Ck~sical trajectory cakuk~tions for the collinea\_r H+H2 exchange reaction weie performed QSiIIg the same poten-. ## I&J merg surface pretiou+ly adopted for exact quantum mechanical calculationr Reactions of bath sound state amjv-ibrationdy excited aate reagent were wwidered, over a relative kine
Comparison of semi-classical, exact quantum, and quasi-classical reactive transition probabilities for the collinear H + H2 reaction
โ Scribed by J.M. Bowman; Aron Kuppermann
- Publisher
- Elsevier Science
- Year
- 1973
- Tongue
- English
- Weight
- 421 KB
- Volume
- 19
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
The classical (CSC), prirnitive (PSC), md uniform (USC) semi-Jassical expressions for reactive transition probabilities of Miller and co-workers have been used to obtain reaction probabilities for the collinear H + Hz exchange reaction. Comparisons with exact quantum results for the 0 4 0 transition reveal that these semi-classical approximations are not very good, especially the CSC and PSC ones. The USC resL:lts are better, but the quasi-classical trajectcry resu!ts give in average a mole accurate description. For this transition, the extra effort required in going from the quasiclassical to the sc~~&~sicai probabilities did not produce an improvement in the results. For the O-1 reactive transition the' USC calculations are I:-. fairly good qualitative ngrcrmen t with the exact quantum results except for an up ward shift of 0.08 eY in the effective threshold cncrgy. They are somewhat better than the microscopically reversed quasi-classical ones.
๐ SIMILAR VOLUMES
Exact quantum mechanical transition probabilities have been calculated for the collinear reaction H f Fzfu = 0) + HF(u' < 11) + F by the state path sum method\_ The "best" extended LEPS surface of Jonathan et al. has been used. The results are in good agreemeat with experimental results and threedim
This work presents a quantum mechanical numerical study of the reactions F + H 2 (v = 0, j = 0-4) ~ HF + H carried out on the T5A potential energy surface. The calculations were performed within the Jz approximation and employed negative imaginary potentials, yielding state-selected cross sections a