>
<td>(68 &#x00D7; 136)</td>
<td>(31.2 &#x00D7; 5)</td>
<td>8 &#x00D7; 8</td>
<td>Polarization diversity and Pattern diversity</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-14">14</xref>]</td>
<td>(3.4&#x2013;3.6), (4.8&#x2013;5.1)<break/>(&#x2013;6 dB)</td>
<td>(41&#x2013;72) LB,<break/>(40&#x2013;85) HB</td>
<td>&#x003E;11.5</td>
<td>&#x003C;0.08 LB<break/>&#x003C;0.05 HB</td>
<td>(75 &#x00D7; 150)</td>
<td>(15 &#x00D7; 7)</td>
<td>8 &#x00D7; 8</td>
<td>Neutralization line</td>
</tr>
<tr>
<td>[<xref ref-type="bibr" rid="ref-33">33</xref>]</td>
<td>(3.4&#x2013;3.8) (5.15&#x2013;5.93) (&#x2013;6)</td>
<td>&#x003E;42</td>
<td>&#x003E;11</td>
<td>&#x003C;0.15</td>
<td>(80 &#x00D7; 150)</td>
<td>(16.2 &#x00D7; 3)</td>
<td>10 &#x00D7; 10</td>
<td>Polarization diversity and Space diversity</td>
</tr>
<tr>
<td>This work</td>
<td>(3.4&#x2013;3.6) (&#x2013;10)</td>
<td>(56&#x2013;66)</td>
<td>&#x003E;15</td>
<td>&#x003C;0.02</td>
<td>(75 &#x00D7; 150)</td>
<td>(9.57 &#x00D7; 5.99)</td>
<td>8 &#x00D7; 8</td>
<td>Self-isolated</td>
</tr>
</tbody>
</table>
</table-wrap>
</sec>
<sec id="s5">
<label>5</label>
<title>Conclusions</title>
<p>In this study, an eight-port MIMO antenna array is introduced and examined for 5G massive MIMO smartphone devices. Very good antenna miniaturization is achieved by utilizing the Hilbert fractal space-filling property. Due to the self-isolated property of the proposed antenna structure, good isolation is achieved (better than 15 dB) without using decoupling elements and/or isolation techniques. The main trait of the self-isolated property is that a single antenna can operate as a radiated and an isolated element simultaneously so that the antenna efficiencies do not decrease. The simulated and measured results of the antenna and MIMO performances obtained, as well as the structure simplicity, compactness, self-isolated property and position independency, show that the proposed eight element MIMO antenna system is a convincing candidate for the future 5G mobile phone devices.</p>
</sec>
</body>
<back><fn-group>
<fn fn-type="other">
<p><bold>Funding Statement:</bold> The authors received no specific funding for this study.</p>
</fn>
<fn fn-type="conflict">
<p><bold>Conflicts of Interest:</bold> The authors declare that they have no conflicts of interest to report regarding the present study.</p>
</fn>
</fn-group>
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