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GAUSSIAN 94 (Revision D.4), Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Gill, P. M. W.; Johnson, B. G.; Robb, M. A.; Cheeseman, J. R.; Keith, T.; Petersson, G. A.; Montgomery, J. A.; Raghavachari, K.; Al-Laham, M. A.; Zakrzewski, V. G.; Ortiz, J. V.; Foresman, J. B.; Cioslowski, J.; Stefanov, B. B.; Nanayakkara, A.; Challacombe, M.; Peng, C. Y.; Ayala, P. Y.; Chen, W.; Wong, M. W.; Andres, J. L.; Replogle, E. S.; Gomperts, R.; Martin, R. L.; Fox, D. J.; Binkley, J. S.; Defrees, D. J.; Baker, J.; Stewart, J. P.; Head-Gordon, M.; Gonzalez, C.; Pople, J. A. Gaussian, Inc.: Pittsburgh, PA, 1995.
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note
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Basis sets were obtained from the Extensible Computational Chemistry Environment Basis Set Database, Version 1.0, as developed and distributed by the Molecular Science Computing Facility, Environmental and Molecular Sciences Laboratory, which is part of the Pacific Northwest Laboratory, P.O. Box 999, Richland, WA 99352, USA, and funded by the U.S. Department of Energy. The Pacific Northwest Laboratory is a multiprogram laboratory operated by Battelle Memorial Institue for the U.S. Department of Energy under contract DE-AC06-76RLO 1830. Contact David Feller, Karen Schuchardt, or Don Jones for additional information.
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0343310201
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note
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29 who showed that the perturbation series for the migratory insertion step fails to converge in some systems. Therefore, we restricted our further geometry optimizations to gradient corrected density functionals.
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44
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0342875132
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note
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It should be noted that, if the DFT energetics are correct and ts1 is only 0.1 kcal/mol less stable than e, then applying the steady-state approximation to e would probably not be valid at room temperature. In this case, the reaction is best thought of as being concerted and the calculated activation energy is 19.8 kcal/mol. However, as noted earlier, we think it is more likely that DFT is underestimating this energy difference and that e is a true intermediate.
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45
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0342875133
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note
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It is also possible that the agostic form e is not involved in the migration step at all. We could envision a third channel, in which ts2 is the transition state between the reactant and the dihapto species, which is then attacked by CO. A detailed kinetic analysis of this third channel leads to conclusions essentially identical with those for channel 2.
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46
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0342875134
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note
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It should be noted that if in fact the QCISD energetics more accurately reflect the relative energies of the stationary points, then the dihapto structure is completely inaccessible from the reactant side due to the very high energy of ts2 at this level. In fact, the B3LYP/lb energetics which we have chosen to use in our kinetic and thermodynamic analyses yield the lowest relative energy for ts2 and therefore represent a best-case scenario for the channel 2 mechanism.
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0001204745
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Connor, J. A.; Zafarani-Moattar, M. T.; Bickerton, J.; El Saied, N. I.; Suradi, S.; Carson, R.; Al Takhin; Skinner, H. A. Organometallics 1982, 1, 1166.
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Zafarani-Moattar, M.T.2
Bickerton, J.3
El Saied, N.I.4
Suradi, S.5
Carson, R.6
Al Takhin7
Skinner, H.A.8
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48
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0342440632
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note
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As alluded to earlier, Calderazzo and Cotton assumed that the solvent effects observed were mainly a function of the bulk dielectric constant stabilizing a polar transition state and not specific solvent participation. In fact, the calculated dipole moments of all of the transition states and intermediates are considerably higher than that of the reactant. From the B3P86/sb calculations, we find the following (in Debye): a (0.3), e (3.0), d (3.0), ts1 (2.4), ts2 (2.7) ts3 (2.1), ts4 (3.8), and ts5 (1.0).
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49
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0342875131
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note
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It is thought that photodissociation of b occurs only for carbonyls cis to the acyl group (ref 19).
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50
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0342440633
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note
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In fact, in their first paper (ref 18) Boese and Ford argued that the similarity of the CO frequencies in methylcyclohexane and THF implied that the dihapto form existed in both solvents. Only in their second paper did they use reactivity arguments to conclude that coordinating solvents explicitly solvated the intermediate.
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