A Route to Carbasugar Analogues - Jonathan Clayden - The ...

A Route to Carbasugar Analogues - Jonathan Clayden - The ... A Route to Carbasugar Analogues - Jonathan Clayden - The ...

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04.11.2014 Views

C42 0.072(7) 0.028(5) 0.057(6) 0.013(5) -0.011(5) 0.009(5) C43 0.071(7) 0.010(4) 0.050(6) 0.002(4) 0.001(5) 0.000(4) C44 0.065(6) 0.030(5) 0.031(5) 0.000(4) -0.003(4) -0.011(4) C45 0.023(4) 0.018(4) 0.024(4) -0.001(3) 0.003(3) -0.002(3) C46 0.021(4) 0.021(4) 0.033(5) 0.006(4) -0.004(4) -0.003(3) C47 0.034(5) 0.016(4) 0.037(5) -0.008(4) -0.003(4) -0.001(3) C48 0.020(4) 0.042(5) 0.031(5) -0.013(4) 0.003(4) -0.011(4) C49 0.029(5) 0.033(5) 0.020(4) 0.003(4) 0.006(3) -0.011(4) C50 0.018(4) 0.021(4) 0.034(4) 0.002(4) 0.004(3) -0.008(3) N1 0.026(4) 0.018(3) 0.019(3) 0.005(3) 0.001(3) -0.003(3) N2 0.029(4) 0.015(3) 0.021(3) 0.000(3) -0.003(3) -0.003(3) O1 0.038(3) 0.015(3) 0.027(3) 0.007(2) -0.011(2) -0.007(2) O2 0.020(3) 0.016(3) 0.029(3) -0.002(2) -0.004(2) -0.004(2) O3 0.021(3) 0.019(3) 0.020(3) 0.006(2) 0.000(2) -0.008(2) O4 0.026(3) 0.015(3) 0.031(3) 0.005(2) 0.003(2) 0.001(2) O5 0.018(3) 0.021(3) 0.028(3) 0.001(2) -0.008(2) 0.001(2) O6 0.018(3) 0.021(3) 0.024(3) 0.000(2) 0.002(2) -0.001(2) _geom_special_details All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. 315

loop_ _geom_bond_atom_site_label_1 _geom_bond_atom_site_label_2 _geom_bond_distance _geom_bond_site_symmetry_2 _geom_bond_publ_flag C1 N1 1.281(8) . ? C1 O1 1.361(7) . ? C1 C4 1.535(9) . ? C2 O1 1.474(7) . ? C2 C14 1.523(9) . ? C2 C3 1.530(8) . ? C2 H2 1.0000 . ? C3 N1 1.476(8) . ? C3 C20 1.501(9) . ? C3 H3 1.0000 . ? C4 C9 1.519(8) . ? C4 C10 1.521(9) . ? C4 C5 1.570(9) . ? C5 C6 1.513(8) . ? C5 C11 1.544(8) . ? C5 H5 1.0000 . ? C6 O2 1.443(7) . ? C6 C7 1.514(8) . ? C6 H6 1.0000 . ? C7 O3 1.459(6) . ? C7 C8 1.488(9) . ? C7 H7 1.0000 . ? C8 C9 1.310(9) . ? C8 H8 0.9500 . ? C9 H9 0.9500 . ? C10 H10A 0.9800 . ? C10 H10B 0.9800 . ? C10 H10C 0.9800 . ? C11 C13 1.504(9) . ? C11 C12 1.546(8) . ? C11 H11 1.0000 . ? C12 H12A 0.9800 . ? C12 H12B 0.9800 . ? C12 H12C 0.9800 . ? C13 H13A 0.9800 . ? C13 H13B 0.9800 . ? C13 H13C 0.9800 . ? C14 C15 1.373(9) . ? C14 C19 1.376(9) . ? C15 C16 1.407(10) . ? C15 H15 0.9500 . ? C16 C17 1.365(10) . ? C16 H16 0.9500 . ? C17 C18 1.372(10) . ? C17 H17 0.9500 . ? C18 C19 1.420(10) . ? C18 H18 0.9500 . ? C19 H19 0.9500 . ? C20 C25 1.381(8) . ? C20 C21 1.402(9) . ? C21 C22 1.367(9) . ? C21 H21 0.9500 . ? C22 C23 1.388(9) . ? C22 H22 0.9500 . ? C23 C24 1.398(9) . ? C23 H23 0.9500 . ? C24 C25 1.393(9) . ? C24 H24 0.9500 . ? C25 H25 0.9500 . ? C26 N2 1.280(8) . ? C26 O4 1.353(8) . ? C26 C29 1.520(9) . ? C27 O4 1.477(7) . ? C27 C39 1.519(9) . ? C27 C28 1.529(9) . ? C27 H27 1.0000 . ? C28 N2 1.482(8) . ? C28 C45 1.504(9) . ? C28 H28 1.0000 . ? C29 C34 1.523(9) . ? 316

C42 0.072(7) 0.028(5) 0.057(6) 0.013(5) -0.011(5) 0.009(5)<br />

C43 0.071(7) 0.010(4) 0.050(6) 0.002(4) 0.001(5) 0.000(4)<br />

C44 0.065(6) 0.030(5) 0.031(5) 0.000(4) -0.003(4) -0.011(4)<br />

C45 0.023(4) 0.018(4) 0.024(4) -0.001(3) 0.003(3) -0.002(3)<br />

C46 0.021(4) 0.021(4) 0.033(5) 0.006(4) -0.004(4) -0.003(3)<br />

C47 0.034(5) 0.016(4) 0.037(5) -0.008(4) -0.003(4) -0.001(3)<br />

C48 0.020(4) 0.042(5) 0.031(5) -0.013(4) 0.003(4) -0.011(4)<br />

C49 0.029(5) 0.033(5) 0.020(4) 0.003(4) 0.006(3) -0.011(4)<br />

C50 0.018(4) 0.021(4) 0.034(4) 0.002(4) 0.004(3) -0.008(3)<br />

N1 0.026(4) 0.018(3) 0.019(3) 0.005(3) 0.001(3) -0.003(3)<br />

N2 0.029(4) 0.015(3) 0.021(3) 0.000(3) -0.003(3) -0.003(3)<br />

O1 0.038(3) 0.015(3) 0.027(3) 0.007(2) -0.011(2) -0.007(2)<br />

O2 0.020(3) 0.016(3) 0.029(3) -0.002(2) -0.004(2) -0.004(2)<br />

O3 0.021(3) 0.019(3) 0.020(3) 0.006(2) 0.000(2) -0.008(2)<br />

O4 0.026(3) 0.015(3) 0.031(3) 0.005(2) 0.003(2) 0.001(2)<br />

O5 0.018(3) 0.021(3) 0.028(3) 0.001(2) -0.008(2) 0.001(2)<br />

O6 0.018(3) 0.021(3) 0.024(3) 0.000(2) 0.002(2) -0.001(2) _geom_special_details<br />

All esds (except the esd in the dihedral angle between two l.s. planes)<br />

are estimated using the full covariance matrix. <strong>The</strong> cell esds are taken<br />

in<strong>to</strong> account individually in the estimation of esds in distances, angles<br />

and <strong>to</strong>rsion angles; correlations between esds in cell parameters are only<br />

used when they are defined by crystal symmetry. An approximate (isotropic)<br />

treatment of cell esds is used for estimating esds involving l.s. planes.<br />

315

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