<?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">CC</journal-id><journal-title-group><journal-title>Computational Chemistry</journal-title></journal-title-group><issn pub-type="epub">2332-5968</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/cc.2019.74009</article-id><article-id pub-id-type="publisher-id">CC-95878</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Development of Predictive QSPR Model of the First Reduction Potential from a Series of Tetracyanoquinodimethane (TCNQ) Molecules by the DFT (Density Functional Theory) Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fatogoma</surname><given-names>Diarrassouba</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>Mawa</surname><given-names>Koné</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kafoumba</surname><given-names>Bamba</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>Yafigui</surname><given-names>Traoré</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>Mamadou</surname><given-names>Guy-Richard Koné</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>Edja</surname><given-names>Florentin Assanvo</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Laboratoire de Chimie Organique et des Substances Naturelles, UFR-SSMT, Université Félix Houphou&amp;amp;#235;t Boigny, Abidjan, C&amp;amp;#244;te d’Ivoire</addr-line></aff><aff id="aff1"><addr-line>Laboratoire de Thermodynamique et de Physico-chimie du Milieu, UFR-SFA, Université Nangui Abrogoua, Abidjan, C&amp;amp;#244;te d’Ivoire</addr-line></aff><pub-date pub-type="epub"><day>30</day><month>09</month><year>2019</year></pub-date><volume>07</volume><issue>04</issue><fpage>121</fpage><lpage>142</lpage><history><date date-type="received"><day>5,</day>	<month>September</month>	<year>2019</year></date><date date-type="rev-recd"><day>19,</day>	<month>October</month>	<year>2019</year>	</date><date date-type="accepted"><day>22,</day>	<month>October</month>	<year>2019</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this work, which consisted to develop a predictive QSPR (Quantitative Structure-Property Relationship) model of the first reduction potential, we were particularly interested in a series of forty molecules. These molecules 
  have constituted our database. Here, thirty molecules were used for the tra
  ining set and ten molecules were used for the test set. For the calculation of the descriptors, all molecules have been firstly optimized with a frequency calculation at B3LYP/6-31G(d,p) theory level. Using statistical analysis methods, a predictive QSPR (Quantitative Structure-Property Relationship) model of the first reduction potential dependent on electronic affinity (EA) only have been developed. The statistical and validation parameters derived from this model have been determined and found interesting. These different parameters and the realized statistical tests have revealed that this model is suitable for predicting the first reduction potential of future TCNQ (tetracyanoquinodimethane) of this same family belonging to its applicability domain with a 95% confidence level.
 
</p></abstract><kwd-group><kwd>Tetracyanoquinodimethane</kwd><kwd> First Reduction Potential</kwd><kwd> QSPR</kwd><kwd> Statistical Analysis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Conjugated simple organic molecules carrying both electron donors and acceptors have recently attracted a lot of attention because of their various and interesting properties. Non-linear optical properties [<xref ref-type="bibr" rid="scirp.95878-ref1">1</xref>], molecular electronic devices [<xref ref-type="bibr" rid="scirp.95878-ref2">2</xref>], artificial photosynthesis models [<xref ref-type="bibr" rid="scirp.95878-ref3">3</xref>] and solvatochromic effects [<xref ref-type="bibr" rid="scirp.95878-ref4">4</xref>] are among their potential applications.</p><p>Intramolecular electron transfer processes are one of the main topics of current interest in physic organic chemistry [<xref ref-type="bibr" rid="scirp.95878-ref5">5</xref>], particularly regarding tetracyanoquinodimethane (TCNQ)-based charge transfer complexes. In fact, TCNQ is an organic electron acceptor with a high electron affinity [<xref ref-type="bibr" rid="scirp.95878-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.95878-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.95878-ref8">8</xref>]. This electron acceptor can react according to an oxidation-reduction process with electron donors to form charge transfer complexes that display electrical properties and various applications. Indeed, it has been used for the synthesis of a large number of charge transfer compounds that have been widely explored as molecular electronics building blocks [<xref ref-type="bibr" rid="scirp.95878-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.95878-ref10">10</xref>], non-linear optics [<xref ref-type="bibr" rid="scirp.95878-ref11">11</xref>] and organic semiconductors [<xref ref-type="bibr" rid="scirp.95878-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.95878-ref13">13</xref>]. Existing TCNQ molecules have generally exhibited exemplary redox properties. Improving their properties and finding molecules with even better properties is therefore a challenge for scientific research. However, in the synthesis of these complexes, the objective of organic chemists is to synthesize thermodynamically stable radical species, which is not an easy task. Also, the two molecules constituting the charge transfer complex must have moderate donor and acceptor powers [<xref ref-type="bibr" rid="scirp.95878-ref14">14</xref>]. Under these conditions, the use of alternative methods for experimentation becomes essential. Among these, QSPR (Quantitative Structure-Property Relationships) methods are of great interest and even recommended according to new regulations [<xref ref-type="bibr" rid="scirp.95878-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.95878-ref16">16</xref>]. They make it possible to develop mathematical models linking physico-chemical properties with molecular structure. They either explain the origin of these properties or predict them for the molecules whose experimental data are not available. Quantum chemistry provides access to a large number of descriptors through its different methods.</p><p>The objective of this work is to develop a predictive QSPR model of the first reduction potential from a series of TCNQ molecules using quantum descriptors, to explain and predict the first reduction potential of the future TCNQ molecules of this same family belonging to its applicability domain.</p></sec><sec id="s2"><title>2. Computational Details</title><sec id="s2_1"><title>2.1. Training Set and Test Set</title><p>In the development of the predictive QSPR model of the first reduction potential, we considered a series of forty Tetracyanoquinodimethane derivatives codified TCNQ [<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>] - [<xref ref-type="bibr" rid="scirp.95878-ref23">23</xref>]. The choice of these molecules is due to the availability of their experimental first reduction potentials. These properties have been all determined by cyclic voltammetry in acetonitrile. These molecules have constituted our database. Thirty of which (75% of the database) were used for the training set and ten molecules (25% of the database) were used for the test set. <xref ref-type="table" rid="table1">Table 1</xref> presents these different molecules with their corresponding experimental first reduction potentials expressed in volts (V).</p><table-wrap-group id="1"><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Series of studied tetracyanoquinodimethane (TCNQ) molecules</title></caption><table-wrap id="1_1"><table><tbody><thead><tr><th align="center" valign="middle"  colspan="4"  >Training set</th></tr></thead><tr><td align="center" valign="middle" >Code</td><td align="center" valign="middle" >Molecule</td><td align="center" valign="middle" >E exp 1 ( V )</td><td align="center" valign="middle" >Reference</td></tr><tr><td align="center" valign="middle" >TCNQ_1</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x3.