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    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">OJC</journal-id>
      <journal-title-group>
        <journal-title>Online Journal of Chemistry</journal-title>
      </journal-title-group>
      <issn pub-type="epub"></issn>
      <issn pub-type="ppub"></issn>
      <publisher>
        <publisher-name>Trend Research Publishing</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.31586/ojc.2021.010104</article-id>
      <article-id pub-id-type="publisher-id">OJC-84</article-id>
      <article-categories>
        <subj-group subj-group-type="heading">
          <subject>Research Article</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>
          Syntheses of Novel Coordination Polymers Using Bis-Imidazole Ligand Having Steric Hindrance and Methoxy Group
        </article-title>
      </title-group>
      <contrib-group>
<contrib contrib-type="author">
<name>
<surname>Fauzi</surname>
<given-names>Billy Oktora Abdilah</given-names>
</name>
<xref rid="af1" ref-type="aff">1</xref>
<xref rid="cr1" ref-type="corresp">*</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Kondo</surname>
<given-names>Mitsuru</given-names>
</name>
<xref rid="af1" ref-type="aff">1</xref>
<xref rid="af2" ref-type="aff">2</xref>
</contrib>
      </contrib-group>
<aff id="af1"><label>1</label> Department of Chemistry, Graduate School of Integrated Science and Technology, Shizuoka University, Shizuoka, Japan</aff>
<aff id="af2"><label>2</label> Green Bio Research Division, Research Institute of Green Science Technology, Shizuoka University, Shizuoka</aff>
<aff id="af3"><label>3</label></aff>
<aff id="af4"><label>4</label>*Correspondence: billy.oktora.a.fauzi.18@shizuoka.ac.jp</aff>
<author-notes>
<corresp id="c1">
<label>*</label>Corresponding author at: Department of Chemistry, Graduate School of Integrated Science and Technology, Shizuoka University, Shizuoka, Japan
</corresp>
</author-notes>
      <pub-date pub-type="epub">
        <day>14</day>
        <month>08</month>
        <year>2021</year>
      </pub-date>
      <volume>1</volume>
      <issue>1</issue>
      <history>
        <date date-type="received">
          <day>14</day>
          <month>08</month>
          <year>2021</year>
        </date>
        <date date-type="rev-recd">
          <day>14</day>
          <month>08</month>
          <year>2021</year>
        </date>
        <date date-type="accepted">
          <day>14</day>
          <month>08</month>
          <year>2021</year>
        </date>
        <date date-type="pub">
          <day>14</day>
          <month>08</month>
          <year>2021</year>
        </date>
      </history>
      <permissions>
        <copyright-statement>&#xa9; Copyright 2021 by authors and Trend Research Publishing Inc. </copyright-statement>
        <copyright-year>2021</copyright-year>
        <license license-type="open-access" xlink:href="http://creativecommons.org/licenses/by/4.0/">
          <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>
        Three novel coordination polymers {[Cu&lt;SUB>2&lt;/SUB>(bitbu-OMe)&lt;SUB>4&lt;/SUB>(SO&lt;SUB>4&lt;/SUB>)&lt;SUB>2&lt;/SUB>]&#x000b7;6MeOH}&lt;SUB>n&lt;/SUB> (<bold>1</bold>), {[Co&lt;SUB>2&lt;/SUB>(bitbu-OMe)&lt;SUB>4&lt;/SUB>(NCS)&lt;SUB>4&lt;/SUB>]&lt;SUB>0.5&lt;/SUB>&#x000b7;2DMF}&lt;SUB>n&lt;/SUB> (<bold>2</bold>), {[Co(bitbu-OMe)&lt;SUB>2&lt;/SUB>(NCS)&lt;SUB>2&lt;/SUB>]&#x000b7;2MeOH}&lt;SUB>n&lt;/SUB> (<bold>3</bold>) (bitbu-OMe = 1,1&#x02019;-[(5-tert-butyl-2-methoxybenzene-1,3-diyl)dimethanediyl]bis(<italic>1H</italic>-imidazole)) are synthesized through a slow evaporation method using solvothermal technique of CuSO&lt;SUB>4&lt;/SUB>&#x000b7;5H&lt;SUB>2&lt;/SUB>O or Co(SCN)&lt;SUB>2 &lt;/SUB>with bitbu-OMe. X-ray diffraction analysis results reveal that <bold>1</bold>, <bold>2</bold>, and <bold>3</bold> have similar two-dimensional layer networks. The study of the effect of the methoxy group in bitbu-OMe towards the stability of ligand conformation in obtained coordination polymers becomes necessary to be conducted in the future to unveil the reason for conformation similarity of ligand in coordination polymers.
