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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
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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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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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note
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2 MECP studied in ref. 9, where only real frequencies are obtained. This is only by chance, however.
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63
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20 See, e.g. refs. 8a-c,e,h; (a) A. J. Lorquet, J. C. Lorquet and W. Forst, Chem. Phys., 1980, 51, 253;
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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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72
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26 L. A. Curtiss, K. Raghavachari, P. C. Redfern, V. Rassolov and J. A. Pople, J. Chem. Phys., 1998, 109, 7764.
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73
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0000090271
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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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31 For a discussion of such cases, see L. Salem and C. Rowland, Angew. Chem., Int. Ed. Engl., 1972, 11, 92.
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32 T. G. Lee, S. C. Park and M. S. Kim, J. Chem. Phys., 1996, 104, 4517, see also Y. M. Rhee, T. G. Lee, S. C. Park and M. S. Kim, J. Chem. Phys., 1997, 106, 1003.
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32 T. G. Lee, S. C. Park and M. S. Kim, J. Chem. Phys., 1996, 104, 4517, see also Y. M. Rhee, T. G. Lee, S. C. Park and M. S. Kim, J. Chem. Phys., 1997, 106, 1003.
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33 Gamess-USA (version of 1st December 1998), M. W. Schmidt, K. K. Baldridge, J. A. Boatz, S. T. Elbert, M. S. Gordon, J. H. Jensen, S. Koseki, N. Matsunaga, K. A. Nguyen, S. J. Su and T. L. Windus together with M. Dupuis and J. A. Montgomery, J. Comput. Chem., 1993, 14, 1347.
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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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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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0008925325
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note
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+ minimum. The KER results are derived from the remaining 341 (333) trajectories.
-
-
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