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.170</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref18">18</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_2</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x4.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.110</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref18">18</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_3</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x5.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.120</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref18">18</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_4</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x6.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.012</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_5</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x7.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.180</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_6</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x8.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.130</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_7</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x9.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.130</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr></tbody></table></table-wrap><table-wrap id="1_2"><table><tbody><thead><tr><th align="center" valign="middle" >TCNQ_8</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x10.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >−0.470</th><th align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</th></tr></thead><tr><td align="center" valign="middle" >TCNQ_9</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x11.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >-0.090</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_10</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x12.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.068</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_11</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x13.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.03</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_12</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x14.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.05</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_13</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x15.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.058</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_14</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x16.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.048</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_15</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x17.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.320</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr></tbody></table></table-wrap><table-wrap id="1_3"><table><tbody><thead><tr><th align="center" valign="middle" >TCNQ_16</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x18.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >+0.200</th><th align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</th></tr></thead><tr><td align="center" valign="middle" >TCNQ_17</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x19.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.360</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_18</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x20.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.370</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_19</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x21.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.340</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_20</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x22.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.290</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref19">19</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_21</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x23.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.300</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref21">21</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_22</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x24.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.010</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref19">19</xref>]</td></tr></tbody></table></table-wrap><table-wrap id="1_4"><table><tbody><thead><tr><th align="center" valign="middle" >TCNQ_23</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x25.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >+0.530</th><th align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref19">19</xref>]</th></tr></thead><tr><td align="center" valign="middle" >TCNQ_24</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x26.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.010</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref22">22</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_25</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x27.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.080</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_26</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x28.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.210</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_27</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x29.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.040</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_28</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x30.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.570</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_29</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x31.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.140</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr></tbody></table></table-wrap><table-wrap id="1_5"><table><tbody><thead><tr><th align="center" valign="middle" >TCNQ_30</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x32.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >−0.026</th><th align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</th></tr></thead><tr><td align="center" valign="middle"  colspan="4"  >Test set</td></tr><tr><td align="center" valign="middle" >TCNQ_31</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x33.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.260</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_32</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x34.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.070</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref19">19</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_33</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x35.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.410</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref19">19</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_34</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x36.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.650</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref19">19</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_35</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x37.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.120</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref23">23</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_36</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x38.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.130</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_37</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x39.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.440</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</td></tr></tbody></table></table-wrap><table-wrap id="1_6"><table><tbody><thead><tr><th align="center" valign="middle" >TCNQ_38</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x40.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >+0.030</th><th align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref17">17</xref>]</th></tr></thead><tr><td align="center" valign="middle" >TCNQ_39</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x41.