<?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">OJIC</journal-id><journal-title-group><journal-title>Open Journal of Inorganic Chemistry</journal-title></journal-title-group><issn pub-type="epub">2161-7406</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojic.2018.81004</article-id><article-id pub-id-type="publisher-id">OJIC-82201</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>
 
 
  Theoretical and Comparative Study of the Complex [RuCl&lt;sub&gt;3&lt;/sub&gt;(H&lt;sub&gt;2&lt;/sub&gt;O)&lt;sub&gt;2&lt;/sub&gt;(Gly)] by Density Functional Theory
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kátia</surname><given-names>Meirelles D. de Sousa</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>Marcio</surname><given-names>Adriano S. Chagas</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>Jesyca</surname><given-names>Mayra F. D. dos Santos</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>Anderson</surname><given-names>D. Galv&amp;atilde;o</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>Fabrício</surname><given-names>Tarso de Moraes</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>Andressa</surname><given-names>Teixeira Barros Nunes Ribeiro</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>Dário</surname><given-names>Batista Fortaleza</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>Kelly</surname><given-names>Aparecida da Encarnação Amorim</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>Wagner</surname><given-names>B. dos Santos</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>Materials Research Lab, Federal University of Mato Grosso—Campus II, Barra do Gar&amp;amp;ccedil;as, Brazil</addr-line></aff><aff id="aff2"><addr-line>Institute of Chemistry, Brasília University, UNB, Brasília, Brazil</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>katiamds0@gmail.com(KMDDS)</email>;<email>wbsantos@ufmt.br(WBDS)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>12</day><month>12</month><year>2017</year></pub-date><volume>08</volume><issue>01</issue><fpage>43</fpage><lpage>53</lpage><history><date date-type="received"><day>28,</day>	<month>December</month>	<year>2017</year></date><date date-type="rev-recd"><day>28,</day>	<month>January</month>	<year>2018</year>	</date><date date-type="accepted"><day>31,</day>	<month>January</month>	<year>2018</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, the use of computational methods was essential to distinguish the three possible isomeric structures of the [RuCl
  <sub>3</sub>(H
  <sub>2</sub>O)
  <sub>2</sub>(Gly)] molecule. The characterization of these molecules was performed using IR, NMR and UV-VIS simulations. Some calculations related to the optimization of structures and properties such as chemical hardness and dipole moment were also conducted. The fac-cis isomer presented promising data when compared to the experimental data, indicating that this is the likely experimentally synthesized isomer. This study demonstrates the technical utility of the computational calculations by virtue of situations that prevent the realization of X-ray diffraction.
 
</p></abstract><kwd-group><kwd>Computational Methods</kwd><kwd> Isomeric Structures</kwd><kwd> Simulations</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Computational calculations are widely used in research to confirm geometric structures and to determine the properties of coordination compounds [<xref ref-type="bibr" rid="scirp.82201-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref4">4</xref>] , especially in cases where obtaining a single crystal for X-ray diffraction is not possible [<xref ref-type="bibr" rid="scirp.82201-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref6">6</xref>] or inconclusive [<xref ref-type="bibr" rid="scirp.82201-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref7">7</xref>] .</p><p>Chagas [<xref ref-type="bibr" rid="scirp.82201-ref8">8</xref>] began to develop the study of the complex [RuCl<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>(Gly)] in 2012. In biological tests performed by Salama [<xref ref-type="bibr" rid="scirp.82201-ref9">9</xref>] , Chagas [<xref ref-type="bibr" rid="scirp.82201-ref8">8</xref>] observed the potential Leishmanicidal activity of its complex. Mart&#237;nez et al. [<xref ref-type="bibr" rid="scirp.82201-ref10">10</xref>] , Iniguez et al. [<xref ref-type="bibr" rid="scirp.82201-ref11">11</xref>] and Barbosa et al. [<xref ref-type="bibr" rid="scirp.82201-ref12">12</xref>] demonstrated that some of their ruthenium compounds exhibited improved antileishmanial activity compared with the reference compound and their free ligand.</p><p>Structural variations depending on the size of the molecule, the position of the ligands and their spatial characteristics such as flatness and three-dimensionality help to understand the action of these molecules in the biological environment, as the interaction of a molecule with a biological receptor depends on this type of structural information [<xref ref-type="bibr" rid="scirp.82201-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref14">14</xref>] . Previous research has shown the utility and exploitation of structural knowledge in areas such as catalytic activity and the use of computational calculations in these studies [<xref ref-type="bibr" rid="scirp.82201-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref16">16</xref>] . Gianferrara, Bratsos and Alessio [<xref ref-type="bibr" rid="scirp.82201-ref17">17</xref>] give a good account of the conditions mentioned in the paragraph beginning, based on some examples such as cisplatin and ruthenium compounds (NAMI-A and KP1019), which are anticancer drugs currently in use and under development, respectively.