Abstract
The interconversion of model compounds {[(NH3)3Cu]2(μ-η2:η2-O2)}2+ (1) and {[(NH3)3Cu]2(μ-O)2}2+ (2) has been examined using multireference second-order perturbation theory with an 8-electron/8-orbital active space. At this level of theory, 1 and 2 are separated by only 0.3 kcal/mol, and the barrier to isomerization is predicted to be very low based on single-point energy calculations for intermediate structures. The flat nature of the potential energy surface along the interconversion coordinate derives from a balancing of Coulomb forces and nondynamic electron correlation. The latter effect depends critically on the significant energy change experienced by the 13a(u) σ(oo)* virtual orbital on passing from one isomer to the other. In addition, solvation electrostatics favor 2 over 1.
Original language | English (US) |
---|---|
Pages (from-to) | 11283-11287 |
Number of pages | 5 |
Journal | Journal of the American Chemical Society |
Volume | 118 |
Issue number | 45 |
DOIs | |
State | Published - Nov 13 1996 |