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0011338168
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note
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The parameter P depends on the radial wave function of the metal atom in the field of ligands and is usually treated as an adjustable parameter.
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41
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0011294761
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note
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ij elements.
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42
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0011333835
-
-
note
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ij is neither symmetrical nor traceless. See ref 14 for a lucid discussion.
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43
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0011363720
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note
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1.
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44
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0011294450
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note
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Formulas 9.248-9.252 of ref 16 have been derived from (9) and (10), restricting the summation over m to the four MOs with the largest d-orbital contributions. In our calculations, we have therefore chosen the four unoccupied MOs with largest computed metal d character.
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45
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0011337298
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note
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-
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0011324766
-
-
note
-
axial vector. This is not the case for any of the complexes studied here.
-
-
-
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53
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0011368265
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In press
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Kaupp, M.; Reviakine, R.; Malkina, O.L.; Arbuznikov, A.; Schimmelpfennig, B.; Malkin; V.G. J. Comput. Chem. In press.
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0001368303
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56
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0000947958
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and references therein
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See, e.g.: van Lenthe, E.; van der Avoird, A.; Hagen, W.R.; Reijerse, E.J. J. Phys. Chem. A 2000, 104, 2070, and references therein.
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57
-
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0011363721
-
-
note
-
Turning this line of reasoning around, from the theoretical orientations of the principal axes, one can estimate the relative sizes of the individual spin-orbit coupling terms.
-
-
-
-
58
-
-
0011283674
-
-
note
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2.
-
-
-
-
59
-
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0011288858
-
-
note
-
2 symmetry. For the two other complexes, we observe small deviations from the indicated directions, cf. below.
-
-
-
-
60
-
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0011331134
-
-
note
-
For the definition of the asymmetry (rhombicity) parameter, cf. ref 14, p 116.
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-
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61
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0001617097
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Belanzoni, P.; Baerends, E.J.; van Asselt, S.; Langewen, P.B. J. Phys. Chem. 1995, 99, 13094.
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Belanzoni, P.1
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62
-
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0011327325
-
-
note
-
y'x', are zero, because of zero nondiagonal elements of the g tensor (cf. section 2).
-
-
-
-
63
-
-
0011333836
-
-
note
-
We note that the asymmetry of the HFC tensor can be influenced also by mixing of the metal 4s orbital into the SOMO, which is symmetry-allowed. This mixing is not considered in the usual interpretations, cf. refs 12, 15, and 16.
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