<?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">JSIP</journal-id><journal-title-group><journal-title>Journal of Signal and Information Processing</journal-title></journal-title-group><issn pub-type="epub">2159-4465</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jsip.2014.54018</article-id><article-id pub-id-type="publisher-id">JSIP-51385</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 Approximated Expression for the Residual ISI Obtained by Blind Adaptive Equalizer and Biased Input Signals
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>issim</surname><given-names>Panizel</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>Monika</surname><given-names>Pinchas</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 Electrical and Electronic Engineering, Ariel University, Ariel, Israel</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>nissimpanizel@gmail.com(IP)</email>;<email>monika.pinchas@gmail.com(MP)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>10</month><year>2014</year></pub-date><volume>05</volume><issue>04</issue><fpage>155</fpage><lpage>178</lpage><history><date date-type="received"><day>21</day>	<month>August</month>	<year>2014</year></date><date date-type="rev-recd"><day>18</day>	<month>September</month>	<year>2014</year>	</date><date date-type="accepted"><day>15</day>	<month>October</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>
 
 
  Recently, two expressions (for the noiseless and noisy case) were proposed for the residual inter-symbol interference (ISI) obtained by blind adaptive equalizers, where the error of the equalized output signal may be expressed as a polynomial function of order 3. However, those expressions are not applicable for biased input signals. In this paper, a closed-form approximated expression is proposed for the residual ISI applicable for the noisy and biased input case. This new proposed expression is valid for blind adaptive equalizers, where the error of the equalized output signal may be expressed as a polynomial function of order 3. The new proposed expression depends on the equalizer’s tap length, input signal statistics, channel power, SNR, step-size parameter and on the input signal’s bias. Simulation results indicate a high correlation between the simulated results and those obtained from our new proposed expression.
 
</p></abstract><kwd-group><kwd>Blind Adaptive Equalizers</kwd><kwd> Deconvolution</kwd><kwd> Inter-Symbol Interference (ISI)</kwd><kwd> Convolutional Noise</kwd><kwd> Residual ISI</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Blind equalization is used in various applications such as: signal processing, digital communication, speech and image processing. Generally, a communication system may be presented by a signal transmitted via a com- munication channel added with white noise as illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The channel is not ideal due to reflections and delays caused by the physical environment such as: ground, buildings and cables. Those reflections and delays cause distortion of the received signal which is referred as ISI. In order to overcome the irreducible</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Block diagram of a baseband communication system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x5.png"/></fig><p>degradation in performance caused by the ISI, a blind adaptive equalizer, may be implemented in those systems [<xref ref-type="bibr" rid="scirp.51385-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.51385-ref12">12</xref>] . Blind de-convolution algorithms are essentially adaptive filtering algorithms designed such that they do not require the external supply of a desired response to generate the error signal in the output of the adaptive equalization filter [<xref ref-type="bibr" rid="scirp.51385-ref13">13</xref>] . The algorithm itself generates an estimate of the desired response by applying a non- linear transformation to sequences involved in the adaptation process [<xref ref-type="bibr" rid="scirp.51385-ref13">13</xref>] . Blind equalization methods are of great importance in digital signal communication systems, as they allow channel equalization at the receiver without the use of training signals which consume considerable channel capacity. In blind equalization, there is no wasted data on training symbols, therefore bandwidth is saved [<xref ref-type="bibr" rid="scirp.51385-ref6">6</xref>] . Since blind equalizers do not require any known training sequence for the startup period, they are also useful for point-to-multipoint network applications, such as the fiber to the curb (FTTC) systems [<xref ref-type="bibr" rid="scirp.51385-ref14">14</xref>] . Generally, blind methods are classified according to the location of their nonlinearity in the receiver [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] . We may classify blind equalization methods [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] as follows: 1) Polyspectral algorithms; 2) Bussgang-type algorithms; 3) Probabilistic algorithms. In the first type, the non- linearity is located at the output of the channel, right before the equalizer’s filter. The non-linearity has thus the function of estimating the channel and feeding that information to the equalizer for adaptation purposes. In the second type, the nonlinearity is found at the output of the equalizer’s filter and it is memoryless function. Among Bussgang type algorithms we may find Godard’s algorithm [<xref ref-type="bibr" rid="scirp.51385-ref7">7</xref>] which will also used in this paper. In the third type, the nonlinearity is combined with the data detection process. Algorithms with the third type can extract considerable information from relatively little data [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] , but this is often accomplished at a huge com- putational cost.