<?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.2017.82004</article-id><article-id pub-id-type="publisher-id">JSIP-76079</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>
 
 
  A New Equalization Performance Analyzing Method for Blind Adaptive Equalizers Inspired by Maximum Time Interval Error
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guilad</surname><given-names>Suissa</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>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>monikap@ariel.ac.il(MP)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>05</month><year>2017</year></pub-date><volume>08</volume><issue>02</issue><fpage>42</fpage><lpage>64</lpage><history><date date-type="received"><day>February</day>	<month>22,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>May</month>	<year>7,</year>	</date><date date-type="accepted"><day>May</day>	<month>10,</month>	<year>2017</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Up to now, the Mean Square Error (MSE) criteria, the residual Inter-Symbol Interference (ISI) and the Bit-Error-Rate (BER) were used to analyze the equalization performance of a blind adaptive equalizer in its convergence state. In this paper, we propose an additional tool (additional to the ISI, MSE and BER) for analyzing the equalization performance in the convergence region based on the Maximum Time Interval Error (MTIE) criterion that is used for the specification of clock stability requirements in telecommunications standards. This new tool preserves the short term statistical information unlike the already known tools (BER, ISI, MSE) that lack this information. Simulation results will show that the equalization performance of a blind adaptive equalizer obtained in the convergence region for two different channels is seen to be approximately the same from the residual ISI and MSE point of view while this is not the case with our new proposed tool. Thus, our new proposed tool might be considered as a more sensitive tool compared to the ISI and MSE method.
 
</p></abstract><kwd-group><kwd>Blind Equalizer</kwd><kwd> ISI</kwd><kwd> MSE</kwd><kwd> BER</kwd><kwd> MTIE</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In data communication, signals transmitted between remote locations often encounter a signal-altering physical channel (in wired communications or in wireless communications). These physical channels may cause signal distortion, including echoes and frequency-selective filtering of the transmitted signal [<xref ref-type="bibr" rid="scirp.76079-ref1">1</xref>] . In digital communications, a critical manifestation of distortion is ISI, whereby symbols transmitted before and after a given symbol corrupt the detection of that symbol. All physical channels (at high enough data rates) tend to exhibit ISI [<xref ref-type="bibr" rid="scirp.76079-ref1">1</xref>] .</p><p>An effective way to overcome the ISI is using adaptive equalization technology. An adaptive equalizer is an inverse filter which reduces the effects of ISI by deconvolving the transmitted data sequence from the time varying channel response [<xref ref-type="bibr" rid="scirp.76079-ref2">2</xref>] . The conventional approach for adaptive filtering usually requires a training sequence where the desired response is compared to the received symbols and an estimated error is produced which helps adjusting the coefficients of the adaptive filter [<xref ref-type="bibr" rid="scirp.76079-ref3">3</xref>] .</p><p>When a training session is impossible or very costly, blind equalizers are a convenient solution. Blind equalization 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.76079-ref4">4</xref>] . The algorithm itself generates an estimate of the desired response by applying a nonlinear transformation to sequences involved in the adaptation process [<xref ref-type="bibr" rid="scirp.76079-ref4">4</xref>] . Adaptive equalizers are widely used in digital communications systems to remove the ISI introduced by dispersive channels [<xref ref-type="bibr" rid="scirp.76079-ref5">5</xref>] . In order to avoid the transmission of pilot sequences and use the channel bandwidth in an efficient manner the blind equalization techniques are highly desirable. A popular approach for the blind adaptation of finite impulse response (FIR) equalizers is the constant modulus algorithm [<xref ref-type="bibr" rid="scirp.76079-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref7">7</xref>] and its variant known as multi modulus algorithm [<xref ref-type="bibr" rid="scirp.76079-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref10">10</xref>] due to their low computational cost [<xref ref-type="bibr" rid="scirp.76079-ref5">5</xref>] .</p><p>Today, in order to analyze the equalization performance, namely, to see how much the equalizer overcomes the ISI, the ISI, the MSE or the BER are simulated. The ISI, BER and MSE provide long term statistical information in the steady state region (convergence state). Thus, for instance, there may be cases where two different simulation results obtained in the convergence region with different channels (but using the same algorithm for reducing the ISI), may lead approximately to the same residual ISI but may have different short term statistical information. Namely, in the short term, there may be seen different amounts of errors for the two different channels. Thus, one channel is preferable over the other. Therefore, the following question may arise: is it possible to get also short term statistical information of the blind adaptive equalization performance in the convergence region?