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- <a name="top"></a><h1 class="suptitle">supplementary materials</h1><br /><div class="buttonlinks"><a href="./index.html" target="_parent"><img src="../../../../../graphics/htmlborder.gif" alt="HTML version" align="top" border="0" /></a><a href="./at2552.pdf" ><img src="../../../../../graphics/pdfborder.gif" alt="pdf version" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/sendcif?at2552sup1" ><img src="../../../../../graphics/cifborder.gif" alt="cif file" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/sendcif?at2552sup1&Qmime=cif" ><img src="../../../../../graphics/3dviewborder.gif" alt="3d view" align="top" border="0" /></a><a href="./at2552Isup2.hkl" ><img src="../../../../../graphics/structurefactorsborder.gif" alt="structure factors" align="top" border="0" /></a><a href="./at2552sup0.html" ><img src="../../../../../graphics/supplementarymaterialsborder.gif" alt="supplementary materials" align="top" border="0" /></a><a href="./at2552checkcif.html" ><img src="../../../../../graphics/checkcifborder.gif" alt="CIF check report" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/similar?wordList=diaquadimethanolbis%20or%20tetrazol%20or%20benzoato%20or%20zinc&from=at2552" ><img src="../../../../../graphics/similarpapersborder.gif" alt="similar papers" align="top" border="0" /></a> <a href="../../../../../../services/openaccess.html"><img src="../../../../../../logos/free.gif" alt="Open access" align="top" border="0" /></a></div><p class="scheme"><img src="./at2552contents.gif" alt="at2552 scheme" /></p><div class="bibline"><p><i>Acta Cryst.</i> (2008). E<b>64</b>, m624 [ <font size="2"><a title="Open URL link" href="http://dx.doi.org/10.1107/S1600536808008490">doi:10.1107/S1600536808008490</a></font> ]</p></div>
- <h3>Diaquadimethanolbis[4-(1<span class="it"><i>H</i></span>-tetrazol-1-yl)benzoato]zinc(II) dihydrate</h3><h3><a href="http://scripts.iucr.org/cgi-bin/citedin?search_on=name&author_name=Zhang,%20S.-M.">S.-M. Zhang</a></h3>
- <div class="abstract">
- <a name="abstract"></a>
- <div class="heading2">Abstract <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>In the title compound, [Zn(C<span class="inf"><sub>8</sub></span>H<span class="inf"><sub>5</sub></span>N<span class="inf"><sub>4</sub></span>O<span class="inf"><sub>2</sub></span>)<span class="inf"><sub>2</sub></span>(CH<span class="inf"><sub>3</sub></span>OH)<span class="inf"><sub>2</sub></span>(H<span class="inf"><sub>2</sub></span>O)<span class="inf"><sub>2</sub></span>]·2H<span class="inf"><sub>2</sub></span>O, the Zn<span class="sup"><sup>II</sup></span> ion lies on an inversion centre and is coordinated by two O atoms from two 4-(tetrazol-1-yl)benzoate ligands, two O atoms from two methanol molecules and two O atoms from two water molecules in a slightly distorted octahedral geometry. In addition, there are two uncoordinated water molecules in the crystal structure. The crystal structure is stabilized by intermolecular O-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />O hydrogen bonds.</p></div>
- <!-- endabstractdiv -->
- <div class="contentslist">
- <ul>
- <li class="comment"><a title="Comment" href="#comment">Comment</a></li>
- <li class="relatedliterature"><a title="Related literature" href="#relatedliterature">Related literature</a></li>
- <li class="experimental"><a title="Experimental" href="#experimental">Experimental</a></li>
- <li class="refinement"><a title="Refinement" href="#refinement">Refinement</a></li>
- <li class="computingdetails"><a title="Computing details" href="#computingdetails">Computing details</a></li>
- <li class="figures"><a title="Figures" href="#figures">Figures</a></li>
- <li><a title="(I)" href="#chemicalname1">Diaquadimethanolbis[4-(1H-tetrazol-1-yl)benzoato]zinc(II) dihydrate </a><ul>
- <li><a title="Crystal data" href="#crystaldata1">Crystal data</a></li>
- <li><a title="Data collection" href="#datacollection1">Data collection</a></li>
- <li><a title="Refinement data" href="#refinementdata1">Refinement data</a></li>
- <li class="specialdetails"><a title="Special details" href="#specialdetails1">Special details</a></li>
- <li class="licoords"><a title="Fractional atomic coordinates" href="#fractionalatomiccoordinates1">Fractional atomic coordinates</a></li>
- <li class="liadps"><a title="Atomic displacement parameters" href="#atomicdisplacement1">Atomic displacement parameters</a></li>
- <li class="ligeomlong"><a title="Geometric parameters" href="#geometricparameters1">Geometric parameters</a></li>
- <li class="lihbondslong"><a title="Hydrogen-bond geometry" href="#hydrogen-bondgeometry1">Hydrogen-bond geometry</a></li>
- <li class="ligeomshort"><a title="Geometric parameters" href="#geometricparameters1">Geometric parameters</a></li>
- <li class="lihbondsshort"><a title="Hydrogen-bond geometry" href="#hydrogen-bondgeometry1">Hydrogen-bond geometry</a></li>
- </ul></li>
- <li class="acknowledgements"><a title="Acknowledgements" href="#acknowledgements">Acknowledgements</a></li>
- <li class="publreferences"><a title="References" href="#publreferences">References</a></li>
- </ul>
- </div>
- <!-- endcontentslistdiv -->
- <div class="comment">
- <a name="comment"></a>
- <div class="heading2">
- Comment <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>Coordination architectures formed from 1<i>H</i>-tetrazol and its derivatives
- have attracted wide attentions in recent years, due to not only their
- fascinating structures and topologies, but also their potential applications
- in luminescence, magnetism and gas storage (Dinca, <i>et al.</i>, 2006;
- Li,
- <i>et al.</i>, 2007). However, there are rare reports (Zou, <i>et
- al.</i>,
- 2005) of the coordination systems using the benzoic acids with
- N-heterocycle
- as ligands. So we synthesized several coordination compounds by such ligands.