</p><p>This study used computational methods to determine the possible geometric isomers of the compound [RuCl<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>(Gly)], in comparison with experimental data, illustrating the usefulness of computational methods to elucidate the possible geometrical structures of a compound in situations in which a single crystal for X-ray diffraction cannot be obtained.</p></sec><sec id="s2"><title>2. Methodology</title><p>All calculations were performed using the Gaussian program package 09 [<xref ref-type="bibr" rid="scirp.82201-ref18">18</xref>] . The geometries were optimized by the DFT method (Density Functional Theory) and the functional hybrid meta-GGA M06-2x [<xref ref-type="bibr" rid="scirp.82201-ref19">19</xref>] , and confirmed by vibrational analysis. The basis set used was 6-311++G(d,p) [<xref ref-type="bibr" rid="scirp.82201-ref20">20</xref>] for all atoms except for Ruthenium, which was treated with the basis sets SDD (Stuttgart/double-ζ Dresden) and ECP (effective core potential) for the innermost electrons of the ruthenium atom [<xref ref-type="bibr" rid="scirp.82201-ref21">21</xref>] . The harmonic vibrational frequencies were calculated with the analytical second derivative, without the presence of imaginary frequencies. For the calculations of 35 excited states, the time dependent method (TDDFT) with an open layer was used with a polarized solid model to determine the effect of the solvent water molecule through IEF (integral equation formalism). For the comparison of nuclear magnetic resonance, the calculation was performed by the GIAO method (Atomic Orbital Measure Independent) [<xref ref-type="bibr" rid="scirp.82201-ref22">22</xref>] for <sup>13</sup>C and <sup>1</sup>H in the presence of the solvent water. All DFT calculations employed the keyword int (grid = ultrafine). All calculations were performed at the Federal University of Mato Grosso, Laborat&#243;rio de Estudos de Materiais. All experimental data were obtained for comparison of the findings [<xref ref-type="bibr" rid="scirp.82201-ref8">8</xref>] .</p></sec><sec id="s3"><title>3. Results and Discussion</title><p>The [RuCl<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>(Gly)] molecule described by Chagas [<xref ref-type="bibr" rid="scirp.82201-ref8">8</xref>] , can generate three possible geometric isomers: fac-cis-diaquotrischloroglycinatoruthenium III, mer-cis-diaquotrischloroglycinatoruthenium III and mer-trans-diaquotrischloroglycinatoruthenium III. As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>To determine which isomer was synthesized by Chagas [<xref ref-type="bibr" rid="scirp.82201-ref8">8</xref>] , computational methods were used to investigate the characteristics of each isomer compared to the experimental data.</p><sec id="s3_1"><title>3.1. Energy of the Geometrical Isomers</title><p><xref ref-type="table" rid="table1">Table 1</xref> shows the data obtained from the energy optimization of each isomer. The data show that the mer-trans isomer showed the largest relative difference when compared to the fac-cis molecule with the lowest energy. The fac-cis molecule, with lower energy compared to the other two isomers, had greater stability. However, the energies of the three structures were very close and the lowest energy does not guarantee formation of the compound experimentally. Thus, IR, UV-vis and NMR simulations were performed to elucidate the structure [<xref ref-type="bibr" rid="scirp.82201-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref23">23</xref>] .</p></sec><sec id="s3_2"><title>3.2. Infrared Simulation</title><p>The infrared frequencies of the three isomers showed similar values to each other. It was also observed that, when compared to the experimental data, the fac-cis and mer-trans isomers demonstrated a closer approximation as show in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>The fac isomer showed lower frequencies than the mer isomers for the same bandwidth allocations in regions below 1000 cm<sup>−1</sup>. However, a difference was</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Relative energies of isomers of the molecule [RuCl<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>gly]</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Molecules</th><th align="center" valign="middle" >Optmization energy (Hartree)</th><th align="center" valign="middle" >Relative energies (kCal∙mol<sup>−</sup><sup>1</sup>)</th></tr></thead><tr><td align="center" valign="middle" >fac-cis</td><td align="center" valign="middle" >−1912.7912080</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" >mer-cis</td><td align="center" valign="middle" >−1912.7794975</td><td align="center" valign="middle" >7,35</td></tr><tr><td align="center" valign="middle" >mer-trans</td><td align="center" valign="middle" >−1912.7661652</td><td align="center" valign="middle" >15,71</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Calculated frequency by DFT of isomers [RuCl<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>(Gly)], and FTIR<sub>med</sub> (4000 - 600 cm<sup>−1</sup>) with approximate assignment bands</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >(fac-cis)</th><th align="center" valign="middle" >(mer-cis)</th><th align="center" valign="middle" >(mer-trans)</th><th align="center" valign="middle" >Experimental</th><th align="center" valign="middle" >Assigned bands</th></tr></thead><tr><td align="center" valign="middle" >1791</td><td align="center" valign="middle" >1848</td><td align="center" valign="middle" >1730</td><td align="center" valign="middle" >1664</td><td align="center" valign="middle" >νa (COO<sup>−</sup>)</td></tr><tr><td align="center" valign="middle" >1395</td><td align="center" valign="middle" >1290</td><td align="center" valign="middle" >1454</td><td align="center" valign="middle" >1388</td><td align="center" valign="middle" >νs (COO<sup>−</sup>)</td></tr><tr><td align="center" valign="middle" >1665 - 1595</td><td align="center" valign="middle" >1667 - 1613</td><td align="center" valign="middle" >1654 - 