</p><p>A major topic of discussion in standard bodies dealing with network synchronization [<xref ref-type="bibr" rid="scirp.76079-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref13">13</xref>] is clock noise characterization and measurement [<xref ref-type="bibr" rid="scirp.76079-ref14">14</xref>] . MTIE is historically one of the main time-domain quantities for the specification of clock stability requirements in telecommunications standards [<xref ref-type="bibr" rid="scirp.76079-ref14">14</xref>] . Among the quantities considered in international standards for specification of phase and frequency stability requirements, the MTIE has played historically a major role for characterizing time and frequency performance in digital telecommunications networks [<xref ref-type="bibr" rid="scirp.76079-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref19">19</xref>] and is a rough measure of the peak time deviation of a clock with respect to a known reference [<xref ref-type="bibr" rid="scirp.76079-ref20">20</xref>] .</p><p>The purpose of this work is to provide an additional tool (additional to the ISI, MSE and BER) for diagnosing equalization performance in the steady state region based on the MTIE method used in the telecommunication area. Simulation results will show that our new proposed tool provides us short term as well as long term statistical information and is able to show differences in the equalization performance comparison obtained in the convergence state even when it is quite difficult to see it with the MSE and ISI method.</p><p>The paper is organized as follows: after having described the system under consideration in Section II, Section III describes our new proposed tool for analyzing the equalization performance in the convergence region based on the MTIE. In Section IV simulation results are given using our new proposed tool compared with the existing methods (MSE, ISI) and Section V is our conclusion.</p></sec><sec id="s2"><title>2. System Description</title><p>In this section we consider the system described in <xref ref-type="fig" rid="fig1">Figure 1</xref> with the following assumptions:</p><p>1) The input sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x2.png" xlink:type="simple"/></inline-formula> belongs to a real or two independent quadrature carrier case constellation input with variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x3.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x4.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x5.png" xlink:type="simple"/></inline-formula> are the real and imaginary parts of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x6.png" xlink:type="simple"/></inline-formula> respectively.</p><p>2) The unknown channel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x7.png" xlink:type="simple"/></inline-formula> is a possibly non-minimum phase linear time-invariant filter, FIR filter.</p><p>3) The equalizer <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x8.png" xlink:type="simple"/></inline-formula> is a FIR filter.</p><p>4) The noise <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x9.png" xlink:type="simple"/></inline-formula> is an additive Gaussian white noise with zero mean and variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x10.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x11.png" xlink:type="simple"/></inline-formula>is the expectation operator and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x12.png" xlink:type="simple"/></inline-formula> is the conjugate operation).</p><p>For simplicity, we use in this paper only the 16QAM constellation input (<xref ref-type="fig" rid="fig2">Figure 2</xref>) for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x13.png" xlink:type="simple"/></inline-formula>. The sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x14.png" xlink:type="simple"/></inline-formula> is transmitted through the channel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x15.png" xlink:type="simple"/></inline-formula> and is corrupted with noise<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x16.png" xlink:type="simple"/></inline-formula>. Therefore, the equalizer’s input sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x17.png" xlink:type="simple"/></inline-formula> may be written as:</p><disp-formula id="scirp.76079-formula82"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x18.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x19.png" xlink:type="simple"/></inline-formula> denotes the convolution operation. The equalized output sequence is defined by:</p><disp-formula id="scirp.76079-formula83"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x20.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x21.png" xlink:type="simple"/></inline-formula> is the sum of the convolutional error due to non-ideal coefficients</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Block diagram of a communication system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x22.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> 16QAM Constellation Diagram</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x23.png"/></fig><p>of the equalizer (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula> is the Kronecker delta function) and the noise error passed via the filter (equalizer). It should be pointed out that for the noiseless and ideal case the equalized output is a delayed version of the input multiplied by a constant phase shift (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x27.png" xlink:type="simple"/></inline-formula> is a constant delay and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x28.png" xlink:type="simple"/></inline-formula> is a constant phase shift). But, according to [<xref ref-type="bibr" rid="scirp.76079-ref21">21</xref>] , we can assume in (2) that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x29.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x30.png" xlink:type="simple"/></inline-formula>, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x31.png" xlink:type="simple"/></inline-formula> does not affect the reconstruction of the original input sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x32.