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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="./at2619.pdf" ><img src="../../../../../graphics/pdfborder.gif" alt="pdf version" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/sendcif?at2619sup1" ><img src="../../../../../graphics/cifborder.gif" alt="cif file" align="top" border="0" /></a><a href="http://scripts.iucr.org/cgi-bin/sendcif?at2619sup1&Qmime=cif" ><img src="../../../../../graphics/3dviewborder.gif" alt="3d view" align="top" border="0" /></a><a href="./at2619Isup2.hkl" ><img src="../../../../../graphics/structurefactorsborder.gif" alt="structure factors" align="top" border="0" /></a><a href="./at2619sup0.html" ><img src="../../../../../graphics/supplementarymaterialsborder.gif" alt="supplementary materials" align="top" border="0" /></a><a href="./at2619checkcif.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=trifluoromethyl%20or%20hexahydropyrimidine&from=at2619" ><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="./at2619contents.gif" alt="at2619 scheme" /></p><div class="bibline"><p><i>Acta Cryst.</i> (2008). E<b>64</b>, o1840-o1841 [ <font size="2"><a title="Open URL link" href="http://dx.doi.org/10.1107/S1600536808027232">doi:10.1107/S1600536808027232</a></font> ]</p></div>
- <h3>2-[2-Chloro-5-(trifluoromethyl)phenyl]hexahydropyrimidine monohydrate</h3><h3><a href="http://scripts.iucr.org/cgi-bin/citedin?search_on=name&author_name=Fun,%20H.-K.">H.-K. Fun</a> and <a href="http://scripts.iucr.org/cgi-bin/citedin?search_on=name&author_name=Kia,%20R.">R. Kia</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>The molecule of the title compound, C<span class="inf"><sub>11</sub></span>H<span class="inf"><sub>12</sub></span>ClF<span class="inf"><sub>3</sub></span>N<span class="inf"><sub>2</sub></span>·H<span class="inf"><sub>2</sub></span>O, is a substituted hexahydropyrimidine. There are two crystallographically independent molecules (<span class="it"><i>A</i></span> and <span class="it"><i>B</i></span>) and two water molecules in the asymmetric unit of the title compound. Intermolecular C-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />Cl (× 2), C-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />F, and C-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />N (× 2) hydrogen bonds generate <span class="it"><i>S</i></span>(5) ring motifs. The dihedral angle between the two benzene rings is 8.17 (11)°. The F atoms in molecule <span class="it"><i>B</i></span> are disordered over four positions with refined site-occupancies of <span class="it"><i>ca</i></span> 0.35/0.19/0.29/0.17 for the four components. In the crystal structure, molecules are arranged into one-dimensional extended chains along the <span class="it"><i>c</i></span> axis and are further stacked along the <span class="it"><i>a</i></span> axis by directed four-membered O-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />O-H interactions, forming two-dimensional networks parallel to the <span class="it"><i>ac</i></span> plane. The short distances between the centroids of the benzene rings (3.8002-3.8327 Å) indicate the existence of <img alt="[pi]" border="0" src="/logos/entities/pi_rmgif.gif" />-<img alt="[pi]" border="0" src="/logos/entities/pi_rmgif.gif" /> interactions. In addition, the crystal structure is further stabilized by N-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />O, O-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />N (× 4), N-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />Cl and C-H<img alt="..." border="0" src="/logos/entities/ctdot_rmgif.gif" />O (× 2) hydrogen-bonding interactions.</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">2-[2-Chloro-5-(trifluoromethyl)phenyl]hexahydropyrimidine monohydrate </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="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>Hexahydropyrimidines are prepared classically by condensations of substituted
- propane-1,3-diamines with aldehydes and ketones. Hexahydropyrimidines are
- biologically important. <i>N,N'</i>-Bisalkylhexahydro pyrimidines are
- effective against Ehrlich carcinoma, LK lymphoma, and Staphylococcus aureus.