</p><p>Up to now, the performance of a chosen equalizer (the achievable residual ISI) for biased input signals could be obtained only via simulation. According to [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] , the equalization performance depends on the nature of the equalizer (on the memoryless nonlinearity as already was mentioned before), on the channel characteristics, on the added noise, on the step-size parameter used in the adaptation process which will be explained later in this paper, on the equalizer’s tap length and on the input signal statistics. Fast convergence speed and reaching a residual ISI where the eye diagram is considered to be open are the main requirements from a blind equalizer. Fast convergence speed may be obtained by increasing the step-size parameter. But increasing the step-size parameter may lead to a higher residual ISI which might not meet any more the system’s requirements [<xref ref-type="bibr" rid="scirp.51385-ref6">6</xref>] . Recently [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] , proposed a closed-form approximated expression for the residual ISI for the noiseless and noisy case respectively. However, those expressions [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] are not applicable for biased input signals.</p><p>In this paper, we propose for the noisy and biased input signal case a closed-form approximated expression for the residual ISI that depends on the equalizer’s tap length, input signal statistics, channel power, SNR, step- size parameter and on the input signal’s bias. Since the channel power is measurable, there is no need anymore to carry out any simulation with various step-size parameters in order to reach the required residual ISI.</p><p>The paper is organized as follows: after having described the system under consideration in Section 2, the closed-form approximated expression for the achievable residual ISI is introduced in Section 3. In Section 4, simulation results are presented and the conclusion is given in Section 5.</p></sec><sec id="s2"><title>2. System Description</title><p>The system under consideration is the same system as shown in [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] and is illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>. We consider the following assumptions:</p><p>1. The input sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x6.png" xlink:type="simple"/></inline-formula> represents a two independent biased quadrature carriers case constellation input where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x7.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x8.png" xlink:type="simple"/></inline-formula> are the real and imaginary parts of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x9.png" xlink:type="simple"/></inline-formula> respectively.</p><p>2. The biased input sequence mean is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x10.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x11.png" xlink:type="simple"/></inline-formula> is the expectation operator.</p><p>3.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x12.png" xlink:type="simple"/></inline-formula>.</p><p>4. The unknown channel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x13.png" xlink:type="simple"/></inline-formula> is modeled as a non-minimum phase FIR filter, which has zeros far from the unit circle.</p><p>5. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x14.png" xlink:type="simple"/></inline-formula>is the equalizer’s tap-delay line.</p><p>6. The noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x15.png" xlink:type="simple"/></inline-formula> is an added Gaussian white noise with zero mean and consists of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x16.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x17.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x18.png" xlink:type="simple"/></inline-formula> are the real and imaginary parts of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x19.png" xlink:type="simple"/></inline-formula> respectively as well as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x20.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x21.png" xlink:type="simple"/></inline-formula> are independent. Both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x22.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x23.png" xlink:type="simple"/></inline-formula> have zero mean and their variances are denoted as:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x24.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x25.png" xlink:type="simple"/></inline-formula>.</p><p>7. The variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x26.png" xlink:type="simple"/></inline-formula> is denoted as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x27.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x28.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x29.png" xlink:type="simple"/></inline-formula> is the conjugate operation on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x30.png" xlink:type="simple"/></inline-formula>.</p><p>The transmitted sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x31.png" xlink:type="simple"/></inline-formula> is sent through the channel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x32.png" xlink:type="simple"/></inline-formula> and is interfered with noise<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x33.png" xlink:type="simple"/></inline-formula>. Therefore, the equalizer’s input sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x34.png" xlink:type="simple"/></inline-formula> may be written as:</p><disp-formula id="scirp.51385-formula144"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x35.png"  xlink:type="simple"/></disp-formula><p>where “<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x36.png" xlink:type="simple"/></inline-formula>” denotes the convolution operation. The ideal equalized output may be written as [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] :</p><disp-formula id="scirp.51385-formula145"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x37.png"  xlink:type="simple"/></disp-formula><p>where D is a constant delay and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x38.png" xlink:type="simple"/></inline-formula> is a constant phase shift. Therefore, in the ideal case we may write [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] :</p><disp-formula id="scirp.51385-formula146"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x39.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x40.png" xlink:type="simple"/></inline-formula> is the Kronecker delta function. In this article, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x41.png" xlink:type="simple"/></inline-formula>and D are neglected since the delay D does not influence the source signal recovery and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x42.png" xlink:type="simple"/></inline-formula> can be removed by a decision device [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] . Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x43.png" xlink:type="simple"/></inline-formula> is unknown, it is assumed that some initial guess <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x44.png" xlink:type="simple"/></inline-formula> has been selected for the impulse response of the equalizer [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] . Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x45.png" xlink:type="simple"/></inline-formula> be the system’s impulse response from the transmitted signal to the equalizer’s output for the noiseless case. Therefore, we may write:</p><disp-formula id="scirp.51385-formula147"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x46.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x47.png" xlink:type="simple"/></inline-formula> stands for the difference (error) between the ideal value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x48.png" xlink:type="simple"/></inline-formula> and the guess<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x49.png" xlink:type="simple"/></inline-formula>, i.e.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x50.png" xlink:type="simple"/></inline-formula>, [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] . It is assumed that in the latter stages of the de-convolutional process,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x51.png" xlink:type="simple"/></inline-formula>. Convolving <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x52.png" xlink:type="simple"/></inline-formula> with the received sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x53.png" xlink:type="simple"/></inline-formula> (1), we obtain:</p><disp-formula id="scirp.51385-formula148"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x54.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x55.png" xlink:type="simple"/></inline-formula> is the noise that succeeded passing the equalizer.</p><p>Substituting (4) into (5) yields:</p><disp-formula id="scirp.51385-formula149"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x56.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x57.png" xlink:type="simple"/></inline-formula> is the convolutional noise, that causes the residual intersymbol interference (ISI) appearance which is derived from the difference between the ideal equalizer’s coefficients and those chosen in the system. Generally, the ISI is used as an equalizer’s performance measure and is defined as:</p><disp-formula id="scirp.51385-formula150"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x58.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x59.png" xlink:type="simple"/></inline-formula> is the component of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x60.png" xlink:type="simple"/></inline-formula>, given in (4), having the maximal absolute value.</p><p>Next, let us define:</p><disp-formula id="scirp.51385-formula151"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x61.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x62.png" xlink:type="simple"/></inline-formula> has the statistically property of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x63.png" xlink:type="simple"/></inline-formula>. The mean of the convolutional noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x64.png" xlink:type="simple"/></inline-formula> may be written as:</p><disp-formula id="scirp.51385-formula152"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x65.png"  xlink:type="simple"/></disp-formula><p>since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x66.png" xlink:type="simple"/></inline-formula>, (9) may be written as:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x67.png" xlink:type="simple"/></inline-formula>. The mean of the equalizer’s output noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x68.png" xlink:type="simple"/></inline-formula> may be written as:</p><disp-formula id="scirp.51385-formula153"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x69.png"  xlink:type="simple"/></disp-formula><p>according to assumption 6 from this section,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x70.png" xlink:type="simple"/></inline-formula>. Therefore, (10) may be written as:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x71.png" xlink:type="simple"/></inline-formula>. The mean of (6) may be written with the help of (9) and (10) as:</p><disp-formula id="scirp.51385-formula154"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x72.png"  xlink:type="simple"/></disp-formula><p>Therefore, we may have with the help of (11):</p><disp-formula id="scirp.51385-formula155"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x73.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x74.png" xlink:type="simple"/></inline-formula> has the statistically property of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x75.png" xlink:type="simple"/></inline-formula>. Our next step is performing the adaptation mecha- nism of the equalizer which is based on a predefined cost function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x76.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.51385-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref18">18</xref>] . Thus, according to [<xref ref-type="bibr" rid="scirp.51385-ref19">19</xref>] by using (12) the update equation is given by:</p><disp-formula id="scirp.51385-formula156"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x77.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x78.png" xlink:type="simple"/></inline-formula> is the step-size, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x79.png" xlink:type="simple"/></inline-formula>is the equalizer’s vector, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x80.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x81.png" xlink:type="simple"/></inline-formula> is the</p><p>equalizer’s tap length. The operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x82.png" xlink:type="simple"/></inline-formula> denotes for transpose of the function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x83.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. Residual ISI for the Noisy Case with Biased Input Signal</title><p>In this section, a closed-form approximated expression is derived for the residual ISI valid for biased input signals.</p><p>Theorem: Consider the following assumptions:</p><p>1. The source signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x84.png" xlink:type="simple"/></inline-formula> is a rectangular biased 16QAM (Quadrature Amplitude Modulation) signal (where the real part of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x85.png" xlink:type="simple"/></inline-formula> is independent with the imaginary part of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x86.png" xlink:type="simple"/></inline-formula>) with a known mean.