1589</td><td align="center" valign="middle" >1571</td><td align="center" valign="middle" >δ ( NH 3 + )</td></tr><tr><td align="center" valign="middle" >1510</td><td align="center" valign="middle" >1516</td><td align="center" valign="middle" >1513</td><td align="center" valign="middle" >1490</td><td align="center" valign="middle" >δs( NH 3 + )</td></tr><tr><td align="center" valign="middle" >1479</td><td align="center" valign="middle" >1472</td><td align="center" valign="middle" >1491</td><td align="center" valign="middle" >1441</td><td align="center" valign="middle" >δ(CH<sub>2</sub>)</td></tr><tr><td align="center" valign="middle" >1344</td><td align="center" valign="middle" >1373</td><td align="center" valign="middle" >1348</td><td align="center" valign="middle" >1334 - 1322</td><td align="center" valign="middle" >ρw(CH<sub>2</sub>)</td></tr><tr><td align="center" valign="middle" >1118</td><td align="center" valign="middle" >1112</td><td align="center" valign="middle" >1125</td><td align="center" valign="middle" >1155 - 1110</td><td align="center" valign="middle" >ρr( NH 3 + )</td></tr><tr><td align="center" valign="middle" >1015</td><td align="center" valign="middle" >1027</td><td align="center" valign="middle" >1003</td><td align="center" valign="middle" >1043</td><td align="center" valign="middle" >ν (C-N) + ν (C-C)</td></tr><tr><td align="center" valign="middle" >905</td><td align="center" valign="middle" >910</td><td align="center" valign="middle" >924</td><td align="center" valign="middle" >927</td><td align="center" valign="middle" >ρr(CH<sub>2</sub>)</td></tr><tr><td align="center" valign="middle" >871</td><td align="center" valign="middle" >894</td><td align="center" valign="middle" >897</td><td align="center" valign="middle" >889</td><td align="center" valign="middle" >ν (CCN)</td></tr><tr><td align="center" valign="middle" >676</td><td align="center" valign="middle" >-----</td><td align="center" valign="middle" >-----</td><td align="center" valign="middle" >684</td><td align="center" valign="middle" >ρw(COO<sup>−</sup>)</td></tr><tr><td align="center" valign="middle" >617</td><td align="center" valign="middle" >635</td><td align="center" valign="middle" >647</td><td align="center" valign="middle" >607</td><td align="center" valign="middle" >δ(COO<sup>−</sup>)</td></tr></tbody></table></table-wrap><p>Not observed. νa: Asymmetrical stretch; νs: Symmetrical stretch; δa: Asymmetrical bending; δs: symmetrical bending; ρw: Wagging deformation; ρr: Rocking deformation.</p><p>not observed between mer-trans and mer-cis, which did not conform to any general pattern.</p><p>R M S = 1 n − 1 ∑ i n ( v i c a l − v i exp ) 2</p><p>The root mean square error (RMSE) between the experimental and the calculated frequency of the molecules were 42.44 cm<sup>−1</sup> (fac-cis), 75.67 cm<sup>−1</sup> (mer-cis) and 37.36 cm<sup>−1</sup> (mer-trans), with the lowest RMSE found for the mer-trans molecule, according to the above equation [<xref ref-type="bibr" rid="scirp.82201-ref24">24</xref>] . The overestimated values of the calculated frequency were due to neglecting anharmonicity. The calculation was performed on a single molecule, disregarding intermolecular interactions [<xref ref-type="bibr" rid="scirp.82201-ref25">25</xref>] .</p><p>The theoretical and experimental spectra in <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref> showed characteristic peaks related to the glycine molecule and the compound. The carboxylate group showed variations between asymmetric and symmetric peaks, which assisted in the distinction of the three isomeric structures of the theoretical spectra as fac-cis (396 cm<sup>−1</sup>), mer-cis (558 cm<sup>−1</sup>) and mer-trans (276 cm<sup>−1</sup>). This distinction was observed in a previous work was well Alam et al. [<xref ref-type="bibr" rid="scirp.82201-ref26">26</xref>] . The</p><p>experimental spectrum showed a variation between asymmetric and symmetric peaks of 276 cm<sup>−1</sup>. The peak at 676 cm<sup>−1</sup> was assigned to a “wagging” group (COO<sup>−</sup>) in the fac-cis isomer and was not observed in the mer isomers.</p></sec><sec id="s3_3"><title>3.3. Ultraviolet-Visible Simulation</title><p><xref ref-type="table" rid="table3">Table 3</xref> shows the data on electron density-related oscillator strength. Ligand charge transfer to the metal (LMCT) can be evidenced by the HOMO and</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Electronic density of the molecular frontier orbitals</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Isomers</th><th align="center" valign="middle" >Homo (orbitals)</th><th align="center" valign="middle" >Characteristics</th><th align="center" valign="middle" >Lumo (orbitals)</th></tr></thead><tr><td align="center" valign="middle" >fac-cis</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/4-1310179x9.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >State 16 Orbital 58β → 64β Energy 7.59 (eV)</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/4-1310179x10.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >mer-cis</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/4-1310179x11.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >State 14 Orbital 59β → 64β Energy 7.08 (eV)</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/4-1310179x12.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >mer-trans</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/4-1310179x13.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >State 14 Orbital 60β → 64β Energy 6.96 (eV)</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/4-1310179x14.png" xlink:type="simple"/></inline-formula></td></tr></tbody></table></table-wrap><p>LUMO, referring to the excited states shown in <xref ref-type="table" rid="table4">Table 4</xref>. The excited state closest to the experimental value was presented by the fac-cis molecule.