<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">IJCNS</journal-id><journal-title-group><journal-title>International Journal of Communications, Network and System Sciences</journal-title></journal-title-group><issn pub-type="epub">1913-3715</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijcns.2017.105B012</article-id><article-id pub-id-type="publisher-id">IJCNS-76555</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject></subj-group></article-categories><title-group><article-title>
 
 
  Spatial Correlation Characteristics Analysis of Multi-Beam Channels of Mobile Satellite System
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ziming</surname><given-names>Su</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiang</surname><given-names>Fei</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yuxin</surname><given-names>Cheng</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jianjun</surname><given-names>Wu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Institute of Advanced Communications, EECS, Peking University, Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>26</day><month>05</month><year>2017</year></pub-date><volume>10</volume><issue>05</issue><fpage>127</fpage><lpage>137</lpage><history><date date-type="received"><day>March</day>	<month>20,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>May</month>	<year>23,</year>	</date><date date-type="accepted"><day>May</day>	<month>26,</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   
   Due to the influence of scatterers around the receiving antenna, the multipath signal in satellite mobile communication systems is correlated with each other which would influence the system performance. There is no systematic standard on the channel modelling of the wideband satellite channel at present, so the study of the modelling of the wideband satellite channel is of great importance. In this paper, firstly we created a multi-beam model which can figure out the antenna gain of the nth component beam. Secondly, we combined the characteristics of multi-beam satellite channel and the distribution of the scatterers, and set up a three-dimension random channel model. This model is more realistic for satellite communication system since it considers the height of scatterers. According to the channel models, we had the formula of spatial correlation coefficient. We used the formula to calculate the relationship between spatial correlation coefficient and the interval of antennas. The result shows that the spatial correlation exists and cannot be ignored while modeling for mobile satellite system. 
  
 
</p></abstract><kwd-group><kwd>Satellite MIMO</kwd><kwd> Spatial Correlation</kwd><kwd> Multi-Beam</kwd><kwd> Scatterers</kwd><kwd> Channel Model</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The development of wideband multimedia service has raised demand of speed and spectrum efficiency of a new generation mobile-satellite communication system. In the condition of limitation of power, it is significant to make use of space resource to increase system performance. Under the influence of the distribution of scatterer near the receiver antenna, channel fading has spatial correlation in mobile-satellite communication system.</p><p>Compatible with LTE standard will be a trend for the new generation of mobile-satellite communication system. Because multiple-input multiple-output (MIMO) is an important part of LTE standard, the research of channel spatial correlation has certain reference value.</p><p>Currently, the commonly used classical satellite channel models are Loo model, Lutz model, Fontan model etc.</p><p>In terms of research regarding channel spatial correlation characteristics, a spatial Rayleigh-fading correlation model for MIMO has been proposed in [<xref ref-type="bibr" rid="scirp.76555-ref1">1</xref>]. This model assumes uniform distribution of the scatterers with respect to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x2.png" xlink:type="simple"/></inline-formula>, the angle-of-arrival (AOA) at the subscriber unit. The model also assumes that all received rays are equal in power, which is not a realistic assumption for multipath environments. An extension of this model for Rician-fading channels appeared in [<xref ref-type="bibr" rid="scirp.76555-ref2">2</xref>], which assumes von Mises angular distribution for scatterers.</p><p>Moreover, Mahmoud developed a geometrical based hyperbolic channel (GBHC) model for macrocells in [<xref ref-type="bibr" rid="scirp.76555-ref3">3</xref>]. A combination of the model in [<xref ref-type="bibr" rid="scirp.76555-ref3">3</xref>] and scalar stochastic fading model for local scatterers was presented in [<xref ref-type="bibr" rid="scirp.76555-ref4">4</xref>]. The GBHC model is a two-dimension model, which assumed that the scatterers are arranged circularly around the mobile station (MS), and the distances between the MS and scatterers are subject statistically to a hyperbolic distribution.</p><p>This paper mainly researches spatial correlation of multi-beam channels of mobile satellite system. Different from current spatial correlation research, we create a three-dimension channel model based on stochastic geometric model, which considers the height of scatterers, and deducts spatial correlation coefficient among channels with numeric calculation and analysis.</p></sec><sec id="s2"><title>2. Satellite Channel Model</title><sec id="s2_1"><title>2.1. Multi-Beam Model</title><p>Satellite multiple beam antenna (MBA) began to develop in the 1970s to 1980s. Single Feed per Beam (SFB) technology was adopted in the early stage. Later, multiple feeds per beam (MFB) technology was employed. Compared with phased-array antenna, feed beam of MBA is more narrow, and stronger. So the MBA has been widely used in satellite mobile communication systems in 1990s.