</p><p>2. The convolutional noise<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x87.png" xlink:type="simple"/></inline-formula>, is a zero mean, white Gaussian process with variance<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x88.png" xlink:type="simple"/></inline-formula>. The real and imaginary parts of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x89.png" xlink:type="simple"/></inline-formula> are denoted as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x90.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x91.png" xlink:type="simple"/></inline-formula> respectively. In the following we denote<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x92.png" xlink:type="simple"/></inline-formula>.</p><p>3. The convolutional noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x93.png" xlink:type="simple"/></inline-formula> and the source signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x94.png" xlink:type="simple"/></inline-formula> are independent.</p><p>4. The gain between the source and equalized output signal is equal to one.</p><p>5. The convolutional noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x95.png" xlink:type="simple"/></inline-formula> is independent with the equalizer's output noise<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x96.png" xlink:type="simple"/></inline-formula>.</p><p>6.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x97.png" xlink:type="simple"/></inline-formula>.</p><p>7. The signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x98.png" xlink:type="simple"/></inline-formula> is independent with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x99.png" xlink:type="simple"/></inline-formula>.</p><p>8. The added noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x100.png" xlink:type="simple"/></inline-formula> is i.i.d with zero mean.</p><p>9. The channel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x101.png" xlink:type="simple"/></inline-formula> has real coefficients.</p><p>10. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x102.png" xlink:type="simple"/></inline-formula>can be expressed as a polynomial function of order 3 of the equalized output namely as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x103.png" xlink:type="simple"/></inline-formula>.</p><p>11. The signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x104.png" xlink:type="simple"/></inline-formula> is i.i.d.</p><p>12. The equalizer’s output noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x105.png" xlink:type="simple"/></inline-formula> has variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x106.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x107.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x108.png" xlink:type="simple"/></inline-formula> are the equalizer’s output variances real and imaginary parts of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x109.png" xlink:type="simple"/></inline-formula> respectively. It is assumed that: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x110.png" xlink:type="simple"/></inline-formula></p><p>13.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x111.png" xlink:type="simple"/></inline-formula>.</p><p>The residual ISI expressed in dB units may be defined as:</p><disp-formula id="scirp.51385-formula157"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x112.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x113.png" xlink:type="simple"/></inline-formula> is the absolute value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x114.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x115.png" xlink:type="simple"/></inline-formula> is defined by:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x116.png" xlink:type="simple"/></inline-formula>for and</p><p>or</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x119.png" xlink:type="simple"/></inline-formula>for</p><p>and</p><disp-formula id="scirp.51385-formula158"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x121.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.51385-formula159"><graphic  xlink:href="http://html.scirp.org/file/7-3400365x122.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51385-formula160"><graphic  xlink:href="http://html.scirp.org/file/7-3400365x123.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51385-formula161"><graphic  xlink:href="http://html.scirp.org/file/7-3400365x124.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51385-formula162"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x125.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51385-formula163"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x126.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x127.png" xlink:type="simple"/></inline-formula> is the channel length, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x128.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x129.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x130.png" xlink:type="simple"/></inline-formula>are properties of the chosen equalizer and found by</p><disp-formula id="scirp.51385-formula164"><graphic  xlink:href="http://html.scirp.org/file/7-3400365x131.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x132.png" xlink:type="simple"/></inline-formula> is the real part of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x133.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x134.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x135.png" xlink:type="simple"/></inline-formula>are the real and imaginary parts of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x136.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x137.png" xlink:type="simple"/></inline-formula>is the</p><p>variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x138.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x139.png" xlink:type="simple"/></inline-formula>is the real part of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x140.png" xlink:type="simple"/></inline-formula>), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x141.png" xlink:type="simple"/></inline-formula>is the variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x142.