- The hexahydropyrimidine skeleton occurs in alkaloids such as verbamethine and
- verbametrine. <i>N</i>-Substituted hexahydropyrimidines are synthetic
- intermediates for recently discovered spermidine-nitroimidazole drugs for the
- treatment of A549 lung carcinoma and structural units in new trypanothione
- reductase inhibiting ligands for the regulation of oxidative stress in
- parasitic cells. Benzo-fused hexahydropyrimidines or
- 1,2,3,4-tetrahydroquinazolines are potential <i>R</i>-adrenergic blockers and
- possess antiplatelet activity.</p><p>In the title compound (I) (Fig. 1), intramolecular C—H···Cl (<i>x</i> 2),
- C—H···F, and C—H···N (<i>x</i> 2) hydrogen bonds generate <i>S</i>(5) ring
- motifs (Bernstein <i>et al.</i>, 1995). The bond lengths and angles are
- within
- normal ranges (Allen <i>et al.</i>, 1987). There are two
- crystallographically
- independent molecules (A, and B) and two water molecules in the asymmetric
- unit of the title compound. The dihedral angle between the two benzene rings
- is 8.17 (11)°. The pyrimidine rings in molecules A and B adopt chair
- conformation with the puckering parameter (Cremer & Pople, 1975)
- Q=0.603 (3)°;
- <span style="font-family:Times">θ</span>=1.2 (3)°; <span style="font-family:Times">φ</span>=31 (9)° for ring A and Q=0.601 (3)°; <span style="font-family:Times">θ</span>=2.5 (3)°; <span style="font-family:Times">φ</span>=48 (6)°
- for ring B. The CF<sub>3</sub> fragment in molecule B, was disordered over four
- positions with the refined site-occupancies of
- 0.351 (7)/0.189 (5)/0.289 (9)/0.168 (6) for these four components, respectively.
- In the crystal structure, molecules are arranged into 1-D extended chains along
- the <i>c</i>-axis and are further stacked along the <i>a</i>-axis by directed
- four-membered O—H···O—H interactions to form 2-D networks which is
- parralell to <i>ac</i>-plane. The short distances between the centroids of the
- benzene rings prove an existence of <span style="font-family:Times">π</span>-<span style="font-family:Times">π</span> interactions with distances of
- 3.8002–3.8327 Å. In addition, the crystal structure is further stabilized
- by N—H···O, O—H···N (<i>x</i> 4), N—H···Cl, and C—H···O (<i>x</i> 2)
- hydrogen bonding interactions.</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 bond-lengts data, see: Allen <i>et al.</i> (1987). For hydrogen-bond
- motifs,
- see: Bernstein <i>et al.</i> (1995). For ring conformations, see:
- Cremer &
- Pople (1975). For related literature and properties, see, for example:
- Riebsomer & Morey (1950); Finch <i>et al.</i> (1952); Drandarov
- <i>et al.</i>
- (1999); Siddiqui <i>et al.</i> (1999); Horvath (1997);
- Katritzky <i>et al.</i>
- (2002).</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>The title compound was synthesized based on the previous method (Finch <i>et
- al.</i>, 1952). Single crystals suitable for <i>X</i>-ray diffraction
- were
- obtained by evaporation of an ethanol solution at room temperature.</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 bound to the N atoms and water molecules were initially found from the
- difference Fourier map and refined freely with the parent atoms. The rest of
- the hydrogen atoms were positioned geometrically and refined as
- riding model with
- <i>U</i><sub>iso</sub>(H) = 1.2 <i>U</i><sub>eq</sub>(C). The disordered fluorine atoms of the
- CF<sub>3</sub> fragment in molecule B were refined isotropically using C—F bonds
- distance restraint of 1.300 (5). Their displacement parameters were restrained
- using rigid bond model.</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>APEX2</i> (Bruker, 2005); cell refinement: <i>APEX2</i>; data reduction: <i>SAINT</i> (Bruker, 2005); program(s) used to solve structure: <i>SHELXTL</i> (Sheldrick, 2008); program(s) used to refine structure: <i>SHELXTL</i> (Sheldrick, 2008); molecular graphics: <i>SHELXTL</i> (Sheldrick, 2008); software used to prepare material for publication: <i>SHELXTL</i> (Sheldrick, 2008) and <i>PLATON</i> (Spek, 2003).</p>
- </div>
- <!-- endcomputingdetailsdiv -->
- <div class="schemes">
- <a href="./at2619scheme1.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="./at2619fig1.html"><img width="100" src="./at2619fig1thm.gif" alt="[Figure 1]" align="middle"/></a>
- </td><td class="nodecs" valign="middle" >
- <font size="2">Fig. 1. The molecular structure of (I), showing 40% probability displacement