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x33.png" xlink:type="simple"/></inline-formula> can be removed by a decision device. Next we turn to the adaptation mechanism of the equalizer [<xref ref-type="bibr" rid="scirp.76079-ref22">22</xref>] - [<xref ref-type="bibr" rid="scirp.76079-ref28">28</xref>] by using Godard’s algorithm [<xref ref-type="bibr" rid="scirp.76079-ref6">6</xref>] :</p><disp-formula id="scirp.76079-formula84"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x34.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x35.png" xlink:type="simple"/></inline-formula> is the step-size parameter, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x36.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x37.png" xlink:type="simple"/></inline-formula> is the equalizer’s tap length.</p></sec><sec id="s3"><title>3. New Tool for Equalization Performance Analysis</title><p>In this section we introduce our new proposed tool for the blind equalization performance analysis based on a network clock synchronization measurement method, namely, the MTIE measurement method.</p><p>For a given clock, the time error function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x38.png" xlink:type="simple"/></inline-formula> between its time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x39.png" xlink:type="simple"/></inline-formula> and a reference time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x40.png" xlink:type="simple"/></inline-formula> is defined as [<xref ref-type="bibr" rid="scirp.76079-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref29">29</xref>] :</p><disp-formula id="scirp.76079-formula85"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x41.png"  xlink:type="simple"/></disp-formula><p>Thus, the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x42.png" xlink:type="simple"/></inline-formula> which is the maximum peak-to-peak variation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x43.png" xlink:type="simple"/></inline-formula> (4) for all the possible observation intervals <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x44.png" xlink:type="simple"/></inline-formula> within a measurement period <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x45.png" xlink:type="simple"/></inline-formula> (see <xref ref-type="fig" rid="fig3">Figure 3</xref> recalled from [<xref ref-type="bibr" rid="scirp.76079-ref20">20</xref>] ) can be defined according to [<xref ref-type="bibr" rid="scirp.76079-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.76079-ref29">29</xref>] as:</p><disp-formula id="scirp.76079-formula86"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x46.png"  xlink:type="simple"/></disp-formula><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Definition of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x48.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x47.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The clock TIE and MTIE measurements in the OSA 4520 GPS-SP, a stand-alone GPS receiver. (a) The clock TIE measurement the in OSA 4520 GPS-SP GPS receiver. (b) The lower line is the clock MTIE measurement in the OSA 4520 GPS-SP GPS receiver while the upper line is ITU-T G.811 recommendation</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x49.png"/></fig><p>An example of a MTIE measurement of a clock is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref> (recalled from [<xref ref-type="bibr" rid="scirp.76079-ref30">30</xref>] ) where <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) are the TIE and MTIE measurements respectively according to [<xref ref-type="bibr" rid="scirp.76079-ref20">20</xref>] . Please note that according to <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) the clock has less time errors for small intervals while the time error increases for bigger intervals i.e. the clock has less time errors in short term and the time error increases in long term.</p><p>Next, we adopt the concept of the MTIE measurement method from the telecommunication area to the world of equalization performance. Based on (2), we denote</p><disp-formula id="scirp.76079-formula87"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x50.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x51.png" xlink:type="simple"/></inline-formula> belongs to a real or two independent quadrature carrier case constellation input, we refer in the following only to the real parts of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x52.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x53.png" xlink:type="simple"/></inline-formula> to produce <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x54.png" xlink:type="simple"/></inline-formula> (6). Next, based on (5), we introduce<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x55.png" xlink:type="simple"/></inline-formula>, the maximum peak-to-peak variation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x56.png" xlink:type="simple"/></inline-formula> (6) for all the possible observation intervals <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x57.png" xlink:type="simple"/></inline-formula> (see <xref ref-type="fig" rid="fig5">Figure 5</xref>) which can be defined as:</p><disp-formula id="scirp.76079-formula88"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x58.png"  xlink:type="simple"/></disp-formula><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Peak-to-peak of the error sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x60.png" xlink:type="simple"/></inline-formula> within <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x61.png" xlink:type="simple"/></inline-formula> samples</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x59.png"/></fig><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> ConE and MConE measurements of an equalization process using Godard’s algorithm with Signal to Noise Ratio (SNR) 20 [dB], the equalizer step size was set to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x63.png" xlink:type="simple"/></inline-formula>. The equalizer’s tap length was set to 13. (a) ConE measurement of an equalization process. (b) MConE measurement of an equalization process.