<?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">CN</journal-id><journal-title-group><journal-title>Communications and Network</journal-title></journal-title-group><issn pub-type="epub">1949-2421</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/cn.2013.54040</article-id><article-id pub-id-type="publisher-id">CN-39588</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>
 
 
  Direction of Arrival Estimation under Spread Spectrum Reference Signal Assisted Radio
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>heodoros</surname><given-names>N. Kaifas</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Physics, Aristotle University, Thessaloniki, Greece</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>tkaif@physics.auth.gr</email></corresp></author-notes><pub-date pub-type="epub"><day>14</day><month>11</month><year>2013</year></pub-date><volume>05</volume><issue>04</issue><fpage>323</fpage><lpage>327</lpage><history><date date-type="received"><day>September</day>	<month>25,</month>	<year>2013</year></date><date date-type="rev-recd"><day>October</day>	<month>22,</month>	<year>2013</year>	</date><date date-type="accepted"><day>October</day>	<month>30,</month>	<year>2013</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>
 
 
  In the present work, a direction of arrival estimator
  ,
   under spread spectrum reference 
  of 
  signal
  -
  assisted radio operating in a Rayleigh fading channel
  ,
   is proposed. The analysis, which 
  is 
  appl
  ied
   
  to
   general receiver antenna array conf
  i
  gur
  a
  tions, demonstrate
  s
   the high performance of the estimator which is due to the double dispreading (code word and reference signal). The probability distribution function of the estimator is extracted and the system’s robustness in regard to large number of interferers is demonstrated.
 
</p></abstract><kwd-group><kwd>DOA Estimator; Spread Spectrum; Smart Antenna System</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Under the pressure of the telecommunications requirements, in 4G and much more in 5G [<xref ref-type="bibr" rid="scirp.39588-ref1">1</xref>], radios must be equipped with high performance systems that could acquire and use all available information about the channel [<xref ref-type="bibr" rid="scirp.39588-ref2">2</xref>]. Here we focus on Direction of Arrival (DOA), estimation. The system is assumed to be implemented in every carrier of the multicarrier spread spectrum system [<xref ref-type="bibr" rid="scirp.39588-ref1">1</xref>]. Both spread spectrum technology and the information of the reference/pilot bits are employed. Indeed, after the code word dispreading of the array’s output vector, the pilot signal is used to perform the second dispreading. The resulted vector is used as the weight vector of the array. The produced power in the far field is written in quadratic form and its average is computed. The maximum of the produced beam is the DOAs estimate. In the current work, the functionality of the proposed system is addressed and its performance is, both analytically and numerically, verified. In fact, after the Probability Distribution Function (PDF) of the estimator is extracted, its potential to cope with very large number of interferers exhibiting fine resolution is demonstrated.</p><p>The paper is organized as follows: First, in Section 2, the signal and system models are given for an uplink scenario of a spread spectrum system. Then, in Section 3, the double dispreading function is studied and in Section 4 the proper convergence of the far-field is demonstrated. The PDF of the estimator is extracted in Section 6 where its statistical properties are presented. Numerical evaluation of the proposed system’s performance follows and last, conclusions are stated.