<?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.2015.72011</article-id><article-id pub-id-type="publisher-id">CN-56045</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>
 
 
  An Estimation of Achievable Rate for Digital Transmissions over MIMO Channels
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>inbao</surname><given-names>Zhang</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>Song</surname><given-names>Chen</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Qing</surname><given-names>He</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Beijing Engineering Research Center of EMC and GNSS Technology for Rail Transportation, Beijing, China</addr-line></aff><aff id="aff1"><addr-line>School of Electronic and Information Engineering, Beijing Jiaotong University, Beijing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>jbzhang@bjtu.edu.cn(IZ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>03</month><year>2015</year></pub-date><volume>07</volume><issue>02</issue><fpage>117</fpage><lpage>124</lpage><history><date date-type="received"><day>23</day>	<month>March</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>24</month>	<year>April</year>	</date><date date-type="accepted"><day>30</day>	<month>April</month>	<year>2015</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>
 
 
  Achievable rate (AR) is significant to communications. As to multi-input multi-output (MIMO) digital transmissions with finite alphabets inputs, which greatly improve the performance of communications, it seems rather difficult to calculate accurate AR. Here we propose an estimation of con-siderable accuracy and low complexity, based on Euclidean measure matrix for given channel states and constellations. The main contribution is explicit expression, non-constraints to MIMO schemes and channel states and constellations, and controllable estimating gap. Numerical results show that the proposition is able to achieve enough accurate AR computation. In addition the estimating gap given by theoretical deduction is well agreed.
 
</p></abstract><kwd-group><kwd>Achievable Rate</kwd><kwd> Digital MIMO Transmissions</kwd><kwd> Analytical Estimation</kwd><kwd> Low-Complexity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Achievable rate (AR), defined as information entropy collected from receiving signals―mutual information, is a fundamental means to evaluate and optimize communications. It is demonstrated that AR is inputs related, and achieves its maximum―channel capacity with Gaussian inputs [<xref ref-type="bibr" rid="scirp.56045-ref1">1</xref>] . Despite optimal, Gaussian inputs are rarely used in practice. Instead, digital transmissions with inputs from finite-alphabet constellations, such as m-PSK and etc., are more common, which depart significantly from Gaussian inputs. Therefore, a considerable AR gap exists between the two inputs [<xref ref-type="bibr" rid="scirp.56045-ref2">2</xref>] . Besides, many results have shown that multi-input multi-output (MIMO) greatly improves the performance of digital transmissions [<xref ref-type="bibr" rid="scirp.56045-ref3">3</xref>] . Consequently AR computation for digital transmissions over MIMO channels is motivated.</p><p>Reconsider definition of mutual information in [<xref ref-type="bibr" rid="scirp.56045-ref1">1</xref>] . When it comes to finite-alphabet constellations and MIMO propagation matrix, it involves multi-dimensional integral to calculate AR, which leads to impractical implementation. And then various estimations are proposed. Monte Carlo method [<xref ref-type="bibr" rid="scirp.56045-ref4">4</xref>] is the most common. Despite accuracy, not only it is too implicit for analytical applications, but also it costs too much computational complexity as order of modulation and MIMO increases. Particle method [<xref ref-type="bibr" rid="scirp.56045-ref5">5</xref>] is proposed to reduce the complexity. However, it remains implicit. Aiming analytical solution, lower bounds and approximations for AR are proposed in [<xref ref-type="bibr" rid="scirp.56045-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.56045-ref6">6</xref>] and [<xref ref-type="bibr" rid="scirp.56045-ref7">7</xref>] respectively, showing validity under certain scenarios. Unfortunately, limitation remains. Lower bound in [<xref ref-type="bibr" rid="scirp.56045-ref2">2</xref>] requires unitary inputs―matrix having orthonormal columns [<xref ref-type="bibr" rid="scirp.56045-ref8">8</xref>] . For wireless MIMO channels, such assumption is rarely achieved. As to approximations in [<xref ref-type="bibr" rid="scirp.56045-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.56045-ref7">7</xref>] , constellations and MIMO channels related tuning factor is indispensable to the estimating accuracy, which also introduces limitation. Moreover, gap between true AR and lower bounds/approximations is not analyzed in the mentioned work.</p><p>Comparing to current proposals, the main contribution of this letter is to propose AR estimation of low complexity, analytically explicit expression and controllable gap, without constraints to inputs and MIMO channels. This work is organized as follows. Section 2 formulates the problem and premiss; Section 3 describes details of proposed solution, and analyzes estimating gap; Section 4 gives numerical results, and further discuss on computational complexity and estimating gap; finally conclusions are drawn in Section 5.