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x143.png" xlink:type="simple"/></inline-formula> is given by: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x144.png" xlink:type="simple"/></inline-formula></p><p>Comments:</p><p>1. It should be noted that assumptions 2 - 5, are precisely similar to those made by [<xref ref-type="bibr" rid="scirp.51385-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.51385-ref20">20</xref>] .</p><p>2. It should be mentioned out that our expression for the residual ISI (14) looks quite similar to the residual ISI expression given in [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] . But, they are very different since the input signal <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x145.png" xlink:type="simple"/></inline-formula> is biased in our case, while in [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] it is unbiased. Thus, the expression for B (17), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x146.png" xlink:type="simple"/></inline-formula>(in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x147.png" xlink:type="simple"/></inline-formula>) (15) and ISI are different.</p><p>Proof:</p><p>By using (5), (8) and (12), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x148.png" xlink:type="simple"/></inline-formula>may be written as:</p><disp-formula id="scirp.51385-formula165"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x149.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x150.png" xlink:type="simple"/></inline-formula> is the unbiased equalizer’s output (the equalizer’s output with zero mean). Next, we develop <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x151.png" xlink:type="simple"/></inline-formula> by using (4):</p><disp-formula id="scirp.51385-formula166"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x152.png"  xlink:type="simple"/></disp-formula><p>Substituting (19) into (18) and by using (4) we obtain:</p><disp-formula id="scirp.51385-formula167"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x153.png"  xlink:type="simple"/></disp-formula><p>By substituting (8) into (20) and using the relation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x154.png" xlink:type="simple"/></inline-formula> we obtain:</p><disp-formula id="scirp.51385-formula168"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x155.png"  xlink:type="simple"/></disp-formula><p>Please note that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x156.png" xlink:type="simple"/></inline-formula>. Thus, (21) is quite similar to the case where the sent and equalized output signals are unbiased as in [<xref ref-type="bibr" rid="scirp.51385-ref15">15</xref>] , [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] . Thus, we may use the equations for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x157.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x158.png" xlink:type="simple"/></inline-formula> from [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] . However, the expressions for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x159.png" xlink:type="simple"/></inline-formula>, B and ISI need to be developed from the beginning since the input signal is biased unlike in [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] . Let us define<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x160.png" xlink:type="simple"/></inline-formula>. According to [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] :</p><disp-formula id="scirp.51385-formula169"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x161.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x162.png" xlink:type="simple"/></inline-formula>. Therefore, by substituting (8) and (1) into (22), we obtain:</p><disp-formula id="scirp.51385-formula170"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x163.png"  xlink:type="simple"/></disp-formula><p>From (23) we obtain:</p><disp-formula id="scirp.51385-formula171"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x164.png"  xlink:type="simple"/></disp-formula><p>which may be written as:</p><disp-formula id="scirp.51385-formula172"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x165.png"  xlink:type="simple"/></disp-formula><p>By using assumptions 6, 7, 8 and 11 (from this section) we obtain:</p><disp-formula id="scirp.51385-formula173"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x166.png"  xlink:type="simple"/></disp-formula><p>Let us define:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x167.png" xlink:type="simple"/></inline-formula>. Therefore, (26) becomes:</p><disp-formula id="scirp.51385-formula174"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x168.png"  xlink:type="simple"/></disp-formula><p>Our next step is developing the following expression:</p><disp-formula id="scirp.51385-formula175"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x169.png"  xlink:type="simple"/></disp-formula><p>which is a part of the expression for B (27). Since the channel’s impulse response decays in time, (28) may be written as:</p><disp-formula id="scirp.51385-formula176"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x170.png"  xlink:type="simple"/></disp-formula><p>By substituting (29) into (27) we obtain:</p><disp-formula id="scirp.51385-formula177"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x171.png"  xlink:type="simple"/></disp-formula><p>Next, we turn to calculate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x172.png" xlink:type="simple"/></inline-formula>:</p><p>We recall the expression for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x173.png" xlink:type="simple"/></inline-formula> and convolve both sides with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x174.png" xlink:type="simple"/></inline-formula> as it was done in [<xref ref-type="bibr" rid="scirp.51385-ref21">21</xref>] :</p><disp-formula id="scirp.51385-formula178"><graphic  xlink:href="http://html.scirp.org/file/7-3400365x175.png"  xlink:type="simple"/></disp-formula><p>Therefore, for the latter stages of the de-convolution process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x176.png" xlink:type="simple"/></inline-formula> may be approximated by:</p><disp-formula id="scirp.51385-formula179"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x177.png"  xlink:type="simple"/></disp-formula><p>From (31), we obtain:</p><disp-formula id="scirp.51385-formula180"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x178.png"  xlink:type="simple"/></disp-formula><p>Next, the expectation operator is applied on (32):</p><disp-formula id="scirp.51385-formula181"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x179.png"  xlink:type="simple"/></disp-formula><p>By