- And here we report the structure of title compound (I).</p><p>The structure of (I) consists of discrete neutral unit
- [Zn(C<sub>8</sub>H<sub>5</sub>N<sub>4</sub>O<sub>2</sub>)<sub>2</sub>(CH<sub>3</sub>OH)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>], and two lattice water
- molecules (Fig. 1), atom Zn1 lies on an inversion centre and is coordinated by
- two O atoms from two 4-(tetrazol-1-yl) benzoate ligands, two O atoms from two
- methanol molecules and two O atoms from two water molecules in a distorted
- octahedral geometry.The metal ion of (I) is bonded to the carboxyl group of
- 4-(tetrazol-1-yl) benzoate, which is remarkably different from our previous
- reported compound that using the same ligand with N donor coordinating to
- metal ion (Zhang <i>et al.</i>, 2007). The crystal stacking of (I)
- (Fig. 2) is
- stabilized by the intermolecular O—H···O hydrogen bonds (Table 2).</p>
- </div>
- <!-- endcommentdiv -->
- <div class="relatedliterature">
- <a name="relatedliterature"></a>
- <div class="heading2">
- Related literature <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>For related literature, see: Zou <i>et al.</i> (2005); Dinca <i>et
- al.</i>
- (2006); Li <i>et al.</i> (2007); Zhang & Du (2007).</p>
- </div>
- <!-- endrelatedliteraturediv -->
- <div class="experimental">
- <a name="experimental"></a>
- <div class="heading2">
- Experimental <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>A solution of Zn(NO<sub>3</sub>)<sub>2</sub>.6H<sub>2</sub>O (0.1 mmol) in water (5 ml) was added to a
- solution of 4-(tetrazol-1-yl) benzoic acid (38 mg, 0.2 mmol) and sodium
- hydroxide (8 mg, 0.2 mmol) in methanol (5 mL). The reaction mixture was
- stirred for 30 min and then filtered. Colourless crystals of (I) suitable for
- X-ray diffraction were obtained by slow evaporation after two weeks [yield:
- 46%].</p>
- </div>
- <!-- endexperimentaldiv -->
- <div class="refinement">
- <a name="refinement"></a>
- <div class="heading2">
- Refinement <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>H atoms of C were included in calculated positions and treated in the
- subsequent refinement as riding atoms, with C—H = 0.93 and 0.96 Å and
- <i>U</i><sub>iso</sub>(H) = 1.2 and 1.5 <i>U</i><sub>eq</sub>(C,<i>N</i>). The H atoms of water
- was located in Fourier difference map and refined without restraint.</p>
- </div>
- <!-- endrefinementdiv -->
- <div class="computingdetails">
- <a name="computingdetails"></a>
- <div class="heading2">
- Computing details <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><p>Data collection: <i>SMART</i> (Bruker, 1998); cell refinement: <i>SAINT</i> (Bruker, 1998); data reduction: <i>SAINT</i> (Bruker, 1998); program(s) used to solve structure: <i>SHELXS97</i> (Sheldrick, 2008); program(s) used to refine structure: <i>SHELXL97</i> (Sheldrick, 2008); molecular graphics: <i>SHELXTL</i> (Sheldrick, 2008); software used to prepare material for publication: <i>SHELXTL</i> (Sheldrick, 2008).</p>
- </div>
- <!-- endcomputingdetailsdiv -->
- <div class="schemes">
- <a href="./at2552scheme1.gif"></a>
- </div>
- <!-- endschemesdiv -->
- <div class="figures">
- <div class="tablewrap">
- <a name="figures"></a>
- <div class="heading2">
- Figures <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div --><table style="table-layout:fixed" width="100%" class="nodecs">
- <colgroup span="2">
- <col width="110"></col>
- <col></col>
- </colgroup>
- <tr><td class="nodecs" align="center" width="110">
- <a href="./at2552fig1.html"><img width="100" src="./at2552fig1thm.gif" alt="[Figure 1]" align="middle"/></a>
- </td><td class="nodecs" valign="middle" >
- <font size="2">Fig. 1. The molecular structure of (I), with 30% probability displacement ellipsoids.