</p></sec><sec id="s2"><title>2. Problem Formulation</title><sec id="s2_1"><title>2.1. Notations and Definitions</title><p>This work uses the following notations. Italic character in lower and upper case denotes variable. Bold italic character in lower and upper case denotes vector and matrix respectively. The superscript <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x5.png" xlink:type="simple"/></inline-formula> denotes conjugate transposition. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x6.png" xlink:type="simple"/></inline-formula>is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x7.png" xlink:type="simple"/></inline-formula> identity matrix. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x8.png" xlink:type="simple"/></inline-formula>is the element of matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x9.png" xlink:type="simple"/></inline-formula> at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x10.png" xlink:type="simple"/></inline-formula> row and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x11.png" xlink:type="simple"/></inline-formula> column. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x12.png" xlink:type="simple"/></inline-formula>is the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x13.png" xlink:type="simple"/></inline-formula> element of vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x14.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x15.png" xlink:type="simple"/></inline-formula>denotes the trace of square matrix. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x16.png" xlink:type="simple"/></inline-formula>is Euclidean norm of matrix and vector. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x17.png" xlink:type="simple"/></inline-formula>denotes the expectation of random variable. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x18.png" xlink:type="simple"/></inline-formula>is Dirac delta function. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x19.png" xlink:type="simple"/></inline-formula>is a complex Gaussian random scalar, and its real and imaginary components are independent and identically normal distributed with zero-mean and variance of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula>is a real Gaussian random scalar normal distributed with zero-mean and variance of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula>is the complex space, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula> is the real space. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x25.png" xlink:type="simple"/></inline-formula>means that space―<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x26.png" xlink:type="simple"/></inline-formula>is consisted of elements―<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x27.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x28.png" xlink:type="simple"/></inline-formula>denotes <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x29.png" xlink:type="simple"/></inline-formula> tensor space based on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x30.png" xlink:type="simple"/></inline-formula>. Operation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x31.png" xlink:type="simple"/></inline-formula> is cartesian product of space.</p></sec><sec id="s2_2"><title>2.2. Signal Model and Premise</title><p>Consider digital transmissions over <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x32.png" xlink:type="simple"/></inline-formula> MIMO channels, following assumptions are premised.</p><p>•<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x33.png" xlink:type="simple"/></inline-formula>, is an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x34.png" xlink:type="simple"/></inline-formula> complex propagation matrix, known to receiver.</p><p>•<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula>, is an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x36.png" xlink:type="simple"/></inline-formula> transmitted symbol vector. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x37.png" xlink:type="simple"/></inline-formula>is independently and uniformly selected from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x38.png" xlink:type="simple"/></inline-formula> normalized finite-alphabet constellation―<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x39.png" xlink:type="simple"/></inline-formula>:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x40.png" xlink:type="simple"/></inline-formula>. Moreover, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x41.png" xlink:type="simple"/></inline-formula>may differ with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x42.png" xlink:type="simple"/></inline-formula>. Thus</p><disp-formula id="scirp.56045-formula700"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x43.png"  xlink:type="simple"/></disp-formula><p>Define<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x44.png" xlink:type="simple"/></inline-formula>. Consequently<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x45.png" xlink:type="simple"/></inline-formula>:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x46.