- ellipsoids. For clarity, only hydrogen atoms of the water molecules and those
- H atoms involved in intramolecular and intermolecular interactions (shown as
- dashed lines) were drawn. Open bonds indicate the minor disordered component.</font>
- </td></tr>
- <tr><td class="nodecs" align="center" width="110">
- <a href="./at2619fig2.html"><img width="100" src="./at2619fig2thm.gif" alt="[Figure 2]" align="middle"/></a>
- </td><td class="nodecs" valign="middle" >
- <font size="2">Fig. 2. The crystal packing of the major component of (I), viewed down the
- <i>a</i>-axis, showing 1-D extended
- chains along the <i>c</i>-axis and stacking of these chains along the
- <i>a</i>-axis. Intra and intermolecular interactions are shown as dashed
- lines.</font>
- </td></tr>
- <tr><td class="nodecs" align="center" width="110">
- <a href="./at2619fig3.html"><img width="100" src="./at2619fig3thm.gif" alt="[Figure 3]" align="middle"/></a>
- </td><td class="nodecs" valign="middle" >
- <font size="2">Fig. 3. The crystal structure of the major component of (I), showing 1-D extended
- chains along the
- <i>a</i>-axis.</font>
- </td></tr>
- </table>
- </div>
- </div>
- <!-- endfiguresdiv -->
- <div class="datablock1">
- <div class="heading2">
- <a name="chemicalname1"></a>2-[2-Chloro-5-(trifluoromethyl)phenyl]hexahydropyrimidine monohydrate <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" >C<sub>11</sub>H<sub>12</sub>Cl<sub>1</sub>F<sub>3</sub>N<sub>2</sub>·H<sub>2</sub>O<sub>1</sub></td><td width="50%" class="tabledata" ><i>F</i><sub>000</sub> = 1168</td></tr><tr><td width="50%" class="tabledata" ><i>M</i><i><sub>r</sub></i> = 282.69</td><td width="50%" class="tabledata" ><i>D</i><sub>x</sub> = 1.496 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 6400 reflections</td></tr><tr><td width="50%" class="tabledata" ><i>a</i> = 7.0745 (2) Å</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span> = 2.4–23.0º</td></tr><tr><td width="50%" class="tabledata" ><i>b</i> = 18.6119 (5) Å</td><td width="50%" class="tabledata" >µ = 0.33 mm<span style="font-family:Times"><sup>−</sup></span><sup>1</sup></td></tr><tr><td width="50%" class="tabledata" ><i>c</i> = 19.0631 (5) Å</td><td width="50%" class="tabledata" ><i>T</i> = 100.0 (1) K</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">β</span> = 91.010 (2)º</td><td width="50%" class="tabledata" >Block, colourless</td></tr><tr><td width="50%" class="tabledata" ><i>V</i> = 2509.65 (12) Å<sup>3</sup></td><td width="50%" class="tabledata" >0.24 × 0.05 × 0.02 mm</td></tr><tr><td width="50%" class="tabledata" ><i>Z</i> = 8</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 SMART APEXII CCD area-detector <br />diffractometer</td><td width="50%" class="tabledata" >7308 independent reflections</td></tr><tr><td width="50%" class="tabledata" >Radiation source: fine-focus sealed tube</td><td width="50%" class="tabledata" >4995 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> = 0.053</td></tr><tr><td width="50%" class="tabledata" ><i>T</i> = 100.0(1) K</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span><sub>max</sub> = 30.1º</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">φ</span> and <span style="font-family:Times">ω</span> scans</td><td width="50%" class="tabledata" ><span style="font-family:Times">θ</span><sub>min</sub> = 2.1º</td></tr><tr><td width="50%" class="tabledata" >Absorption correction: multi-scan<br />(SADABS; Bruker, 2005)</td><td width="50%" class="tabledata" ><i>h</i> = <span style="font-family:Times">−</span>9→9</td></tr><tr><td width="50%" class="tabledata" ><i>T</i><sub>min</sub> = 0.924, <i>T</i><sub>max</sub> = 0.992</td><td width="50%" class="tabledata" ><i>k</i> = <span style="font-family:Times">−</span>26→20</td></tr><tr><td width="50%" class="tabledata" >30107 measured reflections</td><td width="50%" class="tabledata" ><i>l</i> = <span style="font-family:Times">−</span>16→26</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" >Secondary atom site location: difference Fourier map</td></tr><tr><td width="50%" class="tabledata" >Least-squares matrix: full</td><td width="50%" class="tabledata" >Hydrogen site location: inferred from neighbouring sites</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>)] = 0.064</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>wR</i>(<i>F</i><sup>2</sup>) = 