      </abstract>
      <kwd-group>
        <kwd-group><kwd>Coordination Polymer; Bis-Imidazole; Methoxy Group</kwd>
</kwd-group>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
<title>Introduction</title><p>In recent work, our laboratory has succeeded in developing a two-dimensional coordination polymer prepared from a bis-imidazole ligand called bitb and CuSO<sub>4</sub>.5H<sub>2</sub>O. This two-dimensional coordination polymer has the ability to encapsulate perchlorate ions in aqueous solutions by converting their two-dimensional layer network into coordination capsules [
<xref ref-type="bibr" rid="R1">1</xref>,<xref ref-type="bibr" rid="R2">2</xref>]. The development of coordination polymers continued with the development of a chain-like one-dimensional coordination polymer prepared from a bis-benzimidazole ligand having three methoxy groups called bbitrmob and CuSO<sub>4</sub>.5H<sub>2</sub>O. This one-dimensional coordination polymer has a stable structure as a result of the C-H&#x26;#x000b7;&#x26;#x000b7;&#x26;#x000b7;O interaction provided by the methoxy group. Single-crystal X-ray diffraction revealed that the chain-like one-dimensional coordination polymer encapsulates a crystalline water molecule within each void [
<xref ref-type="bibr" rid="R3">3</xref>]. Herein, we report three two-dimensional coordination polymers constructed from a bis-imidazole ligand having a tert-butyl and a methoxy group called bitbu-OMe and reveal their structure characterization.</p>
</sec><sec id="sec2">
<title>Materials and Methods</title><p>All reagents and solvents are available commercially and used without further purification. In the part of the syntheses of new multinuclear metal complexes, the slow evaporation method [
<xref ref-type="bibr" rid="R4">4</xref>] with solvothermal technique [
<xref ref-type="bibr" rid="R5">5</xref>] is used to grow a single crystal of metal complexes. Single crystal X-ray structure measurement is conducted using Rigaku VariMax with a Saturn diffractometer. Powder X-ray diffraction (PXRD) measurement is conducted using the Rigaku Smart Lab. Nuclear magnetic resonance (NMR) measurement is conducted using JEOL ECA-600 Spectrometer. Elemental analysis (EA) measurement is conducted using Euro Vector EA3000. Fourier transform infrared (FTIR) spectrum is recorded using PerkinElmer FT-IR Spectrometer Frontier. Ultraviolet/Visible (UV/Vis) reflection spectrum is recorded using JASCO V-570 UV/Vis/NIR Spectrometer.</p>
</sec><sec id="sec3">
<title>Results and Discussion</title><title>3.1. Syntheses of bitbu-OMe</title><p><bold>The bitbu-OMe </bold>was first introduced by Qin et al [
<xref ref-type="bibr" rid="R6">6</xref>]. Here we report the different way to synthesize<bold> bitbu-OMe</bold> using different reagents. Imidazole (2.72 g, 40 mmol), NaOH (3.20 g, 80 mmol), and THF (100 ml) are added into round bottom flask. The mixture is stirred at room temperature until the mixture became suspension (&#x26;#x000b1; 1 hour). 1,3-bis(bromomethyl)-5-<italic>tert</italic>-butyl-2-methoxybenzene (7.00 g, 20 mmol) in THF (100 mL) is added into the suspension by drop wish. The solution is stirred at room temperature for 3 hours. The orange solution and precipitate are separated by filtration. The precipitate is ished with THF (50 mL x 1). The obtained orange solution is evaporated <italic>in vacuo</italic>. The crude product is dissolved in CH<sub>2</sub>Cl<sub>2</sub> (40 mL). The organic solution is ished with water (100 mL <math><semantics><mrow><mo>×</mo></mrow></semantics></math> 3) and dried over MgSO<sub>4</sub> and filtered. The solution is evaporated <italic>in vacuo</italic>. The crude product is purified with column chromatography with eluent CH<sub>2</sub>Cl<sub>2</sub>/Me<sub>2</sub>CO 4:1. The obtained product is evaporated <italic>in vacuo</italic>. The solid product is recrystallized from Me<sub>2</sub>CO/H<sub>2</sub>O. The broken white crystals are obtained.</p>
