Reaction of [V(IV)OL(1)(Im)] (H(2)L(1) = S-methyl-3-((2-hydroxyphenyl)methyl)dithiocarbazate) with [V(V)OL(OCH(3))] allows isolation of (ImH)[L(1)OV-(&mgr;-O)-VOL] complexes 2 (H(2)L = H(2)L(2) = S-methyl-3-((5-bromo-2-hydroxyphenyl)methyl)dithiocarbazate) and 3 (H(2)L = H(2)L(1)), one of which (2) has ligand asymmetry not previously known in this type of complex. In the solid state, (ImH)[L(1)OV-(&mgr;-O)-VOL(2)] (2) provides an example of a divanadium(IV,V) compound with a syn angular [V(2)O(3)](3+) core structure that exhibits crystallographically imposed mirror symmetry due to static disorder. Crystals of 2 are orthorhombic, space group Pnma, with a = 10.740(2) Å, b = 18.912(4) Å, c = 17.163(4) Å, and Z = 4. In toluene at room temperature, both 2 and 3 have 8-line EPR spectra, characteristic of trapped-valence structure. When acetonitrile is added to these solutions, the spectra reveal 15-line features with asymmetric distortions that smooth out with the lowering of temperature. This probably has its origin in a solvent-dependent equilibrium involving two magnetically inequivalent structural forms of the divanadium(IV,V) compound, with syn angular and anti linear structures of the [V(2)O(3)](3+) core. Variable temperatures (298-220 K) (51)V NMR spectroscopic studies in solution also support this view. In acetonitrile, both 2 and 3 exhibit an intervalence transfer band in the near-IR region at ca. 970 nm (epsilon, 1600 and 1480 M(-)(1) cm(-)(1) for 2 and 3, respectively) and they undergo one-electron reversible oxidation at ca. 0.40 V (vs SCE) due to the V(IV)V(V)/V(V)V(V) couple.

A method is proposed to estimate the amount of 2/2 contamination inherent in area-detector [charge-coupled device (CCD) or image plate] data using Mo radiation. The intensity increase due to the Mo 2/2 contribution to Ih~ has been determined by measurement of the intensity for reflections where h, k or l is half-integral, i.e. reflections where there is no contribution from 2, for three crystals using two different CCD diffractometers. This information is present in all data sets obtained with area detectors but is usually ignored. The correction thus determined has been applied to nine data sets. The improvement to the data, as measured from the leastsquares refinement, is shown to be insignificant for routine data sets, even for the weak low-angle reflections. Some reduction in the number of 'observed' systematic absences is noted, thus improving space-group assignments. In addition, for strongly diffracting crystals, incorrect unit cells may be obtained owing to the presence of strong 2/2 reflections at the reciprocal-lattice nodes.

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