0.145</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>) + (0.0411<i>P</i>)<sup>2</sup> + 3.5237<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>S</i> = 1.08</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" >7308 reflections</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>max</sub> = 0.61 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >379 parameters</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>min</sub> = <span style="font-family:Times">−</span>0.60 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >41 restraints</td><td width="50%" class="tabledata" >Extinction correction: none</td></tr><tr><td width="50%" class="tabledata" >Primary atom site location: structure-invariant direct methods</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" >C<sub>11</sub>H<sub>12</sub>Cl<sub>1</sub>F<sub>3</sub>N<sub>2</sub>·H<sub>2</sub>O<sub>1</sub></td><td width="50%" class="tabledata" ><i>V</i> = 2509.65 (12) Å<sup>3</sup></td></tr><tr><td width="50%" class="tabledata" ><i>M</i><i><sub>r</sub></i> = 282.69</td><td width="50%" class="tabledata" ><i>Z</i> = 8</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> = 7.0745 (2) Å</td><td width="50%" class="tabledata" >µ = 0.33 mm<span style="font-family:Times"><sup>−</sup></span><sup>1</sup></td></tr><tr><td width="50%" class="tabledata" ><i>b</i> = 18.6119 (5) Å</td><td width="50%" class="tabledata" ><i>T</i> = 100.0 (1) K</td></tr><tr><td width="50%" class="tabledata" ><i>c</i> = 19.0631 (5) Å</td><td width="50%" class="tabledata" >0.24 × 0.05 × 0.02 mm</td></tr><tr><td width="50%" class="tabledata" ><span style="font-family:Times">β</span> = 91.010 (2)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 SMART APEXII CCD area-detector <br />diffractometer</td><td width="50%" class="tabledata" >7308 independent reflections</td></tr><tr><td width="50%" class="tabledata" >Absorption correction: multi-scan<br />(SADABS; Bruker, 2005)</td><td width="50%" class="tabledata" >4995 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> = 0.924, <i>T</i><sub>max</sub> = 0.992</td><td width="50%" class="tabledata" ><i>R</i><sub>int</sub> = 0.053</td></tr><tr><td width="50%" class="tabledata" >30107 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>)] = 0.064</td><td width="50%" class="tabledata" >41 restraints</td></tr><tr><td width="50%" class="tabledata" ><i>wR</i>(<i>F</i><sup>2</sup>) = 0.145</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> = 1.08</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>max</sub> = 0.61 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >7308 reflections</td><td width="50%" class="tabledata" >Δ<span style="font-family:Times">ρ</span><sub>min</sub> = <span style="font-family:Times">−</span>0.60 e Å<span style="font-family:Times"><sup>−</sup></span><sup>3</sup></td></tr><tr><td width="50%" class="tabledata" >379 parameters</td><td width="50%" class="tabledata" ></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>Experimental</b>. The low-temperature data was collected with the Oxford Cyrosystem Cobra
- low-temperature attachment.</p></td></tr>
- <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" >Occ. (<1)</td></tr><tr><td class="tabledata" >Cl1A</td><td class="tabledata" >0.20441 (9)</td><td class="tabledata" >0.10260 (4)</td><td class="tabledata" >0.33890 (4)</td><td class="tabledata" >0.02426 (16)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >F1A</td><td class="tabledata" >0.1451 (3)</td><td class="tabledata" >0.40379 (9)</td><td class="tabledata" >0.52585 (9)</td><td class="tabledata" >0.0364 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >F2A</td><td class="tabledata" >0.0671 (3)</td><td class="tabledata" >0.44306 (10)</td><td class="tabledata" >0.42408 (11)</td><td class="tabledata" >0.0431 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >F3A</td><td class="tabledata" >0.3579 (2)</td><td class="tabledata" >0.43149 (10)</td><td class="tabledata" >0.45284 (10)</td><td class="tabledata" >0.0382 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >N1A</td><td class="tabledata" >0.0590 (3)</td><td class="tabledata" >0.15070 (12)</td><td class="tabledata" >0.56007 (12)</td><td class="tabledata" >0.0182 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >N2A</td><td class="tabledata" >0.3521 (3)</td><td class="tabledata" >0.10898 (12)</td><td class="tabledata" >0.51715 (12)</td><td class="tabledata" >0.0182 