<p>Yield: 4.63 g (71.50%). <sup>1</sup>H NMR (600 MHz, DMSO-d<sup>6</sup>): &#x26;#x003b4; = 7.70 (s, 2H), 7.14 (s, 2H), 7.01 (s, 2H), 6.89 (s, 2H), 5.20 (s, 4H), 3.67 (s, 3H), 1.13 (s, 9H). Elemental analysis (EA) Calcd. For C<sub>19</sub>H<sub>24</sub>N<sub>4</sub>O (324.42): C, 70.34; H, 7.46; N, 17.27. Found: C, 70.55; H, 7.34; N, 16.95.</p>
<p><bold>Scheme 1</bold><bold>.</bold> Scheme of syntheses of bitbu-OMe</p>
<title>3.2. Syntheses of Novel Coordination Polymers</title><title>3.2.1. Synthesis of</title><p>Single crystals of <bold>1</bold> are prepared by reacting bitbu-OMe and CuSO<sub>4</sub>&#x26;#x000b7;5H<sub>2</sub>O. The bitbu-OMe (0.0648 g, 0.200 mmol) is diluted in 20 mL MeOH, CuSO<sub>4</sub>&#x26;#x000b7;5H<sub>2</sub>O (0.0250 g, 0.100 mmol) is diluted in 20 mL MeOH. 2 mL of each solution is taken, and these solutions taken are mixed in straight tube slowly for 1 day. Later, purple block crystals are obtained.</p>
<p>The powder of <bold>1 </bold>is prepared by reacting bitbu-OMe (0.0648 g, 0.200 mmol) diluted in 20 mL MeOH and CuSO<sub>4</sub>&#x26;#x000b7;5H<sub>2</sub>O (0.0250 g, 0.100 mmol) diluted in 20 mL MeOH. These solutions are mixed and stirred in 100 mL round bottom flask for 1 day. Later, purple powder is obtained with yield of 0.0695 g (~76.83 %).</p>
<title>3.2.2. Synthesis of</title><p>Single crystals of <bold>2</bold> are prepared by reacting bitbu-OMe and Co(SCN)<sub>2</sub>. The bitbu-OMe (0.0648 g, 0.200 mmol) is diluted in 20 mL DMF, Co(SCN)<sub>2</sub> (0.0175 g, 0.100 mmol) is diluted in 20 mL MeOH. 2 mL of each solution is taken, and these solutions taken are mixed in straight tube slowly for 1 week. Later, pink crystals are obtained.</p>
<p>The powder of <bold>2 </bold>is prepared by reacting bitbu-OMe (0.0648 g, 0.200 mmol) diluted in 20 mL DMF and Co(SCN)<sub>2</sub> (0.0175 g, 0.100 mmol) diluted in 20 mL MeOH. These solutions are mixed and stirred in 100 mL round bottom flask for 1 week. Later, light pink powder is obtained with yield of 0.0843 g (~86.91 %).</p>
<title>3.2.3. Synthesis of</title><p>Single crystals of <bold>3 </bold>are prepared by reacting bitbu-OMe and Co(SCN)<sub>2</sub>. The bitbu-OMe (0.0259 g, 0.080 mmol) is diluted in 20 mL MeOH, and Co(SCN)<sub>2</sub> (0.014 g, 0.080 mmol) is diluted in 20 mL MeOH. 2 mL of each solution is taken, and these solutions taken are mixed in straight tube slowly for 1 week. Later, pink crystals are obtained.</p>
<p>The powder of <bold>3 </bold>is prepared by reacting bitbu-OMe (0.0648 g, 0.200 mmol) diluted in 50 mL MeOH with Co(SCN)<sub>2</sub> (0.035 g, 0.200 mmol) diluted in 50 mL MeOH. These solutions are mixed and stirred in 200 mL round bottom flask for 1 day. Later, light gray powder is obtained with yield of 0.0893 g (~50.73 %).</p>
<title>3.3. Structure Characterizations of Novel Multinuclear Metal Complexes</title><p>Single crystal data integration and reduction are conducted using VESTA software [
<xref ref-type="bibr" rid="R7">7</xref>].</p>
<title>3.3.1. Structure Characterization of 1</title><p>The single-crystal X-ray diffraction analysis result reveals that <bold>1 </bold>consists of a two-dimensional layer coordination polymer crystallized in the monoclinic system with the space group <italic>P</italic>2<sub><italic>1</italic></sub>. Cu(II) ion (Cu1) has a square pyramidal environment with one oxygen atom (O3) from SO<sub>4</sub><sup>2- </sup>ligand attached to the axial side of Cu1. <bold>1</bold> becomes neutralized as the result of the coordination bonds between Cu(II) and SO<sub>4</sub><sup>2-</sup> ligand. Thus, four nitrogen atoms from four different bitbu-OMe (N1, N4, N5, and N8) are attached to the equatorial side of Cu1. Cu1-N1, Cu1-N4, Cu1-N5, Cu1-N8, and Cu1-O3 distances are approximately 1.997 &#x26;#x000c5;, 2.018 &#x26;#x000c5;, 2.010 &#x26;#x000c5;, 2.017 &#x26;#x000c5;, and 2.212 &#x26;#x000c5; respectively.</p>
