<?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>Int'l J. 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.2014.77025</article-id><article-id pub-id-type="publisher-id">IJCNS-48123</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>Amplify and Forward Relaying Systems for Collocated Antennas</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mahmud</surname><given-names>Al-Naser</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Salem</surname><given-names>Salamah</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Electronic Engineering Technology, Public Authority of Applied Education and Training, Al Shuwaik, Kuwait</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mj.alnaser@paaet.edu.kw(MA)</email>;<email>sh.salamah@paaet.edu.kw(SS)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>07</month><year>2014</year></pub-date><volume>07</volume><issue>07</issue><fpage>235</fpage><lpage>242</lpage><history><date date-type="received"><day>22</day>	<month>May</month>	<year>2014</year></date><date date-type="rev-recd"><day>22</day>	<month>June</month>	<year>2014</year>	</date><date date-type="accepted"><day>10</day>	<month>July</month>	<year>2014</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>
	Cooperative relaying for a system that consists of different
configurations of a collocated and uniform linear antenna is analyzed. The amplify-and-forward
relaying (AF) and selection combining (S-AF) schemes based on maximal ratio
combining (MRC) method for single- and multi-relay are investigated. In this
study, the bit-error-rate (BER) expression for collocated and uniform linear
antenna in cooperative communication system over flat Rayleigh fading channel
is derived. The result for 3-element collocated antennas (tripole) shows
improvement in performance over dual-polarized antennas. Also increasing number
of tripole antenna does not add improvement.
</p></abstract><kwd-group><kwd>Cooperative Communications</kwd><kwd> Fading Channels</kwd><kwd> Relay</kwd><kwd> Antennas</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Relay systems have been widely investigated in wireless communications as a way to overcome deep fading and therefore enhance signal quality in multi-path fading channels. In relaying network we have a two-hop link where the signal is transmitted in the first hop from a source to a relay node and in the second hop the signal at the relay node is retransmitted to the destination. At the same time, the source will transmit another copy of the signal directly to the destination. Therefore, the signal is transmitted from the source directly and via a relay node, so, the destination will receive the transmitted signal from two links referred as source-relay-destination and source-destination link. Now the signal received at the relay is forwarded to the destination by implementing two schemes known as amplify forward (AF) and decode forward (DF) [<xref ref-type="bibr" rid="scirp.48123-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.48123-ref3">3</xref>] . In AF, the received signal at relay is amplified and re-transmitted. In DF, the received signal at relay is decoded then retransmitted again to destination. Earlier research was focused on employing single- and multi-antenna system for cooperative diversity technique to exploit fading channels [<xref ref-type="bibr" rid="scirp.48123-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.48123-ref4">4</xref>] . In [<xref ref-type="bibr" rid="scirp.48123-ref3">3</xref>] , the symbol error probability was derived for dual hop with single antenna in Rayleigh and Nakagami m-fading channels and the outage performance of communication system was investigated for AF and DF relaying network. Cooperative communication for a multi-relay network with multiple-input multiple-output network to exploit spatial diversity is investigated in [<xref ref-type="bibr" rid="scirp.48123-ref4">4</xref>] . Here, the relays and users cooperate in sharing information which in turn increases capacity and coverage area of wireless communications. Other techniques utilizing relays equipped with multi-antennas and multi-relay network are investigated where an infrastructure-based relaying deploying multi-antennas on a relay is presented in the work of Adinoyi et al. [<xref ref-type="bibr" rid="scirp.48123-ref5">5</xref>] . To decrease number of relay nodes and thus reducing cost, a single antenna is deployed at source and destination while multi-antennas are fixed on receiver side of relays. The receiver criterion is based on threshold relaying with MRC and selection combining. Also cooperative communication is studied when relay selection scenario applied for the best relay link. It was shown that selection relaying can achieve same diversity order as AF [<xref ref-type="bibr" rid="scirp.48123-ref6">6</xref>] -[<xref ref-type="bibr" rid="scirp.48123-ref8">8</xref>] . Furthermore, deploying multi-antennas at the source or relays receiver side shows improvement as number of antennas increased from 1 to 2 for high and low SNR but increasing antennas more than 2, did not add significant improvement in performance at high SNR [<xref ref-type="bibr" rid="scirp.48123-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.48123-ref10">10</xref>] .