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C1A</td><td class="tabledata" >0.1928 (3)</td><td class="tabledata" >0.18840 (15)</td><td class="tabledata" >0.37603 (14)</td><td class="tabledata" >0.0195 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C2A</td><td class="tabledata" >0.2034 (3)</td><td class="tabledata" >0.24683 (16)</td><td class="tabledata" >0.33062 (14)</td><td class="tabledata" >0.0226 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2AA</td><td class="tabledata" >0.2129</td><td class="tabledata" >0.2397</td><td class="tabledata" >0.2825</td><td class="tabledata" >0.027*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C3A</td><td class="tabledata" >0.1998 (3)</td><td class="tabledata" >0.31528 (16)</td><td class="tabledata" >0.35780 (14)</td><td class="tabledata" >0.0227 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H3AA</td><td class="tabledata" >0.2056</td><td class="tabledata" >0.3548</td><td class="tabledata" >0.3280</td><td class="tabledata" >0.027*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C4A</td><td class="tabledata" >0.1874 (3)</td><td class="tabledata" >0.32524 (14)</td><td class="tabledata" >0.42968 (14)</td><td class="tabledata" >0.0193 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C5A</td><td class="tabledata" >0.1752 (3)</td><td class="tabledata" >0.26648 (14)</td><td class="tabledata" >0.47436 (14)</td><td class="tabledata" >0.0169 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H5AA</td><td class="tabledata" >0.1667</td><td class="tabledata" >0.2739</td><td class="tabledata" >0.5224</td><td class="tabledata" >0.020*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C6A</td><td class="tabledata" >0.1758 (3)</td><td class="tabledata" >0.19653 (14)</td><td class="tabledata" >0.44817 (13)</td><td class="tabledata" >0.0163 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C7A</td><td class="tabledata" >0.1603 (3)</td><td class="tabledata" >0.13238 (14)</td><td class="tabledata" >0.49649 (13)</td><td class="tabledata" >0.0176 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H7AA</td><td class="tabledata" >0.0946</td><td class="tabledata" >0.0932</td><td class="tabledata" >0.4719</td><td class="tabledata" >0.021*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C8A</td><td class="tabledata" >0.0401 (4)</td><td class="tabledata" >0.08749 (15)</td><td class="tabledata" >0.60549 (14)</td><td class="tabledata" >0.0234 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H8AA</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0277</td><td class="tabledata" >0.0498</td><td class="tabledata" >0.5805</td><td class="tabledata" >0.028*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H8AB</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0309</td><td class="tabledata" >0.1000</td><td class="tabledata" >0.6468</td><td class="tabledata" >0.028*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C9A</td><td class="tabledata" >0.2355 (4)</td><td class="tabledata" >0.06120 (16)</td><td class="tabledata" >0.62705 (15)</td><td class="tabledata" >0.0246 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H9AA</td><td class="tabledata" >0.2249</td><td class="tabledata" >0.0184</td><td class="tabledata" >0.6558</td><td class="tabledata" >0.030*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H9AB</td><td class="tabledata" >0.3003</td><td class="tabledata" >0.0979</td><td class="tabledata" >0.6545</td><td class="tabledata" >0.030*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C10A</td><td class="tabledata" >0.3474 (4)</td><td class="tabledata" >0.04425 (15)</td><td class="tabledata" >0.56176 (15)</td><td class="tabledata" >0.0240 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H10A</td><td class="tabledata" >0.4751</td><td class="tabledata" >0.0300</td><td class="tabledata" >0.5749</td><td class="tabledata" >0.029*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H10B</td><td class="tabledata" >0.2883</td><td class="tabledata" >0.0049</td><td class="tabledata" >0.5362</td><td class="tabledata" >0.029*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C11A</td><td class="tabledata" >0.1886 (4)</td><td class="tabledata" >0.40020 (15)</td><td class="tabledata" >0.45793 (15)</td><td class="tabledata" >0.0224 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >Cl1B</td><td class="tabledata" >0.70385 (9)</td><td class="tabledata" >0.13065 (3)</td><td