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Crystallographic position Multiplicity

As distinct from the multiple O sites, on the multiple Mg sites (see 10 and 11) the adsorbed H atom bridges all the neighboring Mg atoms, with equal Mg-H bond lengths. Since the characteristic Mg-H bond length is close to the length of the Mg-0 bond, the adsorbed H atom nearly fits the crystallographic position of the extracted O atom at these Mg defect sites. [Pg.137]

The X-ray structure of the dibromine complex with toluene (measured at 123 K) is more complicated, and shows multiple crystallographically independent donor/acceptor moieties [68]. Most important, however, is the fact that in all cases the acceptor shows an over-the-rim location that is similar to that in the benzene complex. In both systems, the acceptor is shifted by 1.4 A from the main symmetry axis, the shortest Br C distances of 3.1 A being significantly less than the sum of the van der Waals radii of 3.55 A [20]. Furthermore, the calculated hapticity in the benzene/Br2 complex (x] = 1.52) is midway between the over-atom (rj = 1.0) and over-bond (rj = 2.0) coordination. In the toluene complex, the latter varies from rj = 1.70 to 1.86 (in four non-equivalent coordination modes) and thus lies closer to the over-bond coordination model. Moreover, the over-bond bromine is remarkably shifted toward the ortho- and para-carbons that correspond to the positions of highest electron density (and lead to the transition states for electrophilic aromatic bromination [12]). Such an experimental location of bromine is in good agreement with the results of high level theoretical... [Pg.156]

Small molecule crystallographers are familiar with these concepts, since it is routine to measure data at low temperature to improve precision by reduction of thermal motion, and structures are often done at multiple temperatures to assess the origins of disorder in atomic positions. Albertsson et al. (1979) have reported the analysis of the crystal structure of Z)(-l-)-tartaric acid at 295, 160, 105, and 35 K. Figure 22 shows the individual isotropic. S-factors for the atoms in the structure at each of these temperatures the smooth variation of B with T is apparent. Below 105 K, B is essentially identical for all atoms and is also temperature independent the value of B = 0.7 agrees well with the expected zero-point vibradonal value. However, even for this simple structure, not all of the atoms show B vs T behavior at high temperature which extrapolates to 0 A at 0 K. [Pg.348]

The clock example illustrates most principles of importance in discrete symmetry groups with translation, also known as crystallographic symmetry groups. For simplicity consider a two-dimensional unit cell with a two-fold axis T, pictured as a pointed ellipse, and two mirror planes my and mu-To construct a multiplication table any general position (not coincident with... [Pg.33]


See other pages where Crystallographic position Multiplicity is mentioned: [Pg.253]    [Pg.186]    [Pg.16]    [Pg.285]    [Pg.115]    [Pg.116]    [Pg.51]    [Pg.187]    [Pg.266]    [Pg.288]    [Pg.322]    [Pg.135]    [Pg.129]    [Pg.131]    [Pg.58]    [Pg.18]    [Pg.66]    [Pg.183]    [Pg.257]    [Pg.8]    [Pg.268]    [Pg.163]    [Pg.187]    [Pg.489]    [Pg.344]    [Pg.213]    [Pg.1021]    [Pg.178]    [Pg.131]    [Pg.177]    [Pg.1126]    [Pg.798]    [Pg.634]    [Pg.60]    [Pg.516]    [Pg.26]    [Pg.343]    [Pg.38]    [Pg.59]    [Pg.228]    [Pg.58]    [Pg.374]    [Pg.56]    [Pg.495]    [Pg.122]    [Pg.508]    [Pg.372]   
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Crystallographic position

Multiplicity, positions

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