</p><p>The values related to states 19 and 26 (fac-cis), 19 and 22 (mer-cis) and 22 and 27 (mer-trans) show π-π* type transitions relating to the glycine binder. The greatest contribution of the chlorides to the metal center occurred in states 19, 16 and 19 of the fac-cis structures, mer-cis and mer-trans, respectively.</p></sec><sec id="s3_4"><title>3.4. Molecular Properties</title><p>The HOMO is the occupied orbital with the highest energy that has the ability to donate electrons, while the LUMO is the unoccupied orbital with the least energy that has the ability to accept electrons; the difference between them can explain charge transfer within a molecule [<xref ref-type="bibr" rid="scirp.82201-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref28">28</xref>] . The HOMO and LUMO data energies as well as their differences are shown in <xref ref-type="table" rid="table5">Table 5</xref>.</p><p>The range of energy between HOMO and LUMO as well as the hardness and chemical dipole moment may provide additional information. The fac-cis molecule had the largest energy difference and greater chemical hardness, making it more stable kinetically and less favorable to adding electrons to LUMO or extracting electrons from HOMO, i.e. this molecule had low chemical reactivity [<xref ref-type="bibr" rid="scirp.82201-ref29">29</xref>] [<xref ref-type="bibr" rid="scirp.82201-ref30">30</xref>] .</p><p>The dipole moment implies that the higher the stronger value is an intermolecular interaction [<xref ref-type="bibr" rid="scirp.82201-ref30">30</xref>] , The mer-trans molecule should form stronger intermolecular bonds than the other two isomers, for example with other molecules or DNA bases, as shown previously Pramanik et al. [<xref ref-type="bibr" rid="scirp.82201-ref30">30</xref>] and Das et al. [<xref ref-type="bibr" rid="scirp.82201-ref31">31</xref>] .</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Excitation energies (eV), Oscillator strength (f) and wave length (nm) calculated and experimental</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Molecules</th><th align="center" valign="middle" >States</th><th align="center" valign="middle" >λ (nm)</th><th align="center" valign="middle" >eV</th><th align="center" valign="middle" >f</th><th align="center" valign="middle" >exp</th></tr></thead><tr><td align="center" valign="middle"  rowspan="4"  >fac-cis</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >314.98</td><td align="center" valign="middle" >3.9363</td><td align="center" valign="middle" >0.0162</td><td align="center" valign="middle"  rowspan="5"  >290 (LMCT)</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >287.49</td><td align="center" valign="middle" >4.3127</td><td align="center" valign="middle" >0.0260</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >257.63</td><td align="center" valign="middle" >4.8124</td><td align="center" valign="middle" >0.0087</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >238.53</td><td align="center" valign="middle" >5.1979</td><td align="center" valign="middle" >0.0093</td></tr><tr><td align="center" valign="middle"  rowspan="4"  >mer-cis</td><td align="center" valign="middle" >14</td><td align="center" valign="middle" >319.96</td><td align="center" valign="middle" >3.8750</td><td align="center" valign="middle" >0.0101</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >304.82</td><td align="center" valign="middle" >4.0675</td><td align="center" valign="middle" >0.0161</td><td align="center" valign="middle"  rowspan="7"  >230 (π-π*)</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >263.97</td><td align="center" valign="middle" >4.6969</td><td align="center" valign="middle" >0.0292</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >251.81</td><td align="center" valign="middle" >4.9236</td><td align="center" valign="middle" >0.0079</td></tr><tr><td align="center" valign="middle"  rowspan="4"  >mer-trans</td><td align="center" valign="middle" >14</td><td align="center" valign="middle" >321.58</td><td align="center" valign="middle" >3.8555</td><td align="center" valign="middle" >0.0119</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >283.60</td><td align="center" valign="middle" >4.3718</td><td align="center" valign="middle" >0.0170</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >257.28</td><td align="center" valign="middle" >4.8190</td><td align="center" valign="middle" >0.0223</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >244.79</td><td align="center" valign="middle" >5.0648</td><td align="center" valign="middle" >0.0337</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Calculated data of some molecular properties</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Molecules</th><th align="center" valign="middle" >Homo eV</th><th align="center" valign="middle" >Lumo eV</th><th align="center" valign="middle" >Homo-lumo gap ∆(eV)</th><th align="center" valign="middle" >Chemical hardness (η)</th><th align="center" valign="middle" >Dipole moment &#181; (Debye)</th></tr></thead><tr><td align="center" valign="middle" >fac-cis</td><td align="center" valign="middle" >−8.2584</td><td align="center" valign="middle" >−2.2746</td><td align="center" valign="middle" >5.9838</td><td align="center" valign="middle" >2.9919</td><td align="center" valign="middle" >7.6920</td></tr><tr><td align="center" valign="middle" >mer-cis</td><td align="center" valign="middle" >−8.2682</td><td align="center" valign="middle" >−2.5070</td><td align="center" valign="middle" >5.7612</td><td align="center" valign="middle" >2.8806</td><td align="center" valign="middle" >6.3862</td></tr><tr><td align="center" valign="middle" >mer-trans</td><td align="center" valign="middle" >−7.7153</td><td align="center" valign="middle" >−2.2888</td><td align="center" valign="middle" >5.4265</td><td align="center" valign="middle" >2.7133</td><td align="center" valign="middle" >12.5112</td></tr></tbody></table></table-wrap><p>According to the Koopman theorem, the chemical hardness η can be described by the following equation, η = E L u m o − E H o m o 2 [<xref ref-type="bibr" rid="scirp.82201-ref32">32</xref>] .