<fig id="fig1">
<label>Figure 1</label>
<caption>
<p>The coordination environment of <b>1</b> around the Cu(II) center represented by thermal ellipsoids of 40% probability. Hydrogen atoms and solvent molecules are omitted for clarity. Color code: blue, copper; cyan, nitrogen; black, carbon; red, oxygen; yellow, sulfur.</p>
</caption>
<graphic xlink:href="84.fig.001" />
</fig><table-wrap id="tab1">
<label>Table 1</label>
<caption>
<p><b></b> Selected angle [degree] of <b>1</b>.</p>
</caption>

<table>
<thead>
<tr>
<th align="left" colspan="3">Angle</th>
<th align="left">Degree (<sup>o</sup>)</th>
<th align="center"></th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">N1</td>
<td align="left">Cu1</td>
<td align="left">O3</td>
<td align="left">96.0 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Cu1</td>
<td align="left">N4</td>
<td align="left">88.9 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Cu1</td>
<td align="left">N8</td>
<td align="left">168.5 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Cu1</td>
<td align="left">N5</td>
<td align="left">90.1 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N4</td>
<td align="left">Cu1</td>
<td align="left">O3</td>
<td align="left">97.6 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N8</td>
<td align="left">Cu1</td>
<td align="left">O3</td>
<td align="left">95.4 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N8</td>
<td align="left">Cu1</td>
<td align="left">N4</td>
<td align="left">90.8 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Cu1</td>
<td align="left">O3</td>
<td align="left">91.4 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Cu1</td>
<td align="left">N4</td>
<td align="left">171.0 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Cu1</td>
<td align="left">N8</td>
<td align="left">88.4 (2)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left" colspan="4">
<hr />
</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>

</fn>
</table-wrap-foot>
</table-wrap><p>The single-crystal X-ray diffraction analysis result also reveals that <bold>1</bold> has rhombic grid style [
<xref ref-type="bibr" rid="R8">8</xref>]. Interestingly, each SO<sub>4</sub><sup>2-</sup> ligand results hydrogen bonding with one crystalline methanol molecule that has hydrogen bonding with another crystalline methanol molecule.</p>
<fig id="fig2">
<label>Figure 2</label>
<caption>
<p>Infinite structures of <b>1</b> viewed along an axis showing hydrogen bonding between SO<sub>4</sub><sup>2-</sup> ligand and crystalline methanol molecules.</p>
</caption>
<graphic xlink:href="84.fig.002" />
</fig><title>3.3.2. Structure Characterization of 2</title><p>The single-crystal X-ray diffraction analysis result reveals that <bold>2 </bold>consists of a two-dimensional layer coordination polymer with rhombic grid style [
<xref ref-type="bibr" rid="R8">8</xref>] crystallized in the monoclinic system with the space group <italic>P</italic>2<sub><italic>1</italic></sub><italic>/</italic>c. Co(II) ion (Co1) has a octahedral environment with two nitrogen atoms from two SCN<sup>- </sup>ligands (N5 and N5*) attached to the axial side of Co1. <bold>2</bold> becomes neutralized as the result of the coordination bonds between Co(II) and two SCN<sup>-</sup> ligands. Thus, four nitrogen atoms from four different bitbu-OMe (N1, N1*, N4, and N4*) are attached to the equatorial side of Co1. Co1-N1 and Co1-N1* have the same distance, which is approximately 2.133 &#x26;#x000c5;. Co1-N4 and Co1-N4* have the same distance, which is approximately 2.183 &#x26;#x000c5;. Co1-N5 and Co1-N5* have the same distance, which is approximately 2.094 &#x26;#x000c5;.</p>