- [Symmetry code: (A) -x+1, -y, -z+2.]</font>
- </td></tr>
- <tr><td class="nodecs" align="center" width="110">
- <a href="./at2552fig2.html"><img width="100" src="./at2552fig2thm.gif" alt="[Figure 2]" align="middle"/></a>
- </td><td class="nodecs" valign="middle" >
- <font size="2">Fig. 2. A portion of the crystal stacking structure, showing the intermolecular
- O—H···O, hydrogen bonds as dashed lines.</font>
- </td></tr>
- </table>
- </div>
- </div>
- <!-- endfiguresdiv -->
- <div class="datablock1">
- <div class="heading2">
- <a name="chemicalname1"></a>Diaquadimethanolbis[4-(1H-tetrazol-1-yl)benzoato]zinc(II) dihydrate <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- </div>
- <!-- endheading2div -->
- <div class="tablewrapcrystaldatalong">
- <a name="crystaldata1"></a><span class="heading3">Crystal data</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >[Zn(C<sub>8</sub>H<sub>5</sub>N<sub>4</sub>O<sub>2</sub>)<sub>2</sub>(CH<sub>4</sub>O)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>]·2H<sub>2</sub>O</td><td width="50%" class="tabledata" ><i>F</i><sub>000</sub> = 600</td></tr><tr><td width="50%" class="tabledata" ><i>M</i><i><sub>r</sub></i> = 579.84</td><td width="50%" class="tabledata" ><i>D</i><sub>x</sub> = 1.611 Mg m<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >Monoclinic, <i>P</i>2<sub>1</sub>/<i>c</i></td><td width="50%" class="tabledata" >Mo <i>K</i><span style="font-family:Times">α</span> radiation <br /><span style="font-family:Times">λ</span> = 0.71073 Å</td></tr><tr><td width="50%" class="tabledata" >Hall symbol: -P 2ybc</td><td width="50%" class="tabledata" >Cell parameters from 11248 reflections</td></tr><tr><td width="50%" class="tabledata" ><i>a</i> = 13.220 (3) Å</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span> = 3.1–27.6º</td></tr><tr><td width="50%" class="tabledata" ><i>b</i> = 7.1551 (14) Å</td><td width="50%" class="tabledata" >µ = 1.10 mm<span style="font-family:Times"><sup>−</sup></span><sup>1</sup></td></tr><tr><td width="50%" class="tabledata" ><i>c</i> = 12.636 (3) Å</td><td width="50%" class="tabledata" ><i>T</i> = 293 (2) K</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">β</span> = 90.24 (3)º</td><td width="50%" class="tabledata" >Block, colourless</td></tr><tr><td width="50%" class="tabledata" ><i>V</i> = 1195.3 (4) Å<sup>3</sup></td><td width="50%" class="tabledata" >0.20 × 0.18 × 0.16 mm</td></tr><tr><td width="50%" class="tabledata" ><i>Z</i> = 2</td><td width="50%" class="tabledata" ></td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapcrystaldatalongdiv -->
- <div class="tablewrapdatacollectionlong">
- <a name="datacollection1"></a><span class="heading3">Data collection</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >Bruker P4 <br />diffractometer</td><td width="50%" class="tabledata" >2746 independent reflections</td></tr><tr><td width="50%" class="tabledata" >Radiation source: fine-focus sealed tube</td><td width="50%" class="tabledata" >2359 reflections with <i>I</i> > 2<span style="font-family:Times">σ</span>(<i>I</i>)</td></tr><tr><td width="50%" class="tabledata" >Monochromator: graphite</td><td width="50%" class="tabledata" ><i>R</i><sub>int</sub> = 0.045</td></tr><tr><td width="50%" class="tabledata" ><i>T</i> = 293(2) K</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span><sub>max</sub> = 27.5º</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">ω</span> scans</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span><sub>min</sub> = 3.1º</td></tr><tr><td width="50%" class="tabledata" >Absorption correction: multi-scan<br />(SADABS; Bruker, 1998)</td><td width="50%" class="tabledata" ><i>h</i> = <span style="font-family:Times">−</span>17→17</td></tr><tr><td width="50%" class="tabledata" ><i>T</i><sub>min</sub> = 0.810, <i>T</i><sub>max</sub> = 0.844</td><td width="50%" class="tabledata" ><i>k</i> = <span style="font-family:Times">−</span>9→9</td></tr><tr><td width="50%" class="tabledata" >12254 measured reflections</td><td width="50%" class="tabledata" ><i>l</i> = <span style="font-family:Times">−</span>16→16</td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapdatacollectionlongdiv -->
- <div class="tablewraprefinementdatalong">
- <a name="refinementdata1"></a><span class="heading3">Refinement</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >Refinement on <i>F</i><sup>2</sup></td><td width="50%" class="tabledata" >Hydrogen site location: inferred from neighbouring sites</td></tr><tr><td width="50%" class="tabledata" >Least-squares matrix: full</td><td width="50%" class="tabledata" >H atoms treated by a mixture of<br /> independent and constrained refinement</td></tr><tr><td width="50%" class="tabledata" ><i>R</i>[<i>F</i><sup>2</sup> > 2<span style="font-family:Times">σ</span>(<i>F</i><sup>2</sup>)] = 0.032</td><td width="50%" class="tabledata" >  <i>w</i> = 1/[<span style="font-family:Times">σ</span><sup>2</sup>(<i>F</i><sub>o</sub><sup>2</sup>) + (0.0297<i>P</i>)<sup>2</sup> + 0.5826<i>P</i>] <br />where <i>P</i> = (<i>F</i><sub>o</sub><sup>2</sup> + 2<i>F</i><sub>c</sub><sup>2</sup>)/3</td></tr><tr><td width="50%" class="tabledata" ><i>wR</i>(<i>F</i><sup>2</sup>) = 0.076</td><td width="50%" class="tabledata" >(Δ/<span style="font-family:Times">σ</span>)<sub>max</sub> = 0.001</td></tr><tr><td width="50%" class="tabledata" ><i>S</i> = 1.04</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>max</sub> = 0.29 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >2746 reflections</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>min</sub> = <span style="font-family:Times">−</span>0.23 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >188 parameters</td><td width="50%" class="tabledata" >Extinction correction: SHELXL97 (Sheldrick, 2008), Fc<sup>*</sup>=kFc[1+0.001xFc<sup>2</sup><span style="font-family:Times">λ</span><sup>3</sup>/sin(2<span style="font-family:Times">θ</span>)]<sup>-1/4</sup></td></tr><tr><td width="50%" class="tabledata" >Primary atom site location: structure-invariant direct methods</td><td width="50%" class="tabledata" >Extinction coefficient: 0.0228 (12)</td></tr><tr><td width="50%" class="tabledata" >Secondary atom site location: difference Fourier map</td><td width="50%" class="tabledata" ></td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewraprefinementdatalongdiv -->
- <div class="tablewrapcrystaldatashort">
- <a name="crystaldata1"></a><span class="heading3">Crystal data</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >[Zn(C<sub>8</sub>H<sub>5</sub>N<sub>4</sub>O<sub>2</sub>)<sub>2</sub>(CH<sub>4</sub>O)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>]·2H<sub>2</sub>O</td><td width="50%" class="tabledata" ><i>V</i> = 1195.3 (4) Å<sup>3</sup></td></tr><tr><td width="50%" class="tabledata" ><i>M</i><i><sub>r</sub></i> = 579.84</td><td width="50%" class="tabledata" ><i>Z</i> = 2</td></tr><tr><td width="50%" class="tabledata" >Monoclinic, <i>P</i>2<sub>1</sub>/<i>c</i></td><td width="50%" class="tabledata" >Mo <i>K</i><span style="font-family:Times">α</span></td></tr><tr><td width="50%" class="tabledata" ><i>a</i> = 13.220 (3) Å</td><td width="50%" class="tabledata" >µ = 1.10 mm<span style="font-family:Times"><sup>−</sup></span><sup>1</sup></td></tr><tr><td width="50%" class="tabledata" ><i>b</i> = 7.1551 (14) Å</td><td width="50%" class="tabledata" ><i>T</i> = 293 (2) K</td></tr><tr><td width="50%" class="tabledata" ><i>c</i> = 12.636 (3) Å</td><td width="50%" class="tabledata" >0.20 × 0.18 × 0.16 mm</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">β</span> = 90.24 (3)º</td><td width="50%" class="tabledata" ></td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapcrystaldatashortdiv -->
- <div class="tablewrapdatacollectionshort">
- <a name="datacollection1"></a><span class="heading3">Data collection</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" >Bruker P4 <br />diffractometer</td><td width="50%" class="tabledata" >2746 independent reflections</td></tr><tr><td width="50%" class="tabledata" >Absorption correction: multi-scan<br />(SADABS; Bruker, 1998)</td><td width="50%" class="tabledata" >2359 reflections with <i>I</i> > 2<span style="font-family:Times">σ</span>(<i>I</i>)</td></tr><tr><td width="50%" class="tabledata" ><i>T</i><sub>min</sub> = 0.810, <i>T</i><sub>max</sub> = 0.844</td><td width="50%" class="tabledata" ><i>R</i><sub>int</sub> = 0.045</td></tr><tr><td width="50%" class="tabledata" >12254 measured reflections</td><td width="50%" class="tabledata" ></td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewrapdatacollectionshortdiv -->
- <div class="tablewraprefinementdatashort">
- <a name="refinementdata1"></a><span class="heading3">Refinement</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="80%" summary="" class="tabledata">
- <colgroup span="2">
- <col width="50%"></col>
- <col width="50%"></col>
- </colgroup>
- <tr><td width="50%" class="tabledata" ><i>R</i>[<i>F</i><sup>2</sup> > 2<span style="font-family:Times">σ</span>(<i>F</i><sup>2</sup>)] = 0.032</td><td width="50%" class="tabledata" >188 parameters</td></tr><tr><td width="50%" class="tabledata" ><i>wR</i>(<i>F</i><sup>2</sup>) = 0.076</td><td width="50%" class="tabledata" >H atoms treated by a mixture of<br /> independent and constrained refinement</td></tr><tr><td width="50%" class="tabledata" ><i>S</i> = 1.04</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>max</sub> = 0.29 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >2746 reflections</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>min</sub> = <span style="font-family:Times">−</span>0.23 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr></table><!-- endtabledatatable -->
- </div>
- <!-- endtablewraprefinementdatashortdiv -->
- <div class="specialdetails">
- <div class="tablewrap">
- <a name="specialdetails1"></a><span class="heading3">Special details</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan -->
- <table style="table-layout:fixed" width="100%" class="tabledata">
- <tr><td class="tabledata"><p><b>Geometry</b>. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes)
- are estimated using the full covariance matrix. The cell e.s.d.'s are taken
- into account individually in the estimation of e.s.d.'s in distances, angles
- and torsion angles; correlations between e.s.d.'s in cell parameters are only
- used when they are defined by crystal symmetry. An approximate (isotropic)
- treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s.
- planes.</p></td></tr>
- <tr><td class="tabledata"><p><b>Refinement</b>. Refinement of <i>F</i><sup>2</sup> against ALL reflections. The weighted <i>R</i>-factor
- <i>wR</i> and goodness of fit <i>S</i> are based on <i>F</i><sup>2</sup>, conventional
- <i>R</i>-factors <i>R</i> are based on <i>F</i>, with <i>F</i> set to zero for
- negative <i>F</i><sup>2</sup>. The threshold expression of <i>F</i><sup>2</sup> >
- <span style="font-family:Times">σ</span>(<i>F</i><sup>2</sup>) is used only for calculating <i>R</i>-factors(gt) <i>etc</i>.
- and is not relevant to the choice of reflections for refinement.