substituting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x180.png" xlink:type="simple"/></inline-formula> we obtain:</p><disp-formula id="scirp.51385-formula182"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x181.png"  xlink:type="simple"/></disp-formula><p>From assumption 12 (in this section) we obtain:</p><disp-formula id="scirp.51385-formula183"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x182.png"  xlink:type="simple"/></disp-formula><p>It should be pointed out that (35) looks similar to the equalizer's output noise variance at [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] . But, in our case</p><p>here (35), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x183.png" xlink:type="simple"/></inline-formula>is biased while in [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] it is not. Therefore, the value for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x184.png" xlink:type="simple"/></inline-formula> is different here from that in [<xref ref-type="bibr" rid="scirp.51385-ref16">16</xref>] .</p><p>Next, we turn to calculate the expression for the residual ISI applicable for the biased case. For that purpose,</p><p>we calculate first the expression for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x185.png" xlink:type="simple"/></inline-formula>. By using (4) and (5) and assuming the noiseless case, we obtain:</p><disp-formula id="scirp.51385-formula184"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x186.png"  xlink:type="simple"/></disp-formula><p>Thus, by using (8), we obtain:</p><disp-formula id="scirp.51385-formula185"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x187.png"  xlink:type="simple"/></disp-formula><p>which may be written as:</p><disp-formula id="scirp.51385-formula186"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x188.png"  xlink:type="simple"/></disp-formula><p>From (38) we obtain:</p><disp-formula id="scirp.51385-formula187"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x189.png"  xlink:type="simple"/></disp-formula><p>By applying the expectation operator on both sides of (39) and using assumption 11 (from this section), we obain:</p><disp-formula id="scirp.51385-formula188"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x190.png"  xlink:type="simple"/></disp-formula><p>Thus, the expression for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x191.png" xlink:type="simple"/></inline-formula> (for the noiseless case) may be written with the help of (6) by:</p><disp-formula id="scirp.51385-formula189"><label>(41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x192.png"  xlink:type="simple"/></disp-formula><p>By using assumption 3 (from this section), (41) may be written as:</p><disp-formula id="scirp.51385-formula190"><label>(42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x193.png"  xlink:type="simple"/></disp-formula><p>Next, we turn to calculate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x194.png" xlink:type="simple"/></inline-formula>. By using (8) we obtain:</p><disp-formula id="scirp.51385-formula191"><label>(43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x195.png"  xlink:type="simple"/></disp-formula><p>Substituting (43) into (42) we obtain:</p><disp-formula id="scirp.51385-formula192"><label>(44)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x196.png"  xlink:type="simple"/></disp-formula><p>Substituting (44) into (40) leads to:</p><disp-formula id="scirp.51385-formula193"><label>(45)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x197.png"  xlink:type="simple"/></disp-formula><p>For the ideal case, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x198.png" xlink:type="simple"/></inline-formula>(4)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x199.png" xlink:type="simple"/></inline-formula>. Thus, at the convergence state, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x200.png" xlink:type="simple"/></inline-formula>(4) is very small compared to</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x201.png" xlink:type="simple"/></inline-formula>(4). Thus, by looking at the element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x202.png" xlink:type="simple"/></inline-formula> from (45), we may neglect all</p><p>multiplications of different index elements. Then (45) may be written as:</p><disp-formula id="scirp.51385-formula194"><label>(46)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x203.png"  xlink:type="simple"/></disp-formula><p>By using (43), we may write (46) as:</p><disp-formula id="scirp.51385-formula195"><label>(47)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x204.png"  xlink:type="simple"/></disp-formula><p>From (7), (47) may be written for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x205.png" xlink:type="simple"/></inline-formula> as:</p><disp-formula id="scirp.51385-formula196"><label>(48)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x206.png"  xlink:type="simple"/></disp-formula><p>From assumptions 2 and 13 (from this section), we may use the relation:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x207.png" xlink:type="simple"/></inline-formula>. Therefore, (48) may be written as:</p><disp-formula id="scirp.51385-formula197"><label>(49)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x208.png"  xlink:type="simple"/></disp-formula><p>This completes our proof.</p></sec><sec id="s4"><title>4. Simulation</title><p>In this section, our new proposed expression for the residual ISI (14) was tested via simulation, where we used Godard’s algorithm [<xref ref-type="bibr" rid="scirp.51385-ref7">7</xref>] . In our simulation we used various step-size parameters, tap length, types of channels, SNR and biased input signals. The equalizer’s taps for Godard's algorithm [<xref ref-type="bibr" rid="scirp.51385-ref7">7</xref>] were updated according to:</p><disp-formula id="scirp.51385-formula198"><label>(50)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x209.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x210.png" xlink:type="simple"/></inline-formula>is the step-size. The values for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x211.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x212.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x213.png" xlink:type="simple"/></inline-formula> corresponding to Godard’s [<xref ref-type="bibr" rid="scirp.51385-ref7">7</xref>] algorithm are defined as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x214.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x215.