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >+0.260</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref20">20</xref>]</td></tr><tr><td align="center" valign="middle" >TCNQ_40</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/3-1710117x42.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.020</td><td align="center" valign="middle" >[<xref ref-type="bibr" rid="scirp.95878-ref22">22</xref>]</td></tr></tbody></table></table-wrap></table-wrap-group></sec><sec id="s2_2"><title>2.2. Computational Theory Level and Softwares</title><p>The GaussView 5.0 [<xref ref-type="bibr" rid="scirp.95878-ref24">24</xref>] software was used to represent the 3D structure and visualize the studied molecules. Then, the Gaussian 09 software [<xref ref-type="bibr" rid="scirp.95878-ref25">25</xref>] was used for optimization and frequency calculation (temperature 298.15 Kevin, pressure 1 atmosphere, in vacuum). The theory level used is B3LYP/6-31G(d,p). As for 2D structures, they have been designed with ChemSketch [<xref ref-type="bibr" rid="scirp.95878-ref26">26</xref>]. The EXCEL software [<xref ref-type="bibr" rid="scirp.95878-ref27">27</xref>] was used for graphic representation. The XLSTAT software [<xref ref-type="bibr" rid="scirp.95878-ref28">28</xref>] was used for modeling and statistical tests. For the calculation of the observation levers, the Minitab 18 [<xref ref-type="bibr" rid="scirp.95878-ref29">29</xref>] software was used.</p></sec><sec id="s2_3"><title>2.3. Statistical Analysis</title><p>To develop a QSPR model, a data analysis method is required. This method quantifies the relationship between the studied property and the molecular structure (descriptors). There are several methods for the implementation of a model and the analysis of its statistical data. But the one we used in our study is Simple Linear Regression (SLR) (a single explanatory variable). Generally speaking, the equation of the simple regression is of the form:</p><p>Y = a 0 + a 1 X (1)</p><p>with Y standing for the studied property, X represents the explanatory variable in correlation with the studied property and a 0 , a 1 are the model regression constants.</p><p>The selection of descriptors is a crucial step in QSPR modeling. In this study, the selection of descriptors was based on two criteria described as follows:</p><p>• Criterion 1</p><p>There must be a linear dependence relationship between the first reduction potential and the descriptors. Under these conditions we shall have | R | ≥ 0.50 [<xref ref-type="bibr" rid="scirp.95878-ref30">30</xref>] with R, the linear correlation coefficient of the line E e x p = f ( D e s c r i p t e u r i ) .</p><p>• Criterion 2</p><p>The descriptors must be independent from one another. To do this, the partial correlation coefficient a i j between the descriptors i and j must be less than 0.70 ( a i j &lt; 0.70 ) [<xref ref-type="bibr" rid="scirp.95878-ref30">30</xref>]. For a multilinear regression, the coefficients R and a i j are expressed as follows:</p><p>R = C O V ( X , Y ) S X ⋅ S Y (2)</p><p>and</p><p>a i j = C O V ( X i , X i ) V a r ( X i ) (3)</p><p>The relationships (4), (5), (6) and (7) were used to calculate many statistical and validation parameters:</p><p>ESS = ∑ ​ ( Y i , c a l − Y &#175; e x p ) 2 (4)</p><p>TSS = ∑ ​ ( Y i , e x p − Y &#175; e x p ) 2 (5)</p><p>RSS = ∑ ​ ( Y i , e x p − Y i , c a l ) 2 (6)</p><p>TSS = ESS + RSS (7)</p><p>where TSS is total sum of squares, ESS stands for extended sum of squares and RSS is residual sum of squares.</p><p>• Determination coefficient (R<sup>2</sup>) [<xref ref-type="bibr" rid="scirp.95878-ref31">31</xref>]</p><p>The determination coefficient is given by the following relationship:</p><p>R 2 = 1 − ∑ ​ ( Y i , e x p − Y i , c a l ) 2 ∑ ​ ( Y i , e x p − Y &#175; e x p ) 2 = 1 − RSS TSS (8)</p><p>with</p><p>R = ∑ ​ ( Y i , c a l − Y &#175; e x p ) 2 ∑ ​ ( Y i , e x p − Y &#175; e x p ) 2 = ESS TSS (9)</p><p>• Standard deviation (s) [<xref ref-type="bibr" rid="scirp.95878-ref32">32</xref>]</p><p>It is an indicator of dispersion. It provides information on how the distribution of data is performed around the average. The closer its value is to 0, the better the adjustment and the more reliable will be the prediction.</p><p>s = ∑ ​ ( Y i , e x p − Y i , c a l ) 2 n − p − 1 = RSS n − p − 1 (10)</p><p>• Adjusted determination coefficient ( R adjusted 2 ) [<xref ref-type="bibr" rid="scirp.95878-ref33">33</xref>]</p><p>It allows to measure the robustness of a model unlike R 2 . This coefficient is used in multiple regressions because it considers the number of descriptors parameters of the model.</p><p>R adjusted 2 = 1 − ( n − Intercept ) n − p − 1 ⋅ RSS TSS = 1 − ( n − Intercept ) n − p − 1 ⋅ ( 1 − R 2 ) (11)</p><p>• Fisher-Snedecor coefficient (F) [<xref ref-type="bibr" rid="scirp.95878-ref34">34</xref>]</p><p>It allows to test the global significance of linear regression. A globally significant regression equation contains at least a relevant explanatory variable to explain the dependent variable. The Fisher-Snedecor coefficient is related to the determination coefficient by the following relationship:</p><p>F = n − p − 1 p ⋅ ESS RSS = n − p − 1 p ⋅ R 2 1 − R 2 (12)</p><p>• Kubinyi Criterion (FIT) [<xref ref-type="bibr" rid="scirp.95878-ref35">35</xref>]</p><p>It measures the size or robustness of the model. The smaller the FIT, the more robust the model is, meaning that the model has more variables.</p><p>FIT = n − p − 1 ( n + p ) 2 ⋅ R 2 1 − R 2 (13)</p><p>• Cross-validation coefficient ( Q LOO 2 ) [<xref ref-type="bibr" rid="scirp.95878-ref36">36</xref>]</p><p>It measures the accuracy of the prediction on the data of the training set</p><p>Q LOO 2 = 1 − ∑ ​ ( y i , e x p − y i , p r e d ) 2 ∑ ​ ( y i , e x p − y &#175; e x p ) 2 = 1 − PRESS TSS (14)</p><p>• Cross-validation criteria (PRESS) [<xref ref-type="bibr" rid="scirp.95878-ref36">36</xref>]</p><p>As the sum of the quadratic prediction errors, PRESS (Prediction Sum of Squares) is defined by the relationship:</p><p>PRESS = ∑ ​ ( y i , e x p − y i , p r e d ) 2 (15)</p><p>This criterion is used to select models with good predictive power (we always look for the smallest PRESS). A Standard Deviation of Error of Prediction (SDEP) is calculated from PRESS:</p><p>SDEP = ∑ ​ ( y i , e x p − y i , p r e d ) 2 n = PRESS n (16)</p><p>In these expressions, n is the number of molecules in the training set, p is the number of explanatory variables. y i , e x p and y i , p r e d are respectively the experimental and predicted values of property for molecule i and y &#175; e x p is the average value of the property for the training set.</p><p>• Todeschini’s parameter ( R c P 2 ) [<xref ref-type="bibr" rid="scirp.95878-ref37">37</xref>]</p><p>R c P 2 is the corrected form of P.P. Roy’s parameter noted R P 2 [<xref ref-type="bibr" rid="scirp.95878-ref38">38</xref>]. It allows to know if the model is due to chance correlations or not. If this parameter is greater than 0.50, the model is not due to a chance correlations. It is defined as:</p><p>R c P 2 = R R 2 − R r 2 (17)</p><p>with R r 2 , the average value of R r i 2 of the models obtained with the randomized property.</p><p>• External validation coefficient ( Q e x t 2 ) [<xref ref-type="bibr" rid="scirp.95878-ref39">39</xref>]</p><p>It measures the accuracy of the prediction on the test set data.</p><p>Q e x t 2 = 1 − n n e x t PRESS ( test ) TSS (18)</p><p>here, n<sub>ext</sub> refers to the number of test set compounds.</p><p>• Parameter (RMSEP) [<xref ref-type="bibr" rid="scirp.95878-ref39">39</xref>]</p><p>External predictive ability of QSPR model may further be determined by the Root Mean Square Error in Prediction given by:</p><p>RMSEP = ∑ ​ ( y e x p ( test ) − y p r e d ( test ) ) 2 n e x t (19)</p><p>• Roy K. and al. parameters ( r m 2 &#175; and Δ r m 2 ) [<xref ref-type="bibr" rid="scirp.95878-ref40">40</xref>]</p><p>For the acceptable prediction, the value of Δ r m 2 should preferably be lower than 0.20 when the value of r m 2 &#175; is more than 0.50.