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x47.png" xlink:type="simple"/></inline-formula>. So we have</p><disp-formula id="scirp.56045-formula701"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x48.png"  xlink:type="simple"/></disp-formula><p>•<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x49.png" xlink:type="simple"/></inline-formula>, is an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x50.png" xlink:type="simple"/></inline-formula> independent complex additional white Gaussian noise (AWGN) vector, and</p><disp-formula id="scirp.56045-formula702"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x51.png"  xlink:type="simple"/></disp-formula><p>•<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x52.png" xlink:type="simple"/></inline-formula>, is an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x53.png" xlink:type="simple"/></inline-formula> receiving symbol vector. Hence, AR is defined as mutual information [<xref ref-type="bibr" rid="scirp.56045-ref1">1</xref>] ,</p><disp-formula id="scirp.56045-formula703"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x54.png"  xlink:type="simple"/></disp-formula><p>Note that, Equation (4) is AR value for the whole transmitting and receiving vector. Considering spatial multiplexing mode of MIMO, AR value for each element in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x55.png" xlink:type="simple"/></inline-formula> is also needed, so we formulate the problem as estimation of AR for both vector and each element in the vector.</p></sec></sec><sec id="s3"><title>3. Low-Complexity Solution</title><p>Firstly, Equation (4) is rewritten as</p><disp-formula id="scirp.56045-formula704"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x56.png"  xlink:type="simple"/></disp-formula><p>Given <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x57.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x58.png" xlink:type="simple"/></inline-formula>, the posterior probability is,</p><disp-formula id="scirp.56045-formula705"><graphic  xlink:href="http://html.scirp.org/file/5-6101492x59.png"  xlink:type="simple"/></disp-formula><p>Given<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x60.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.56045-formula706"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x61.png"  xlink:type="simple"/></disp-formula><p>Definition: Euclidean measure matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x62.png" xlink:type="simple"/></inline-formula> for given constellation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x63.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x64.png" xlink:type="simple"/></inline-formula> is as</p><disp-formula id="scirp.56045-formula707"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x65.png"  xlink:type="simple"/></disp-formula><p>Recall Equation (3), and then Equation (6) is rewritten as</p><disp-formula id="scirp.56045-formula708"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x66.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x67.png" xlink:type="simple"/></inline-formula> is combination of AWGNs,</p><disp-formula id="scirp.56045-formula709"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x68.png"  xlink:type="simple"/></disp-formula><p>Then normalize <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x69.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.56045-formula710"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x70.png"  xlink:type="simple"/></disp-formula><p>So we rewrite Equation (8) as</p><disp-formula id="scirp.56045-formula711"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x71.png"  xlink:type="simple"/></disp-formula><p>Theorem 1. AR is estimated by exponentially weighted average of Euclidean measure matrix as</p><disp-formula id="scirp.56045-formula712"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x72.png"  xlink:type="simple"/></disp-formula><p>Proof. see Appendix 1.</p><p>Theorem 2. AR is decomposed as</p><disp-formula id="scirp.56045-formula713"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x73.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x74.png" xlink:type="simple"/></inline-formula> denotes the sub-vector excluding <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x75.png" xlink:type="simple"/></inline-formula> from<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x76.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. see Appendix 2.</p><p>With Theorem 1 and 2, the formulated problem in Section 2 is solved.</p><p>Theorem 3. Gap between true and estimated AR given in proposition 1 is bounded by exponentially weighted average of minimum Euclidean measure as</p><disp-formula id="scirp.56045-formula714"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x77.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x78.png" xlink:type="simple"/></inline-formula> denotes the minimum among non-zero elements in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x79.png" xlink:type="simple"/></inline-formula> column of Euclidean measure matrix.</p><p>Proof. see Appendix 3.</p><p>Recalling Theorem 3, the gap between true and estimated AR for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x80.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.56045-formula715"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x81.