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x210.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x216.png" xlink:type="simple"/></inline-formula> respectively and are given by:</p><disp-formula id="scirp.51385-formula199"><label>(51)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-3400365x217.png"  xlink:type="simple"/></disp-formula><p>Two different input sources were considered: 1) A biased 16QAM, a modulation using &#177; {1, 3} levels for in- phase and quadrature components in addition to a given bias. The bias is the same for the real and imaginary axes. 2) A uniformly distributed input signal within [−0.5, 1.5] for the x and y axis where the two axis are independent. The following five different channels were used:</p><p>Channel 1: The channel parameters were taken according to [<xref ref-type="bibr" rid="scirp.51385-ref22">22</xref>] :</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x218.png" xlink:type="simple"/></inline-formula>.</p><p>Channel 2: The channel parameters were determined according to [<xref ref-type="bibr" rid="scirp.51385-ref17">17</xref>] :</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x219.png" xlink:type="simple"/></inline-formula>.</p><p>Channel 3: The channel parameters were determined according to [<xref ref-type="bibr" rid="scirp.51385-ref20">20</xref>] :</p><disp-formula id="scirp.51385-formula200"><graphic  xlink:href="http://html.scirp.org/file/7-3400365x220.png"  xlink:type="simple"/></disp-formula><p>Channel 4: The channel parameters are:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x221.png" xlink:type="simple"/></inline-formula>.</p><p>Channel 5: The channel parameters were determined according to [<xref ref-type="bibr" rid="scirp.51385-ref23">23</xref>] :</p><disp-formula id="scirp.51385-formula201"><graphic  xlink:href="http://html.scirp.org/file/7-3400365x222.png"  xlink:type="simple"/></disp-formula><p>Figures 2-9 are the simulated performance of (50) for the biased 16QAM input case, namely the ISI as a function of iteration number for various step-size parameters, channel characteristics, various SNR values and for three different biases, compared with the calculated residual ISI expression (14) proposed in this paper. According to Figures 2-9, the residual ISI obtained by (14) is very close to the simulated results.</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16 QAM biased source input going through channel 1 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x224.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s tap length and input signal mean parameters were set to 43 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x223.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 2 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x226.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s tap length and input signal mean para- meters were set to 13 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x225.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 3 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x228.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s tap length and input signal mean parameters were set to 67 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x227.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 1 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x230.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s tap length and input signal mean parameters were set to 53 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x229.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 3 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x232.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s tap length and input signal mean parameters were set to 41 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x231.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel4 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x234.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s tap length and input signal mean para- meters were set to 193 and 2 + j2 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x233.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 4 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x236.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s tap length and input signal mean para- meters were set to 193 and 2 + j2 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x235.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel5 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x238.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s tap length and input signal mean parameters were set to 123 and 1 + j1 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x237.png"/></fig><p>Figures 10-18 are the simulated performance of (50) for the biased 16QAM input case, namely the ISI as a function of iteration number for various equalizer's tap length, channel characteristics, various SNR values and for two different biases, compared with the calculated residual ISI expression (14). Figures 10-18 show a high correlation between the simulated results and those calculated with (14).</p><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 2 for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x240.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 5e−6 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x239.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 3 for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x242.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 1e−6 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x241.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 1 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x244.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 2e−6 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x243.png"/></fig><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 2 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x246.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 5e−6 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x245.png"/></fig><fig id="fig14"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>4</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 1 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x248.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 2e−6 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x247.png"/></fig><fig id="fig15"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>5</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 3 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x250.