<?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">JBiSE</journal-id><journal-title-group><journal-title>Journal of Biomedical Science and Engineering</journal-title></journal-title-group><issn pub-type="epub">1937-6871</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jbise.2013.64064</article-id><article-id pub-id-type="publisher-id">JBiSE-30532</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  On the basis of the morphology of the T-wave alternans: A Poincare mapping method research
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ui</surname><given-names>Guo</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>Jie</surname><given-names>Zhao</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>Fei</surname><given-names>Li</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>Tiantian</surname><given-names>Li</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Physics and Electronics, Shandong Normal University, Jinan, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>zhaojie286@gmail.com(JZ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>29</day><month>04</month><year>2013</year></pub-date><volume>06</volume><issue>04</issue><fpage>504</fpage><lpage>507</lpage><history><date date-type="received"><day>4</day>	<month>December</month>	<year>2012</year></date><date date-type="rev-recd"><day>1</day>	<month>February</month>	<year>2013</year>	</date><date date-type="accepted"><day>15</day>	<month>February</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   Presently T-wave alternans (TWA) has become a clinical index of non-invasive diagnosis for heart sudden death prediction, and detecting T-wave alternate accurately is particularly important. This paper introduces an algorithm for detecting TWA using Poincare mapping method which is a technique for nonlinear dynamic systems to display periodic behavior. Sample series of beat to beat cycles were selected to prepare Poincare mapping method. Vector Angle Index (VAI), which is the mean of the difference between <em>θ</em><em><sub>i</sub></em><sub></sub> (the angle between the line connecting the i point to the origin and the X axis) and 45 degrees was used to present the presence or absence of TWA. The value of 0.9 rad ≤ VAI ≤ 1.03 rad is accepted as a level determinative for presence of TWA. VAI via Poincare mapping method (PM) is used for correlation analysis with T-wave alternans voltage (V<sub>twa</sub>) by way of the spectral method (SM). The cross-correlation coefficient between V<sub>twa</sub> and VAI is γ = 0.8601. The algorithm can identify the absence and presence of TWA accurately and provide idea for further study of TWA-PM. 
 
</p></abstract><kwd-group><kwd>T-Wave Alternans; Poincare Mapping Method; Spectral Method; Vector Angle Index (VAI)</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. INTRODUCTION</title><p>A number of studies recently indicate that ventricular arrhythmias are one of the primary causes of cardiac death, and the microvolt T-wave alternans (MTWA) is an important index for ventricular arrhythmias prediction. TWA is a phenomenon of electro cardio variation that beat to beat variation of T-wave morphology and polarity at constant heart rate is embodied in neat cardiac rhythm [<xref ref-type="bibr" rid="scirp.30532-ref1">1</xref>].</p><p>In accordance with the statistical method difference of TWA detection, the methods with pathologic significance of detecting MTWA are divided into three kinds: Short Time Fourier Transform (STFT), symbol transform and nonlinear methods [<xref ref-type="bibr" rid="scirp.30532-ref2">2</xref>]. The Spectral method (SM) which is one kind of STFT is the most mature. Nonlinear methods include Poincare mapping (PM), moving average (MMA) method, etc.