<fig id="fig3">
<label>Figure 3</label>
<caption>
<p>(<b>a</b>)<b> </b>The coordination environment of <b>2</b> around the Co(II) center represented by thermal ellipsoids of 40% probability. Hydrogen atoms and solvent molecules are omitted for clarity. (<b>b</b>) Infinite structures of <b>2</b> viewed along an axis. Color code: magenta, cobalt; cyan, nitrogen; black, carbon; yellow, sulfur.</p>
</caption>
<graphic xlink:href="84.fig.003" />
</fig><table-wrap id="tab2">
<label>Table 2</label>
<caption>
<p><b></b> Selected angle [degree] of <b>2</b>.</p>
</caption>

<table>
<thead>
<tr>
<th align="left" colspan="3">Angle</th>
<th align="left">Degree (<sup>o</sup>)</th>
<th align="center"></th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">N4</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">180.0</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">89.78  (10)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">90.22  (10)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1*</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">89.78 (10)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1*</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">90.22  (10)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Co1</td>
<td align="left">N1*</td>
<td align="left">180.0</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">89.29  (11)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">90.71  (11)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">90.71  (11)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">89.29  (11)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N1</td>
<td align="left">90.79  (12)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N1*</td>
<td align="left">90.79  (12)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N1</td>
<td align="left">89.21  (12)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N1*</td>
<td align="left">89.21  (12)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N5*</td>
<td align="left">180.0</td>
<td align="center"></td>
</tr>
<tr>
<td align="left" colspan="4">
<hr />
</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>

</fn>
</table-wrap-foot>
</table-wrap><title>3.3.3. Structure Characterization of 3</title><p>The single-crystal X-ray diffraction analysis result reveals that <bold>3 </bold>consists of a two-dimensional layer coordination polymer with rhombic grid style [
<xref ref-type="bibr" rid="R8">8</xref>] crystallized in the monoclinic system with the space group <italic>P</italic>2<sub><italic>1</italic></sub><italic>/</italic>c. Co(II) ion (Co1) has a octahedral environment with two nitrogen atoms from two SCN<sup>- </sup>ligands (N5 and N5*) attached to the axial side of Co1. <bold>3</bold> becomes neutralized as the result of the coordination bonds between Co(II) and two SCN<sup>-</sup> ligands. Thus, four nitrogen atoms from four different bitbu-OMe (N1, N1*, N4, and N4*) are attached to the equatorial side of Co1. Co1-N1 and Co1-N1* have the same distance, which is approximately 2.1378 &#x26;#x000c5;. Co1-N4 and Co1-N4* have the same distance, which is approximately 2.1461 &#x26;#x000c5;. Co1-N5 and Co1-N5* have the same distance, which is approximately 2.1344 &#x26;#x000c5;.</p>
<fig id="fig4">
<label>Figure 4</label>
<caption>
<p>The coordination environment of <b>3</b> around the Co(II) center represented by thermal ellipsoids of 40% probability. Hydrogen atoms and solvent molecules are omitted for clarity. Color code: magenta, cobalt; cyan, nitrogen; black, carbon; yellow, sulfur.</p>