</p></sec><sec id="s2"><title>2. Signal and System Model</title><p>Consider an uplink scenario in an asynchronous spread spectrum system with P mobile users. Let</p><disp-formula id="scirp.39588-formula134810"><label>(1)</label><graphic position="anchor" xlink:href="7-6101264\cc3d62ae-02a8-44d9-b101-a5e99d9e8404.jpg"  xlink:type="simple"/></disp-formula><p>be an N-bit sequence for the p-th user with the i-th bit equal to<img src="7-6101264\ce7dee51-285f-431f-891a-7c854338bf11.jpg" />. Subscript T denotes the transpose operation. Also, let</p><disp-formula id="scirp.39588-formula134811"><label>(2)</label><graphic position="anchor" xlink:href="7-6101264\01629fd8-4e83-4302-ab36-714c7a353165.jpg"  xlink:type="simple"/></disp-formula><p>be an <img src="7-6101264\f0b12fdb-eab4-47af-b3e8-a6e29be2bd99.jpg" />-chip sequence for the p-th user with the i-th chip equal to<img src="7-6101264\49493c67-8c06-4928-a6b1-1e31b7c6fc32.jpg" />. <img src="7-6101264\3f38fa50-ac5d-430d-89e7-eae79edb44be.jpg" />is spread by<img src="7-6101264\6eae3656-2aa5-4991-8c67-b03fada963d5.jpg" />. Thus, the respective transmitted signal can be represented by a <img src="7-6101264\d06e4482-d8b9-474b-99f9-5cdbf2e933f7.jpg" /> vector:</p><disp-formula id="scirp.39588-formula134812"><label>(3)</label><graphic position="anchor" xlink:href="7-6101264\47dd6a9e-0b97-4419-8d8b-8fc2327db523.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="7-6101264\47c614be-4fff-4983-bc89-1231d9ebb610.jpg" /> is the kronecker product.</p><p>Since, the uplink operates asynchronously the orthogonal property of the code vectors breaks down and their elements should be modeled as independent identically distributed (i.i.d.), binary RVs with zero mean. The same mathematical modeling is given to the data bits from the different incoming signals.</p><p>To represent the received signal one has to consider a receiver with an antenna array. So, we assume that the array consists of M elements and receives signals from P users that arrive at the array from different directions<img src="7-6101264\46d9ba9c-66ab-4a17-9d1a-3e51185e1f43.jpg" />. The direction—response vector associated with the p-th user is given by<img src="7-6101264\8bf51266-531e-4b82-b636-5a3780a6fb8b.jpg" />. The respective signal can be given in the form of a <img src="7-6101264\ce20d67f-94e2-4beb-bedc-9dae069a0e47.jpg" /> matrix with elements:</p><disp-formula id="scirp.39588-formula134813"><label>(4)</label><graphic position="anchor" xlink:href="7-6101264\78d40d68-5b09-4f04-84c2-306f536c572f.jpg"  xlink:type="simple"/></disp-formula><p><img src="7-6101264\71f37e20-7ea6-45ab-83fd-aa42a4c56789.jpg" />is the received complex signal amplitude. The <img src="7-6101264\0ca1dadf-4d7e-4be6-95df-f4ddb54aaf64.jpg" /> random variable (RV), has a Rayleigh PDF and the phase of <img src="7-6101264\e2384074-668c-42af-b52c-1ecdcd1ebcf5.jpg" /> is uniformly distributed in the domain (-π, +π). At this point we make the usual and practical assumption that the fading process is constant for a time period of a block of Ν successive bits.</p><p>The received base-band signal across the receiving antenna array can be expressed as:</p><disp-formula id="scirp.39588-formula134814"><label>(5)</label><graphic position="anchor" xlink:href="7-6101264\4e1250a0-8afa-48f2-98fc-d7f851363f1b.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="7-6101264\8d8843cf-2123-4db7-a6e3-4d17690993bb.jpg" /> is an <img src="7-6101264\aa6853fe-ad15-4d87-bc45-af4f5380ed27.jpg" /> matrix with elements representing spatially and temporally white complex Gaussian noise with zero mean and variance<img src="7-6101264\08184a00-54b6-4360-b715-d05d9c921472.jpg" />.