</title></caption><fig id ="fig6_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x62.png"/></fig></fig-group><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x64.png" xlink:type="simple"/></inline-formula> is the length of the interval window (in terms of discrete samples).</p><p>An example for a MConE measurement belonging to an equalization process in the convergence state is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref> where <xref ref-type="fig" rid="fig6">Figure 6</xref>(a) and <xref ref-type="fig" rid="fig6">Figure 6</xref>(b) are the ConE (6) and MConE (7) measurements respectively.</p><p>The resemblance between the example in <xref ref-type="fig" rid="fig4">Figure 4</xref> and the example in <xref ref-type="fig" rid="fig6">Figure 6</xref> is due to the nature of the time error (<xref ref-type="fig" rid="fig4">Figure 4</xref>(a)) and the error <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x65.png" xlink:type="simple"/></inline-formula> (<xref ref-type="fig" rid="fig6">Figure 6</xref>(a)). In both TE (4) and ConE (6) calculations, a reference signal is needed (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x66.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x67.png" xlink:type="simple"/></inline-formula> for the TE and ConE calculations respectively).</p></sec><sec id="s4"><title>4. Simulations Results</title><p>In this section we present several simulation results using the MConE tool for obtaining the blind adaptive equalization performance using Godard’s algorithm [<xref ref-type="bibr" rid="scirp.76079-ref6">6</xref>] with a 16QAM input sequence for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x68.png" xlink:type="simple"/></inline-formula>, compared to the existing methods (ISI and MSE).</p><p>As already mentioned earlier in this paper, our new proposed tool for diagnosing equalization performance in the steady state region might be considered as a more sensitive tool compared to the ISI and MSE method. But, it should be kept in mind that not every difference seen in the equalization performance comparison with our new proposed tool automatically leads to errors in the recovered symbols. Thus, to see this, we denote in the following Error Accumulation as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x69.png" xlink:type="simple"/></inline-formula> (8) defined by:</p><disp-formula id="scirp.76079-formula89"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-3400492x70.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x71.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x72.png" xlink:type="simple"/></inline-formula> is the distinction threshold (e.g. in 16QAM the threshold is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x73.png" xlink:type="simple"/></inline-formula> for the real or the imaginary part). Since we deal in this paper with real or two independent quadrature carrier case constellation (16 QAM), we consider only the real parts of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x74.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x75.png" xlink:type="simple"/></inline-formula> for calculating (6), (7) and (8). From (8), the probability of error as a function of time can be obtained. The following channels <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x76.png" xlink:type="simple"/></inline-formula> were used:</p><p>Channel 1 according to [<xref ref-type="bibr" rid="scirp.76079-ref31">31</xref>] :</p><disp-formula id="scirp.76079-formula90"><graphic  xlink:href="http://html.scirp.org/file/2-3400492x77.png"  xlink:type="simple"/></disp-formula><p>Channel 2 according to [<xref ref-type="bibr" rid="scirp.76079-ref22">22</xref>] :</p><disp-formula id="scirp.76079-formula91"><graphic  xlink:href="http://html.scirp.org/file/2-3400492x78.png"  xlink:type="simple"/></disp-formula><p>Channel 3 according to [<xref ref-type="bibr" rid="scirp.76079-ref32">32</xref>] :</p><disp-formula id="scirp.76079-formula92"><graphic  xlink:href="http://html.scirp.org/file/2-3400492x79.png"  xlink:type="simple"/></disp-formula><p>Figures 7-10 show the simulation results for the ISI, MSE, MConE and Accumulated Error (8) respectively for various tap length values (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x80.png" xlink:type="simple"/></inline-formula>), SNR = 20[dB] and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x81.png" xlink:type="simple"/></inline-formula>. According to <xref ref-type="fig" rid="fig8">Figure 8</xref> it is very difficult to see for which equalizer’s tap length (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x82.png" xlink:type="simple"/></inline-formula>), better equalization performance is obtained from the MSE point of view. From <xref ref-type="fig" rid="fig7">Figure 7</xref> the equalization performance from the ISI point of view is very close for the case of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x83.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x84.png" xlink:type="simple"/></inline-formula>. However, according to <xref ref-type="fig" rid="fig9">Figure 9</xref>, the difference in the equalization performance between the various equalizer’s tap length is seen very clearly. The difference in the equalization performance for the various equalizer’s tap length is also seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>0 in the short range while in the long term the difference in the equalization performance resembles the difference in equalization performance as is seen in <xref ref-type="fig" rid="fig7">Figure 7</xref>.