</p></sec><sec id="s3_5"><title>3.5. Nuclear Magnetic Resonance Simulation (nmr)</title><p><xref ref-type="table" rid="table6">Table 6</xref> is presented the magnetic resonance of <sup>13</sup>C and <sup>1</sup>H in comparison with experimental data.</p><p>The NMR theoretical data indicate overestimated values. These overestimated values can be explained by the method and the basis set, resulting in poor results [<xref ref-type="bibr" rid="scirp.82201-ref33">33</xref>] . Another explanation for such high values is that the simulation was performed on a single molecule, meaning that various types of chemical interactions were not considered theoretically [<xref ref-type="bibr" rid="scirp.82201-ref25">25</xref>] .</p><p>The NMR data for the mer-cis isomer provided a close approximation to the experimental data of the group (COO<sup>−</sup>), but the other NMR results were poorly related to the other two structures. Therefore, a correction of the basis sets and/or the method may provide better results in general.</p></sec></sec><sec id="s4"><title>4. Conclusions</title><p>Although some experimental data showed overestimated values, the spectral characteristics were maintained according to the experimental data.</p><table-wrap id="table6" ><label><xref ref-type="table" rid="table6">Table 6</xref></label><caption><title> Magnetic resonance <sup>13</sup>C and <sup>1</sup>H</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameters</th><th align="center" valign="middle" >fac-cis</th><th align="center" valign="middle" >mer-cis</th><th align="center" valign="middle" >mer-trans</th><th align="center" valign="middle" >Experimental</th></tr></thead><tr><td align="center" valign="middle" >C ( COO ) −</td><td align="center" valign="middle" >192.15</td><td align="center" valign="middle" >188.93</td><td align="center" valign="middle" >193.77</td><td align="center" valign="middle" >172.61</td></tr><tr><td align="center" valign="middle" >C ( CH 2 )</td><td align="center" valign="middle" >43.93</td><td align="center" valign="middle" >47.06</td><td align="center" valign="middle" >44.69</td><td align="center" valign="middle" >41.69</td></tr><tr><td align="center" valign="middle" >H ( CH 2 )</td><td align="center" valign="middle" >1.85 2.39</td><td align="center" valign="middle" >3.87 5.84</td><td align="center" valign="middle" >2.82 3.35</td><td align="center" valign="middle" >3.45 -</td></tr><tr><td align="center" valign="middle" >H ( NH 3 )</td><td align="center" valign="middle" >5.07 6.52</td><td align="center" valign="middle" >5.50 6.72</td><td align="center" valign="middle" >3.60 4.05</td><td align="center" valign="middle" >4.64 4.71</td></tr></tbody></table></table-wrap><p>The fac-cis-diaquotrischloroglycinatoruthenium III and mer-trans-diaquo- trischloroglycinatoruthenium III isomer presented data indicating greater stability compared to the other two isomers and was confirmed by optimizing data from the UV-vis simulation, the energy of the frontier orbitals and the chemical hardness, which supported its greater stability.</p><p>The fac-cis-diaquotrischloroglycinatoruthenium III and mer-trans-diaquo- trischloroglycinatoruthenium III isomer presented the lowest RMSE in comparison with the other structures. The difference between the RMSE of the mer-trans and fac-cis isomers was relatively small compared to the mer-cis isomer, which had the highest value. Thus, observing only the frequency values cannot differentiate between two isomers, but allowed us to discard the mer-cis isomer, which showed the worst results.</p><p>The observation of the theoretical spectrum suggests the mer-trans structure. The mer-trans structure showed higher reactivity compared to the other structures, which implies that this molecule can be modified easily as a function of applied energy compared to the other two structures.</p><p>Analyzing the results in general, the fac-cis-diaquotrischloroglycinatoruthe- nium III isomer presented results suggesting that this was the molecule synthesized by Chagas [<xref ref-type="bibr" rid="scirp.82201-ref8">8</xref>] .</p><p>The data relating to the properties of these three molecules may assist in future studies addressing structural modifications and interactions with the biological environment, since the molecule [RuCl<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>(Gly)] has been shown to possess antileishmanial activity.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work was supported by CAPES.</p></sec><sec id="s6"><title>Supporting Information</title><p>The orientation of the three structures is presented.</p></sec><sec id="s7"><title>Cite this paper</title><p>de Sousa, K.M.D., Chagas, M.A.S., dos Santos, J.M.F.D., Galv&#227;o, A.D., de Moraes, F.T., Ribeiro, A.T.B.N., Fortaleza, D.B., da Encarna&#231;&#227;o Amorim, K.A. and dos Santos, W.B. (2018) Theoretical and Comparative Study of the Complex [RuCl<sub>3</sub>(H<sub>2</sub>O)<sub>2</sub>(Gly)] by Density Functional Theory. Open Journal of Inorganic Chemistry, 8, 43-53. https://doi.org/10.4236/ojic.2018.81004</p></sec></body><back><ref-list><title>References</title><ref id="scirp.82201-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Chong, E., Xue, W., Storr, T., Kennepohl, P. and Schafer, L.L. (2015) Pyridonate-Supported Titanium(III). Benzylamine as an Easy-To-Use Reductant. Organometallics, 34, 4941-4945. https://doi.org/10.1021/acs.organomet.5b00469</mixed-citation></ref><ref id="scirp.82201-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">El-Sonbati, A.Z., Diab, M.A., Shoair, A.F., El-Bindary, A.A. and Barakat, A.M. (2016) Potentiometric, Thermodynamics and Theoretical Calculations of Some Rhodanine Derivatives. Journal of Molecular Liquids, 216, 821-829. 