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Numerical Results</title><p>To verify Theorem 1, 2 and 3, numerical results are provided. For generality, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x82.png" xlink:type="simple"/></inline-formula>complex propagation matrixes consisted of independent Gaussian distributed elements are used as MIMO channels,</p><disp-formula id="scirp.56045-formula716"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x83.png"  xlink:type="simple"/></disp-formula><p>Also high and low correlated scenarios with correlation coefficient of 0.1 and 0.9 are considered respectively,</p><disp-formula id="scirp.56045-formula717"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x84.png"  xlink:type="simple"/></disp-formula><p>where correlation matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x85.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x86.png" xlink:type="simple"/></inline-formula> are generated with spatial channel model and correlation coefficient [<xref ref-type="bibr" rid="scirp.56045-ref3">3</xref>] .</p><p>The 3 transmitted symbols in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x87.png" xlink:type="simple"/></inline-formula> are modulated by BPSK, 8PSK and 16QAM respectively. True AR is computed by Monte Carlo method [<xref ref-type="bibr" rid="scirp.56045-ref4">4</xref>] . And estimated AR is computed with Theorem 1 and 2.</p><p>Numerical results in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> show that the proposed estimation is able to achieve enough accurate AR over complex Gaussian random MIMO channel. And according to Equation (6) and (12), the calculation complexity is reduced to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x88.png" xlink:type="simple"/></inline-formula> exponentiations and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x89.png" xlink:type="simple"/></inline-formula> logarithms, instead of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x90.png" xlink:type="simple"/></inline-formula> integrals.</p><p>Despite slightness, numerical results show that the gap remains. However, such estimating gap can be quantized by Equation (14) and (15), and numerical results are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. According to <xref ref-type="fig" rid="fig1">Figure 1</xref> and</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> AR for 2 &#215; 3 random Gaussian distributed MIMO channels with transmitting and receiving correlation coefficient of 0.1</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6101492x91.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> AR for 2 &#215; 3 random Gaussian distributed MIMO channels with transmitting and receiving correlation coefficient of 0.9</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6101492x92.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Gap between true and estimated AR for 2 &#215; 3 random Gaussian distributed MIMO channels with transmitting and receiving correlation coefficient of 0.1 and 0.9, computed with Equations (14) and (15)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-6101492x93.png"/></fig><p><xref ref-type="fig" rid="fig2">Figure 2</xref>, the maximum gap between estimated and true AR is lower than 0.0733 bits/symbol, which agrees well to theoretic bound of 0.0603 bits/symbol given in <xref ref-type="fig" rid="fig3">Figure 3</xref>, which is computed by Theorem 3.</p></sec><sec id="s5"><title>5. Conclusion</title><p>A low-complexity AR estimation is presented in this work. Numerical results show that it is accurate enough, and the deductive theoretic bound of estimating gap is well matched. Moreover, the most encouraging thing is that, the proposed estimation is of no constraints to finite-alphabet constellations and MIMO channels. Besides, as shown in Equation (12), this proposition deduces integral of AR calculation into an weighted average of Euclidean measure matrix for given channel states and constellations, which is explicit enough for analytical applications.</p></sec><sec id="s6"><title>Acknowledgements</title><p>We thank the Editor and the referee for their comments. This work is funded by the NSFC program (61172021 and 61471030), the Fundamental Research Funds for the Central Universities (2014JBZ023), Beijing city science and technology special program (Z141101004414091), and Research on the development of science and technology plan Chinese Railway Corporation (2014X012-B, Z2014-X002). This support is greatly appreciated.</p></sec><sec id="s7"><title>Appendix</title><sec id="s7_1"><title>1. Proof of Theorem 1</title><p>Proof. Following approximations are easily achieved with numerical methods,</p><disp-formula id="scirp.56045-formula718"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x94.png"  xlink:type="simple"/></disp-formula><p>Although gap still remains, following deduction will show that such gap makes no difference on AR computations. Define</p><disp-formula id="scirp.56045-formula719"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x95.png"  xlink:type="simple"/></disp-formula><p>To prove of Equation (12) equals to prove</p><disp-formula id="scirp.56045-formula720"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x96.