</p><p>Since future wireless system trends require wireless terminals small in size, the advantage of using multiple antennas at a relay node will be limited by the space separation between antennas and thus correlation of wireless terminals will affect the system performance. In this paper the study of cooperative communication is applied for collocated antennas known as “vector antenna” (VA) implemented at a relay node over independent and identically distributed Rayleigh fading channels. Vector antenna can independently detect or excite all six EM field components enabling the communication system to access additional signaling dimensions, which may enhance performance in the same way as antenna arrays [<xref ref-type="bibr" rid="scirp.48123-ref11">11</xref>] . These extra dimensions can provide additional diversity to combat signal fading, allow the system to spatially leverage bandwidth by transmitting multiple separable signals in the same bandwidth, and improve the suppression of interference in a multiuser environment. Also, “tripole” antenna that consists of three mutually-orthogonal dipoles by Andrew et al. [<xref ref-type="bibr" rid="scirp.48123-ref12">12</xref>] have shown through simulation, that this antenna improves on the capacity of scalar and dual-polarized antennas for a simple propagation example involving a line-of-sight component and one reflected path. The end-to-end performance for a relay network employing vector and ULA antennas based on MRC are investigated and using AF and selection schemes and an expression for bit error rate for BPSK is derived. Since we are investigating the advantage of collocated antennas in relay network, AF and selection schemes are selected.</p><p>The organization of this paper is as follows: in Section 2 the system model is introduced for VA and ULA in a relay network and the output SNR is analyzed. In Section 3 the BER analysis for AF and S-AF schemes is presented. Finally, simulation of the system presented is compared with theoretical values of the equation derived.</p></sec><sec id="s2"><title>2. System Model</title><p>BPSK modulation is considered for a relay communication network that consists of two-hop channel as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. In the first hop signals are transmitted from a single linear antenna at the source to the receiver side of relay node and in the second hop the received signal is transmitted from the transmitter side of relay node to the destination. The receiver side of the relay node is equipped with a vector antenna and the transmitter side with a uniform linear antenna. The source and destination nodes will use a single linear antenna. The channel assumed to be flat fading slowly time varying and the direct link from source to destination is considered only in S-AF.</p><p>For a single vector antenna at the receiver side of relay node, each arriving multipath component is a two- dimensional vector<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\192037c4-4a77-43c2-b5d9-3b2d524f31e7.png" xlink:type="simple"/></inline-formula>, consist of horizontally and vertically polarized components of the electric field. For narrowband sinusoidal signals, it is convenient to write the signal in terms of its complex envelope Z, where</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\58d4a61e-996d-4a68-8c39-f6b244743eaa.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\485fef09-ff3f-4c59-8db6-c949389f327e.png" xlink:type="simple"/></inline-formula> is the carrier frequency. For any polarized signal, the complex envelope</p><p>can be written as</p><disp-formula id="scirp.48123-formula1034"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\beca2258-6a33-434a-a7fa-3e05cb8dd701.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\d8055155-90ad-4311-a565-d4c74f2755d5.png" xlink:type="simple"/></inline-formula> are the amplitude, phase, orientation angle, and ellipticity angle, respectively [<xref ref-type="bibr" rid="scirp.48123-ref13">13</xref>] . Since the signal is a function of the transmitted data, the amplitude, phase and polarization angles vary with time, and</p><fig id="fig1"><label>Figure 1</label><caption><p> Multi-relays system with vector antenna and ULA</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\d8ef2728-af11-49ae-8665-18177e6302c9.png"/></fig><p>we write<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\218eb50a-d590-4f67-bf61-e83876d738e8.png" xlink:type="simple"/></inline-formula>.