</p><p>r m 2 &#175; = r m 2 + r ′ m 2 2 (20)</p><p>Δ r m 2 = | r m 2 − r ′ m 2 | (21)</p><p>here</p><p>r m 2 = r 2 ( 1 − r 2 − r 0 2 ) (22)</p><p>and</p><p>r ′ m 2 = r 2 ( 1 − r 2 − r ′ 0 2 ) (23)</p><p>The parameters r 2 and r 0 2 are the determination coefficients between the observed and predicted values of the compounds (training set or test set) with and without intercept, respectively. The parameter r ′ 0 2 bears the same meaning but uses the reversed axes.</p><p>• External validation criteria or “Tropsha’s criteria” [<xref ref-type="bibr" rid="scirp.95878-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.95878-ref41">41</xref>]</p><p>There are five such criteria:</p><p>v Criterion 1: R e x t 2 &gt; 0.70</p><p>v Criterion 2: Q e x t 2 &gt; 0.60</p><p>v Criterion 3: | R e x t 2 − R 0 2 | R e x t 2 &lt; 0.1 and 0.85 &lt; k &lt; 1.15</p><p>v Criterion 4: | R e x t 2 − R ′ 0 2 | R e x t 2 &lt; 0.1 and 0.85 &lt; k ′ &lt; 1.15</p><p>v Criterion 5: | R e x t 2 − R 0 2 | &lt; 0.3</p><p>where, R e x t 2 stands for the determination coefficient of molecules for the test set; R 0 2 represents the determination coefficient of the regression between predicted and experimental values for the test set without intercept; R ′ 0 2 is the determination coefficient of the regression between experimental and predicted values for the test set without intercept; k stands for the slope of the correlation line (values predicted according to the experimental values with intercept = 0) and k ′ is the slope of the correlation line (experimental values according to the predicted values with intercept = 0). Ouanlo Ouattara et al. [<xref ref-type="bibr" rid="scirp.95878-ref42">42</xref>] reported that if at least 3/5 of the Tropsha’s criteria are verified, the QSPR model developed is considered as a successful model in predicting of the studied property.</p><p>• Lever (h<sub>ii</sub>) [<xref ref-type="bibr" rid="scirp.95878-ref43">43</xref>]</p><p>The lever is a kind of distance from the barycentre of the points in the space of the explanatory variables. It identifies observations that are abnormally far from others. For observation i</p><p>h i i = x i ( X T X ) − 1 x i T       ( i = 1 , ⋯ , n ) (24)</p><p>where x<sub>i</sub> is the line vector of the descriptors of compound i and X is the matrix of the model derived from the values of the descriptors of the training set. The index T refers to the transposed matrix/vector. The critical value of lever h<sup>*</sup> is, in</p><p>general, set to 3 ( p + 1 ) n [<xref ref-type="bibr" rid="scirp.95878-ref44">44</xref>], where n is the number of compounds in the</p><p>training set and p is the number of model descriptors. If a compound has a residual and a lever that exceeds the critical value h* then this compound is considered outside the applicability domain of the developed model.</p></sec><sec id="s2_4"><title>2.4. Calculation of Molecular Descriptor</title><p>The descriptor considered in this work is electronic affinity (EA). This descriptor has been calculated according to Koopmans [<xref ref-type="bibr" rid="scirp.95878-ref45">45</xref>] approach: the electronic affinity is the opposite of LUMO energy.</p><p>EA = − E LUMO (25)</p><p>where LUMO is the Lowest Unoccupied Molecular Orbital. <xref ref-type="table" rid="table2">Table 2</xref> reports the values of this descriptor for both the training set and the test set.</p></sec><sec id="s2_5"><title>2.5. Submission of the Descriptor to the Selection Criterion 1</title><p>The calculated descriptor (electronic affinity) will be subject to selection criterion 1 because it is the lone considered descriptor (<xref ref-type="table" rid="table3">Table 3</xref>).</p></sec></sec><sec id="s3"><title>3. Resultats and Discussion</title><sec id="s3_1"><title>3.1. QSPR Model</title><p>The regression equation of the predictive QSPR (Quantitative Structure-Property Relationship) model of the first reduction potential dependent to electronic affinity (EA) is given below:</p><p>E t h e o 1 = − 2.5314 + 0.5708 ∗ EA</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title>Descriptor values expressed in eV, at B3LYP/6-31G(d,p) theory level</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="4"  >Training set</th><th align="center" valign="middle"  colspan="2"  >Test set</th></tr></thead><tr><td align="center" valign="middle" >CODE</td><td align="center" valign="middle" >EA</td><td align="center" valign="middle" >CODE</td><td align="center" valign="middle" >EA</td><td align="center" valign="middle" >CODE</td><td align="center" valign="middle" >EA</td></tr><tr><td align="center" valign="middle" >TCNQ_1</td><td align="center" valign="middle" >4.7196</td><td align="center" valign="middle" >TCNQ_16</td><td align="center" valign="middle" >4.7253</td><td align="center" valign="middle" >TCNQ_31</td><td align="center" valign="middle" >4.7153</td></tr><tr><td align="center" valign="middle" >TCNQ_2</td><td align="center" valign="middle" >4.6219</td><td align="center" valign="middle" >TCNQ_17</td><td align="center" valign="middle" >3.8607</td><td align="center" valign="middle" >TCNQ_32</td><td align="center" valign="middle" >4.5776</td></tr><tr><td align="center" valign="middle" >TCNQ_3</td><td align="center" valign="middle" >4.5302</td><td align="center" valign="middle" >TCNQ_18</td><td align="center" valign="middle" >3.8297</td><td align="center" valign="middle" >TCNQ_33</td><td align="center" valign="middle" >5.0778</td></tr><tr><td align="center" valign="middle" >TCNQ_4</td><td align="center" valign="middle" >4.5376</td><td align="center" valign="middle" >TCNQ_19</td><td align="center" valign="middle" >3.8085</td><td align="center" valign="middle" >TCNQ_34</td><td align="center" valign="middle" >5.5402</td></tr><tr><td align="center" valign="middle" >TCNQ_5</td><td align="center" valign="middle" >4.2251</td><td align="center" valign="middle" >TCNQ_20</td><td align="center" valign="middle" >4.9545</td><td align="center" valign="middle" >TCNQ_35</td><td align="center" valign="middle" >4.7109</td></tr><tr><td align="center" valign="middle" >TCNQ_6</td><td align="center" valign="middle" >4.3299</td><td align="center" valign="middle" >TCNQ_21</td><td align="center" valign="middle" >5.0348</td><td align="center" valign="middle" >TCNQ_36</td><td align="center" valign="middle" >4.8048</td></tr><tr><td align="center" valign="middle" >TCNQ_7</td><td align="center" valign="middle" >4.4298</td><td align="center" valign="middle" >TCNQ_22</td><td align="center" valign="middle" >4.3152</td><td align="center" valign="middle" >TCNQ_37</td><td align="center" valign="middle" >3.5692</td></tr><tr><td align="center" valign="middle" >TCNQ_8</td><td align="center" valign="middle" >3.708</td><td align="center" valign="middle" >TCNQ_23</td><td align="center" valign="middle" >5.2544</td><td align="center" valign="middle" >TCNQ_38</td><td align="center" valign="middle" >4.5944</td></tr><tr><td align="center" valign="middle" >TCNQ_9</td><td align="center" valign="middle" >4.438</td><td align="center" valign="middle" >TCNQ_24</td><td align="center" valign="middle" >4.4573</td><td align="center" valign="middle" >TCNQ_39</td><td align="center" valign="middle" >4.9333</td></tr><tr><td align="center" valign="middle" >TCNQ_10</td><td align="center" valign="middle" >4.6023</td><td align="center" valign="middle" >TCNQ_25</td><td align="center" valign="middle" >4.8206</td><td align="center" valign="middle" >TCNQ_40</td><td align="center" valign="middle" >4.4605</td></tr><tr><td align="center" valign="middle" >TCNQ_11</td><td align="center" valign="middle" >4.5517</td><td align="center" valign="middle" >TCNQ_26</td><td align="center" valign="middle" >4.8021</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >TCNQ_12</td><td align="center" valign="middle" >4.4094</td><td align="center" valign="middle" >TCNQ_27</td><td align="center" valign="middle" >4.5060</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >TCNQ_13</td><td align="center" valign="middle" >4.5582</td><td align="center" valign="middle" >TCNQ_28</td><td align="center" valign="middle" >3.3972</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >TCNQ_14</td><td align="center" valign="middle" >4.5253</td><td align="center" valign="middle" >TCNQ_29</td><td