reaction probabilities of reaction on the DIMKP PES (upper panel) and the XXZLG PES (lower panel). As discussed in Ref. 41, results of Xu et al. (Ref. 24) on the XXZLG PES have been shifted back by to make a one-to-one comparison with our results.
Final vibrational distribution of the reaction probability of for the DIMKP PES.
Same as Fig. 2 but for the XXZLG PES.
Minimum energy path of the reaction as a function of for the DIMKP and XXZLG PESs.
Convergence of the reaction probabilities as functions of the collision energy for the DIMKP PES (upper panel) and for the XXZLG PES (lower panel). See text for the definition of the sets employed.
Same as Fig. 5 but for the rate coefficients as functions of the temperature.
Rate coefficients of as functions of the temperature.
reaction probability of for the DIMKP PES for different values of the matching distance and the number of hyperspherical channels at different collision energies .
Same as Table I but for the XXZLG PES.
Rate coefficients of in units of for different temperatures.
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