- <i>R</i>-factors based on <i>F</i><sup>2</sup> are statistically about twice as large
- as those based on <i>F</i>, and <i>R</i>- factors based on ALL data will be
- even larger.</p></td></tr></table>
- </div>
- </div>
- <!-- endspecialdetailsdiv -->
- <div class="tablewrapcoords">
- <a name="fractionalatomiccoordinates1"></a> <span class="heading3">Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å<sup>2</sup>)</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="100%" summary="" class="tabledata"><tr><td class="tabledata" > </td><td class="tabledata" ><i>x</i></td><td class="tabledata" ><i>y</i></td><td class="tabledata" ><i>z</i></td><td class="tabledata" ><i>U</i><sub>iso</sub>*/<i>U</i><sub>eq</sub></td><td class="tabledata" ></td></tr><tr><td class="tabledata" >Zn1</td><td class="tabledata" >0.5000</td><td class="tabledata" >0.0000</td><td class="tabledata" >1.0000</td><td class="tabledata" >0.02298 (11)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O1</td><td class="tabledata" >0.63696 (9)</td><td class="tabledata" >0.0452 (2)</td><td class="tabledata" >0.92928 (10)</td><td class="tabledata" >0.0313 (3)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O2</td><td class="tabledata" >0.73211 (10)</td><td class="tabledata" >0.1468 (2)</td><td class="tabledata" >1.06367 (10)</td><td class="tabledata" >0.0399 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C2</td><td class="tabledata" >0.97854 (12)</td><td class="tabledata" >0.0991 (2)</td><td class="tabledata" >0.77039 (14)</td><td class="tabledata" >0.0231 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >N4</td><td class="tabledata" >1.06694 (11)</td><td class="tabledata" >0.0940 (2)</td><td class="tabledata" >0.70586 (12)</td><td class="tabledata" >0.0243 (3)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C5</td><td class="tabledata" >0.80990 (13)</td><td class="tabledata" >0.1028 (2)</td><td class="tabledata" >0.89760 (14)</td><td class="tabledata" >0.0228 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >N3</td><td class="tabledata" >1.06465 (12)</td><td class="tabledata" >0.1453 (3)</td><td class="tabledata" >0.60316 (13)</td><td class="tabledata" >0.0339 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C4</td><td class="tabledata" >0.90418 (13)</td><td class="tabledata" >0.1480 (3)</td><td class="tabledata" >0.93867 (14)</td><td class="tabledata" >0.0259 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H4</td><td class="tabledata" >0.9104</td><td class="tabledata" >0.1793</td><td class="tabledata" >1.0098</td><td class="tabledata" >0.031*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >N1</td><td class="tabledata" >1.21854 (12)</td><td class="tabledata" >0.0669 (3)</td><td class="tabledata" >0.64661 (14)</td><td class="tabledata" >0.0342 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C7</td><td class="tabledata" >0.88492 (14)</td><td class="tabledata" >0.0580 (3)</td><td class="tabledata" >0.72624 (15)</td><td class="tabledata" >0.0282 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H7</td><td class="tabledata" >0.8786</td><td class="tabledata" >0.0294</td><td class="tabledata" >0.6547</td><td class="tabledata" >0.034*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C3</td><td class="tabledata" >0.98863 (14)</td><td class="tabledata" >0.1470 (3)</td><td class="tabledata" >0.87560 (15)</td><td class="tabledata" >0.0274 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H3</td><td class="tabledata" >1.0516</td><td class="tabledata" >0.1782</td><td class="tabledata" >0.9035</td><td class="tabledata" >0.033*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C8</td><td class="tabledata" >0.71954 (13)</td><td class="tabledata" >0.0989 (3)</td><td class="tabledata" >0.96960 (14)</td><td class="tabledata" >0.0256 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C1</td><td class="tabledata" >1.16184 (14)</td><td class="tabledata" >0.0462 (3)</td><td class="tabledata" >0.72993 (16)</td><td class="tabledata" >0.0291 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1</td><td class="tabledata" >1.1840</td><td class="tabledata" >0.0047</td><td class="tabledata" >0.7958</td><td class="tabledata" >0.035*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C6</td><td class="tabledata" >0.80137 (14)</td><td class="tabledata" >0.0608 (3)</td><td class="tabledata" >0.79125 (15)</td><td class="tabledata" >0.0279 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H6</td><td class="tabledata" >0.7380</td><td class="tabledata" >0.0339</td><td class="tabledata" >0.7629</td><td class="tabledata" >0.033*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >N2</td><td class="tabledata" >1.15560 (13)</td><td class="tabledata" >0.1290 (3)</td><td class="tabledata" >0.56869 (14)</td><td class="tabledata" >0.0375 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O3</td><td class="tabledata" >0.54347 (11)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.2616 (2)</td><td class="tabledata" >1.06193 (13)</td><td class="tabledata" >0.0380 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C9</td><td class="tabledata" >0.63908 (16)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.3252 (3)</td><td class="tabledata" >1.0949 (2)</td><td class="tabledata" >0.0470 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H9A</td><td class="tabledata" >0.6907</td><td class="tabledata" ><span style="font-family:Times">−</span>0.2579</td><td class="tabledata" >1.0578</td><td class="tabledata" >0.071*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H9B</td><td class="tabledata" >0.6451</td><td class="tabledata" ><span style="font-family:Times">−</span>0.4563</td><td class="tabledata" >1.0799</td><td