align="center" valign="middle" >4.0640</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >TCNQ_15</td><td align="center" valign="middle" >4.8269</td><td align="center" valign="middle" >TCNQ_30</td><td align="center" valign="middle" >4.4714</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title>Submission of the descriptor to the selection criterion 1</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Equation</th><th align="center" valign="middle" >Coefficient of corr&#233;lation | R |</th><th align="center" valign="middle" >Descriptors is selected if | R | ≥ 0.50</th></tr></thead><tr><td align="center" valign="middle" >E e x p 1 = f ( EA )</td><td align="center" valign="middle" >0.9605</td><td align="center" valign="middle" >selected</td></tr></tbody></table></table-wrap><p>n = 30 ;     R = 0.9605 ;     R 2 = 0.9225 ;     R adjusted 2 = 0.9197 ;     s = 0.0694 ; F = 333.3279 ;     FIT = 0.3469 ;     p -value &lt; 0.000 ;     TSS = 1.7407 ; ESS = 1.6058 ;     α = 95 %</p><p>The positive sign of the coefficient of the EA in the regression equation of model shows that the first reduction potential increases with electronic affinity. There is therefore a direct correlation between the explanatory variable and the studied property. Examination of the above parameters shows that the correlation coefficient is very high ( R = 0.9605 ). This high value indicates that there is a strong correlation between the first reduction potential and the selected descriptor. The determination coefficient R 2 = 0.9225 shows that 92.25% of the experimental variance of the first reduction potential is explained by the model's descriptor alone. In addition, the standard deviation ( s = 0.0694 ) tends towards 0, indicating a good fit and high reliability of the prediction. The p-value is less than 0.0001 so 1 − α = 0.05 (5% risk). It is therefore clear that the regression equation of the model is highly significant for predicting the first reduction potential of the series of studied molecules. This global significance is confirmed by the very high Fischer value (F = 333.3279). Under these conditions, the only explanatory variable (electronic affinity) of the regression equation is very relevant to explain the studied property (first reduction potential). In addition, the experimental variance is TSS = 1.7407 when the theoretical variance due to the model is ESS = 1.6058. It is important to note that this relationship of dependence between the first reduction potential and electronic affinity has been corroborated by the work of Peter W. Kenny [<xref ref-type="bibr" rid="scirp.95878-ref46">46</xref>] who showed that the first reduction potential is a function of LUMO energy. He developed a predictive QSPR model dependent only on LUMO energy calculated at HF/6-31G(d) theory level, from a series of sixteen analogous TCNQ molecules with statistical parameters ( n = 16 ; R 2 = 0.969 ; F = 436 ; s = 0.04   V ; α = 95 % ). However, the internal and external validations of this model have not been studied. It is also important to note that a QSPR (Quantitative Structure-Property Relationship) model can be obtained in a hazardous way. Therefore, one must always make sure of its stability. To do this, both internal and external validations methods are performed.</p></sec><sec id="s3_2"><title>3.2. Internal Validation of the Model</title><p>For internal validation, the Leave-One-Out (LOO) procedure and the property of the randomization test have been used.</p><p>• Leave-One-Out procedure</p><p><xref ref-type="table" rid="table4">Table 4</xref> indicates that the value of Q LOO 2 = 0.9136 . The model is therefore excellent as seen Q LOO 2 &gt; 0.90 [<xref ref-type="bibr" rid="scirp.95878-ref47">47</xref>]. In addition, 91.36 % of the molecules in the training set have their redox potentials predicted by this model. With regard to the molecules of the training set, this model therefore has a high predictive power. This result shows that model is not very sensitive to this operation of setting apart a molecule and putting it back into the training set (Leave-One-Out procedure). This justifies the stability of this model. For r m 2 ( LOO ) &#175; , its value is greater than 0.50 when that of Δ r m 2 ( LOO ) is less than 0.20. Consequently, for the prediction of the redox potential, the model is acceptable. Moreover, to ensure that the model is not due to chance correlations, the Y-randomization test of the property has been realized. A circular permutation of the property has been made (29 iterations).</p><p>• Y-randomization test</p><p>The average values of the Y-randomization parameters are shown in <xref ref-type="table" rid="table5">Table 5</xref>.</p><p><xref ref-type="table" rid="table5">Table 5</xref> shows that the average value of R r 2 tends to 0 ( R r 2 = 0.0600 ), showing that the equation of the regression line only determines 6.00% of the point distribution (redox potential). In addition, there is scatter around the regression line confirmed by a high standard deviation ( s r = 0.2415 ). The very low value of the statistic F r shows that the equation of the model obtained with the randomized property is not significant. As for Todeschini’s parameter R c P 2 , its value is greater than 0.50 ( R c P 2 &gt; 0.50 ). This confirms that the established model is not due to chance correlations.</p></sec><sec id="s3_3"><title>3.3. External Validation of the Model</title><p>The external validation only concerns the molecules of the test set. <xref ref-type="table" rid="table6">Table 6</xref> reports the statistical parameters of the external validation of the model.</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Statistical parameters of the LOO internal validation of the model</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n</th><th align="center" valign="middle" >Q LOO 2</th><th align="center" valign="middle" >r m 2 ( LOO ) &#175;</th><th align="center" valign="middle" >Δ r m 2 ( LOO )</th><th align="center" valign="middle" >PRESS</th><th align="center" valign="middle" >SDEP</th></tr></thead><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >0.9136</td><td align="center" valign="middle" >0.9136</td><td align="center" valign="middle" >0.0000</td><td align="center" valign="middle" >0.1504</td><td align="center" valign="middle" >0.0708</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Mean values of the randomization parameters</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Randomized parameter</th><th align="center" valign="middle" >R r 2</th><th align="center" valign="middle" >s r</th><th align="center" valign="middle" >F r</th><th align="center" valign="middle" >R c P 2</th></tr></thead><tr><td align="center" valign="middle" >Average value</td><td align="center" valign="middle" >0.0600</td><td align="center" valign="middle" >0.2415</td><td align="center" valign="middle" >1.9987</td><td align="center" valign="middle" >0.8920</td></tr></tbody></table></table-wrap><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> Statistical parameters of the external validation of the model</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n e x t</th><th align="center" valign="middle" >R e x t 2</th><th align="center" valign="middle" >Q e x t 2</th><th align="center" valign="middle" >R 0 2</th><th align="center" valign="middle" >R ′ 0 2</th><th align="center" valign="middle" >r m 2 ( test ) &#175;</th><th align="center" valign="middle" >Δ r m 2 ( test )</th><th align="center" valign="middle" >RMSEP</th></tr></thead><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >0.9617</td><td align="center" valign="middle" >0.9504</td><td align="center" valign="middle" >0.9613</td><td align="center" valign="middle" >0.9617</td><td align="center" valign="middle" >0.9521</td><td align="center" valign="middle" >0.0096</td><td align="center" valign="middle" >0.0536</td></tr></tbody></table></table-wrap><p>From the analysis of the data in <xref ref-type="table" rid="table6">Table 6</xref>, it appears that the model has a very high predictive power because Q e x t 2 = 0.9504 . This shows that, 95.04% of molecules of the test set have their redox potentials predicted by the model. Also, 96.17 % of the experimental variance of the first reduction potential is explained by the descriptor model. For r m 2 ( test ) &#175; , its value is greater than 0.50 while that of Δ r m 2 ( test ) is less than 0.2. Thus, this model is acceptable for the prediction of the redox potential of the test set molecules. In addition, the five (05) criteria of external validation (Tropsha’s criteria) have been verified.