</p><p>According to the structure, MBA can be divided to three categories: phased array antenna, reflector antenna and lens antenna. In this paper, we use reflector antenna to create multi-beam model.</p><p>As is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the distance of ground receiver to center of component beam is different, which makes the signal strength varies.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the space relationship among satellite, user u and component beam center n. h is the height of satellite orbit. R is radius of the earth.</p><p>According to <xref ref-type="fig" rid="fig2">Figure 2</xref>, suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x3.png" xlink:type="simple"/></inline-formula> is the angle of ground receiver u to satellite and component beam center n to satellite, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x4.png" xlink:type="simple"/></inline-formula>can be given by</p><disp-formula id="scirp.76555-formula119"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x5.png"  xlink:type="simple"/></disp-formula><p>where d<sub>Sn</sub> and d<sub>Su</sub> are the distance between satellite and component beam center n and user u respectively. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x6.png" xlink:type="simple"/></inline-formula>is the distance between sub-satellite point and user u.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Component beam schematic diagram</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76555x7.png"/></fig><p>Suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x8.png" xlink:type="simple"/></inline-formula> is the normalized far-field radiation pattern of component beam, the adoption of different radiation pattern results different antenna gain, when the direction angle is the same. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x9.png" xlink:type="simple"/></inline-formula>represents the antenna gain of the n<sup>th</sup> component beam. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x10.png" xlink:type="simple"/></inline-formula> can be written as</p><disp-formula id="scirp.76555-formula120"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x11.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x12.png" xlink:type="simple"/></inline-formula> can be calculated by (1), G<sub>max,n</sub> is the maximum gain of the n<sup>th</sup> component beam.</p></sec><sec id="s2_2"><title>2.2. Mobile Satellite Channel Model</title><p>In satellite communication, a signal is fading during propagation. Those fading may cause by environment and various attenuation facts, for instance cloud attenuation, rain attenuation and ionospheric scintillation. Taking into account this paper research mainly discusses spatial correlation, since attenuation facts like cloud attenuation and ionospheric scintillation are stay the same for a long time, we focus on the influence of ground environment near receiver, namely the multipath which arise from scattering, reflection, refraction or diffraction of the radiated energy off scatterers that lie in the environment.</p><p>For satellite communication, typically the height of the ground receiver is lower than nearby scatterers. The received signals in the both horizontal and</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Three-dimension component beam model</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76555x13.png"/></fig><p>vertical plane are distributed. While establishing the channel model, we need to consider the height of scatterers, so the traditional two-dimensional geometric channel model no longer applies. Assuming that scatterers are distributed in a right cylinder which has ground receiver as it bottom center, a three-dimension geometry channel model is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. A large picture of ground receiver in the model is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><p>For a downlink of satellite communication system, we assume that p and q are the number of satellite antennas, l and m are the number of ground antennas,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x15.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x14.png" xlink:type="simple"/></inline-formula>. N<sub>r</sub> and N<sub>r</sub> are the maximum number of transmitting antenna and receiving antenna. The received signal is given by</p><disp-formula id="scirp.76555-formula121"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x16.png"  xlink:type="simple"/></disp-formula><p>where, H(t) is channel impulse response, n(t) is noise. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x17.png" xlink:type="simple"/></inline-formula>represents convolution.</p><p>The received signal includes direct-path and multipath component in satellite communication system. So the channel impulse response is given by</p><disp-formula id="scirp.76555-formula122"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x18.png"  xlink:type="simple"/></disp-formula><p>where H<sub>loS</sub>(t) is impulse response of direct-path, H<sub>NLoS</sub>(t) is impulse response of multipath. H<sub>loS</sub>(t) and H<sub>NLoS</sub>(t) are both N<sub>T</sub> &#215; N<sub>R</sub> matrix. K is Rician Index, which describes ratio of direct-path power and multipath power (unit is dB). The value of K depends on angel of elevation from ground receiver to satellite, carrier frequency and environment around receiver. In this paper, since the interval between ground antennas is much small than shadow fading in different states, we</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> 3-Dimension geometry channel model</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76555x19.