https://doi.org/10.1016/j.molliq.2016.01.084</mixed-citation></ref><ref id="scirp.82201-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Sheng, H.W., Luo, W.K., Alamgir, F.M., Bai, J.M. and Ma, E. (2006) Atomic Packing and Short-To-Medium-Range Order in Metallic Glasses. Nature, 439, 419-425.</mixed-citation></ref><ref id="scirp.82201-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Bertoli, A.C., Garcia, J.S., Trevisan, M.G., Ramalho, T.C. and Freitas, M.P. (2016) Interactions Fulvate-Metal (Zn2+, Cu2+ and Fe2+): Theoretical Investigation of Thermodynamic, Structural and Spectroscopic Properties. BioMetals, 29, 275-285.  
https://doi.org/10.1007/s10534-016-9914-8</mixed-citation></ref><ref id="scirp.82201-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Das, P., Sarmah, P.P., Borah, M. and Phukan, A.K. (2009) Low-Spin, Mononuclear, Fe(III) Complexes With P,N Donor Hemilabile Ligands: A Combined Experimental and Theoretical Study. Inorganica Chimica Acta, 362, 5001-5011. 
https://doi.org/10.1016/j.ica.2009.08.006</mixed-citation></ref><ref id="scirp.82201-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">de Oliveira, R.S., Boffo, E.F., Reis, F.C.C., Nikolaou, S., Andriani, K.F., Caramori, G.F. and Doro, F.G. (2016) A Ruthenium Polypyridyl Complex with the Antihypertensive Drug Valsartan: Synthesis, Theoretical Calculations and Interaction Studies with Human Serum Albumin. Polyhedron, 114, 232-241.  
https://doi.org/10.1016/j.poly.2015.12.029</mixed-citation></ref><ref id="scirp.82201-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Bhattacharjee, J., Das, S., Reddy, T.D.N., Nayek, H.P., Mallik, B.S. and Panda, T.K. (2016) Alkali Metal and Alkaline Earth Metal Complexes with the Bis(borane-diphenylphosphanyl)amido Ligand—Synthesis, Structures, and Catalysis for Ring-Opening Polymerization of ε-Caprolactone. Zeitschrift für anorganische und allgemeine Chemie, 642, 118-127. 
https://doi.org/10.1002/zaac.201500593</mixed-citation></ref><ref id="scirp.82201-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Chagas, M.A.S., Galv&amp;atilde;o, A.D., de Moraes, F.T., Ribeiro, A.T.B.N., de Siqueira, A.B., de Assis Salama, I.C.C., Arrais-Silva, W.W., de Sousa, K.M.D., de Sousa Pereira, C.C. and dos Santos, W.B. (2017) Synthesis, Characterization and Analysis of Leishmanicide Ability of the Compound [Ru(Cl)3(H2O)2(gly)]. Open Journal of Inorganic Chemistry, 7, 89-101. https://doi.org/10.4236/ojic.2017.74006</mixed-citation></ref><ref id="scirp.82201-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Salama, I.C.C.D.A. (2013) Análise Biológica Dos Compostos Rutênio, Lupeol E Boldina No Modelo Experimental Das Leishmanioses. Disserta&amp;atilde;o de Mestrado, Universidade Federal do Mato Grosso-Campus Universitário do Araguaia.</mixed-citation></ref><ref id="scirp.82201-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Martínez, A., Carreon, T., Iniguez, E., Anzellotti, A., Sánchez, A., Tyan, M., Sattler, A., Herrera, L., Maldonado, R.A. and Sánchez-Delgado, R.A. (2012) Searching for New Chemotherapies for Tropical Diseases: Ruthenium-Clotrimazole Complexes Display High in Vitro Activity against Leishmania Major and Trypanosoma Cruzi and Low Toxicity toward Normal Mammalian Cells. Journal of Medicinal Chemistry, 55, 3867-3877. https://doi.org/10.1021/jm300070h</mixed-citation></ref><ref id="scirp.82201-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Iniguez, E., Sánchez, A., Vasquez, M.A., Martínez, A., Olivas, J., Sattler, A., Sánchez-Delgado, R.A. and Maldonado, R.A. (2013) Metal-Drug Synergy: New Ruthenium(II) Complexes of Ketoconazole Are Highly Active against Leishmania Major and Trypanosoma Cruzi and Nontoxic to Human or Murine Normal Cells. Journal of Biological Inorganic Chemistry, 18, 779-790.  