</p><p>Verification of Tropsha’s criteria</p><p>Criterion 1: R e x t 2 = 0.9617 &gt; 0.70</p><p>Criterion 2: Q e x t 2 = 0.9504 &gt; 0.60</p><p>Criterion 3: | R e x t 2 − R 0 2 | R e x t 2 = 0.0004 &lt; 0.1 and k = 0.9905 avec 0.85 &lt; k &lt; 1.15</p><p>Criterion 4: | R e x t 2 − R ′ 0 2 | R e x t 2 = 0.0000 &lt; 0.1 and k ′ = 0.9797 avec 0.85 &lt; k ′ &lt; 1.15</p><p>Criterion 5: | R e x t 2 − R 0 2 | = 0.0004 &lt; 0.3</p><p>At this level, we see that all five (05) Tropsha criteria are verified. As a result, the developed model is very efficient in predicting the first reduction potential of the series of studies molecules.</p></sec><sec id="s3_4"><title>3.4. Correlation between the Predicted Values by the Model and the Experimental Values</title><p>In <xref ref-type="fig" rid="fig1">Figure 1</xref>, all points tend to approach the regression line. This figure therefore shows a strong linear correlation between the predicted values of the first reduction potential by model and the experimental values. As for <xref ref-type="fig" rid="fig2">Figure 2</xref>, it shows that the predicted values by the model and the experimental values evolve in a similar way, particularly for the test set. Thus, these graphs confirm that the model is validated and is very efficient in predicting the redox potential. This reflects the adequacy of the theory level used to develop this model.</p></sec><sec id="s3_5"><title>3.5. Model Normality Tests</title><p>• Shapiro-Wilk’s test [<xref ref-type="bibr" rid="scirp.95878-ref48">48</xref>]</p><p>The data in <xref ref-type="table" rid="table7">Table 7</xref> shows that the calculated p-value is greater than 1 − α = 0.05 (5% threshold). Thus, the theoretical values of the first reduction potential obtained from the model follow a normal distribution law. This normal distribution is confirmed by the distribution of the point cloud according to the first bisector in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>• Durbin-Watson’s test [<xref ref-type="bibr" rid="scirp.95878-ref49">49</xref>]</p><p>The values in <xref ref-type="table" rid="table8">Table 8</xref> show that the calculated p-value is greater than 1 − α = 0.05 (5% threshold). It is therefore clear that the residues are not autocorrelated (zero correlation). Under these conditions, these residues do not contain information that can influence the model’s prediction of the first reduction potential. This interpretation is confirmed by the random distribution of the point cloud in <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><table-wrap id="table7" ><label><xref ref-type="table" rid="table7">Table 7</xref></label><caption><title> Values of the parameters of Shapiro-Wilk’s test</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Shapiro-Wilk’s parameter (W)</th><th align="center" valign="middle" >p-value</th><th align="center" valign="middle" >1 − α</th></tr></thead><tr><td align="center" valign="middle" >0.9539</td><td align="center" valign="middle" >0.1036</td><td align="center" valign="middle" >0.05</td></tr></tbody></table></table-wrap><table-wrap id="table8" ><label><xref ref-type="table" rid="table8">Table 8</xref></label><caption><title> Values of the parameters of Durbin-Watson’s test</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Durbin-Watson’s parameter (d)</th><th align="center" valign="middle" >p-value</th><th align="center" valign="middle" >1 − α</th></tr></thead><tr><td align="center" valign="middle" >1.8705</td><td align="center" valign="middle" >0.3402</td><td align="center" valign="middle" >0.05</td></tr></tbody></table></table-wrap></sec><sec id="s3_6"><title>3.6. Applicability Domain (AD) of the Model</title><p>The Applicability Domain (AD) has been determined by analyzing Williams’s diagram of <xref ref-type="fig" rid="fig5">Figure 5</xref>.</p><p>The examination of the Williams diagram shows that for training and test set, all observations have their standardized residuals between &#177;3 standard deviation units (&#177;3σ) [<xref ref-type="bibr" rid="scirp.95878-ref50">50</xref>]. This justifies the absence of outliers. The choice “3 units of standard deviation” was made because our data follow a normal distribution law. Indeed, for leverage effect, a value of 3 is commonly used as a limit value for accepting predictions because the points between &#177;3 standard deviation units cover on average 99% of the data that follow a normal distribution law [<xref ref-type="bibr" rid="scirp.95878-ref51">51</xref>]. With regard to the levers of the training set, except for the observation TCNQ_28, all the others have their levers below the threshold value (h<sup>*</sup> = 0.2000). In the case of the test set, it is observation TCNQ_34, which has its lever above the critical value. However, the value of a lever above the critical value does not always indicate an outlier for the developed model. Compounds of training set with levers above the threshold value with low residues stabilize the model and increase its accuracy. They are called “good influential points”. On the other hand, compounds with h<sub>ii</sub> greater than the critical value h<sup>*</sup> with large residues are called “bad influencing points” [<xref ref-type="bibr" rid="scirp.95878-ref51">51</xref>]. As a result, our elaborate QSPR (Quantitative Structure-Property Relationship) model does not show any evidence of aberrant observation of molecules in either set. The molecule TCNQ_28 is a “good influence point”. The results of the external validation showed that the model is suitable for predicting future redox potentials of TCNQ of this same family belonging to its applicability domain.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>The objective of this study was to develop a predictive QSPR (Quantitative Structure-Property Relationship) model linking the first reduction potential from a series of tetracyanoquinodimethane molecules analogous to quantum descriptors from the conceptual density functional theory. A predictive QSPR model dependent to electronic affinity has been developed. The determination coefficient R 2 = 0.9225 of this model shows that 92.25% of the experimental variance of the first reduction potential is explained by the model’s descriptor alone. The Fisher coefficient of this model is very high ( F = 333.3279 ) indicating that the regression equation is highly significant. The standard deviations ( s = 0.0694 ) are well below 0.50 indicating a good fit and high reliability of the prediction. Regarding the parameters of the internal and external validations, they revealed that the model is validated and is assumed to predict efficiently the first reduction potential. The cross-validation coefficient Q LOO 2 = 0.9136 indicates that 91.36% of molecules of the training set have their predicted first reduction potential. Regarding the external validation coefficient, Q e x t 2 = 0.9504 , it shows that 95.04% of the test set molecules have their predicted first reduction potentials. Thus, to search for new tetracyanoquinodimethane (TCNQ) acceptors of this same family with the desired first reduction potentials, one can play on electronic affinity.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Diarrassouba, F., Kon&#233;, M., Bamba, K., Traor&#233;, Y., Kon&#233;, M.G.