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Large picture of ground receiver</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76555x20.png"/></fig><p>can approximate that received signal shallow fading of two antennas are the same.</p><p>In the model shown in <xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref>, R<sub>m</sub> and R<sub>l</sub> are the m<sup>th</sup> and the l<sup>th</sup> antenna in ground receiver respectively, T<sub>p</sub> and T<sub>q</sub> are the p<sup>th</sup> antenna and the q<sup>th</sup> antenna in satellite respectively. x − y plane is parallel to horizontal surface, and is perpendicular to OO<sub>R</sub>. O<sub>R</sub> is the midpoint of two antennas R<sub>m </sub>and R<sub>l </sub>ground projection line. O<sub>S</sub> is the point of intersection of x axis and y axis and also the midpoint of x − y plane projection line of two antennas T<sub>p</sub> and T<sub>q</sub>. O<sub>T</sub> is the center of transmitting antenna array. H<sub>S,max</sub> is the maximum height of scatterers distribution. R<sub>S,max</sub> is the maximum range of scatterer distribution (the maximum radius). <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula> represent projection of T<sub>p</sub> and T<sub>q</sub> in x − y plane respectively. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula>is the angle between projection of transmitting antennas array <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula> and x axis. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula>is the angle of receiving antennas array R<sub>m</sub> R<sub>l</sub> and x axis. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x27.png" xlink:type="simple"/></inline-formula>is the angle of R<sub>m </sub>R<sub>l</sub> and x − y plane. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x28.png" xlink:type="simple"/></inline-formula>is the angle between segment of receiving antenna arrays and satellite and x-y plane, namely the elevation. d<sub>T</sub> and d<sub>R</sub> is the distance of adjacent antenna on satellite and ground respectively. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x29.png" xlink:type="simple"/></inline-formula>is the central angle between sub-satellite point and receiver antenna. To facilitate the analysis, d<sub>a→b</sub> represent distance of a and b. the distance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x30.png" xlink:type="simple"/></inline-formula> and O<sub>R</sub> is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x31.png" xlink:type="simple"/></inline-formula>. And the distance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x32.png" xlink:type="simple"/></inline-formula> and O<sub>T</sub> is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x33.png" xlink:type="simple"/></inline-formula>.</p><p>According to the model, the impulse responses of sub channel from T<sub>p</sub> to R<sub>l </sub>can be written as</p><disp-formula id="scirp.76555-formula123"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x34.png"  xlink:type="simple"/></disp-formula><p>Since the large number of hypothetical scatterers in the model, let S<sub>n</sub> be the n<sup>th</sup> scatterer. Let R<sub>S,max</sub> and H<sub>S,max</sub> represent the radius and height of cylinder in the model, namely, the maximum distance and height of scatterers distribution. R<sub>S(n)</sub> is the distance between O<sub>R</sub> and S<sub>n</sub> projection in x-y plane,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula>. H<sub>S</sub><sub>(n)</sub> is the height of S<sub>n</sub>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x36.png" xlink:type="simple"/></inline-formula>. Without considering the height of ground antennas, the n<sup>th</sup> scatterer elevation in scattering path can be approximately shown as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x37.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x38.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x39.png" xlink:type="simple"/></inline-formula> respectively describe the leaving angle and arriving angle of the n<sup>th</sup> path, which is influenced by S<sub>n</sub>. In the model, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x40.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x41.png" xlink:type="simple"/></inline-formula>, R<sub>S</sub><sub>(n)</sub>, H<sub>S</sub><sub>(n)</sub> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x42.png" xlink:type="simple"/></inline-formula> are all random variables.</p><p>In multi-beam channels of mobile satellite system, the impulse responses of sub <sub>channel</sub> from T<sub>p</sub> to R<sub>l</sub> can be written in terms of (5). Considering the influence from component beam on to received signal, the direct-path component of the channel response can be written as</p><disp-formula id="scirp.76555-formula124"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x43.png"  xlink:type="simple"/></disp-formula><p>And multipath component of the channel response can be written as</p><disp-formula id="scirp.76555-formula125"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x44.png"  xlink:type="simple"/></disp-formula><p>For the large number of scatterers, according to Central Limit Theorem, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x45.png" xlink:type="simple"/></inline-formula>is a deterministic process. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x46.png" xlink:type="simple"/></inline-formula>is a complex Gaussian process with a low-pass nonzero mean, and its envelop <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x47.png" xlink:type="simple"/></inline-formula> consistent with Rayleigh distribution.</p><p>In (6), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x48.png" xlink:type="simple"/></inline-formula>is gain of satellite antenna p. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x49.png" xlink:type="simple"/></inline-formula>is angle that ground antenna l deviates from beam center p. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x50.png" xlink:type="simple"/></inline-formula>is gain of ground antenna l. Generally, ground antenna is omnidirectional antenna, so<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x51.png" xlink:type="simple"/></inline-formula>.</p><p>In (7), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x52.png" xlink:type="simple"/></inline-formula>is the n<sup>th</sup> multipath component random phase. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x53.png" xlink:type="simple"/></inline-formula>is carrier frequency. A (n) is the amplitude of multipath component which is influenced by the n<sup>th</sup> scatterer. K<sub>pl</sub> represents sub-channel Rician Index from T<sub>p</sub> to R<sub>l</sub>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x54.png" xlink:type="simple"/></inline-formula>.</p></sec></sec><sec id="s3"><title>3. Multi-Beam Spatial Correlation Characteristics</title><sec id="s3_1"><title>3.1. Definition of Spatial Correlation</title><p>In the early stage of channel research, multi-antenna technology will get a huge channel capacity upgrade in the independent and identically distributed (iid) Rayleigh channel [<xref ref-type="bibr" rid="scirp.76555-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.76555-ref6">6</xref>], under the assumption that the interval between the antennas is large enough and the angle of arrival (AOA) angular spread is sufficiently large. However, in an actual mobile communication system, the angular spread of the received signal AOA is not large enough under the affection of the interval among antennas and scatterers distribution around. It results that the fading of received signal among different antennas and the signal received among the same antenna from different transmitting antenna are not statistically independent. So the correlation exists. This correlation is called by spatial correlation, its definition is written as</p><disp-formula id="scirp.76555-formula126"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x55.png"  xlink:type="simple"/></disp-formula><p>where p and q are two transmitting antennas. l and m are two receiving antennas. h<sub>pl</sub>(t) represents channel response of antenna p to l. In the same way, h<sub>qm</sub>(t) represents channel response of antenna q to m. E[•] is expectation. ρ<sub>pl,qm</sub> is correlation coefficient between received signal of antenna l and m.</p></sec><sec id="s3_2"><title>3.2. Analysis of Multi-Beam Spatial Correlation</title><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x56.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x57.png" xlink:type="simple"/></inline-formula> are both zero-mean random process (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x58.png" xlink:type="simple"/></inline-formula>),<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x59.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x60.png" xlink:type="simple"/></inline-formula> are deterministic process, can be written as</p><disp-formula id="scirp.76555-formula127"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x61.png"  xlink:type="simple"/></disp-formula><p>According to the model shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The spatial correlation coefficient of direct-path component is</p><disp-formula id="scirp.76555-formula128"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x62.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x63.png" xlink:type="simple"/></inline-formula>, which is described the distance of transmitting antenna p and q. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x64.png" xlink:type="simple"/></inline-formula>is the distance of receiving antenna m and l.</p><p>Also, the spatial correlation coefficient of multipath component is</p><disp-formula id="scirp.76555-formula129"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x65.png"  xlink:type="simple"/></disp-formula><p>Since the large number of scatterers around ground receiver antennas (a larger number N), R<sub>S</sub>, H<sub>S</sub> and α<sub>R</sub><sub> </sub>can replace the discrete variables R<sub>S(n)</sub>, H<sub>S(n)</sub> and α<sub>R,n</sub> as an approximation. (11) can change into integral form</p><disp-formula id="scirp.76555-formula130"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x66.png"  xlink:type="simple"/></disp-formula><p>R<sub>S</sub>, which is the distance of scatterer and ground receiver, can be described by hyperbolic distribution [<xref ref-type="bibr" rid="scirp.76555-ref4">4</xref>]. The height of scatterer H<sub>S</sub>, which PDF depends on environment around receiver, is normally described by normal distribution [<xref ref-type="bibr" rid="scirp.76555-ref7">7</xref>], Lon-normal distribution [<xref ref-type="bibr" rid="scirp.76555-ref8">8</xref>] etc. The normal distribution is used for modeling in this paper. In ground wireless communication system, the arrival angle of multipath signal is described by evenly distribution [<xref ref-type="bibr" rid="scirp.76555-ref9">9</xref>] or Laplace distribution. But in mobile satellite communication system, Laplace distribution is more suitable under testing in urban area [<xref ref-type="bibr" rid="scirp.76555-ref10">10</xref>], which is affected by the number and the distribution of scatterers around ground receiver.