</p><p>The article presents the Poincare mapping (PM) [<xref ref-type="bibr" rid="scirp.30532-ref3">3</xref>] based on nonlinear dynamic theory to detect MTWA and compares the result with that of Spectral method. The result is proved to be of Strong correlation between both of the quantitative index. The main process for TWA detection is as follows: marr wavelet transform based on the a’trous algorithm was adopted to select feature points from Electrocardiograph (ECG), and QT interphase measurement formula was used for improving the T-wave analysis window. Then spectral method and Poincare mapping were carried out on detecting TWA, and we can attain the figures of simulation results of power spectra and Poincare maps and their quantitative indexes namely V<sub>twa</sub> (of SM) and VAI (of PM). This algorithm was applied in MIT/BIH Arrhythmia database and European ECG ST-T database, and the cross-correlation coefficient between V<sub>twa</sub> and VAI is &#227; = 0.8601.</p></sec><sec id="s2"><title>2. METHOD</title><sec id="s2_1"><title>2.1. ECG Preprocessing</title><p>Firstly, the measured ECG S was filtered, and in this paper, integral coefficient was used to eliminate 50 HZ power-line interference, and then the signal was filtered using threshold denoising algorithm by applying bior 2.2 wavelet [<xref ref-type="bibr" rid="scirp.30532-ref4">4</xref>]. In reference to the a’trous algorithm, the marr wavelet transform was carried out in one to four scales and<img src="11-70376\1aae514a-4e0e-4b35-b9f5-49654c18ef3e.jpg" />, <img src="11-70376\ecfdd04d-6f74-46d5-81ca-b9905e49a275.jpg" />can be observed [<xref ref-type="bibr" rid="scirp.30532-ref5">5</xref>]. The <img src="11-70376\24ad1970-975c-465a-8b09-1344f2ea8a51.jpg" /> represented wavelet detail part, while <img src="11-70376\7d765a8e-28fc-4eaa-8242-732d9a36e650.jpg" /> represented wavelet approximation part. Marr wavelet is second derivative wavelet basis, so the peak points after being transformed were the same as those in the original signal.</p></sec><sec id="s2_2"><title>2.2. T-Wave Alternans Detection</title><p>With the aim of detecting MTWA more accurately, this article adopts a T wave analysis window method that L = 128 ECG complex was selected for TWA measurement and there were m = 7 sampling points in every cardiac cycle [<xref ref-type="bibr" rid="scirp.30532-ref6">6</xref>]. The starting point of the T-wave window was located at <img src="11-70376\61b9f36c-ef7e-48c1-badb-c07c1f68537b.jpg" /> after the R peak, and QT interphase measurement formula was used for determination of the point terminating the T-wave analysis window as formula:</p><disp-formula id="scirp.30532-formula23995"><label>(1)</label><graphic position="anchor" xlink:href="11-70376\ea1fb729-6847-40be-891a-7fa4ea6641f1.jpg"  xlink:type="simple"/></disp-formula><p>The T-wave analysis window was divided equally into m parts in a cardiac cycle, and the sampling interval was ID between two sampling points [<xref ref-type="bibr" rid="scirp.30532-ref7">7</xref>]. Accordingly, the sampling point <img src="11-70376\a88684c7-7418-49a4-a118-a18b18646b03.jpg" /> can be attained as equation:</p><p><img src="11-70376\0373e3ed-8fdd-464c-8210-7997397f0089.jpg" />&#160;&#160; (2)</p><p>In line with the (1) and (2), 7 &#215; L selected samples of T-wave can be get across L consecutive heartbeat cycle and 7 sampling points in a cardiac cycle. At the same time, we obtain a set of signal samples<img src="11-70376\45717880-fb0a-4fb2-ae9a-5db34a109481.jpg" />, and a new sequence with subtraction between adjacent samples <img src="11-70376\308a56f7-5c43-41e7-bf43-bf41b11fac04.jpg" /> is formed. When the sequence of feature point <img src="11-70376\3468fc55-e38e-492a-97e4-3ca4a96bb2b2.jpg" /> was known [<xref ref-type="bibr" rid="scirp.30532-ref8">8</xref>], the Poincare maps could be drawn in two ways: one was constructed by <img src="11-70376\e281e97b-fbe5-4c53-b5ee-45a6101f1754.jpg" /> vs<img src="11-70376\c45ac680-f418-40ba-b907-739ee76b8f7f.jpg" />, the other was constructed by plotting second-order different plots <img src="11-70376\93d8350d-e7fb-4a9c-a7f4-e32a23763743.jpg" /> vs<img src="11-70376\68da57bd-ca95-4e29-bf05-71a1d3f492d6.jpg" />, in which i was the index identifying beat number [<xref ref-type="bibr" rid="scirp.30532-ref9">9</xref>]. The congregating distribution of the Poincare maps can be shown and the different shapes and quantitative indexes from which we can get the information we want. A sample VAI measurement between clusters to quantify TWA by way of Poincare map is proposed:</p><disp-formula id="scirp.30532-formula23996"><label>(3)</label><graphic position="anchor" xlink:href="11-70376\5d88fe07-93b5-4b45-ba1c-e171619dfd25.