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x97.png" xlink:type="simple"/></inline-formula> is an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x98.png" xlink:type="simple"/></inline-formula> ascending sorted vector, and</p><disp-formula id="scirp.56045-formula721"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x99.png"  xlink:type="simple"/></disp-formula><p>Use inductive reasoning, define <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x100.png" xlink:type="simple"/></inline-formula> as the gap,</p><disp-formula id="scirp.56045-formula722"><label>. (22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x101.png"  xlink:type="simple"/></disp-formula><p>For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x102.png" xlink:type="simple"/></inline-formula>, recalling Equation (7), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x103.png" xlink:type="simple"/></inline-formula>constantly equals to 0,</p><disp-formula id="scirp.56045-formula723"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x104.png"  xlink:type="simple"/></disp-formula><p>Then assume</p><disp-formula id="scirp.56045-formula724"><label>. (24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x105.png"  xlink:type="simple"/></disp-formula><p>This implies that, within the operative domain of</p><disp-formula id="scirp.56045-formula725"><graphic  xlink:href="http://html.scirp.org/file/5-6101492x106.png"  xlink:type="simple"/></disp-formula><p>following approximation is valid.</p><disp-formula id="scirp.56045-formula726"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x107.png"  xlink:type="simple"/></disp-formula><p>Recall Equation (18), for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x108.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.56045-formula727"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x109.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.56045-formula728"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x110.png"  xlink:type="simple"/></disp-formula><p>And the right side of Equation (22) is</p><disp-formula id="scirp.56045-formula729"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x111.png"  xlink:type="simple"/></disp-formula><p>So that</p><disp-formula id="scirp.56045-formula730"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x112.png"  xlink:type="simple"/></disp-formula><p>Using monotonic property of exponentiation and logarithm, it is demonstrated that,</p><disp-formula id="scirp.56045-formula731"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x113.png"  xlink:type="simple"/></disp-formula><p>Recalling Equation (23), (24) and (30), assigning<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x114.png" xlink:type="simple"/></inline-formula>, Equation (21) is proved. And then Theorem 1 is proved by substituting Equation (21) in Equation (11).</p></sec><sec id="s7_2"><title>2. Proof of Theorem 2</title><p>Proof. Use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x116.png" xlink:type="simple"/></inline-formula> to denote the sub-set of all possible values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x117.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x118.png" xlink:type="simple"/></inline-formula>, and then recall Equation (5), using <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x119.png" xlink:type="simple"/></inline-formula> to denote the targeting sub-vector of computation, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x120.png" xlink:type="simple"/></inline-formula> to denote the sub-vector excluding <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x121.png" xlink:type="simple"/></inline-formula> from<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x122.png" xlink:type="simple"/></inline-formula>. We have,</p><disp-formula id="scirp.56045-formula732"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x123.png"  xlink:type="simple"/></disp-formula><p>Then designate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x124.png" xlink:type="simple"/></inline-formula> to denote the sub-vector excluding <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x125.png" xlink:type="simple"/></inline-formula> from<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x126.png" xlink:type="simple"/></inline-formula>, and Theorem 2 is proved.</p></sec><sec id="s7_3"><title>3. Proof of Theorem 3</title><p>Proof. Recall Equation (12) and (30), the maximum gap between true and estimated AR value for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x127.png" xlink:type="simple"/></inline-formula> is as follows,</p><disp-formula id="scirp.56045-formula733"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x128.png"  xlink:type="simple"/></disp-formula><p>Since that the sequence of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-6101492x129.png" xlink:type="simple"/></inline-formula> is ascending sorted, and then we have,</p><disp-formula id="scirp.56045-formula734"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-6101492x130.png"  xlink:type="simple"/></disp-formula><p>Theorem 3 is proved.</p></sec></sec></body><back><ref-list><title>References</title><ref id="scirp.56045-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Shannon, C.E. 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