</p></sec><sec id="s3"><title>3. Double Dispreading Function</title><p>In order to pick out the signal of the <img src="7-6101264\2cc0d3fc-5bc0-40f9-b76c-65d62712720e.jpg" />-th user, a codematched filter containing the specified, and properly time aligned, PN sequence, <img src="7-6101264\61f4b797-b8ff-4f54-93e0-b755f1dabade.jpg" />, is applied to <img src="7-6101264\8ff1b209-0899-41a1-80c0-57dc1af32ef5.jpg" /> performing the first dispreading function:</p><disp-formula id="scirp.39588-formula134815"><label>(6)</label><graphic position="anchor" xlink:href="7-6101264\3de6e64a-c312-40c8-b6b9-26c2ad63e790.jpg"  xlink:type="simple"/></disp-formula><p>where we have defined:</p><disp-formula id="scirp.39588-formula134816"><label>(7)</label><graphic position="anchor" xlink:href="7-6101264\8ebbbcc1-3bc6-48bc-9e37-51546951925f.jpg"  xlink:type="simple"/></disp-formula><p>It is easy to prove that:</p><disp-formula id="scirp.39588-formula134817"><label>(8)</label><graphic position="anchor" xlink:href="7-6101264\a0404036-f3af-49c9-84e7-50bb8b7c839c.jpg"  xlink:type="simple"/></disp-formula><p>Thus, using the Central Limit Theorem, that holds for big P<sub>G</sub>, the RV <img src="7-6101264\cd385d22-18b9-4042-adb5-784fc1be395e.jpg" /> is a Gaussian random variable with zero mean and variance equal to P<sub>G</sub>.</p><p>Also for the term <img src="7-6101264\62141aa9-f234-44e1-9090-a4bed8e97239.jpg" /> it is:</p><disp-formula id="scirp.39588-formula134818"><label>(9)</label><graphic position="anchor" xlink:href="7-6101264\6a2e8416-dad8-4fee-bcda-7df78e3042c0.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="7-6101264\566e4dbd-949e-4793-bbdf-4d87e3f9c831.jpg" /> is the M&#215;M unit matrix. The Central Limit Theorem holds for this case also.</p><p>Now, assuming that there exist a reference signal, <img src="7-6101264\c7f76dd8-3376-4c80-8f87-de7b1fd6bd4f.jpg" />, which is highly correlated with<img src="7-6101264\8f683f14-96a1-4f64-8f04-e1aba08e1a35.jpg" />, we can perform the second dispreading forming the inner-product of <img src="7-6101264\030fa2e6-6e9e-49df-bfa5-30506f9e2e74.jpg" /> and<img src="7-6101264\c94d43c9-c7db-4732-8d0b-dc60a184aa92.jpg" />:</p><disp-formula id="scirp.39588-formula134819"><label>(10)</label><graphic position="anchor" xlink:href="7-6101264\641d4627-aa13-40e9-b264-f1f58e24d75c.jpg"  xlink:type="simple"/></disp-formula><p>In (10), using<img src="7-6101264\5f9b363e-2ebd-4000-b82a-ef9874ae1b6c.jpg" />, we have defined:</p><disp-formula id="scirp.39588-formula134820"><label>(11)</label><graphic position="anchor" xlink:href="7-6101264\5b7247d1-4e99-4bf5-a772-ea9035e01b20.jpg"  xlink:type="simple"/></disp-formula><p>The average value of the <img src="7-6101264\a389d455-73c0-4690-9438-61995a2adfeb.jpg" /> vector, using Equations (8), (9) and (11), reads:</p><disp-formula id="scirp.39588-formula134821"><label>(12)</label><graphic position="anchor" xlink:href="7-6101264\b75a340e-2318-4b5b-81d7-dc5725d9eae2.jpg"  xlink:type="simple"/></disp-formula><p>The previous equation can be used to give the array’s response vector for the signal of interest (SOI). This can form the basis for the development of a robust DOA estimation algorithm.</p><p>Using (12), the angle of arrival <img src="7-6101264\387861dd-a817-44a4-ab75-0a1c81588564.jpg" /> can be computed using various techniques. Here we use <img src="7-6101264\4bceb1b0-a755-4641-8c42-727c29921d97.jpg" /> to find the array’s power pattern. The DOA estimate is given by the angle of the pattern’s maximum. Details are given next.</p></sec><sec id="s4"><title>4. Convergence of the Produced Average Far-Field Pattern</title><p>Using <img src="7-6101264\b37aa611-91f2-4bf9-ba28-ba00ccdd69bc.jpg" /> for the array’s weight vector, the produced power pattern is given by:</p><disp-formula id="scirp.39588-formula134822"><label>(13)</label><graphic position="anchor" xlink:href="7-6101264\4d96df9d-1ba5-4d82-941a-64511b1b88b2.jpg"  xlink:type="simple"/></disp-formula><p>This pattern can be farther improved by using the average value:</p><disp-formula id="scirp.39588-formula134823"><label>(14)</label><graphic position="anchor" xlink:href="7-6101264\669a98fe-fe12-4213-84cd-a03e123a39f9.jpg"  xlink:type="simple"/></disp-formula><p>So, we define the average power pattern by using the following:</p><disp-formula id="scirp.39588-formula134824"><label>(15)</label><graphic