class="tabledata" >0.071*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H9C</td><td class="tabledata" >0.6467</td><td class="tabledata" ><span style="font-family:Times">−</span>0.3050</td><td class="tabledata" >1.1696</td><td class="tabledata" >0.071*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O2W</td><td class="tabledata" >0.43377 (14)</td><td class="tabledata" >0.4734 (2)</td><td class="tabledata" >0.16558 (13)</td><td class="tabledata" >0.0340 (3)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O1W</td><td class="tabledata" >0.54904 (11)</td><td class="tabledata" >0.14327 (19)</td><td class="tabledata" >1.13919 (10)</td><td class="tabledata" >0.0289 (3)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1WA</td><td class="tabledata" >0.5471</td><td class="tabledata" >0.0718</td><td class="tabledata" >1.1898</td><td class="tabledata" >0.043*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2WA</td><td class="tabledata" >0.378 (2)</td><td class="tabledata" >0.457 (4)</td><td class="tabledata" >0.156 (2)</td><td class="tabledata" >0.053 (9)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2WB</td><td class="tabledata" >0.463 (2)</td><td class="tabledata" >0.382 (4)</td><td class="tabledata" >0.156 (2)</td><td class="tabledata" >0.061 (10)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1WB</td><td class="tabledata" >0.612 (2)</td><td class="tabledata" >0.155 (4)</td><td class="tabledata" >1.121 (2)</td><td class="tabledata" >0.058 (8)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H3M</td><td class="tabledata" >0.5060 (19)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.325 (4)</td><td class="tabledata" >1.088 (2)</td><td class="tabledata" >0.047 (8)*</td><td class="tabledata" ></td></tr></table>
- </div>
- <!-- endtablewrapcoordsdiv -->
- <div class="tablewrapadps">
- <a name="atomicdisplacement1"></a> <span class="heading3">Atomic displacement parameters (Å<sup>2</sup>)</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><table style="table-layout:fixed" width="100%" summary="" class="tabledata"><tr><td class="tabledata" > </td><td class="tabledata" ><i>U</i><sup>11</sup></td><td class="tabledata" ><i>U</i><sup>22</sup></td><td class="tabledata" ><i>U</i><sup>33</sup></td><td class="tabledata" ><i>U</i><sup>12</sup></td><td class="tabledata" ><i>U</i><sup>13</sup></td><td class="tabledata" ><i>U</i><sup>23</sup></td></tr><tr><td class="tabledata" >Zn1</td><td class="tabledata" >0.01705 (16)</td><td class="tabledata" >0.02848 (18)</td><td class="tabledata" >0.02340 (17)</td><td class="tabledata" >0.00002 (12)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.00056 (11)</td><td class="tabledata" >0.00133 (13)</td></tr><tr><td class="tabledata" >O1</td><td class="tabledata" >0.0173 (6)</td><td class="tabledata" >0.0487 (9)</td><td class="tabledata" >0.0279 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0049 (6)</td><td class="tabledata" >0.0003 (5)</td><td class="tabledata" >0.0000 (6)</td></tr><tr><td class="tabledata" >O2</td><td class="tabledata" >0.0265 (7)</td><td class="tabledata" >0.0670 (11)</td><td class="tabledata" >0.0261 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0095 (7)</td><td class="tabledata" >0.0019 (6)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0061 (7)</td></tr><tr><td class="tabledata" >C2</td><td class="tabledata" >0.0174 (9)</td><td class="tabledata" >0.0241 (9)</td><td class="tabledata" >0.0279 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0001 (7)</td><td class="tabledata" >0.0021 (7)</td><td class="tabledata" >0.0030 (7)</td></tr><tr><td class="tabledata" >N4</td><td class="tabledata" >0.0191 (7)</td><td class="tabledata" >0.0275 (8)</td><td class="tabledata" >0.0261 (8)</td><td class="tabledata" >0.0008 (6)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0003 (6)</td><td class="tabledata" >0.0027 (7)</td></tr><tr><td class="tabledata" >C5</td><td class="tabledata" >0.0184 (8)</td><td class="tabledata" >0.0231 (9)</td><td class="tabledata" >0.0270 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0014 (7)</td><td class="tabledata" >0.0000 (7)</td><td class="tabledata" >0.0016 (7)</td></tr><tr><td class="tabledata" >N3</td><td class="tabledata" >0.0277 (9)</td><td class="tabledata" >0.0455 (10)</td><td class="tabledata" >0.0284 (9)</td><td class="tabledata" >0.0043 (7)</td><td class="tabledata" >0.0021 (7)</td><td class="tabledata" >0.0072 (8)</td></tr><tr><td class="tabledata" >C4</td><td class="tabledata" >0.0240 (9)</td><td class="tabledata" >0.0310 (10)</td><td class="tabledata" >0.0227 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0040 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0023 (7)</td><td class="tabledata" >0.0004 (8)</td></tr><tr><td class="tabledata" >N1</td><td class="tabledata" >0.0239 (9)</td><td class="tabledata" >0.0384 (9)</td><td class="tabledata" >0.0403 (10)</td><td class="tabledata" >0.0029 (7)</td><td class="tabledata" >0.0040 (7)</td><td class="tabledata" >0.0031 (8)</td></tr><tr><td class="tabledata" >C7</td><td class="tabledata" >0.0244 (9)</td><td class="tabledata" >0.0352 (10)</td><td class="tabledata" >0.0249 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0018 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0025 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0039 (8)</td></tr><tr><td class="tabledata" >C3</td><td class="tabledata" >0.0190 (9)</td><td class="tabledata" >0.0330 (10)</td><td class="tabledata" >0.0301 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0040 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0053 (7)</td><td class="tabledata" >0.0009 (8)</td></tr><tr><td class="tabledata" >C8</td><td class="tabledata" >0.0199 (9)</td><td class="tabledata" >0.0283 (10)</td><td class="tabledata" >0.0287 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0013 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0004 (7)</td><td class="tabledata" >0.0038 (8)</td></tr><tr><td class="tabledata" >C1</td><td class="tabledata" >0.0214 (9)</td><td class="tabledata" >0.0331 (11)</td><td class="tabledata" >0.0328 (10)</td><td class="tabledata" >0.0023 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0020 (8)</td><td class="tabledata" >0.0010 (8)</td></tr><tr><td class="tabledata" >C6</td><td class="tabledata" >0.0179 (9)</td><td class="tabledata" >0.0362 (10)</td><td class="tabledata" >0.0294 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0033 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0039 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0030 (8)</td></tr><tr><td class="tabledata" >N2</td><td class="tabledata" >0.0290 (9)</td><td class="tabledata" >0.0478 (11)</td><td class="tabledata" >0.0358 (10)</td><td class="tabledata" >0.0035 (8)</td><td class="tabledata" >0.0080 (7)</td><td class="tabledata" >0.0093 (8)</td></tr><tr><td class="tabledata" >O3</td><td class="tabledata" >0.0261 (7)</td><td class="tabledata" >0.0373 (9)</td><td class="tabledata" >0.0505 (9)</td><td class="tabledata" >0.0028 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0007 (7)</td><td class="tabledata" >0.0194 (7)</td></tr><tr><td class="tabledata" >C9</td><td class="tabledata" >0.0323 (12)</td><td class="tabledata" >0.0468 (14)</td><td class="tabledata" >0.0620 (15)</td><td class="tabledata" >0.0093 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0041 (11)</td><td class="tabledata" >0.0120 (12)</td></tr><tr><td class="tabledata" >O2W</td><td class="tabledata" >0.0277 (8)</td><td class="tabledata" >0.0361 (9)</td><td class="tabledata" >0.0382 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0020 (7)</td><td class="tabledata" >0.0031 (7)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0057 (7)</td></tr><tr><td class="tabledata" >O1W</td><td class="tabledata" >0.0251 (7)</td><td class="tabledata" >0.0359 (8)</td><td class="tabledata" >0.0257 (7)</td><td class="tabledata" >0.0002 (6)</td><td class="tabledata" >0.0004 (6)</td><td class="tabledata" >0.0029 (6)</td></tr></table>
- </div>
- <!-- endtablewrapadpsdiv -->
- <div class="tablewrapgeomlong">
- <a name="geometricparameters1"></a> <span class="heading3">Geometric parameters (Å, °)</span><!-- endheading3span --> <span class="toplink"><a class="buttons" href="#top">top</a></span><!-- endtoplinkspan --><!-- startgeom --><table style="table-layout:fixed" width="100%" summary="" class="tabledata">
- <colgroup span="4">
- <col width="30%"></col>
- <col width="20%"></col>
- <col width="30%"></col>
- <col width="20%"></col>
- </colgroup>
- <tr><td width="30%" class="tabledata" >Zn1—O1</td><td width="20%" class="tabledata" >2.0483 (14)</td><td width="30%" class="tabledata" >C4—H4</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >Zn1—O1<sup>i</sup></td><td width="20%" class="tabledata" >2.0483 (14)</td><td width="30%" class="tabledata" >N1—C1</td><td width="20%" class="tabledata" >1.304 (3)</td></tr><tr><td width="30%" class="tabledata" >Zn1—O3</td><td width="20%" class="tabledata" >2.1078 (15)</td><td width="30%" class="tabledata" >N1—N2</td><td width="20%" class="tabledata" >1.361 (2)</td></tr><tr><td width="30%" class="tabledata" >Zn1—O3<sup>i</sup></td><td width="20%" class="tabledata" >2.1078 (15)</td><td width="30%" class="tabledata" >C7—C6</td><td width="20%" class="tabledata" >1.379 (3)</td></tr><tr><td width="30%" class="tabledata" >Zn1—O1W<sup>i</sup></td><td width="20%" class="tabledata" >2.1342 (14)</td><td width="30%" class="tabledata" >C7—H7</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >Zn1—O1W</td><td width="20%" class="tabledata" >2.1342 (14)</td><td width="30%" class="tabledata" >C3—H3</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >O1—C8</td><td width="20%" class="tabledata" >1.263 (2)</td><td width="30%" class="tabledata" >C1—H1</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >O2—C8</td><td width="20%" class="tabledata" >1.247 (2)</td><td width="30%" class="tabledata" >C6—H6</td><td width="20%" class="tabledata" >0.9300</td></tr><tr><td width="30%" class="tabledata" >C2—C3</td><td width="20%" class="tabledata" >1.379 (3)</td><td width="30%" class="tabledata" >O3—C9</td><td width="20%" class="tabledata" >1.405 (2)</td></tr><tr><td width="30%" class="tabledata" >C2—C7</td><td width="20%" class="tabledata" >1.387 (2)</td><td width="30%" class="tabledata" >O3—H3M</td><td width="20%" class="tabledata" >0.75 (3)</td></tr><tr><td width="30%" class="tabledata" >C2—N4</td><td width="20%" class="tabledata" >1.428 (2)</td><td width="30%" class="tabledata" >C9—H9A</td><td width="20%" class="tabledata" >0.9600</td></tr><tr><td width="30%" class="tabledata" >N4—C1</td><td width="20%" class="tabledata" >1.334 (2)</td><td width="30%" class="tabledata" >C9—H9B</td><td width="20%" class="tabledata" >0.9600</td></tr><tr><td width="30%" class="tabledata" >N4—N3</td><td width="20%" class="tabledata" >1.349 (2)</td><td width="30%" class="tabledata" >C9—H9C</td><td width="20%" class="tabledata" >0.9600</td></tr><tr><td width="30%" class="tabledata" >C5—C6</td><td width="20%" class="tabledata" >1.381 (3)</td><td width="30%" class="tabledata" >O2W—H2WA</td><td width="20%" class="tabledata" >0.75 (3)</td></tr><tr><td width="30%" class="tabledata" >C5—C4</td><td width="20%" class="tabledata" >1.386 (2)</td><td width="30%" class="tabledata" >O2W—H2WB</td><td width="20%" class="tabledata" >0.77 (3)</td></tr><tr><td width="30%" class="tabledata" >C5—C8</td><td