-R. and Assanvo, E.F. (2019) Development of Predictive QSPR Model of the First Reduction Potential from a Series of Tetracyanoquinodimethane (TCNQ) Molecules by the DFT (Density Functional Theory) Method. Computational Chemistry, 7, 121-142. https://doi.org/10.4236/cc.2019.74009</p></sec></body><back><ref-list><title>References</title><ref id="scirp.95878-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Prasad, P.N. and Ulrich, D.R. (1988) Nonlinear Optical and Electroactive Polymers. Springer, Boston, 444 p. https://doi.org/10.1007/978-1-4613-0953-6</mixed-citation></ref><ref id="scirp.95878-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Cuevas, J.C. and Scheer, E. (2010) Molecular Electronics: An Introduction to Theory and Experiment. World Scientific Publishing Co. Pte. Ltd., Singapore, 709 p. https://doi.org/10.1142/7434</mixed-citation></ref><ref id="scirp.95878-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Joran, A.D., et al. (1987) Effect of Exothermicity on Electron Transfer Rates in Photosynthetic Molecular Models. Nature, 327, 508-511. https://doi.org/10.1038/327508a0</mixed-citation></ref><ref id="scirp.95878-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Shen, X.Y., et al. (2013) Effects of Substitution with Donor-Acceptor Groups on the Properties of Tetraphenylethene Trimer: Aggregation-Induced Emission, Solvatochromism, and Mechanochromism. The Journal of Physical Chemistry, 117, 7334-7347. https://doi.org/10.1021/jp311360p</mixed-citation></ref><ref id="scirp.95878-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Marcus, R.A. (1993) Electron Transfer Reactions in Chemistry. Theory and Experiment. Reviews of Modern Physics, 65, 599-610. https://doi.org/10.1103/RevModPhys.65.599</mixed-citation></ref><ref id="scirp.95878-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Klots, C.E., Compton, R.N. and Raaen, V.F. (1974) Electronic and Ionic Properties of Molecular TTF and TCNQ. The Journal of Chemical Physics, 60, 1177-1178. https://doi.org/10.1063/1.1681130</mixed-citation></ref><ref id="scirp.95878-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Milián, B., Pou-Amérigo, R., Viruela, R. and Ortí, E. (2004) On the Electron Affinity of TCNQ. Chemical Physics Letters, 391, 148-151. https://doi.org/10.1016/j.cplett.2004.04.102</mixed-citation></ref><ref id="scirp.95878-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Zhu, G.Z. and Wang, L.S. (2015) Communication: Vibrationally Resolved Photoelectron Spectroscopy of the Tetracyanoquinodimethane (TCNQ) Anion and Accurate Determination of the Electron Affinity of TCNQ. The Journal of Chemical Physics, 143, Article ID: 221102. https://doi.org/10.1063/1.4937761</mixed-citation></ref><ref id="scirp.95878-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">P&amp;#229;lsson, L.O., et al. (2003) Orientation and Solvatochromism of Dyes in Liquid Crystals. Molecular Crystals and Liquid Crystals, 402, 43-53. https://doi.org/10.1080/744816685</mixed-citation></ref><ref id="scirp.95878-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Bloor, D., et al. (2001) Matrix Dependence of Light Emission from TCNQ Adducts. Journal of Materials Chemistry, 11, 3053-3062. https://doi.org/10.1039/b104992p</mixed-citation></ref><ref id="scirp.95878-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Cole, J.M., et al. (2002) Charge-Density Study of the Nonlinear Optical Precursor DED-TCNQ at 20 K. Physical Review B, 65, Article ID: 125107. https://doi.org/10.1103/PhysRevB.65.125107</mixed-citation></ref><ref id="scirp.95878-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Bando, P., et al. (1994) Single-Component Donor-Acceptor Organic Semiconductors Derived from TCNQ. The Journal of Organic Chemistry, 59, 4618-4629. https://doi.org/10.1021/jo00095a042</mixed-citation></ref><ref id="scirp.95878-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Arena, A., Patanè, S. and Saitta, G. (1988) Study of a New Organic Semiconductor Based on TCNQ and of Its Junction with Doped Silicon (TCNQ = 7, 7’8, 8’ Tetracyanoquinodimethane). Il Nuovo Cimento, 20, 907-913. https://doi.org/10.1007/BF03185493</mixed-citation></ref><ref id="scirp.95878-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Wheland, R.C. (1976) Correlation of Electrical Conductivity in Charge-Transfer Complexes with Redox Potentials, Steric Factors, and Heavy Atom Effects. Journal of the American Chemical Society, 98, 3926-3930. https://doi.org/10.1021/ja00429a031</mixed-citation></ref><ref id="scirp.95878-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Règlement (CE) n° 1907/2006 du Parlement Européen et du Conseil du 18 décembre 2006 concernant l’enregistrement, l’évaluation et l’autorisation des substances chimiques, ainsi que les restrictions applicables à ces substances (REACH), instituant une agence européenne des produits chimiques, modifiant la directive 1999/45/CE et abrogeant le règlement (CEE) n° 793/93 du Conseil et le règlement (CE) n° 1488/94 de la Commission ainsi que la directive 76/769/CEE du Conseil et les directives 91/155/CEE, 93/67/CEE, 93/105/CE et 2000/21/CE de la Commission.</mixed-citation></ref><ref id="scirp.95878-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Margossian, N. (2008) Le règlement REACH—La règlementationeuropéenne sur les produits chimiques. Dunod/L’Usine Nouvelle, Paris.</mixed-citation></ref><ref id="scirp.95878-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Delaney, J.J. (1997) Synthesis of New Heterocyclic TCNQ Analogues. Doctorate of Philosophy, Dublin City University (School of Chemical Sciences), Dublin, 202 p.</mixed-citation></ref><ref id="scirp.95878-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Andersen, J.R. and Jorgensen, O. (1979) Organic Metals. Mono- and 2,5-Di-Substituted 7,7,8,8-Tetracyano-P-Quinodimethanes and Conductivities of Their Charge-Transfer Complexes. Royal Chemical Society, Journal of Perkin Transactions, 1, 3095-3098. https://doi.org/10.1039/P19790003095</mixed-citation></ref><ref id="scirp.95878-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Wheland, R.C. and Gillson, J.L. (1976) Synthesis of Electrically Conductive Organic Solids. Journal of the American Chemical Society, 98, 3916-3925. https://doi.org/10.1021/ja00429a030</mixed-citation></ref><ref id="scirp.95878-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Ferraris, J.P. and Saito, G. (1978) Organic Metals with Asymmetric Acceptors: The Monofluorotetracyanoquino-Dimethane Anion. Journal of the Chemical Society, Chemical Communications, No. 22, 992-993. https://doi.org/10.1039/C39780000992</mixed-citation></ref><ref id="scirp.95878-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Saito, G. and Ferraris, J.P. (1979) Difluorotetracyanoquinodimethane: Electron Affinity Cut-Off for “Metallic” Behaviour in a Tetrathiafulvalene Salt. Journal of the Chemical Society, Chemical Communications, No. 22, 1027-1029. https://doi.org/10.1039/C39790001027</mixed-citation></ref><ref id="scirp.95878-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Tsubata, Y., Suzuki, T., Yamashita, Y., Mukai, T. and Miyashi, T. (1992) Tetracyanoquinodimethanes Fused with 13, s-Thiadiazole and Pyrazine Units. Heterocycles, 33, 337-348. https://doi.org/10.3987/COM-91-S44</mixed-citation></ref><ref id="scirp.95878-ref23"><label>23</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Yamashita</surname><given-names> Y. </given-names></name>,<etal>et al</etal>. (<year>1989</year>)<article-title>Novel Electron Acceptors and Donors Containing Fused-Hetero-cycles</article-title><source> Journal of Synthetic Organic Chemistry</source><volume> 47</volume>,<fpage> 1108</fpage>-<lpage>1117</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.95878-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Dennington, R., Keith, T. and Millam, J. (2009) GaussView Version 5. Semichem Inc., Shawnee Mission.</mixed-citation></ref><ref id="scirp.95878-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Frisch, M.J., Trucks, G.W., Schlegel, H.B., Scuseria, G.E., Robb, M.A., Cheeseman, J.R., Scalmani, G., Barone, V., Mennucci, B., Petersson, G.A., Nakatsuji, H., Caricato, M., Li, X., Hratchian, H.P., Izmaylov, A.F., Bloino, J., Zheng, G., Sonnenberg, J.L., Hada, M., Ehara, M., Toyota, K., Fukuda, R., Hasegawa, J., Ishida, M., Nakajima, T., Honda, Y., Kitao, O., Nakai, H., Vreven, T., Montgomery, J.A., Peralta, J.E., Ogliaro, F., Bearpark, M., Heyd, J.J., Brothers, E., Kudin, K.N., Staroverov, V.N., Kobayashi, R., Normand, J., Raghavachari, K., Rendell, A., Burant, J.C., Iyengar, S.S., Tomasi, J., Cossi, M., Rega, N., Millam, J.M., Klene, M., Knox, J.E., Cross, J.B., Bakken, V., Adamo, C., Jaramillo, J., Gomperts, R., Stratmann, R.E., Yazyev, O., Austin, A.J., Cammi, R., Pomelli, C., Ochterski, J.W., Martin, R.L., Morokuma, K., Zakrzewski, V.G., Voth, G.A., Salvador, P., Dannenberg, J.J., Dapprich, S., Daniels, A.D., Farkas, O., Foresman, J.B., Ortiz, J.V., Cioslowski, J. and Fox, D.J. (2009) Gaussian 09, Revision A.02. Gaussian, Inc., Wallingford.