</p><p>Figures 11-14 show the simulation results for the ISI, MSE, MConE and Accumulated Error (8) respectively for two different channels (channel 2 (CH2) and channel 3 (CH3)) and for two different step sizes (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x85.png" xlink:type="simple"/></inline-formula>for channel</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> ISI as a function of iteration number for various equalizer’s tap length. The averaged results were obtained from 50 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x86.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> MSE as a function of iteration number for various equalizer’s tap length. The averaged results were obtained from 50 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x87.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> MConE as a function of the window length for various equalizer’s tap length. The averaged results were obtained from 50 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x88.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Error Accumulation as a function of iteration number for various equalizer’s tap length. The averaged results were obtained from 50 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x89.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> ISI as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x90.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> MSE as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x91.png"/></fig><fig id="fig13"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>3</label><caption><title> MConE as a function of the window length for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x92.png"/></fig><fig id="fig14"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>4</label><caption><title> Error Accumulation as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x93.png"/></fig><p>2 and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x94.png" xlink:type="simple"/></inline-formula> for channel 3) where the equalizer’s tap length was set to 13 (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x95.png" xlink:type="simple"/></inline-formula>) and SNR = 20 [dB]. According to <xref ref-type="fig" rid="fig1">Figure 1</xref>2 it is very difficult to see for which channel better equalization performance is obtained from the MSE point of view. From <xref ref-type="fig" rid="fig1">Figure 1</xref>1 the equalization performance from the ISI point of view is very close for the two channel cases (channel 2 and channel 3). However, according to <xref ref-type="fig" rid="fig1">Figure 1</xref>3 the difference between the equalization performance for the two channels is seen very clearly. In addition the difference in the equalization performance for the two channels is also seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>4 in the short range while in the long term the difference in the equalization performance resembles the difference in the equalization performance as is seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>1.</p><p>Figures 15-18 show the simulation results for the ISI, MSE, MConE and Accumulated Error (8) respectively for two different channels (channel 2 (CH2) and channel 3 (CH3)) and for two different step sizes and equalizer’s tap length (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x96.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x97.png" xlink:type="simple"/></inline-formula>for channel 2 and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x98.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x99.png" xlink:type="simple"/></inline-formula>for channel 3) where SNR = 15 [dB]. According to <xref ref-type="fig" rid="fig1">Figure 1</xref>6 it is very difficult to see for which channel better equalization performance is obtained from the MSE point of view. From <xref ref-type="fig" rid="fig1">Figure 1</xref>5 the equalization performance from the ISI point of view is very close for the two channel cases (channel 2 and channel 3). However, according to <xref ref-type="fig" rid="fig1">Figure 1</xref>7 the difference between the equalization performance for the two channels is seen very clearly. In addition the difference in the equalization performance for the two channels is also seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>8 in the short range while in the long term the difference in the equalization performance resembles the difference in the equalization performance as is seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>5.</p><fig id="fig15"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>5</label><caption><title> ISI as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x100.png"/></fig><fig id="fig16"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>6</label><caption><title> MSE as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x101.png"/></fig><fig id="fig17"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>7</label><caption><title> MConE as a function of the window length for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x102.png"/></fig><fig id="fig18"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>8</label><caption><title> Error Accumulation as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x103.png"/></fig><fig id="fig19"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>9</label><caption><title> ISI as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x104.png"/></fig><p>Figures 19-22 show the simulation results for the ISI, MSE, MConE and Accumulated Error (8) respectively for two different channels (channel 1 (CH1) and channel 2 (CH2)) and for two different step sizes and equalizer’s tap length (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x105.