</caption>
<graphic xlink:href="84.fig.004" />
</fig><table-wrap id="tab3">
<label>Table 3</label>
<caption>
<p><b></b> Selected angle [degree] of <b>3</b>.</p>
</caption>

<table>
<thead>
<tr>
<th align="left" colspan="3">Angle</th>
<th align="left">Degree (<sup>o</sup>)</th>
<th align="center"></th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">N1</td>
<td align="left">Co1</td>
<td align="left">N1</td>
<td align="left">180.0</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">90.38  (6)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">90.38  (6)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1*</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">89.62 (6)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N1*</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">89.62 (6)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N4</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">180.0</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N1</td>
<td align="left">89.98  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N1*</td>
<td align="left">90.02  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N1</td>
<td align="left">90.02  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N1*</td>
<td align="left">89.98  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">89.18  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">89.18  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N4</td>
<td align="left">90.82  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5*</td>
<td align="left">Co1</td>
<td align="left">N4*</td>
<td align="left">90.82  (7)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">N5</td>
<td align="left">Co1</td>
<td align="left">N5*</td>
<td align="left">180.0</td>
<td align="center"></td>
</tr>
<tr>
<td align="left" colspan="4">
<hr />
</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn>

</fn>
</table-wrap-foot>
</table-wrap><p>The single-crystal X-ray diffraction analysis result reveals that <bold>3</bold> has voids where each void has an area of approximately 5.37 &#x26;#x000c5; &#x26;#x000d7; 4.424 &#x26;#x000c5;. The length of void is the distance between C1 and C1* minus the van der Waals diameter of carbon atom, and the width of void is the distance between N3 and N3* minus the van der Waals diameter of nitrogen atom (Figure 5) by considering the van der Waals modeling with a 100% radius relativity.</p>
<fig id="fig5">
<label>Figure 5</label>
<caption>
<p>Calculation of the area of void formed in <b>3</b>. Two methanol molecules in void are omitted for clarity. Color code: magenta, cobalt; cyan, nitrogen; black, carbon; yellow, sulfur.</p>
</caption>
<graphic xlink:href="84.fig.005" />
</fig><p>Interestingly, every void formed in <bold>3</bold> encapsulates two methanol molecules (Figure 6). The investigation of its ability to encapsulate other small organic molecules in terms of water purification becomes necessary to be conducted in the future.</p>
<fig id="fig6">
<label>Figure 6</label>
<caption>
<p><b>Figure 6</b>. Infinite structures of <b>3</b> viewed along an axis showing two methanol molecules encapsulated within each void.</p>
</caption>
<graphic xlink:href="84.fig.006" />
</fig><table-wrap id="tab4">
<label>Table 4</label>
<caption>
<p><b></b> Summary of crystallographic data and structure refinement parameters for <b>1</b>-<b>3</b>.</p>
</caption>

<table>
<thead>
<tr>
<th align="left">&#x00026;nbsp;</th>
<th align="left">1</th>
<th align="left">2</th>
<th align="left">3</th>
<th align="center"></th>
</tr>
</thead>
<tbody>
<tr>
<td align="left">Empirical formula</td>
<td align="left">C<sub>82</sub>H<sub>120</sub>Cu<sub>2</sub>N<sub>16</sub>O<sub>18</sub>S<sub>2</sub></td>