</p><p>If the multipath component is reflected or scattered by an object in the far field, then the signal can be approx- imated as a plane wave at the receiver and suppose that the multipath component arrives at the sensor from the direction<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\a88890d8-d0d4-4cef-8ea5-efd6e4826b17.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.48123-formula1035"><label>(2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\cead29de-6def-4e3f-9a84-2ed781ba04fb.png"/></disp-formula><p>nonconductive, homogeneous, and isotropic medium, the received signal can be modeled by [<xref ref-type="bibr" rid="scirp.48123-ref13">13</xref>]</p><disp-formula id="scirp.48123-formula1036"><label>(3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\8c5d230f-7258-4db0-893f-92caf4858500.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\cbe9e9e2-35e6-4dcc-8777-06a561c45b97.png" xlink:type="simple"/></inline-formula> represents thermal noise, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\f9976788-fed8-4777-b0a5-88ede38252fa.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\020197fc-6aea-44f2-940c-479732c43def.png" xlink:type="simple"/></inline-formula> denote the three-dimensional complex envelopes of the electric and magnetic field vectors respectively at the receiver, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\431e1686-a835-4a2f-87a2-03bdb1803b8e.png" xlink:type="simple"/></inline-formula>is the intrinsic impedance of the propagation medium, and</p><disp-formula id="scirp.48123-formula1037"><label>(4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\7dcb1ce8-cd5b-4b89-b143-c41411bdff24.png"/></disp-formula><p>The <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\dd81b23f-6168-4043-b8b6-a211cd7a42f6.png" xlink:type="simple"/></inline-formula> vector antenna system will be used to detect information signal at receiver in the relay system of interest. The transmitted signal of a complex baseband signal of the form</p><disp-formula id="scirp.48123-formula1038"><label>(5)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\a6641d7f-90ab-47ef-b3dd-e4ae63d7fc91.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\e5748183-0b79-4db9-8c3b-aaa0366bd63b.png" xlink:type="simple"/></inline-formula> is a sequence of transmitted information bits. When <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\6113eb33-ff89-47f6-a23c-5d45a39ae827.png" xlink:type="simple"/></inline-formula> is transmitted, the horizontally and vertically polarized components of each multipath component consist of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\88f945ee-7c66-4c51-b318-6385ab04409b.png" xlink:type="simple"/></inline-formula> with some amplitude and phase shift, so that <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\e95db342-7d9e-4ade-8413-ad9ef6cacc13.png" xlink:type="simple"/></inline-formula> for some fixed complex vector <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\0382aefd-cdfc-4d06-938b-3fbe05267ac1.png" xlink:type="simple"/></inline-formula> Then the received signal can be written as</p><disp-formula id="scirp.48123-formula1039"><label>(6)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\823f3dab-2043-4bf6-bc80-7aad2b539c78.png"/></disp-formula><p>with relay system notation, we can write the received signal from source to relay to be</p><disp-formula id="scirp.48123-formula1040"><label>(7)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\7b5aad20-cfe9-4d05-81e4-f747fff2338c.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\06194075-839b-4e19-bd97-636d7ea61659.png" xlink:type="simple"/></inline-formula> is number of relays and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\3a7711eb-6a96-488e-9ec0-ca40a1c72091.png" xlink:type="simple"/></inline-formula> is the transmitted power for the source and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\04a44051-7eec-49ca-956b-0fa9b64176ee.png" xlink:type="simple"/></inline-formula> reflects the change in amplitude, phase, and polarization experienced by the fading component as it propagates from the source to relay. The noise <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\932f09c2-c29b-45e2-ab29-b90dbdb117df.png" xlink:type="simple"/></inline-formula> is zero-mean complex Gaussian vector with covariance<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\24fb6e13-42c2-4534-8fff-97687224e87f.png" xlink:type="simple"/></inline-formula>. With abuse of notation we can write above equation at relay as</p><disp-formula id="scirp.48123-formula1041"><label>(8)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\91784445-6e1d-4b77-a548-68b60647e3d5.png"/></disp-formula><p>where each