197171-55-4Relevant academic research and scientific papers
Neutron diffraction study of the 'elongated' molecular dihydrogen complex [(C5Me5)Os(H2)H2(PPh 3)]+
Gross, Christopher L.,Young, Dianna M.,Schultz, Arthur J.,Girolami, Gregory S.
, p. 3081 - 3082 (1997)
Protonation of the osmium(IV) hydrides (C5Me5)OsH3(L) with HBF4 in diethyl ether afforded the cationic dihydrogen complexes [(C5Me5)Os(H2)H2(L)][BF 4], where L is PPh3 1 or AsPh3 2; a single-crystal neutron diffraction study of 1 reveals that the H-H distance is 1.014(11) A.
Synthesis and NMR studies of [(C5Me5)Os(L)H 2(H2)+] complexes. Evidence of the adoption of different structures by a dihydrogen complex in solution and the solid state
Gross, Christopher L.,Girolami, Gregory S.
, p. 1658 - 1664 (2008/10/09)
Protonation of the osmium(IV) trihydrides (C5Me 5)OsH3(L) with HBF4 in diethyl ether affords the molecular dihydrogen complexes [(C5Me5)Os(H 2)H2(L)][BF4], where L is PPh3 (1), AsPh3 (2), or PCy3 (3). Ruthenium analogues of these species are not stable and instead lose H2 readily. These compounds adopt four-legged piano-stool geometries in which the phosphine ligand is trans to an elongated dihydrogen ligand. For 1 and 2, the coordinated H2 ligand is oriented with its H-H vector nearly parallel with the Os-Ct vector, where Ct is the centroid of the C5Me 5 ring; in contrast, in 3 the H2 ligand is oriented with its H-H vector perpendicular to the Os-Ct vector. In the 1H NMR spectra, exchange between the Os-H and Os-H2 environments can be slowed at low temperatures for the arsine complex 2 (but not for 1 or 3), and separate resonances could be observed for the hydride and dihydrogen sites; the barrier for exchange is approximately 6.0 kcal/mol. Partially deuterated samples were prepared, and H-H distances within the bound H2 ligands were deduced from the observed 1JHD(av) coupling constants. In addition, H-H distances were deduced from the T1(min) values for the osmium-bound hydrogen atoms, after correction for exchange and ligand-induced dipolar relaxation effects. In all cases, the two solution measurements were in agreement but differed from that deduced from neutron diffraction data. Specifically, for 1 the solution data gave a distance of ca. 1.07 vs 1.01 A in the solid state; similarly, for 2 the solution value of ca. 1.15 A was longer than the 1.08 A value seen in the solid state. In both cases, the ～0.06 A lengthening in solution, if real, is the result most likely of one or both of two factors: the effect of removing the BF 4 counterion from the vicinity of the cation and the effect of librational motion that tends to shorten artificially H-H distances deduced from neutron diffraction data. In contrast, for 3 the solution H-H distance of ca. 1.12 A is significantly shorter than the 1.31 A distance determined from the neutron diffraction data. DFT calculations support the hypothesis that different structures are adopted by 3 in solution and in the solid state and that in solution an equilibrium is established between two dihydrogen-dihydride structures, one with a considerably shorter H-H bond than is seen in the solid state.
