Table 1 .
Geometry (Å, degree) |
ΔEBS b | Net Spin c |
||||||||
---|---|---|---|---|---|---|---|---|---|---|
Fe-N(H93) | Fe-O1 | O1-O2 | ∠FeO1O2 | O2⋯Nε(H64) | O2⋯O341 | Fe | O1 | O2 | ||
Hlink-Fixed d | 2.01 | 1.79 | 1.32 | 117.7 | 2.85 | 2.85 | 0.0 | 0.71 | −0.32 | −0.40 |
Full-Opt. e | 2.02 | 1.80 | 1.32 | 117.3 | 2.87 | 2.84 | −1.1 | 0.73 | −0.33 | −0.41 |
Exp. | 2.07 | 1.83 | 1.21 | 115.6 | 2.77 | 1.47 |
The initial geometry of the oxymyoglobin (oxyMb) active site model cluster is taken from the X-ray crystal structure 1MBO,31 which is also given here as the experimental (Exp.) data for comparison.
Relative calculated broken-symmetry state energies in kcal mol−1.
The Mulliken net spin populations (number of unpaired electrons) on Fe, O1, and O2.
During geometry optimization, the positions of the Hlink atoms (replacing the Cα atoms) on His93 and His64 side chains are fixed.
The geometry of the model cluster is fully optimized without constraint.