Binuclear tungsten carbonyl nitrosyls: Comparison with valence isoelectronic Cr2(NO)2(CO)n

Abstract

Density functional theory predicts an unbridged structure for W2(NO)2(CO)8 with a W–W single bond distance of ∼3.2Å analogous to the experimental structures for the isoelectronic species Cr2(NO)2(CO)8 and M2(CO)10 (M=Mn, Tc, Re). The lowest energy structure of the unsaturated W2(NO)2(CO)7 is an unbridged structure linking a W(NO)(CO)4 fragment and a W(NO)(CO)3 fragment through a formal WW double bond similar to Cr2(NO)2(CO)7. For W2(NO)2(CO)6, the lowest energy structure has two bridging CO groups and a WW distance of ∼2.7Å suggesting a formal triple bond. However, an unbridged W2(NO)2(CO)6 structure with a WW triple bond distance of ∼2.8 Å lies within ∼2kcal/mol of this structure suggesting a fluxional system. The energy surface of the even more unsaturated W2(NO)2(CO)5 is more complicated with low energy singlet structures having four-electron donor bridging η2-μ-CO groups, five-electron donor bridging η2-μ-NO groups, or no bridging groups combined with a short WW triple bond distance. The lowest energy structure for the carbonyl-rich W2(NO)2(CO)9 has a bridging NO group and a long ∼4.0 ÅW⋯W distance suggesting the absence of a direct bond. However, loss of CO from W2(NO)2(CO)9 to give W2(NO)2(CO)8 requires only ∼4kcal/mol suggesting that W2(NO)2(CO)9 is not a viable species.