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For detailed discussions of artifactual symmetry breaking in similar molecules, see: Davidson, E.R.; Borden, W.T. J. Phys. Chem. 1983, 87, 4783.
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Jahn, H.A.; Teller, E. Proc. R. Soc. London, Ser. A 1937, 116, 605.
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36
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33845283002
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1987, 109, 5217
-
See for example (a) Schmidt, M.W.; Truong, P.N.; Gordon, M.S. 1987, 109, 5217.
-
-
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Schmidt, M.W.1
Truong, P.N.2
Gordon, M.S.3
-
38
-
-
0011157010
-
-
note
-
. reaction.
-
-
-
-
39
-
-
0011156851
-
-
note
-
y.
-
-
-
-
40
-
-
0011156650
-
-
note
-
3 would decrease. Therefore, with inclusion of overlap in the normalization, the weight of the first configuration in eqs 11 and 12 would be larger than the weight of the second configuration; and the combined weights of the last two configurations would have an intermediate value. Consequently, when overlap is significant, constraining the weights of the configurations in eqs 11 and 12 to be equal disadvantages these doublet wave functions, relative to the quartet, by making the doublets overall slightly antibonding, rather than nonbonding.
-
-
-
-
41
-
-
0011223598
-
-
note
-
.- are allowed to pyramidalize, which lowers the energy of the radical anion by 0.4 kcal/mol, and gives EA = 5.7 kcal/mol.
-
-
-
-
42
-
-
0011193066
-
-
note
-
s geometry with the two equivalent silyls pyramidalized in the opposite direction than the third. The energy of this doublet was computed to be 0.2 kcal/mol lower than that of the fully optimized quartet.
-
-
-
-
43
-
-
0011157193
-
-
note
-
.+ was essentially unchanged.
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-
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