of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\15eaa6f7-252d-4ffb-8dba-c838322f2253.png" xlink:type="simple"/></inline-formula> consists of the appropriate <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\c9d1e527-868a-4949-a6ca-dc6900de8ff9.png" xlink:type="simple"/></inline-formula> components of<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\669fdb7f-e5f7-4b10-afec-eb9d9880c4c3.png" xlink:type="simple"/></inline-formula>. The components of the vector <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\3af281c1-b034-4bed-b5fd-0afa66e9b1d0.png" xlink:type="simple"/></inline-formula> are modeled as i.i.d. zero-mean complex Gaussian random variables and therefore the elements of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\843f6977-c7e1-4d78-ab65-34beda1b2c3b.png" xlink:type="simple"/></inline-formula> are also zero-mean complex Gaussian random variables. The output of MRC at the relay is given by:</p><disp-formula id="scirp.48123-formula1042"><label>(9)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\6d44e69f-f4ea-4203-829e-3c310aa2397a.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\6c84257a-a743-45d9-b40e-a08fde9f7409.png" xlink:type="simple"/></inline-formula> is the SNR of the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\dcbe43f0-b171-47f9-9d31-81eadc026ce5.png" xlink:type="simple"/></inline-formula> relay. The noise <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\dd39d7f4-2a48-42ba-a7e9-d4d437fb9f4a.png" xlink:type="simple"/></inline-formula> is white and assuming equal SNR on all branches. The received signal from <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\da6aff94-fe8c-4b55-9369-fd56d26e9b37.png" xlink:type="simple"/></inline-formula> relay at destination</p><disp-formula id="scirp.48123-formula1043"><label>(10)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\674e5e84-b10c-44c5-ba0a-e2b526e2bc4b.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\0590ed85-99a5-44e5-8cb3-3d0618ac03f2.png" xlink:type="simple"/></inline-formula> is the channel gain from relay node to destination and the gain at the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\1b7b121e-9b97-4ec5-8c0a-abd5e38b70f1.png" xlink:type="simple"/></inline-formula> relay can be written as</p><disp-formula id="scirp.48123-formula1044"><label>(11)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\1cbd36a2-93f8-4ea5-86cd-14a8fedf2af0.png"/></disp-formula><p>The noise <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\4306129d-63ec-45a7-aeed-073ff4b5b5d9.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\816b079c-2ad7-461e-8c33-21d4af2bea1f.png" xlink:type="simple"/></inline-formula> are additive-white-Gaussian noise (AWGN) with zero mean and variance <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\6cd72fc0-b3b4-432a-86fe-e55c1ff44f64.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\9407a278-44cc-424e-83d4-c9c5f82bf9af.png" xlink:type="simple"/></inline-formula> is the transmitted power at the relay. At destination the receiver employ a maximal ratio combining algorithm and the received end-to-end SNR is given by</p><disp-formula id="scirp.48123-formula1045"><label>(12)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\acbe0405-9604-4474-8aab-5626ced2291b.png"/></disp-formula><p>The output SNR at destination can be re-written as</p><disp-formula id="scirp.48123-formula1046"><label>(14)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\05a631db-2c3a-4626-9f3f-223a8fd6542a.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\4fa6575e-ee90-4774-afd6-b65264b63a20.png" xlink:type="simple"/></inline-formula> is the SNR at <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\fd945394-a1b3-41a0-b75a-3cc912316d17.png" xlink:type="simple"/></inline-formula> relay and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\f8e1c5d2-f3bd-4f85-845f-7c11849c5360.png" xlink:type="simple"/></inline-formula> is the SNR at destination from</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\fd1c2f41-a372-4e40-8a8e-97f37dd6aaaa.png" xlink:type="simple"/></inline-formula>relay. The SNR <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\7aba2f20-53fd-4a3c-8518-dccdd3194511.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\cd9ff1a5-463c-4250-9ebd-5daea310e8f2.png" xlink:type="simple"/></inline-formula> are independent and identically distributed. Since the SNR is not mathematically tractable hence for high SNR it can be upper bounded by</p><disp-formula id="scirp.48123-formula1047"><label>(15)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\8d0eb2c6-62c9-48e5-b2bc-e7566c634f01.png"/></disp-formula><p>To simplify the analysis, the noise is ignore at the relay gain. The output SNR of MRC at relay for tripoleatenna is exponentially distributed and follows the Gamma distribution with probability density function pdf given by</p><disp-formula id="scirp.48123-formula1048"><label>(16)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\162877c4-59f5-4cf0-83e1-5b7bce2e632e.