class="tabledata" >0.38275 (3)</td><td class="tabledata" >0.02102 (15)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C11B</td><td class="tabledata" >0.6923 (5)</td><td class="tabledata" >0.43786 (17)</td><td class="tabledata" >0.29294 (17)</td><td class="tabledata" >0.0364 (8)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >F4</td><td class="tabledata" >0.5910 (12)</td><td class="tabledata" >0.4539 (3)</td><td class="tabledata" >0.2403 (5)</td><td class="tabledata" >0.0226 (12)*</td><td class="tabledata" >0.351 (7)</td></tr><tr><td class="tabledata" >F5</td><td class="tabledata" >0.6856 (18)</td><td class="tabledata" >0.4849 (5)</td><td class="tabledata" >0.3431 (5)</td><td class="tabledata" >0.0241 (10)*</td><td class="tabledata" >0.351 (7)</td></tr><tr><td class="tabledata" >F6</td><td class="tabledata" >0.8935 (10)</td><td class="tabledata" >0.4523 (3)</td><td class="tabledata" >0.2682 (4)</td><td class="tabledata" >0.0163 (15)*</td><td class="tabledata" >0.351 (7)</td></tr><tr><td class="tabledata" >F4B</td><td class="tabledata" >0.7521 (16)</td><td class="tabledata" >0.4863 (4)</td><td class="tabledata" >0.3361 (5)</td><td class="tabledata" >0.0226 (12)*</td><td class="tabledata" >0.189 (5)</td></tr><tr><td class="tabledata" >F5B</td><td class="tabledata" >0.716 (2)</td><td class="tabledata" >0.4505 (6)</td><td class="tabledata" >0.2289 (7)</td><td class="tabledata" >0.041 (4)*</td><td class="tabledata" >0.189 (5)</td></tr><tr><td class="tabledata" >F6B</td><td class="tabledata" >0.4747 (12)</td><td class="tabledata" >0.4605 (4)</td><td class="tabledata" >0.2919 (6)</td><td class="tabledata" >0.021 (2)*</td><td class="tabledata" >0.189 (5)</td></tr><tr><td class="tabledata" >F4C</td><td class="tabledata" >0.8220 (14)</td><td class="tabledata" >0.4554 (3)</td><td class="tabledata" >0.2541 (5)</td><td class="tabledata" >0.025 (2)*</td><td class="tabledata" >0.288 (9)</td></tr><tr><td class="tabledata" >F5C</td><td class="tabledata" >0.6978 (15)</td><td class="tabledata" >0.4818 (5)</td><td class="tabledata" >0.3569 (5)</td><td class="tabledata" >0.0241 (10)*</td><td class="tabledata" >0.288 (9)</td></tr><tr><td class="tabledata" >F6C</td><td class="tabledata" >0.5245 (14)</td><td class="tabledata" >0.4566 (3)</td><td class="tabledata" >0.2635 (5)</td><td class="tabledata" >0.027 (2)*</td><td class="tabledata" >0.288 (9)</td></tr><tr><td class="tabledata" >F4D</td><td class="tabledata" >0.639 (2)</td><td class="tabledata" >0.4462 (6)</td><td class="tabledata" >0.2155 (8)</td><td class="tabledata" >0.0226 (12)*</td><td class="tabledata" >0.167 (6)</td></tr><tr><td class="tabledata" >F5D</td><td class="tabledata" >0.619 (2)</td><td class="tabledata" >0.4824 (6)</td><td class="tabledata" >0.3297 (7)</td><td class="tabledata" >0.0241 (10)*</td><td class="tabledata" >0.167 (6)</td></tr><tr><td class="tabledata" >F6D</td><td class="tabledata" >0.866 (2)</td><td class="tabledata" >0.4612 (8)</td><td class="tabledata" >0.2826 (8)</td><td class="tabledata" >0.029 (4)*</td><td class="tabledata" >0.167 (6)</td></tr><tr><td class="tabledata" >N1B</td><td class="tabledata" >0.8534 (3)</td><td class="tabledata" >0.15394 (12)</td><td class="tabledata" >0.20979 (12)</td><td class="tabledata" >0.0178 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >N2B</td><td class="tabledata" >0.5654 (3)</td><td class="tabledata" >0.20191 (12)</td><td class="tabledata" >0.16508 (12)</td><td class="tabledata" >0.0189 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C1B</td><td class="tabledata" >0.6915 (3)</td><td class="tabledata" >0.21978 (14)</td><td class="tabledata" >0.35477 (14)</td><td class="tabledata" >0.0183 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C2B</td><td class="tabledata" >0.6998 (3)</td><td class="tabledata" >0.27234 (15)</td><td class="tabledata" >0.40623 (14)</td><td class="tabledata" >0.0200 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2BA</td><td class="tabledata" >0.7062</td><td class="tabledata" >0.2599</td><td class="tabledata" >0.4535</td><td class="tabledata" >0.024*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C3B</td><td class="tabledata" >0.6985 (4)</td><td class="tabledata" >0.34360 (15)</td><td class="tabledata" >0.38604 (15)</td><td class="tabledata" >0.0230 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H3BA</td><td class="tabledata" >0.7045</td><td class="tabledata" >0.3797</td><td