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This topic has been reviewed extensively; see, inter alia (a) Wentrup, C. Top. Curr. Chem. 1976, 62, 173. (b) Jones, W. M. Acc. Chem. Res. 1977, 10, 353. (c) Jones, W. M.; Brinker, U. H. In Pericyclic Reactions; Marchand, A. P., Lehr, A. E., Eds.; Academic: New York, 1977; Vol. 1, Chapter 3. (d) Wentrup, C. In Reactive Intermediates; Ambramovich, R., Ed.; Plenum: New York, 1980; Vol. 1, Chapter 4. (e) Wentrup, C. Reactive Molecules; Wiley-Interscience: New York, 1984; pp 220, 242. (f) Moss, R. A.; Jones, M., Jr. Reactive Intermediates; Wiley: New York, 1985; Vol. 3, p 91. (g) Jones, W. M. In Rearrangements in Ground and Excited States; De Mayo, P., Ed.; Academic: New York, 1980; Vol. 1, Chapter 3. (h) Wentrup, C. In Methoden der Organischen Chemie (Houben-Weyl); Regitz, M., Ed.; Thieme: Stuttgart, 1989; Vol. E19b, p 824 ff.
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6 singlet potential surface on which 1-4 lie has been accurately described by all three of the different sets of calculations.
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38,39 However, the CASPT2-g1/6-31G* relative energies for 1-4 differ very little from the CASPT2N values; so we report only the CASPT2N results.
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85
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85088544115
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note
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1-4 (hartrees): CASSCF(8,8)/6-31G* -268.49785; CASSCF(8,8)/cc-pVDZ -268.51816; CASPT2N/6-31G* -269.31144; CASPT2N/cc-pVDZ -269.34446.
-
-
-
-
117
-
-
85088542930
-
-
note
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2, followed by intersystem crossing and vibrational relaxation, would provide a low energy pathway for the lowest triplet state of 4 to reach the equilibrium geometry of 3.
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