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(a) Sodupe, M.; Bauschlicher, C. W. J. Phys. Chem. 1991, 95, 8640. It has been pointed out in this work that it is not always straightforward to differentiate between the electrostatic and covalent bonding based on the character of the wave function. Instead, geometrical changes of the ligand were suggested to be a proper identification of the type of bonding. Indeed, we have found from Mulliken population analysis (TZV+P basis) that the net iron charge is 0.7 for the two open and two cyclic structures.
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4143051974
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note
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(b) Again, the Mulliken net iron charges are rather similar for the sextet and quartet methyl structures, being 0.6 and 0.6-0.7, respectively.
-
-
-
-
50
-
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4143080996
-
-
note
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(c) This can be compared with the net iron charges in the initial complexes of +0.9.
-
-
-
-
51
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33751157557
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The other Hartree-Fock estimates of this splitting reported in the literature are similar; the two recent values are 38.0 kcal/mol (Ricca, A.; Bauschlicher, C. W.; Rosi, M. J. Phys. Chem. 1994, 98, 9498) and 38.9 kcal/mol (Heinemann, C.; Schwarz, J.; Koch, W.; Schwarz, H. J. Chem. Phys. 1995, 103, 4551).
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52
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36448998613
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The other Hartree-Fock estimates of this splitting reported in the literature are similar; the two recent values are 38.0 kcal/mol (Ricca, A.; Bauschlicher, C. W.; Rosi, M. J. Phys. Chem. 1994, 98, 9498) and 38.9 kcal/mol (Heinemann, C.; Schwarz, J.; Koch, W.; Schwarz, H. J. Chem. Phys. 1995, 103, 4551).
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0000440423
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It has been suggested that the relative weight of ω in different electronic states can be a measure of how balanced the calculation is. See, e.g.: Fülscher, M. P.; Andersson, K.; Roos, B. O. J. Phys. Chem. 1992, 96, 9204.
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85086527806
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note
-
6A″ (3b) states are nearly degenerate, so the ordering of the two states may change with improving the theoretical method.
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