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\51dab681-59ae-415f-a16f-cef739263800.png" xlink:type="simple"/></inline-formula> is number of tripole antennas at the relay and the pdf of SNR at destination is given by:</p><disp-formula id="scirp.48123-formula1049"><label>(17)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\91a3a837-78ab-4157-8c43-e53a2fd4b776.png"/></disp-formula><p>Now using the results in [<xref ref-type="bibr" rid="scirp.48123-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.48123-ref10">10</xref>] , the moment generation function of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\75723322-e925-4065-be9d-395127362cb1.png" xlink:type="simple"/></inline-formula> is given by:</p><disp-formula id="scirp.48123-formula1050"><label>(18)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\4161b80c-eb38-43d5-9434-286bb3868552.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\e0e2bdcb-1999-4381-9d04-b460eb26f395.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. Error Rate Analysis</title><sec id="s3_1"><title>3.1. Amplify Forward (AF)</title><p>Assuming independent of<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\ed7f8fe2-28f8-43bb-8fdf-0c1305fb2fe4.png" xlink:type="simple"/></inline-formula>, the bit error rate can be derived based on MGF approach in [<xref ref-type="bibr" rid="scirp.48123-ref14">14</xref>] that can be written as</p><disp-formula id="scirp.48123-formula1051"><label>(19)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\b209e72d-f32e-427e-adc6-c4de1242184a.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\2f3fea8c-7b74-49dd-bbb7-da560fa7840e.png" xlink:type="simple"/></inline-formula> for BPSK modulation and independent of<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\d53327f1-8362-4ab6-8999-0114db4c0989.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3_2"><title>3.2. Selective Amplify Forward (S-AF)</title><p>For S-AF only the best relay which contributes most to received SNR is chosen for re-transmission. The received SNR can be expressed as</p><disp-formula id="scirp.48123-formula1052"><label>(20)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\1654ddf3-21bc-471a-a438-77de1f741986.png"/></disp-formula><p>The received SNR for S-AF can be written as</p><disp-formula id="scirp.48123-formula1053"><label>(21)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\f6628f95-d8da-41c0-b6b9-611be0866da5.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\2cf83e4a-fa32-4cad-82b1-6da1ecc13c18.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\99038660-a160-4ff0-975f-a4294f12b52d.png" xlink:type="simple"/></inline-formula>. At high SNR region, using the result</p><p>in [<xref ref-type="bibr" rid="scirp.48123-ref6">6</xref>] for approximation of cumulative distribution function (CDF) of the received SNR for S-AF scheme, the CDF for tripole antenna is given by</p><disp-formula id="scirp.48123-formula1054"><label>(22)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\3a3c9fd9-a60e-49d1-a6d2-adc0a785a5fa.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\3a8870c1-4a78-4ed9-b3ff-7ec7e3a2cc54.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\4ce367c2-4223-47e0-aa42-ed7f38df2dbe.png" xlink:type="simple"/></inline-formula> is exponentially distributed with pdf<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\9d9bbb2d-1710-40c3-8e9e-e7ee05e0aaae.png" xlink:type="simple"/></inline-formula>. Substituting Equation (22)</p><p>in <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\90402df8-d416-43de-94dc-27565a25aa97.png" xlink:type="simple"/></inline-formula> [[<xref ref-type="bibr" rid="scirp.48123-ref6">6</xref>] , equation (6)] and using<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\ea1cff86-a8eb-4c24-b7f5-05ab6b781638.png" xlink:type="simple"/></inline-formula>. The high SNR approximation</p><p>can be written as</p><disp-formula id="scirp.48123-formula1055"><label>(23)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\70f6fde6-e181-4773-b1dc-b3bc18319ccf.png"/></disp-formula></sec></sec><sec id="s4"><title>4. Simulation Results</title><p>In this section, simulation and theoretical results of cooperative communication for AF and S-AF schemes presented. We assume that the multipath components of the received signals are uniformly distributed on a sphere</p><p>where the azimuth angle <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\1c0ff422-cb7a-462e-adff-3f37b0e9dc34.png" xlink:type="simple"/></inline-formula> are i.i.d. and uniform on<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\62df55ac-227f-4af3-8ebd-c79ee48070aa.png" xlink:type="simple"/></inline-formula>, and the elevation angles <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\af3ffeb5-416c-43a9-a48d-c40e7b97768d.png" xlink:type="simple"/></inline-formula> are i.i.d. with</p><p>probability density function</p><disp-formula id="scirp.48123-formula1056"><label>(24)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\621e9e91-0671-4d92-a606-1ca619fa709d.png"/></disp-formula><p>and the polarizations <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\4ebd6ffc-3cb0-4214-9881-0c9c524e3d50.png" xlink:type="simple"/></inline-formula> are i.i.d. CN(0, I). The noise <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\2194b8f1-9666-4d0d-9d83-1a9da2b5bebf.png" xlink:type="simple"/></inline-formula> is spatially and temporally white and Gaussian</p><p>(i.e.