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.30532-formula23997"><label>(4)</label><graphic position="anchor" xlink:href="11-70376\261d724a-be17-4379-a100-12c13c238191.jpg"  xlink:type="simple"/></disp-formula><p>Among them, and <img src="11-70376\b5d3b80d-de3e-4a4a-adf8-ad687a8baee5.jpg" /> denoted the angle between the line connecting the i point to the origin and the X axis; N was the total point of Poincare map. Used for Matlab simulation, 45 degrees were turned into radian system namely for 0.7854. VAI value denoted the dispersed degree of the adjacent T-wave amplitude difference along the 45˚ line. When vector angle index is 0.9 rad ≤ VAI ≤ 1.03 rad, TWA was present in the ECG signal. When VAI &lt; 0.9 rad or VAI &gt; 1.03 rad, there was no TWA. Poincare maps for T-wave detection are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>Spectral method (SM) widely applied to the current detection of TWA is a frequency domain analysis method, and has high accuracy [<xref ref-type="bibr" rid="scirp.30532-ref10">10</xref>]. This paper compared the result of detection by means of Poincare map namely VAI with that of detection by way of Spectral method that is V<sub>twa</sub>, and the correlation analysis proved the effectiveness of PM. Spectral method for T-wave detection are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec></sec><sec id="s3"><title>3. RESULTS</title><p>In the article, we adopted MIT/BIH Arrhythmia database and European ECG ST-T database. The sampling fre-</p><p>quency in former was 360 HZ while in the latter 250 HZ. For purposes of brevity, the signal from these databases was resampled with 200 HZ so that the analysis became simpler. We showed part of the simulation results in <xref ref-type="table" rid="table1">Table 1</xref>. All the datas were from channel 1.</p><p>From the following data in <xref ref-type="table" rid="table1">Table 1</xref>, a significant correlation was found between the alternans voltage determined by the SM and the vector angle index calculated by the PM, and the cross-correlation coefficient between V<sub>twa</sub> and VAI is γ = 0.8601. In the Matlab7.0 environment, the discrete data V<sub>twa</sub> and VAI in <xref ref-type="table" rid="table1">Table 1</xref> were operated by means of Curve Fitting Tool. A curve relation was found as following equation:</p><disp-formula id="scirp.30532-formula23998"><label>(5)</label><graphic position="anchor" xlink:href="11-70376\bf2d99c0-44bf-4edd-bfcd-ea7475ba69df.jpg"  xlink:type="simple"/></disp-formula><p>The fitting curve of V<sub>twa</sub> and VAI are shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. The fitting curve R-square is 0.867.</p><p><xref ref-type="table" rid="table1">Table 1</xref>. Simulation data of some samples.</p><disp-formula id="scirp.30532-formula23999"><graphic  xlink:href="11-70376\255dc9a1-7adf-473f-9164-3ad7233b3bf6.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. CONCLUSION</title><p>According to a lot of the simulation data results, we accepted that the presence of TWA by way of PM is determined on the basis of 0.9 rad ≤ VAI ≤ 1.03 rad. Because of the cross-correlation coefficient between V<sub>twa</sub> and VAI 0.8601, the strong correlation between VAI via PM and V<sub>twa</sub> by means of the mature method of SM is proved. At the same time, it is also shown that Vector Angle can be applied to TWA detection. SP demands the complex of plenty of beat-to-beat circles to detect the presence or absence TWA accurately. By way of PM T-wave alternans voltage between any adjacent beats can be get, and Compared with SP, PM is more simpler [<xref ref-type="bibr" rid="scirp.30532-ref11">11</xref>]. Because the application of PM in heart rate variability has become more mature, we can also get some T-wave alternans statistical information from the area of PM [<xref ref-type="bibr" rid="scirp.30532-ref12">12</xref>], and then whether the area index can reflect the characteristics of nonlinear mechanics TWA quantitative information remains to be established.</p></sec><sec id="s5"><title>5. 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