https://doi.org/10.1007/s00775-013-1024-2</mixed-citation></ref><ref id="scirp.82201-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Barbosa, M.I.F., Corrêa, R.S., de Oliveira, K.M., Rodrigues, C., Ellena, J., Nascimento, O.R., Rocha, V.P.C., Nonato, F.R., Macedo, T.S., Barbosa-Filho, J.M., Soares, M.B.P. and Batista, A.A. (2014) Antiparasitic Activities of Novel Ruthenium/Lapachol Complexes. Journal of Inorganic Biochemistry, 136, 33-39.  
https://doi.org/10.1016/j.jinorgbio.2014.03.009</mixed-citation></ref><ref id="scirp.82201-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Koenig, P.M., Roth, R. and Dietrich, S. (2008) Lock and Key Model System. EPL, 84, 68006/68001-68006/68005. https://doi.org/10.1209/0295-5075/84/68006</mixed-citation></ref><ref id="scirp.82201-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Adhireksan, Z., Davey, G.E., Campomanes, P., Groessl, M., Clavel, C.M., Yu, H., Nazarov, A.A., Yeo, C.H.F., Ang, W.H., Dr&amp;ouml;ge, P., Rothlisberger, U., Dyson, P.J. and Davey, C.A. (2014) Ligand Substitutions between Ruthenium-Cymene Compounds Can Control Protein versus DNA Targeting and Anticancer Activity. Nature Communications, 5, Article No. 3462. https://doi.org/10.1038/ncomms4462</mixed-citation></ref><ref id="scirp.82201-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Credendino, R., Poater, A., Ragone, F. and Cavallo, L. (2011) A Computational Perspective of Olefins Metathesis Catalyzed by N-Heterocyclic Carbene Ruthenium (Pre)Catalysts. Catalysis Science &amp; Technology, 1, 1287-1297.  
https://doi.org/10.1039/c1cy00052g</mixed-citation></ref><ref id="scirp.82201-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Wu, M., Gill, A.M., Yunpeng, L., Falivene, L., Yongxin, L., Ganguly, R., Cavallo, L. and Garcia, F. (2015) Synthesis, Structural Studies and Ligand Influence on the Stability of Aryl-NHC Stabilised Trimethylaluminium Complexes. Dalton Transactions, 44, 15166-15174. https://doi.org/10.1039/C5DT00079C</mixed-citation></ref><ref id="scirp.82201-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Gianferrara, T., Bratsos, I. and Alessio, E. (2009) A Categorization of Metal Anticancer Compounds Based on Their Mode of Action. Dalton Transactions, No. 37, 7588-7598. https://doi.org/10.1039/b905798f</mixed-citation></ref><ref id="scirp.82201-ref18"><label>18</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 Jr., J.A., Peralta, J.E., Ogliaro, F., Bearpark, M.J., Heyd, J., Brothers, E.N., Kudin, K.N., Staroverov, V.N., Kobayashi, R., Normand, J., Raghavachari, K., Rendell, A.P., Burant, J.C., Iyengar, S.S., Tomasi, J., Cossi, M., Rega, N., Millam, N.J., 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, &amp;Ouml;., Foresman, J.B., Ortiz, J.V., Cioslowski, J. and Fox, D.J. (2009) Gaussian 09. Gaussian, Inc. Print., Wallingford.</mixed-citation></ref><ref id="scirp.82201-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Zhao, Y. and Truhlar, D.G. (2008) The M06 Suite of Density Functionals for Main Group Thermochemistry, Thermochemical Kinetics, Noncovalent Interactions, Excited States, and Transition Elements: Two New Functionals and Systematic Testing of Four M06-Class Functionals and 12 Other Functionals. Theoretical Chemistry Accounts, 120, 215-241. https://doi.org/10.1007/s00214-007-0310-x</mixed-citation></ref><ref id="scirp.82201-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Frisch, M.J., Pople, J.A. and Binkley, J.S. (1984) Self-Consistent Molecular Orbital Methods 25. Supplementary Functions for Gaussian Basis Sets. The Journal of Chemical Physics, 80, 3265-3269. https://doi.org/10.1063/1.447079</mixed-citation></ref><ref id="scirp.82201-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Andrae, D., H&amp;auml;uβermann, U., Dolg, M., Stoll, H. and Preuβ, H. (1990) Energy-Adjustedab Initio Pseudopotentials for the Second and Third Row Transition Elements. Theoretica Chimica Acta, 77, 123-141.  