</p><p>When the arrival angle of received signal in x-y plane α<sub>R</sub> is Laplace distribution, the spatial correlation coefficient of multipath component in the received signal is shown as</p><disp-formula id="scirp.76555-formula131"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x67.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x68.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x69.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x70.png" xlink:type="simple"/></inline-formula> are given by (14)</p><disp-formula id="scirp.76555-formula132"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/76555x71.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s4"><title>4. Numeric Results and Analysis</title><p>In this part, the channel spatial correlation coefficient of the signal received by ground antennas is obtained by numeric calculation in multi-beam satellite communication system, which adopt parabolic reflector antenna. All the parameters of simulation are given in <xref ref-type="table" rid="table1">Table 1</xref>, if not specified otherwise.</p><p>The calculation is on the assumption of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x72.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x73.png" xlink:type="simple"/></inline-formula>, which is the angle between component beam p to ground receiver and and carrier frequency is 2 GHz.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows that in term of n<sub>T</sub> = 2, n<sub>R</sub> = 1, the relationship between ground spatial correlation coefficient among three Chinese cities, namely Mohe, Beijing and Shanghai, and the interval of satellite antennas.</p><p>As shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, with the increase of the antenna interval, spatial correlation coefficient among satellite channel showed a decreasing trend, and the higher the latitude, the slower decline.</p><p>Take Beijing as example, let K = 4 dB, <xref ref-type="fig" rid="fig6">Figure 6</xref> shows the relationship among the interval of satellite antennas, ground antennas, and the spatial correlation</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Relationship between the component beam correlation coefficient and the interval of satellite antennas</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76555x74.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Relationship among the interval of antennas and spatial correlation coefficient</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/76555x75.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Simulation parameter</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameter</th><th align="center" valign="middle" >Description</th><th align="center" valign="middle" >Value</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/76555x76.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >Wavelength</td><td align="center" valign="middle" >15 cm</td></tr><tr><td align="center" valign="middle" >f</td><td align="center" valign="middle" >Focal length</td><td align="center" valign="middle" >7.443 m</td></tr><tr><td align="center" valign="middle" >D</td><td align="center" valign="middle" >Diameter of projection plane</td><td align="center" valign="middle" >12.5 m</td></tr><tr><td align="center" valign="middle" >H</td><td align="center" valign="middle" >Bias height</td><td align="center" valign="middle" >2.607 m</td></tr><tr><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Number of feeds</td><td align="center" valign="middle" >37</td></tr><tr><td align="center" valign="middle" >K</td><td align="center" valign="middle" >Rician Index</td><td align="center" valign="middle" >7 dB</td></tr></tbody></table></table-wrap><p>coefficient. With the interval increasing, spatial correlation coefficient showed a decreasing trend, but when the interval is small, the spatial correlation coefficient is still large.</p></sec><sec id="s5"><title>5. Summary/Conclusion</title><p>In this paper, considering that the radio transmission feature and the antenna array feature the affection influence the spatial correlation coefficient, we create a 3-demension channel model. According to the model, we derive the spatial correlation coefficient among component beam which received by ground receiver with numeric calculation and analysis. The result shows that spatial correlation coefficient is still large even if the interval of antennas is small. Therefore, the spatial correlation coefficient cannot be ignored in satellite channel research.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This work is supported by the National Natural Science Foundation of China (No.61371073).</p></sec><sec id="s7"><title>Cite this paper</title><p>Su, Z.M., Fei, X., Cheng, Y.X. and Wu J.J. (2017) Spatial Correlation Characteristics Analysis of Multi-Beam Channels of Mobile Satellite System. Int. J. Communications, Network and System Sciences, 10, 127-137. https://doi.org/10.4236/ijcns.2017.105B012</p></sec></body><back><ref-list><title>References</title><ref id="scirp.76555-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">G.Grillo, Shiu, D.S., Foschini, G.J., Gans, M.J. and Kahn, J.M. (2000) Fading Correlation and Its Effect on the Capacity of Mul-tielement Antenna Systems. 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