width="20%" class="tabledata" >1.505 (2)</td><td width="30%" class="tabledata" >O1W—H1WA</td><td width="20%" class="tabledata" >0.8200</td></tr><tr><td width="30%" class="tabledata" >N3—N2</td><td width="20%" class="tabledata" >1.286 (2)</td><td width="30%" class="tabledata" >O1W—H1WB</td><td width="20%" class="tabledata" >0.87 (3)</td></tr><tr><td width="30%" class="tabledata" >C4—C3</td><td width="20%" class="tabledata" >1.375 (3)</td><td width="30%" class="tabledata" ></td><td width="20%" class="tabledata" ></td></tr><tr><td width="25%" class="tabledata" ></td><td width="25%" class="tabledata" ></td><td width="25%" class="tabledata" ></td><td width="25%" class="tabledata" ></td></tr><tr><td width="30%" class="tabledata" >O1—Zn1—O1<sup>i</sup></td><td width="20%" class="tabledata" >180.00 (3)</td><td width="30%" class="tabledata" >C6—C7—C2</td><td width="20%" class="tabledata" >118.22 (17)</td></tr><tr><td width="30%" class="tabledata" >O1—Zn1—O3</td><td width="20%" class="tabledata" >93.56 (6)</td><td width="30%" class="tabledata" >C6—C7—H7</td><td width="20%" class="tabledata" >120.9</td></tr><tr><td width="30%" class="tabledata" >O1<sup>i</sup>—Zn1—O3</td><td width="20%" class="tabledata" >86.44 (6)</td><td width="30%" class="tabledata" >C2—C7—H7</td><td width="20%" class="tabledata" >120.9</td></tr><tr><td width="30%" class="tabledata" >O1—Zn1—O3<sup>i</sup></td><td width="20%" class="tabledata" >86.44 (6)</td><td width="30%" class="tabledata" >C4—C3—C2</td><td width="20%" class="tabledata" >119.00 (17)</td></tr><tr><td width="30%" class="tabledata" >O1<sup>i</sup>—Zn1—O3<sup>i</sup></td><td width="20%" class="tabledata" >93.56 (6)</td><td width="30%" class="tabledata" >C4—C3—H3</td><td width="20%" class="tabledata" >120.5</td></tr><tr><td width="30%" class="tabledata" >O3—Zn1—O3<sup>i</sup></td><td width="20%" class="tabledata" >180.0</td><td width="30%" class="tabledata" >C2—C3—H3</td><td width="20%" class="tabledata" >120.5</td></tr><tr><td width="30%" class="tabledata" >O1—Zn1—O1W<sup>i</sup></td><td width="20%" class="tabledata" >88.98 (6)</td><td width="30%" class="tabledata" >O2—C8—O1</td><td width="20%" class="tabledata" >125.41 (17)</td></tr><tr><td width="30%" class="tabledata" >O1<sup>i</sup>—Zn1—O1W<sup>i</sup></td><td width="20%" class="tabledata" >91.02 (6)</td><td width="30%" class="tabledata" >O2—C8—C5</td><td width="20%" class="tabledata" >117.92 (16)</td></tr><tr><td width="30%" class="tabledata" >O3—Zn1—O1W<sup>i</sup></td><td width="20%" class="tabledata" >87.75 (6)</td><td width="30%" class="tabledata" >O1—C8—C5</td><td width="20%" class="tabledata" >116.66 (16)</td></tr><tr><td width="30%" class="tabledata" >O3<sup>i</sup>—Zn1—O1W<sup>i</sup></td><td width="20%" class="tabledata" >92.25 (6)</td><td width="30%" class="tabledata" >N1—C1—N4</td><td width="20%" class="tabledata" >109.28 (17)</td></tr><tr><td width="30%" class="tabledata" >O1—Zn1—O1W</td><td width="20%" class="tabledata" >91.02 (6)</td><td width="30%" class="tabledata" >N1—C1—H1</td><td width="20%" class="tabledata" >125.4</td></tr><tr><td width="30%" class="tabledata" >O1<sup>i</sup>—Zn1—O1W</td><td width="20%" class="tabledata" >88.98 (6)</td><td width="30%" class="tabledata" >N4—C1—H1</td><td width="20%" class="tabledata" >125.4</td></tr><tr><td width="30%" class="tabledata" >O3—Zn1—O1W</td><td width="20%" class="tabledata" >92.25 (6)</td><td width="30%" class="tabledata" >C7—C6—C5</td><td width="20%" class="tabledata" >121.35 (17)</td></tr><tr><td width="30%" class="tabledata" >O3<sup>i</sup>—Zn1—O1W</td><td width="20%" class="tabledata" >87.75 (6)</td><td width="30%" class="tabledata" >C7—C6—H6</td><td width="20%" class="tabledata" >119.3</td></tr><tr><td width="30%" class="tabledata" >O1W<sup>i</sup>—Zn1—O1W</td><td width="20%" class="tabledata" >180.0</td><td width="30%" class="tabledata" >C5—C6—H6</td><td width="20%" class="tabledata" >119.3</td></tr><tr><td width="30%" class="tabledata" >C8—O1—Zn1</td><td width="20%" class="tabledata" >129.52 (12)</td><td width="30%" class="tabledata" >N3—N2—N1</td><td width="20%" class="tabledata" >110.75 (16)</td></tr><tr><td width="30%" class="tabledata" >C3—C2—C7</td><td width="20%" class="tabledata" >121.54 (17)</td><td width="30%" class="tabledata" >C9—O3—Zn1</td><td width="20%" class="tabledata" >129.90 (14)</td></tr><tr><td width="30%" class="tabledata" >C3—C2—N4</td><td width="20%" class="tabledata" >118.74 (16)</td><td width="30%" class="tabledata" >C9—O3—H3M</td><td width="20%" class="tabledata" >105 (2)</td></tr><tr><td width="30%" class="tabledata" >C7—C2—N4</td><td width="20%" class="tabledata" >119.72 (16)</td><td width="30%" class="tabledata" >Zn1—O3—H3M</td><td width="20%" class="tabledata" >122 (2)</td></tr><tr><td width="30%" class="tabledata" >C1—N4—N3</td><td width="20%" class="tabledata" >107.84 (15)</td><td width="30%" class="tabledata" >O3—C9—H9A</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C1—N4—C2</td><td width="20%" class="tabledata" >130.34 (16)</td><td width="30%" class="tabledata" >O3—C9—H9B</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >N3—N4—C2</td><td width="20%" class="tabledata" >121.81 (15)</td><td width="30%" class="tabledata" >H9A—C9—H9B</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C6—C5—C4</td><td width="20%" class="tabledata" >118.98 (17)</td><td width="30%" class="tabledata" >O3—C9—H9C</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C6—C5—C8</td><td width="20%" class="tabledata" >121.50 (16)</td><td width="30%" class="tabledata" >H9A—C9—H9C</td><td width="20%" class="tabledata" >109.5</td></tr><tr><td width="30%" class="tabledata" >C4—C5—…
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