position="anchor" xlink:href="7-6101264\98915343-38ab-43cd-a03f-bf67ead64139.jpg"  xlink:type="simple"/></disp-formula><p>Finally we have:</p><disp-formula id="scirp.39588-formula134825"><label>(16)</label><graphic position="anchor" xlink:href="7-6101264\84aef633-8288-4d20-b3ee-ba99bdeb419e.jpg"  xlink:type="simple"/></disp-formula><p>Equation (16) is produced due to the fact that the various terms of the summation are mutually uncorrelated. Also, it is easy to prove:</p><disp-formula id="scirp.39588-formula134826"><label>(17)</label><graphic position="anchor" xlink:href="7-6101264\75d30524-343d-4ade-85e2-95953ab1cee3.jpg"  xlink:type="simple"/></disp-formula><p>Using (17) and (18) in (16) and inserting the result in (15) gives:</p><disp-formula id="scirp.39588-formula134827"><label>(18)</label><graphic position="anchor" xlink:href="7-6101264\c7ba4525-c05e-4756-9667-39546a51408f.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.39588-formula134828"><label>(19)</label><graphic position="anchor" xlink:href="7-6101264\2d8018b4-ca60-4ed7-983d-05c7772379f8.jpg"  xlink:type="simple"/></disp-formula><p>is the array’s power pattern when the maximum is towards the p-th incoming signal.</p><p>To study the pattern’s convergence we can write (18) as:</p><p><img src="7-6101264\b7fbe92f-ab69-4113-a3ef-e6c12e023671.jpg" /></p><p>(20)</p><p>Now it is obvious that increasing ΝP<sub>G</sub>, which means, increasing the Processing Gain and increasing the number of pilot bits, under the assumption that fading and DOAs remain constant, (20) comes to the limit:</p><disp-formula id="scirp.39588-formula134829"><label>(21)</label><graphic position="anchor" xlink:href="7-6101264\eec18241-3307-430b-9bc1-7a20c58c7af6.jpg"  xlink:type="simple"/></disp-formula><p>which results that DOA estimation gets more accurate. This limit does not depend on the number P of the incoming signals. Thus, the method can give the correct result assuming that Ν can get an adequate value.</p><p>In the following we study the statistical properties of the proposed estimator.</p></sec><sec id="s5"><title>5. Statistical Properties of the DOA Estimator</title><p>In the literature, there are methods addressing the statistical properties of DOA estimators. We proceed as in [<xref ref-type="bibr" rid="scirp.39588-ref3">3</xref>] and we assume that the signal to interference plus noise ratio (SINR), is sufficiently high so that the zeros of</p><p><img src="7-6101264\ebe4f8ab-62a3-490d-86a9-1818917243e9.jpg" />are within one Newton iteration step of the true</p><p><img src="7-6101264\ff6b2c6a-ca23-4c19-8f1c-c3cfca0131c1.jpg" />:</p><disp-formula id="scirp.39588-formula134830"><label>(22)</label><graphic position="anchor" xlink:href="7-6101264\27a19d53-a54e-4ae1-9b63-b9808472665d.jpg"  xlink:type="simple"/></disp-formula><p><img src="7-6101264\c755e67f-ae3b-4663-8e5b-07a7486e0b65.jpg" />and <img src="7-6101264\b68e5c84-914e-4b6e-9e62-c72f176ac2ff.jpg" /> denote the first and second derivatives of the power pattern with respect to <img src="7-6101264\5b16ef2f-e353-4130-8236-a8aea39d5a84.jpg" /> calculated at<img src="7-6101264\35bf5540-7b45-4f4e-9c98-dd6054e4664b.jpg" />. Using (20), (22) becomes:</p><disp-formula id="scirp.39588-formula134831"><label>(23)</label><graphic position="anchor" xlink:href="7-6101264\e6d027e8-b321-464b-9f04-ec1e696a5532.jpg"  xlink:type="simple"/></disp-formula><p>By definition we have that:</p><disp-formula id="scirp.39588-formula134832"><label>(24)</label><graphic position="anchor" xlink:href="7-6101264\1e8a8323-e1f3-4d54-9304-67a4d0962b0c.jpg"  xlink:type="simple"/></disp-formula><p>Also, for the denominator of (23), approximately (increasing the <img src="7-6101264\fd1fff5c-b4b0-4249-ac4a-acb0a6793612.jpg" /> product), the next holds:</p><disp-formula id="scirp.39588-formula134833"><label>(25)</label><graphic position="anchor" xlink:href="7-6101264\cb911be3-3ca6-46f0-9a55-87f67ed54467.jpg"  