</mixed-citation></ref><ref id="scirp.95878-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">(2015) ACDLABS 10. Advanced Chemistry Development Inc., Toronto.</mixed-citation></ref><ref id="scirp.95878-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Microsoft&amp;reg; Excel&amp;reg; 2010.</mixed-citation></ref><ref id="scirp.95878-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">(2014) XLSTAT Version 2014.5.03, Copyright Addinsoft 1995-2014.</mixed-citation></ref><ref id="scirp.95878-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Minitab&amp;reg; 18.</mixed-citation></ref><ref id="scirp.95878-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Vessereau, A. (1988) Méthodes statistiques en biologie et en agronomie. Lavoisier (Tec &amp; Doc), Paris, 538 p.</mixed-citation></ref><ref id="scirp.95878-ref31"><label>31</label><mixed-citation publication-type="other" xlink:type="simple">Chatterje, S. and Hadi, A.S. (2006) Regression Analysis by Example. 4th Edition, John Wiley &amp; Son, Inc., Hoboken, 366 p. https://doi.org/10.1002/0470055464</mixed-citation></ref><ref id="scirp.95878-ref32"><label>32</label><mixed-citation publication-type="other" xlink:type="simple">Siegel, A.F. (1997) Practical Business Statistics. IRWIN, 3rd Edition.</mixed-citation></ref><ref id="scirp.95878-ref33"><label>33</label><mixed-citation publication-type="other" xlink:type="simple">Besse, P. (2003) Pratique de la modélisation statistique, Publications du laboratoire de statistique et Probabilité.</mixed-citation></ref><ref id="scirp.95878-ref34"><label>34</label><mixed-citation publication-type="other" xlink:type="simple">Cook, R.D. and Weisberg, S. (1994) An Introduction to Regression Graphics. Wiley Series in Probability and Mathematical Statistics, Hoboken, 265 p. https://doi.org/10.1002/9780470316863</mixed-citation></ref><ref id="scirp.95878-ref35"><label>35</label><mixed-citation publication-type="other" xlink:type="simple">Kubinyi, H. (1994) Variable Selection in QSAR Studies. I. An Evolutionary Algorithm. Quantitative Structure-Activity Relationships, 13, 285-294. https://doi.org/10.1002/qsar.19940130306</mixed-citation></ref><ref id="scirp.95878-ref36"><label>36</label><mixed-citation publication-type="other" xlink:type="simple">Golbraikh, A. and Tropsha, A. (2002) Beware of q2! Journal of Molecular Graphics and Modelling, 20, 269-276. https://doi.org/10.1016/S1093-3263(01)00123-1</mixed-citation></ref><ref id="scirp.95878-ref37"><label>37</label><mixed-citation publication-type="other" xlink:type="simple">Todeschini, R. (2010) Milano, Chemometrics and QSAR Research Group. University of Milano Bicocca, Milano.</mixed-citation></ref><ref id="scirp.95878-ref38"><label>38</label><mixed-citation publication-type="other" xlink:type="simple">Roy, P.P., Paul, S., Mitra, I. and Roy, K. (2009) On Two Novel Parameters for Validation of Predictive QSAR Models. Molecules, 14, 1660-1701. https://doi.org/10.3390/molecules14051660</mixed-citation></ref><ref id="scirp.95878-ref39"><label>39</label><mixed-citation publication-type="other" xlink:type="simple">Consonni, V., Ballabio, D. and Todeschini, R. (2010) Evaluation of Model Predictive Ability by External Validation Techniques. Journal of Chemometrics, 24, 194-201. https://doi.org/10.1002/cem.1290</mixed-citation></ref><ref id="scirp.95878-ref40"><label>40</label><mixed-citation publication-type="other" xlink:type="simple">Roy, K., Mitra, I., Kar, S., Ojha, P.K., Das, R.N. and Kabir, H. (2012) Comparative Studies on Some Metrics for External Validation of QSPR Models. Journal of Chemical Information and Modeling, 52, 396-408. https://doi.org/10.1021/ci200520g</mixed-citation></ref><ref id="scirp.95878-ref41"><label>41</label><mixed-citation publication-type="other" xlink:type="simple">Tropsha, A., Gramatica, P. and Gombar, V.K. (2003) The Importance of Being Earnest: Validation Is the Absolute Essential for Successful Application and Interpretation of QSPR Models. QSAR &amp; Combinatorial Science, 22, 69-77. https://doi.org/10.1002/qsar.200390007</mixed-citation></ref><ref id="scirp.95878-ref42"><label>42</label><mixed-citation publication-type="other" xlink:type="simple">Ouattara, O. and Ziao, N. (2017) Quantum Chemistry Prediction of Molecular Lipophilicity Using Semi-Empirical AM1 and Ab Initio HF/6-311++G Levels. Computational Chemistry, 5, 38-50. https://doi.org/10.4236/cc.2017.51004</mixed-citation></ref><ref id="scirp.95878-ref43"><label>43</label><mixed-citation publication-type="other" xlink:type="simple">Gramatica, P. (2007) Principles of QSAR Models Validation: Internal &amp; External. QSAR and Combinatorial Sciences, 26, 694-701. https://doi.org/10.1002/qsar.200610151</mixed-citation></ref><ref id="scirp.95878-ref44"><label>44</label><mixed-citation publication-type="other" xlink:type="simple">Netzeva, T.I., Worth, A.P., Aldenberg, T., Benigni, R., Cronin, M.T.D., Gramatica, P., Jaworska, J.S., Kahn, S., Klopman, G., Marchant, C.A., Myatt, G., Nikolova-Jeliazkova, N., Patlewicz, G.Y., Perkins, R., Roberts, D.W., Schultz, T.W., Stanton, D.T., Van De Sandt, J.J.M., Tong, W., Veith, G. and Yang, C. (2005) Current Status of Methods for Defining the Applicability Domain of (Quantitative) Structure-Activity Relationships. Alternatives to Laboratory Animals, 33, 155-173. https://doi.org/10.1177/026119290503300209</mixed-citation></ref><ref id="scirp.95878-ref45"><label>45</label><mixed-citation publication-type="other" xlink:type="simple">Koopmans, T. (1933) über die Zuordnung von Wellenfunktionen und Eigenwerten zu den Einzelnen Elektronen Eines Atoms. Physica, 1, 104-113. https://doi.org/10.1016/S0031-8914(34)90011-2</mixed-citation></ref><ref id="scirp.95878-ref46"><label>46</label><mixed-citation publication-type="other" xlink:type="simple">Kenny, P.W. (1995) Prediction of Planarity and Reduction Potential of Derivatives of Tetracyanoquinodimethane Using Ab Initio Molecular Orbital Theory. Journal of the Chemical Society, Perkin Transactions, 2, 907-909. https://doi.org/10.1039/p29950000907</mixed-citation></ref><ref id="scirp.95878-ref47"><label>47</label><mixed-citation publication-type="other" xlink:type="simple">Erikson, L., Jaworska, J., Worth, A., Cromin, M., McDowell, R.M. and Gramatica, P. (2003) Methods for Reliability, Uncertainty Assessment, and Applicability Evaluations of Regression Based and Classification QSPRs. Environmental Health Perspective, 111, 1361-1375. https://doi.org/10.1289/ehp.5758</mixed-citation></ref><ref id="scirp.95878-ref48"><label>48</label><mixed-citation publication-type="other" xlink:type="simple">Shapiro, S.S. and Wilk, M.B. (1965) An Analysis of Variance Test for Normality (Complete Samples). Biometrika, 52, 591-611. https://doi.org/10.1093/biomet/52.3-4.591</mixed-citation></ref><ref id="scirp.95878-ref49"><label>49</label><mixed-citation publication-type="other" xlink:type="simple">Durbin, J. and Watson, G.S. (1951) Testing for Serial Correlation in Least Squares Regression, II. Biometrika, 38, 159-178. https://doi.org/10.1093/biomet/38.1-2.159</mixed-citation></ref><ref id="scirp.95878-ref50"><label>50</label><mixed-citation publication-type="other" xlink:type="simple">Touhami, I., Mokrani, K. and Messadi, D. (2012) Modèles QSRR hybridesalgorithmegénétique-régressionlinéaire multiple des indices de rétention de pyrazines en chromatographie gazeuse. Lebanese Science Journal, 13, 75-88.</mixed-citation></ref><ref id="scirp.95878-ref51"><label>51</label><mixed-citation publication-type="other" xlink:type="simple">Jaworska, J., Nikolova-Jeliazkova, N. and Aldenberg, T. (2005) QSAR Applicability Domain Estimation by Projection of the Training Set in Descriptor Space: A Review. ATLA, 33, 445-459. https://doi.org/10.1177/026119290503300508</mixed-citation></ref></ref-list></back></article>