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 1e−6 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x249.png"/></fig><fig id="fig16"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>6</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 4 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x252.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 1e−6 and 2 + j2 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x251.png"/></fig><fig id="fig17"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>7</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 4 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x254.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 1e−6 and 2 + j2 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x253.png"/></fig><p><xref ref-type="fig" rid="fig1">Figure 1</xref>9 and <xref ref-type="fig" rid="fig2">Figure 2</xref>0 illustrate the simulated performance of (50) for the biased 16QAM input case, namely the ISI as a function of iteration number for various SNR values and two different input biases and channels, compared with the calculated residual ISI expression (14). <xref ref-type="fig" rid="fig1">Figure 1</xref>9 and <xref ref-type="fig" rid="fig2">Figure 2</xref>0 show a high correlation between the simulated results and those calculated with (14).</p><p>Figures 21-23 illustrate the simulated performance of (50) for the biased 16QAM input case, namely the ISI as a function of iteration number for various biases, two different SNR values and three channel cases, compared with the calculated residual ISI expression (14). Figures 21-23 show a high correlation between the simulated results and those calculated with (14).</p><fig id="fig18"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>8</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 4 for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-3400365x256.png" xlink:type="simple"/></inline-formula>. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 1e−6 and 2 + j2 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x255.png"/></fig><fig id="fig19"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>9</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 2 for tap length = 33. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 6e−6 and 2 + j2 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x257.png"/></fig><fig id="fig20"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>0</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 3 for tap length = 41. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and input signal mean parameters were set to 6e−6 and 3 + j3 respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x258.png"/></fig><fig id="fig21"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>1</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 3 for tap length = 41. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and SNR parameters were set to 6e−6 and 10 [dB] respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x259.png"/></fig><fig id="fig22"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>2</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 2 for tap length = 13. The averaged results were obtained in 100 Monte Carlo trials. The equalizer’s step-size and SNR para- meters were set to 6e−6 and 25 [dB] respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x260.png"/></fig><fig id="fig23"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>3</label><caption><title> A comparison between the simulated and calculated residual ISI for the 16QAM biased source input going through channel 5 for tap length = 123. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and SNR parameters were set to 4e−6 and 25 [dB] respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x261.png"/></fig><p>Figures 24-26 illustrate the simulated performance of (50) for the uniformly source input, namely the ISI as a function of iteration number for three different values for the SNR, compared with the calculated residual ISI expression (14). Figures 24-26 show a high correlation between the simulated results and those calculated with (14).</p><fig id="fig24"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>4</label><caption><title> A comparison between the simulated and calculated residual ISI for the uniformly distributed source input within [−0.5 1.5] going through channel 2 for tap length = 67. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and SNR parameters were set to 133e−6 and 40 [dB] respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x262.png"/></fig><fig id="fig25"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>5</label><caption><title> A comparison between the simulated and calculated residual ISI for the uniformly distributed source input within [−0.5 1.5] going through channel 2 for tap length = 67. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and SNR parameters were set to 133e−6 and 20 [dB] respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x263.png"/></fig><fig id="fig26"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>6</label><caption><title> A comparison between the simulated and calculated residual ISI for the uniformly distributed source input within [−0.5 1.5] going through channel 2 for tap length = 67. The averaged results were obtained in 20 Monte Carlo trials. The equalizer’s step-size and SNR parameters were set to 133e−6 and 10 [dB] respectively</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-3400365x264.png"/></fig></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, we proposed an approximated closed-form expression for the residual ISI obtained by blind adaptive equalizer, where the error of the equalized output signal may be expressed as a polynomial function of order 3. This new expression is valid for the noisy and biased input case and depends on the step-size parameter, equalizer’s tap length, SNR, channel power and input signal statistics. This new proposed expression may be considered as a general closed-form expression for the residual ISI, where the previous proposed expressions from the literature are only special cases of it. Simulation results have shown a high correlation between the simulated results for the residual ISI and those that were calculated from our new proposed expression.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.51385-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Pinchas, M. 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