<td align="left">C<sub>46</sub>H<sub>62</sub>CoN<sub>12</sub>O<sub>4</sub>S<sub>2</sub></td>
<td align="left">C<sub>42</sub>H<sub>56</sub>CoN<sub>10</sub>O<sub>4</sub>S<sub>2</sub></td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Formula weight</td>
<td align="left">1809.13</td>
<td align="left">970.12</td>
<td align="left">888.01</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Lattice</td>
<td align="left">'monoclinic'</td>
<td align="left">'monoclinic'</td>
<td align="left">'monoclinic'</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">a, &#x00026;#8491;</td>
<td align="left">9.9795(8)</td>
<td align="left">12.3654(5)</td>
<td align="left">9.9613(3)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">b, &#x00026;#8491;</td>
<td align="left">23.2115(13)</td>
<td align="left">9.3458(3)</td>
<td align="left">23.9517(5)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">c, &#x00026;#8491;</td>
<td align="left">10.0192(9)</td>
<td align="left">23.0053(9)</td>
<td align="left">10.2582(3)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">&#x003b1;, &#x000b0;</td>
<td align="left">90</td>
<td align="left">90</td>
<td align="left">90</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">&#x003b2;, &#x000b0;</td>
<td align="left">112.292(10)</td>
<td align="left">102.590(4)</td>
<td align="left">113.963(4)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">&#x003b3;, &#x000b0;</td>
<td align="left">90</td>
<td align="left">90</td>
<td align="left">90</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">V, &#x00026;#8491;<sup>3</sup></td>
<td align="left">2147.4(3)</td>
<td align="left">2594.67(17)</td>
<td align="left">2236.55(12)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Space group</td>
<td align="left">P2<sub>1</sub> (No. 4)</td>
<td align="left">P2<sub>1</sub>/c (No. 14)</td>
<td align="left">P2<sub>1</sub>/c (No. 14)</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Z</td>
<td align="left">1</td>
<td align="left">2</td>
<td align="left">2</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">&#x003c1;(calcd), g cm<sup>-3</sup></td>
<td align="left">1.399</td>
<td align="left">1.242</td>
<td align="left">1.319</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">&#x003bc;(MoK&#x003b1;),  mm<sup>-1</sup></td>
<td align="left">0.621</td>
<td align="left">0.463</td>
<td align="left">0.529</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Radiateon (&#x003bb;,&#x00026;#8491;)</td>
<td align="left">0.71073</td>
<td align="left">0.71073</td>
<td align="left">0.71073</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Temp, K</td>
<td align="left">173.15</td>
<td align="left">173.15</td>
<td align="left">173.15</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Reflns collected</td>
<td align="left">9762</td>
<td align="left">6941</td>
<td align="left">6126</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Unique reflns</td>
<td align="left">7758</td>
<td align="left">5573</td>
<td align="left">5340</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">Param refined</td>
<td align="left">555</td>
<td align="left">301</td>
<td align="left">273</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">R1 [I &#x00026;gt; 2&#x003c3;(I)]</td>
<td align="left">0.0613</td>
<td align="left">0.0870</td>
<td align="left">0.0556</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">wR2 [all data]</td>
<td align="left">0.1665</td>
<td align="left">0.2345</td>
<td align="left">0.1672</td>
<td align="center"></td>
</tr>
<tr>
<td align="left">GOF</td>
<td align="left">1.034</td>
<td align="left">1.081</td>
<td align="left">1.064</td>
<td align="center"></td>
</tr>
<tr>
<td align="left" colspan="4">
<hr />
</td>
</tr>
</tbody>
</table>