class="tabledata" >0.4197</td><td class="tabledata" >0.028*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C4B</td><td class="tabledata" >0.6883 (4)</td><td class="tabledata" >0.36098 (15)</td><td class="tabledata" >0.31531 (15)</td><td class="tabledata" >0.0226 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C5B</td><td class="tabledata" >0.6763 (3)</td><td class="tabledata" >0.30779 (14)</td><td class="tabledata" >0.26472 (14)</td><td class="tabledata" >0.0204 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H5BA</td><td class="tabledata" >0.6687</td><td class="tabledata" >0.3205</td><td class="tabledata" >0.2176</td><td class="tabledata" >0.024*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C6B</td><td class="tabledata" >0.6756 (3)</td><td class="tabledata" >0.23534 (14)</td><td class="tabledata" >0.28350 (13)</td><td class="tabledata" >0.0167 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C7B</td><td class="tabledata" >0.6615 (3)</td><td class="tabledata" >0.17660 (14)</td><td class="tabledata" >0.22863 (14)</td><td class="tabledata" >0.0181 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H7BA</td><td class="tabledata" >0.5927</td><td class="tabledata" >0.1355</td><td class="tabledata" >0.2477</td><td class="tabledata" >0.022*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C8B</td><td class="tabledata" >0.8473 (4)</td><td class="tabledata" >0.09305 (15)</td><td class="tabledata" >0.16030 (15)</td><td class="tabledata" >0.0241 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H8BA</td><td class="tabledata" >0.7840</td><td class="tabledata" >0.0524</td><td class="tabledata" >0.1814</td><td class="tabledata" >0.029*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H8BB</td><td class="tabledata" >0.9748</td><td class="tabledata" >0.0785</td><td class="tabledata" >0.1488</td><td class="tabledata" >0.029*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C9B</td><td class="tabledata" >0.7411 (4)</td><td class="tabledata" >0.11657 (15)</td><td class="tabledata" >0.09448 (15)</td><td class="tabledata" >0.0243 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H9BA</td><td class="tabledata" >0.8109</td><td class="tabledata" >0.1544</td><td class="tabledata" >0.0714</td><td class="tabledata" >0.029*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H9BB</td><td class="tabledata" >0.7294</td><td class="tabledata" >0.0764</td><td class="tabledata" >0.0623</td><td class="tabledata" >0.029*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >C10B</td><td class="tabledata" >0.5465 (4)</td><td class="tabledata" >0.14364 (15)</td><td class="tabledata" >0.11302 (16)</td><td class="tabledata" >0.0251 (6)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H10C</td><td class="tabledata" >0.4817</td><td class="tabledata" >0.1613</td><td class="tabledata" >0.0712</td><td class="tabledata" >0.030*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H10D</td><td class="tabledata" >0.4723</td><td class="tabledata" >0.1047</td><td class="tabledata" >0.1322</td><td class="tabledata" >0.030*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O1W</td><td class="tabledata" >0.3328 (3)</td><td class="tabledata" >0.80736 (12)</td><td class="tabledata" >0.43314 (11)</td><td class="tabledata" >0.0258 (5)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >O2W</td><td class="tabledata" >0.1595 (3)</td><td class="tabledata" >0.24257 (12)</td><td class="tabledata" >0.16075 (11)</td><td class="tabledata" >0.0240 (4)</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1NA</td><td class="tabledata" ><span style="font-family:Times">−</span>0.054 (5)</td><td class="tabledata" >0.1675 (17)</td><td class="tabledata" >0.5461 (17)</td><td class="tabledata" >0.034 (9)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2NA</td><td class="tabledata" >0.410 (5)</td><td class="tabledata" >0.0988 (19)</td><td class="tabledata" >0.478 (2)</td><td class="tabledata" >0.046 (11)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1NB</td><td class="tabledata" >0.908 (4)</td><td class="tabledata" >0.1397 (17)</td><td class="tabledata" >0.2501 (17)</td><td class="tabledata" >0.029 (9)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2NB</td><td class="tabledata" >0.457 (5)</td><td class="tabledata" >0.2150 (17)</td><td class="tabledata" >0.1772 (16)</td><td class="tabledata" >0.028 (8)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1W1</td><td