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x106.png" xlink:type="simple"/></inline-formula>for channel 1 and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x107.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x108.png" xlink:type="simple"/></inline-formula>for channel 2) where SNR = 20 [dB]. According to <xref ref-type="fig" rid="fig2">Figure 2</xref>0 it is very difficult to see for which channel better equalization performance is obtained from the MSE point of view. From <xref ref-type="fig" rid="fig1">Figure 1</xref>9 the equalization performance from the ISI point of view is very close for the two channel cases (channel 1 and channel 2). However, according to <xref ref-type="fig" rid="fig2">Figure 2</xref>1 the difference between the equalization performance for the two channels is seen very clearly. In addition the difference in the</p><fig id="fig20"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>0</label><caption><title> MSE as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x109.png"/></fig><fig id="fig21"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>1</label><caption><title> MConE as a function of the window length for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x110.png"/></fig><fig id="fig22"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>2</label><caption><title> Error Accumulation as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x111.png"/></fig><fig id="fig23"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>3</label><caption><title> ISI as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x112.png"/></fig><p>equalization performance for the two channels is also seen in <xref ref-type="fig" rid="fig2">Figure 2</xref>2 in the short range while in the long term the difference in the equalization performance resembles the difference in the equalization performance as is seen in <xref ref-type="fig" rid="fig1">Figure 1</xref>9.</p><p>Figures 23-26 show the simulation results for the ISI, MSE, MConE and Accumulated Error (8) respectively for two different channels (channel 1 (CH1) and channel 3 (CH3)) and for two different step sizes and equalizer’s tap length (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x113.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x114.png" xlink:type="simple"/></inline-formula>for channel 1 and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x115.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x116.png" xlink:type="simple"/></inline-formula>for channel 2) where SNR = 20 [dB]. According to <xref ref-type="fig" rid="fig2">Figure 2</xref>4 it is very difficult to see for which channel better equalization performance is obtained from the MSE point of view. From <xref ref-type="fig" rid="fig2">Figure 2</xref>3 the equalization performance from the ISI point of view is very</p><fig id="fig24"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>4</label><caption><title> MSE as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x117.png"/></fig><fig id="fig25"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>5</label><caption><title> MConE as a function of the window length for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x118.png"/></fig><fig id="fig26"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>6</label><caption><title> Error Accumulation as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x119.png"/></fig><fig id="fig27"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>7</label><caption><title> ISI as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x120.png"/></fig><p>close for the two channel cases (channel 1 and channel 3). However, according to <xref ref-type="fig" rid="fig2">Figure 2</xref>5 and <xref ref-type="fig" rid="fig2">Figure 2</xref>6 the difference between the equalization performance for the two channels is seen very clearly.</p><p>Figures 27-30 show the simulation results for the ISI, MSE, MConE and Accumulated Error (8) respectively for two different channels (channel 2 (CH2) and channel 3 (CH3)) and for two different step sizes and equalizer’s tap length (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x121.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x122.png" xlink:type="simple"/></inline-formula>for channel 2 and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x123.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-3400492x124.png" xlink:type="simple"/></inline-formula>for channel 3) where SNR = 20 [dB]. According to <xref ref-type="fig" rid="fig2">Figure 2</xref>8 it is very difficult to see for which channel better equalization performance is obtained from the MSE point of view. From <xref ref-type="fig" rid="fig2">Figure 2</xref>7 the equalization performance from the ISI point of view is very close for the two channel cases (channel 2 and channel 3). However, according</p><fig id="fig28"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>8</label><caption><title> MSE as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x125.png"/></fig><fig id="fig29"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref>9</label><caption><title> MConE as a function of the window length for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x126.png"/></fig><fig id="fig30"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref>0</label><caption><title> Error Accumulation as a function of iteration number for two channel cases. The averaged results were obtained from 100 Monte Carlo trials</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-3400492x127.png"/></fig><p>to <xref ref-type="fig" rid="fig2">Figure 2</xref>9 and <xref ref-type="fig" rid="fig3">Figure 3</xref>0 the difference between the equalization performance for the two channels is seen very clearly.