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Volumn 1, Issue 24, 1999, Pages 5555-5563

Spin-forbidden dehydrogenation of methoxy cation: A statistical view

Author keywords

[No Author keywords available]

Indexed keywords

CATION; DEUTERIUM; ISOTOPE;

EID: 0033572562     PISSN: 14639076     EISSN: None     Source Type: Journal    
DOI: 10.1039/a907723e     Document Type: Article
Times cited : (294)

References (88)
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    • As mentioned below, there is in fact an analytical PES available for the singlet system (see ref. 32). However, from the way this surface was constructed, it is unlikely to be truly global, in that it probably does not describe the regions close to the triplet methoxy minimum very accurately
    • 2 As mentioned below, there is in fact an analytical PES available for the singlet system (see ref. 32). However, from the way this surface was constructed, it is unlikely to be truly global, in that it probably does not describe the regions close to the triplet methoxy minimum very accurately.
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    • and references cited therein
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    • 6 J. C. Tully, J. Chem. Phys., 1990, 93, 1061, and references cited therein. See also M. S. Topaler, M. D. Hack, T. C. Allison, Y.-P. Liu, S. L. Mielke, D. W. Schwenke and D. G. Truhlar, J. Chem. Phys., 1997, 106, 8699; Y. L. Volobuev, M. D. Hack and D. G. Truhlar, J. Phys. Chem. A, 1999, 103, 6225.
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    • 7 For reviews on statistical rate theories, see, e.g., (a) W. Forst, Theory of Unimolecular Reactions, Academic Press, New York, 1973;
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    • The work described in ref. 9 also uses ab initio calculations to determine the parameters needed for applying a non-adiabatic statistical rate theory. Our approach, developed before publication of these papers, is very similar except for the point discussed below in ref. 21
    • 10 The work described in ref. 9 also uses ab initio calculations to determine the parameters needed for applying a non-adiabatic statistical rate theory. Our approach, developed before publication of these papers, is very similar except for the point discussed below in ref. 21.
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    • 16 For studies of reaction mechanisms involving conical intersections, see e.g. M. Garavelli, B. Frabboni, M. Fato, P. Celani, F. Bernardi, M. A. Robb and M. Olivucci, J. Am. Chem. Soc., 1999, 121, 1537; D. R. Yarkony, Acc. Chem. Res., 1998, 31, 511; F. Bernardi, M. Olivucci and M. A. Robb, Chem. Soc. Rev., 1996, 321.
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    • 16 For studies of reaction mechanisms involving conical intersections, see e.g. M. Garavelli, B. Frabboni, M. Fato, P. Celani, F. Bernardi, M. A. Robb and M. Olivucci, J. Am. Chem. Soc., 1999, 121, 1537; D. R. Yarkony, Acc. Chem. Res., 1998, 31, 511; F. Bernardi, M. Olivucci and M. A. Robb, Chem. Soc. Rev., 1996, 321.
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    • note
    • 2 MECP studied in ref. 9, where only real frequencies are obtained. This is only by chance, however.
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    • The values reported in ref. 1 are in each case the magnitude of the two identical non-zero singlet-triplet matrix elements, which explains the apparent difference with the rms values mentioned here
    • 25 The values reported in ref. 1 are in each case the magnitude of the two identical non-zero singlet-triplet matrix elements, which explains the apparent difference with the rms values mentioned here.
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    • 27 For an example of an RRKM calculation using anharmonic vibrational energy levels, see K. M. Christoffel and J. M. Bowman, J. Phys. Chem. A, 1999, 103, 3020.
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    • Cambridge University Press, Cambridge, UK, ch. 5, and references therein
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    • 35 R. Schinke, Photodissociation Dynamics, Cambridge University Press, Cambridge, UK, 1993, ch. 5, and references therein. Also see R. Schinke, J. Phys. Chem., 1988, 92, 3195.
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    • note
    • + minimum. The KER results are derived from the remaining 341 (333) trajectories.


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