class="tabledata" >0.370 (5)</td><td class="tabledata" >0.777 (2)</td><td class="tabledata" >0.402 (2)</td><td class="tabledata" >0.053 (12)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2W1</td><td class="tabledata" >0.440 (5)</td><td class="tabledata" >0.8277 (19)</td><td class="tabledata" >0.4430 (18)</td><td class="tabledata" >0.037 (10)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H1W2</td><td class="tabledata" >0.056 (5)</td><td class="tabledata" >0.2231 (18)</td><td class="tabledata" >0.1680 (18)</td><td class="tabledata" >0.035 (9)*</td><td class="tabledata" ></td></tr><tr><td class="tabledata" >H2W2</td><td class="tabledata" >0.131 (5)</td><td class="tabledata" >0.277 (2)</td><td class="tabledata" >0.1315 (19)</td><td class="tabledata" >0.043 (11)*</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" >Cl1A</td><td class="tabledata" >0.0223 (3)</td><td class="tabledata" >0.0306 (4)</td><td class="tabledata" >0.0199 (3)</td><td class="tabledata" >0.0021 (3)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0001 (2)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0072 (3)</td></tr><tr><td class="tabledata" >F1A</td><td class="tabledata" >0.0535 (11)</td><td class="tabledata" >0.0211 (9)</td><td class="tabledata" >0.0352 (11)</td><td class="tabledata" >0.0018 (8)</td><td class="tabledata" >0.0155 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0009 (8)</td></tr><tr><td class="tabledata" >F2A</td><td class="tabledata" >0.0460 (11)</td><td class="tabledata" >0.0220 (10)</td><td class="tabledata" >0.0606 (14)</td><td class="tabledata" >0.0058 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0230 (10)</td><td class="tabledata" >0.0078 (9)</td></tr><tr><td class="tabledata" >F3A</td><td class="tabledata" >0.0254 (9)</td><td class="tabledata" >0.0295 (10)</td><td class="tabledata" >0.0599 (13)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0107 (7)</td><td class="tabledata" >0.0116 (8)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0090 (9)</td></tr><tr><td class="tabledata" >N1A</td><td class="tabledata" >0.0174 (10)</td><td class="tabledata" >0.0182 (12)</td><td class="tabledata" >0.0192 (11)</td><td class="tabledata" >0.0007 (8)</td><td class="tabledata" >0.0042 (8)</td><td class="tabledata" >0.0018 (9)</td></tr><tr><td class="tabledata" >N2A</td><td class="tabledata" >0.0168 (10)</td><td class="tabledata" >0.0200 (12)</td><td class="tabledata" >0.0180 (12)</td><td class="tabledata" >0.0028 (8)</td><td class="tabledata" >0.0025 (8)</td><td class="tabledata" >0.0027 (9)</td></tr><tr><td class="tabledata" >C1A</td><td class="tabledata" >0.0153 (11)</td><td class="tabledata" >0.0243 (14)</td><td class="tabledata" >0.0188 (13)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0012 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0013 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0022 (11)</td></tr><tr><td class="tabledata" >C2A</td><td class="tabledata" >0.0179 (12)</td><td class="tabledata" >0.0352 (17)</td><td class="tabledata" >0.0146 (13)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0008 (11)</td><td class="tabledata" >0.0013 (10)</td><td class="tabledata" >0.0029 (12)</td></tr><tr><td class="tabledata" >C3A</td><td class="tabledata" >0.0185 (12)</td><td class="tabledata" >0.0286 (16)</td><td class="tabledata" >0.0209 (14)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0020 (10)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0018 (10)</td><td class="tabledata" >0.0100 (12)</td></tr><tr><td class="tabledata" >C4A</td><td class="tabledata" >0.0142 (11)</td><td class="tabledata" >0.0205 (14)</td><td class="tabledata" >0.0232 (14)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0007 (9)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0007 (10)</td><td class="tabledata" >0.0047 (11)</td></tr><tr><td class="tabledata" >C5A</td><td class="tabledata" >0.0152 (11)</td><td class="tabledata" >0.0205 (14)</td><td class="tabledata" >0.0150 (12)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0008 (9)</td><td class="tabledata" >0.0007 (9)</td><td class="tabledata" >0.0005 (10)</td></tr><tr><td class="tabledata" >C6A</td><td class="tabledata" >0.0141 (11)</td><td class="tabledata" >0.0192 (13)</td><td class="tabledata" >0.0155 (12)</td><td class="tabledata" ><span style="font-family:Times">−</span>0.0020 (9)</td><td class="tabledata" ><sp…