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, we proposed a new tool for analyzing the equalization performance in the convergence state which can be considered as an additional tool to the literature known methods (ISI, MSE, BER). The new proposed tool is based on the MTIE criterion that is used for the specification of clock stability requirements in telecommunications standards. This new tool preserves the short term statistical information unlike the BER, ISI and MSE method. Thus, our new proposed tool can supply us short term as well as long term statistical information. Simulation results have shown that with our new proposed tool, difference in the equalization performance comparison was clearly seen in the convergence state while this was not the case with the MSE and ISI method. Thus, our new proposed tool for analyzing the equalization performance in the convergence state might be considered as a more sensitive tool compared to the ISI and MSE method.</p></sec><sec id="s6"><title>Acknowledgments</title><p>We thank the Editor and the referee for their comments.</p></sec><sec id="s7"><title>Cite this paper</title><p>Suissa, G. and Pinchas, M. (2017) A New Equalization Performance Analyzing Method for Blind Adaptive Equalizers Inspired by Maximum Time Interval Error. Journal of Signal and Information Processing, 8, 42-64. https://doi.org/10.4236/jsip.2017.82004</p></sec><sec id="s8"><title>Abbreviations</title><p>MSE- Mean Square Error</p><p>ISI- Intersymbol Interference</p><p>BER- Bit Error Rate</p><p>MTIE- Maximum Time Interval Error</p><p>FIR- Finite Impulse Response</p><p>QAM- Quadrature Amplitude Modulation</p><p>TE- Time Error</p><p>TIE- Time Interval Error</p><p>SNR- Signal to Noise Ratio</p><p>ConE- Convolution Error</p><p>MConE- Maximum Convolution Error</p><p>E A- Error Accumulation</p><disp-formula id="scirp.76079-formula93"><graphic  xlink:href="http://html.scirp.org/file/2-3400492x128.png"  xlink:type="simple"/></disp-formula><p>Submit or recommend next manuscript to SCIRP and we will provide best service for you:</p><p>Accepting pre-submission inquiries through Email, Facebook, LinkedIn, Twitter, etc.</p><p>A wide selection of journals (inclusive of 9 subjects, more than 200 journals)</p><p>Providing 24-hour high-quality service</p><p>User-friendly online submission system</p><p>Fair and swift peer-review system</p><p>Efficient typesetting and proofreading procedure</p><p>Display of the result of downloads and visits, as well as the number of cited articles</p><p>Maximum dissemination of your research work</p><p>Submit your manuscript at: http://papersubmission.scirp.org/</p><p>Or contact jsip@scirp.org</p></sec></body><back><ref-list><title>References</title><ref id="scirp.76079-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Johnson, R., Schniter, P., Endres, T.J., Behm, J.D., Brown, D.R., Casas, R.A., et al. (1998) Blind Equalization Using the Constant Modulus Criterion: A Review. Proceedings of the IEEE, 86, 1927-1950. https://doi.org/10.1109/5.720246</mixed-citation></ref><ref id="scirp.76079-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Weerackody, V. and Kassam, S.A. (1991) Variable Step-Size Blind Adaptive Equalization Algorithms. IEEE International Symposium on Circuits and Systems, 1, 718-721.</mixed-citation></ref><ref id="scirp.76079-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Proakis, J.G. (2001) Digital Communications. In: McGraw-Hill Series in Electrical and Computer Engineering: Communications and Signal Processing, McGraw-Hill.</mixed-citation></ref><ref id="scirp.76079-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Nikias, C.L and Mendel, J.M. (1993) Signal Processing with Higher-Order Spectra. IEEE Signal Processing Magazine, 10, 10-37. https://doi.org/10.1109/79.221324</mixed-citation></ref><ref id="scirp.76079-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Silva, M.T.M. and Arenas-Garcia, J. (2013) A Soft-Switching Blind Equalization Scheme via Convex Combination of Adaptive Filters. IEEE Transactions on Signal Processing, 61, 1171-1182. https://doi.org/10.1109/TSP.2012.2236835</mixed-citation></ref><ref id="scirp.76079-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Godard, D. (1980) Self-Recovering Equalization and Carrier Tracking in Two-Dimensional Data Communication Systems. IEEE Transactions on Communications, 28, 1867-1875. https://doi.org/10.1109/TCOM.1980.1094608</mixed-citation></ref><ref id="scirp.76079-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Treichler, J. and Agee, B. (1983) A New Approach to Multipath Correction of Constant Modulus Signals. IEEE Transactions on Acoustics, Speech, and Signal Processing, 31, 459-472. https://doi.org/10.1109/TASSP.1983.1164062</mixed-citation></ref><ref id="scirp.76079-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Wesolowski, K. (1992) Analysis and Properties of the Modified Constant Modulus Algorithm for Blind Equalization. European Transactions on Telecommunications, 3, 225-230. https://doi.org/10.1002/ett.4460030303</mixed-citation></ref><ref id="scirp.76079-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Oh, K.N. and Chin, Y.O. (1995) Modified Constant Modulus Algorithm: Blind Equalization and Carrier Phase Recovery Algorithm. 1995 IEEE International Conference on Communications, 1, 498-502.</mixed-citation></ref><ref id="scirp.76079-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Yang, J., Werner, J.-J. and Dumont, G.A. (2002) The Multimodulus Blind Equalization and Its Generalized Algorithms. IEEE Journal on Selected Areas in Communications, 20, 997-1015. https://doi.org/10.1109/JSAC.2002.1007381</mixed-citation></ref><ref id="scirp.76079-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Lindsey, W.C., Ghazvinian, F., Hagmann, W.C. and Dessouky, K. (1985) Network Synchronization. Proceedings of the IEEE, 73, 1445-1467. 
