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Volumn , Issue , 2005, Pages 549-578

Interpretation of primary kinetic isotope effects for adiabatic and nonadiabatic proton-transfer reactions in a polar environment

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EID: 84870028316     PISSN: None     EISSN: None     Source Type: Book    
DOI: 10.1201/9781420028027     Document Type: Chapter
Times cited : (16)

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    • While these two regimes are distinctly separated, there may exist real systems where different isotopes will be in different regimes. For example, the proton potential barrier at the solvent TS configuration may be small enough such that the proton ground vibration state may be above the barrier, but still large enough such that the deuteron ground vibration state, with a smaller ZPE, may be below the barrier. The present discussion assumes that all isotopes transfer in the same regime.
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    • RXNis defined throughout as the free energy difference between reactant and product H-bond complexes, a free energy difference that is rarely experimentally determined. The full connection to experimentally determined quantities is discussed in Ref. 43 of Ref. 4.
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    • 2O, and while this change in solvent introduces other possible solvent isotope effects (i.e., viscosity), the rate limiting step in each case has been shown to be a PT step (or a series of PT steps), and thus the measured KIE corresponds to PT.
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    • Sis analogous to the electronic diabatic solvent reorganization energy. Even though the reorganization energies and couplings are analogous, the physical picture behind the two reaction types is quite different. The reorganization energy for proton tunneling is the free energy difference associated with a Franck-Condon-like excitation (all nuclear and solvent modes other than the proton mode are held fixed) of the ground diabatic proton vibrational state at the equilibrium reactant solvent position to the ground product diabatic proton vibrational state, followed by relaxation along the solvent coordinate to the equilibrium solvent product position (see Figure 21.7d).
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    • Discussion of the influence of bending on these results can be found in Refs. 4 and 5a.
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    • The H-bond vibrational mode is assumed to remain significantly unchanged while the reaction coordinate fluctuates from the 0-0 TS to either the 0-1 or 1 -0 TS.
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    • This is particularly true for H atom transfer reactions because they are weakly coupled to a polar environment, i.e., small reorganization energies (cf. H atom transfer reaction in Ref. 1e).
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    • oare obtained.
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