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\aed4f8a3-020f-400a-83f4-ec792aac4694.png" xlink:type="simple"/></inline-formula>). The fading channel is assumed to be a flat fading Rayleigh channel. The trans-</p><p>mitted power for all participate scheme on each relay is<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\2c68b017-e4e6-4e06-9ca8-e2e63e3907c2.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\43ef3542-ea5e-430e-9e17-9555c3c5a481.png" xlink:type="simple"/></inline-formula> is the relay number and total</p><p>transmitted power<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\89a6d12d-4afc-4c96-aac7-d3ed37d7b3da.png" xlink:type="simple"/></inline-formula>. In selective scheme, the transmitted power for each relay is<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\7c98d022-ac8c-404f-a1d8-d7688fcaac95.png" xlink:type="simple"/></inline-formula>. The antenna setting in all simulation will be based on the following setting: the source, destination and transmitter side of the relay will employ ULA while the receiver side relay will have vector antenna that consist of either dual, tripole or 6-element antennas as specified in the figures below.</p><p>In <xref ref-type="fig" rid="fig2">Figure 2</xref>, the results are plotted for 1, 2 and 3 relays where each relay will assume a single tripole antennas. Simulation and theoretical BER are compared. The figure shows that as number of relays increase, BER will decrease and therefore increase of diversity gain. On the other hand the theoretical results came in a very close approximation to our simulation. In <xref ref-type="fig" rid="fig3">Figure 3</xref>, the results shows an increase in the number of tripole antennas on</p><fig id="fig2"><label>Figure 2</label><caption><p> BER for tripole antenna with multi-relays</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\e87e30df-ac03-46e7-9702-0a95e70f704a.png"/></fig><fig id="fig3"><label>Figure 3</label><caption><p> BER simulation for tripole antenna at single and mul- ti-relays</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\5748f9a7-3751-4123-8a7b-beee5492e74a.png"/></fig><p>a relay did not add gain in diversity to the relay system while multi-relay network with single triple antenna would give us significant improvement.</p><p>In <xref ref-type="fig" rid="fig4">Figure 4</xref>, simulation of 2, 3 and 6-element collocated antenna for one relay are compared. The results show that a 2 dB gain at low SNR region for 6 over 2 elements collocated antennas but no gain is noticed in the high SNR region. In <xref ref-type="fig" rid="fig5">Figure 5</xref>, selective relaying simulation for 2 and 3 relay network is presented. The relay with highest SNR is chosen where each relay is equipped with one tripole antennas. As the number of relays increased, diversity improve and on the same figure BER for selection is compared with all participate scheme. The results show that selection (S-AF) outperforms AF scheme in all cases considered.</p></sec><sec id="s5"><title>5. Conclusion</title><p>The study of cooperative communication for collocated antennas setting employed at relay node and ULA at source and destination is investigated. Two schemes of relaying network known as AF and S-AF are presented and closed form BER for tripole antennas is derived. The theoretical and simulation results are compared for one- and multi-relay network. Results shows that tripole antenna outperformed the dual antenna case and the 6-</p><fig id="fig4"><label>Figure 4</label><caption><p> BER simulation for 2, 3 and 6 collocated antennas at single relay</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\87fca7c6-980a-4018-9822-f967509f961b.png"/></fig><fig id="fig5"><label>Figure 5</label><caption><p> BER Simulation for selective vs AF for tripole and <img src="htmlimages\4-9701888x\e2dc42d6-3f43-4162-b257-2abb86259f4b.png" width="85.3750038146973" height="31.875" /> relay</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\4-9701888x\9a7382bf-900d-4a52-8d76-22b7a8aa9730.png"/></fig><p>element vector antenna can add more gain in low SNR region over tripole case. 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