https://doi.org/10.1007/BF01114537</mixed-citation></ref><ref id="scirp.82201-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Wolinski, K., Hinton, J.F. and Pulay, P. (1990) Efficient Implementation of the Gauge-Independent Atomic Orbital Method for NMR Chemical Shift Calculations. Journal of the American Chemical Society, 112, 8251-8260.  
https://doi.org/10.1021/ja00179a005</mixed-citation></ref><ref id="scirp.82201-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Hashem, E., Platts, J.A., Hartl, F., Lorusso, G., Evangelisti, M., Schulzke, C. and Baker, R.J. (2014) Thiocyanate Complexes of Uranium in Multiple Oxidation States: A Combined Structural, Magnetic, Spectroscopic, Spectroelectrochemical, and Theoretical Study. Inorganic Chemistry, 53, 8624-8637.</mixed-citation></ref><ref id="scirp.82201-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Prabavathi, N., Nilufer, A., Krishnakumar, V. and Akilandeswari, L. (2012) Spectroscopic, Electronic Structure and Natural Bond Analysis of 2-aminopyrimidine and 4-aminopyrazolo[3,4-d]pyrimidine: A Comparative Study. Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy, 96, 226-241.  
https://doi.org/10.1016/j.saa.2012.05.015</mixed-citation></ref><ref id="scirp.82201-ref25"><label>25</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Kowalczyk</surname><given-names> I. </given-names></name>,<etal>et al</etal>. (<year>2014</year>)<article-title>Synthesis and Characterization of Alkylammonium Zwitterionic Amino Acids Derivatives by FTIR, NMR Spectroscopy and DFT Calculations</article-title><source> Acta Chimica Slovenica</source><volume> 61</volume>,<fpage> 39</fpage>-<lpage>50</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.82201-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Alam, M.M., Islam, S.M.S., Rahman, S.M.M. and Rahman, M.M. (2010) Simultaneous Preparation of Facial and Meridional Isomer of Cobalt-Amino Acid Complexes and Their Characterization. Journal of Scientific Research, 2, 91-98.</mixed-citation></ref><ref id="scirp.82201-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Sert, Y., Ucun, F., El-Hiti, G.A., Smith, K. and Hegazy, A.S. (2016) Spectroscopic Investigations and DFT Calculations on 3-(Diacetylamino)-2-ethyl-3H quinazolin-4-one. Journal of Spectroscopy, 2016, Article ID: 5396439.  
https://doi.org/10.1155/2016/5396439</mixed-citation></ref><ref id="scirp.82201-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">Chaitanya, K. (2012) Molecular Structure, Vibrational Spectroscopic (FT-IR, FT-Raman), UV-Vis Spectra, First Order Hyperpolarizability, NBO Analysis, HOMO and LUMO Analysis, Thermodynamic Properties of Benzophenone 2,4-Dicarboxylic Acid by Ab Initio HF and Density Functional Method. Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy, 86, 159-173.  
https://doi.org/10.1016/j.saa.2011.09.069</mixed-citation></ref><ref id="scirp.82201-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Pearson, R.G. (2005) Chemical Hardness and Density Functional Theory. Journal of Chemical Sciences, 117, 369-377. https://doi.org/10.1007/BF02708340</mixed-citation></ref><ref id="scirp.82201-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Pramanik, H.A.R., Das, D., Paul, P.C., Mondal, P. and Bhattacharjee, C.R. (2014) Newer Mixed Ligand Schiff Base Complexes from Aquo-N-(2’-Hydroxy Acetophenone) Glycinatocopper(II) as Synthon: DFT, Antimicrobial Activity and Molecular Docking Study. Journal of Molecular Structure, 1059, 309-319.  
https://doi.org/10.1016/j.molstruc.2013.12.009</mixed-citation></ref><ref id="scirp.82201-ref31"><label>31</label><mixed-citation publication-type="other" xlink:type="simple">Das, D., Dutta, A. and Mondal, P. (2015) Interaction of Aquated form of Ruthenium(III) Anticancer Complexes with Normal and Mismatch Base Pairs: A Density Functional Theoretical Study. Computational and Theoretical Chemistry, 1072, 28-36. https://doi.org/10.1016/j.comptc.2015.08.020</mixed-citation></ref><ref id="scirp.82201-ref32"><label>32</label><mixed-citation publication-type="other" xlink:type="simple">Shankar, R., Senthilkumar, K. and Kolandaivel, P. (2009) Calculation of Ionization Potential and Chemical Hardness: A Comparative Study of Different Methods. International Journal of Quantum Chemistry, 109, 764-771.  
https://doi.org/10.1002/qua.21883</mixed-citation></ref><ref id="scirp.82201-ref33"><label>33</label><mixed-citation publication-type="other" xlink:type="simple">Gontrani, L., Mennucci, B. and Tomasi, J. (2000) Glycine and Alanine: A Theoretical Study of Solvent Effects upon Energetics and Molecular Response Properties. Journal of Molecular Structure: Theochem, 500, 113-127.  
https://doi.org/10.1016/S0166-1280(00)00390-0</mixed-citation></ref></ref-list></back></article>