https://doi.org/10.1109/PROC.1985.13317</mixed-citation></ref><ref id="scirp.76079-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Kartaschoff, P. (1991) Synchronization in Digital Communications Networks. Proceedings of the IEEE, 79, 1019-1028. https://doi.org/10.1109/5.84979</mixed-citation></ref><ref id="scirp.76079-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Bellamy, J.C. (1995) Digital Network Synchronization. IEEE Communications Magazine, 33, 70-83. https://doi.org/10.1109/35.372197</mixed-citation></ref><ref id="scirp.76079-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Bregni, S. and Maccabruni, S. (2000) Fast Computation of Maximum Time Interval Error by Binary Decomposition. IEEE Transactions on Instrumentation and Measurement, 49, 1240-1244. https://doi.org/10.1109/19.893262</mixed-citation></ref><ref id="scirp.76079-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">(1996) Definitions and Terminology for Synchronization Networks. ITU-T, Geneva, Switzerland.</mixed-citation></ref><ref id="scirp.76079-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">(1997) Timing Characteristics of Primary Reference Clocks. ITU-T, Geneva, Switzerland.</mixed-citation></ref><ref id="scirp.76079-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">(1998) Timing Requirements of Slave Clocks Suitable for Use as Node Clocks in Synchronization Networks. ITU-T, Geneva, Switzerland.</mixed-citation></ref><ref id="scirp.76079-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">(1996) Timing Characteristics of SDH Equipment Slave Clocks (SEC). ITU-T, Geneva, Switzerland.</mixed-citation></ref><ref id="scirp.76079-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">EN ETSI. 300 462 Transmission and Multiplexing (TM); Generic Requirements for Synchronization Networks.</mixed-citation></ref><ref id="scirp.76079-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Bregni, S. (1996) Measurement of Maximum Time Interval Error for Telecommunications Clock Stability Characterization. IEEE Transactions on Instrumentation and Measurement, 45, 900-906. https://doi.org/10.1109/19.536708</mixed-citation></ref><ref id="scirp.76079-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Nikias, C.L. and Petropulu, A.P. (1993) Higher-Order Spectra Analysis: A Nonlinear Signal Processing Framework. Prentice Hall, Upper Saddle River.</mixed-citation></ref><ref id="scirp.76079-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Pinchas, M. (2012) The Whole Story behind Blind Adaptive Equalizers/Blind Deconvolution. Bentham Science Publishers, Sharjah.</mixed-citation></ref><ref id="scirp.76079-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Li, Y. and Ding, Z. (1996) Global Convergence of Fractionally Spaced Godard (CMA) Adaptive Equalizers. IEEE Transactions on Signal Processing, 44, 818-826.  
https://doi.org/10.1109/78.492535</mixed-citation></ref><ref id="scirp.76079-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Sharma, V. and Raj, V.N. (2005) Convergence and Performance Analysis of Godard Family and Multimodulus Algorithms for Blind Equalization. IEEE Transactions on Signal Processing, 53, 1520-1533. https://doi.org/10.1109/TSP.2005.843725</mixed-citation></ref><ref id="scirp.76079-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Diniz, P.S.R. (1997) Adaptive Filtering. Springer, USA.  
https://doi.org/10.1007/978-1-4419-8660-3</mixed-citation></ref><ref id="scirp.76079-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Chi, C.-Y., Feng, C.-C., Chen, C.-H. and Chen, C.-Y. (2006) Blind Equalization and System Identification: Batch Processing Algorithms, Performance and Applications. Springer Science &amp; Business Media, New York.</mixed-citation></ref><ref id="scirp.76079-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Khan, M.L.R., Wondimagegnehu, M.H. and Shimamura, T. (2009) Blind Channel Equalization with Amplitude Banded Godard and Sato Algorithms. Journal of Communications, 4, 388-395.</mixed-citation></ref><ref id="scirp.76079-ref28"><label>28</label><mixed-citation publication-type="book" xlink:type="simple">Ding, Z. (2000) Adaptive Filters for Blind Equalization. In: Madisetti, V.K. and Williams, D., Eds., The Digital Signal Processing Handbook, Chapter 24. CRC Press, Boca Raton, 1-19. https://doi.org/10.1201/9781420046076-c24</mixed-citation></ref><ref id="scirp.76079-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Dobrogowski, A. and Kasznia, M. (2001) Time Effective Methods of Calculation of Maximum Time Interval Error. IEEE Transactions on Instrumentation and Measurement, 50, 732-741. https://doi.org/10.1109/19.930447</mixed-citation></ref><ref id="scirp.76079-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Oscilloquartz SA 4520 GPS-SP.  
http://syncarchitect.com/downloads/PDF_0012_4520.pdf</mixed-citation></ref><ref id="scirp.76079-ref31"><label>31</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Fiori</surname><given-names> S. </given-names></name>,<etal>et al</etal>. (<year>2001</year>)<article-title>A Contribution to (Neuromorphic) Blind Deconvolution by Flexible Approximated Bayesian Estimation</article-title><source> Signal Processing</source><volume> 81</volume>,<fpage> 2131</fpage>-<lpage>2153</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.76079-ref32"><label>32</label><mixed-citation publication-type="other" xlink:type="simple">Shalvi, O. and Weinstein, E. (1990) New Criteria for Blind Deconvolution of Nonminimum Phase Systems (Channels). IEEE Transactions on Information Theory, 36, 312-321. https://doi.org/10.1109/18.52478</mixed-citation></ref></ref-list></back></article>