</table-wrap><p>Interestingly, the network of <bold>1</bold>, <bold>2</bold>, and <bold>3</bold> is quite similar, with a rhombic grid system as their network system. The investigation about what causes the network of these coordination polymers becoming similar requires further investigation.</p>
</sec><sec id="sec4">
<title>Conclusions</title><p>Based on the research result above, three novel coordination polymers have been constructed from bis-imidazole bridging ligand containing methoxy group and sterical hindrance group <italic>tert</italic>-butyl called bitbu-OMe. Three two-dimensional rhombic grid network coordination polymers have been constructed from bitbu-OMe, namely {[Cu<sub>2</sub>(bitbu-OMe)<sub>4</sub>(SO<sub>4</sub>)<sub>2</sub>]&#x26;#x000b7;6MeOH}<sub>n</sub>(<bold>1</bold>),{[Co<sub>2</sub>(bitbu-OMe)<sub>4</sub>(NCS)<sub>4</sub>]<sub>0.5</sub>&#x26;#x000b7;2DMF}<sub>n</sub>(<bold>2</bold>),{[Co(bitbu-OMe)<sub>2</sub>(NCS)<sub>2</sub>]&#x26;#x000b7;2MeOH}<sub>n </sub>(<bold>3</bold>). The network similarity of these coordination polymers becomes interesting to be investigated in the future to unveil the structure stability factor of them. The presence of two methanol molecules inside of each void formed in <bold>3</bold> becomes evidence that this coordination polymer has the potential to encapsulate small organic matters in aqueous solutions.</p>
<p><bold>Supplementary Materials:</bold> The following are available online at https://www.scipublications.com/Supplementary-Materials/84/s1.pdf,Figure <xref ref-type="fig" rid="figS1"> S1</xref>: (a) <sup>1</sup>H NMR spectra of bisimidazole <italic>tert</italic>-butyl methoxybenzene (bitbu-OMe) in DMSO-d<sup>6</sup>. (b) <sup>13</sup>C NMR spectra of bisimidazole <italic>tert</italic>-butyl methoxybenzene (bitbu-OMe) in DMSO-d<sup>6</sup>,Figure <xref ref-type="fig" rid="figS2"> S2</xref>: IR spectrum of bitbu-OMe,Figure <xref ref-type="fig" rid="figS3"> S3</xref>: IR Spectrum of <bold>1</bold>,Figure <xref ref-type="fig" rid="figS4"> S4</xref>: IR Spectrum of <bold>2</bold>,Figure <xref ref-type="fig" rid="figS5"> S5</xref>: IR Spectrum of <bold>3</bold>,Figure <xref ref-type="fig" rid="figS6"> S6</xref>: UV/Vis/NIR reflection spectrum of <bold>1</bold>,Figure <xref ref-type="fig" rid="figS7"> S7</xref>: UV/Vis/NIR reflection spectrum of <bold>2</bold>,Figure <xref ref-type="fig" rid="figS8"> S8</xref>: UV/Vis/NIR reflection spectrum of <bold>3</bold>,Figure <xref ref-type="fig" rid="figS9"> S9</xref>: (a) Observed PXRD patterns of bulk sample of <bold>1</bold>. (b) The simulated PXRD pattern of <bold>1</bold> based on the single crystal X-ray structures. The patterns are shown in the range from 5<sup>o</sup> to 60<sup>o</sup> for explicit comparison,Figure <xref ref-type="fig" rid="figS10"> S10</xref>: (a) Observed PXRD patterns of bulk sample of <bold>2</bold>. (b) The simulated PXRD pattern of <bold>2</bold> based on the single crystal X-ray structures. The patterns are shown in the range from 5<sup>o</sup> to 60<sup>o</sup> for explicit comparison,Figure <xref ref-type="fig" rid="figS11"> S11</xref>: (a) Observed PXRD patterns of bulk sample of <bold>3</bold>. (b) The simulated PXRD pattern of <bold>3</bold> based on the single crystal X-ray structures. The patterns are shown in the range from 5<sup>o</sup> to 60<sup>o</sup> for explicit comparison.</p>
<p><bold>Acknowledgments:</bold> The first author is thankful to Prof. Mitsuru Kondo from Shizuoka University for providing the opportunity to conduct the research and providing the laboratory facilities to conduct the measurement.</p>
<p><bold>Conflicts of Interest:</bold> The authors declare no conflict of interest.</p>
</sec>
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