xlink:type="simple"/></disp-formula><p>Using (23)-(25) after rearranging the various terms, (22) becomes:</p><disp-formula id="scirp.39588-formula134834"><label>(26)</label><graphic position="anchor" xlink:href="7-6101264\87233aa8-96ff-4922-9bd9-3e2919211a94.jpg"  xlink:type="simple"/></disp-formula><p>The extraction of the PDF of the RV given in (26) is not an easy task since the summation terms can take negative values [<xref ref-type="bibr" rid="scirp.39588-ref4">4</xref>]. We start from (26) which is written as:</p><disp-formula id="scirp.39588-formula134835"><label>(27)</label><graphic position="anchor" xlink:href="7-6101264\be06b706-3abe-4050-981e-23961920c932.jpg"  xlink:type="simple"/></disp-formula><p>The <img src="7-6101264\7abedaac-3789-4ccd-b8fa-ce46645d028f.jpg" /> variable can take the following form:</p><disp-formula id="scirp.39588-formula134836"><label>(28)</label><graphic position="anchor" xlink:href="7-6101264\1e8502cb-4faf-4759-a494-1d07285dee9c.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="7-6101264\2d54bce9-7efa-4ad8-8baa-03e933249f93.jpg" /> are the terms with</p><p><img src="7-6101264\04d53509-2ed2-4c4f-87fb-83fe6d22d6c1.jpg" />.</p><p>So, there are <img src="7-6101264\52dcaa0e-0a9d-4fd3-b807-6dc2d1929efb.jpg" /> positive variables that constitute the <img src="7-6101264\34ce666c-a979-445f-bcf4-238ab4421bd6.jpg" /> RV and <img src="7-6101264\9e81aca4-3493-4b12-9656-a7775d8fffd6.jpg" /> negative variables that their absolute values are summed to form the <img src="7-6101264\13cc3eac-bf7b-4bfe-8636-2aeb2c7a8635.jpg" /> variable. Now, the RV <img src="7-6101264\d44c4b63-b3c9-4540-866a-6883cb1f017d.jpg" /> is distributed like:</p><disp-formula id="scirp.39588-formula134837"><label>(29)</label><graphic position="anchor" xlink:href="7-6101264\0a38d134-cf3a-4f4b-ae02-0b0aca77311a.jpg"  xlink:type="simple"/></disp-formula><p><img src="7-6101264\2c8ca76b-f67b-488a-bd22-69a7e5ff8197.jpg" />is the unit step function. Equation (29) comes from the fact that <img src="7-6101264\aa197439-b1fa-4091-823e-c03b259fcd9a.jpg" /> is Rayleigh distributed with the expected value of the square amplitude equal to<img src="7-6101264\aa303231-a96f-4fc8-b2d3-ecc78857b2e8.jpg" />. The conditioning of <img src="7-6101264\3bac44fd-2a33-413c-941c-1388922bb826.jpg" /> on the angle of arrival of the desired user <img src="7-6101264\ce7121e7-93ed-4ba8-82fe-86e02e696831.jpg" /> is expressed through the<img src="7-6101264\e4c24dd4-0be1-495a-8775-4c336a8862c6.jpg" />.</p><p>After this, it can be easily shown that the RVs <img src="7-6101264\c361357c-11c4-480e-8a70-165ace3f089c.jpg" /> of (28) are distributed like:</p><disp-formula id="scirp.39588-formula134838"><label>(30)</label><graphic position="anchor" xlink:href="7-6101264\1aa64039-3813-4265-83a9-9dad4d07395b.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.39588-formula134839"><label>(31)</label><graphic position="anchor" xlink:href="7-6101264\b207b4d0-4106-417a-8102-a72b74337c61.jpg"  xlink:type="simple"/></disp-formula><p>Now let us define the variable:</p><disp-formula id="scirp.39588-formula134840"><label>(32)</label><graphic position="anchor" xlink:href="7-6101264\12fdd8f3-e3e7-4aa4-b39e-9ea5a98c07df.jpg"  xlink:type="simple"/></disp-formula><p>The random variable <img src="7-6101264\99e912da-2d6c-4adf-92d2-da8c34c42bf3.jpg" /> is distributed like:</p><p><img src="7-6101264\edd78576-4c9c-47fd-a663-90884a37b6f3.jpg" /></p><p>(33)</p><p>The RV λ is distributed like:</p><disp-formula id="scirp.39588-formula134841"><label>(34)</label><graphic position="anchor" xlink:href="7-6101264\43cb4bea-06eb-4eca-b0a7-87071169a0b2.jpg"  xlink:type="simple"/></disp-formula><p>Let us now proceed to the RV ρ. The PDF of ρ is given by the following:</p><disp-formula id="scirp.39588-formula134842"><label>(35)</label><graphic position="anchor" xlink:href="7-6101264\34ef4e71-9032-4efd-942f-527094312f3d.jpg"  xlink:type="simple"/></disp-formula><p>Before closing the section devoted to the statistical properties of the estimator a note is in order. The PDF of the estimator is conditioned on the DOAs of the signals not of interest and the SOI. Nevertheless, it can be easily proved that the averaging over the DOAs still gives <img src="7-6101264\c5af072c-3af6-42de-bd4d-a8b2f859be2a.jpg" /> and<img src="7-6101264\33e7f480-889d-48e3-854f-b96bcdb407ae.jpg" />.