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Small Curvature Semiclassical Adiabatic

Hancock et al. [1989] used a version of the small curvature semiclassical adiabatic approach introduced by Truhlar et al. [1982] to calculate the temperature dependence of the rate constant, as shown in Figure 6.29. Variations in k(T) below the crossover point (25-30 K) are due to changes in the prefactor due to zero-point vibrations of the H atom in the crystal. Obviously, the gas-phase model does not take these into account. The absolute values of the rate constant differ by 1-2 orders of magnitude from the experimental ones for the same reason. [Pg.208]

Renormalized Davidson correction, 137 Small Curvature Semiclassical Adiabatic Thermodynamical cycle, 382 Variable metric optimization method, 321... [Pg.222]


See other pages where Small Curvature Semiclassical Adiabatic is mentioned: [Pg.392]    [Pg.250]    [Pg.204]    [Pg.392]    [Pg.291]    [Pg.36]    [Pg.39]    [Pg.79]    [Pg.195]    [Pg.232]    [Pg.204]    [Pg.392]    [Pg.250]    [Pg.204]    [Pg.392]    [Pg.291]    [Pg.36]    [Pg.39]    [Pg.79]    [Pg.195]    [Pg.232]    [Pg.204]    [Pg.284]    [Pg.421]    [Pg.194]    [Pg.386]    [Pg.388]   


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Small-curvature semiclassical adiabatic ground

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