</p></sec><sec id="s6"><title>6. Numerical Performance Evaluation</title><p>In the current section a verification of the extracted PDF of the DOA estimator is given. A computer code was written to simulate the receiver and the signal models. The statistical sampling (Monte Carlo), simulation parameters are as follows: The signal to noise ratio, in the case of a single receiver, is the same for every user. All users have the same power. The average fading power is set equal to 1 while the fading is assumed to be Rayleigh. A Uniform Linear Array (ULA), having seven omnidirectional elements with λ/2 interelement distance is used. The number of interfering signals is set equal to 30. The DOA of the SOI is set equal to 30˚. The DOAs of the P users are uniformly distributed between<img src="7-6101264\4aafc67e-d4ac-41a8-8d3f-3abbcd599f7c.jpg" />. The processing gain is set equal to 16. The PDF of the estimated DOA is given in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>The continuous curve is produced from Equation (21) while the histogram presents the Monte Carlo extracted PDF after using 10<sup>3</sup> realizations of the spatial signature. The horizontal axis is the estimation angle in degrees<img src="7-6101264\24fe13ab-06d7-46a2-9287-02ff934064f6.jpg" />, while in the vertical axis, the absolute occurrence of the events is represented. For example nearly 300 (287), times out of a total of 10<sup>3</sup> the estimator produced an outcome between 30˚ &#177; 0.025˚. If we characterize as accurate an estimate in the area 30˚ &#177; 0.5˚ then the estimator produces an accurate estimate approximately 90% of the trials.</p></sec><sec id="s7"><title>7. Conclusions</title><p>A double dispreading based DOA estimator is proposed for a spread spectrum reference of signal-assisted radio. A closed form relation for the PDF of the estimator is extracted to assess its performance. Instead of following the usual path, assuming DOA estimates corrupted by simple additive white noise, the realistic scenario of Rayleigh fading is addressed.</p><p>From the theoretical derivation, the estimator’s ability to provide accurate estimates, even in the case of large</p><p>number of interferers, is demonstrated.</p><p>The proposed DOA method is readily integrable in the Multicarrier spread spectrum systems [<xref ref-type="bibr" rid="scirp.39588-ref1">1</xref>].</p></sec><sec id="s8"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.39588-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">K. Fazel and S. Kaiser, “Multi-Carrier and Spread Spec- trum Systems: From OFDM and MC-CDMA to LTE and WiMAX,” 2nd Edition, John Wiley &amp; Sons, London, 2008.</mixed-citation></ref><ref id="scirp.39588-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">L. C. Godara, “Smart Antennas,” CRC Press, New York, 2004.</mixed-citation></ref><ref id="scirp.39588-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">F. Li, H. Liu and R. J. Vaccaro, “Performance Analysis for DOA Estimation Algorithms: Unification, Simplification and Observation,” IEEE Transactions on Aerospace and Electronic Systems, Vol. 29, No. 10, 1993, pp. 1170-1184.</mixed-citation></ref><ref id="scirp.39588-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">M. K. Simon and M.-S. Alouini, “On the Difference of Two Chisquare Variates with Application to Outage Probability Computation,” IEEE Transactions on Communications, Vol. 49, No. 11, 2001, pp. 1946-1954.</mixed-citation></ref></ref-list></back></article>