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How to observe the elusive resonances in H or D + H sub 2 yields H sub 2 or HD + H reactive scattering

Journal Article · · Journal of Physical Chemistry; (USA)
DOI:https://doi.org/10.1021/j100154a007· OSTI ID:5926152
Short-lived collision complexes in H or D + H{sub 2} (v = j = 0) {yields} H{sub 2} or HD ({nu}{prime},j{prime}) + H reactive scattering give rise to broad resonance structure. Though this structure is not observable in the energy dependence of the integral cross section, it is readily seen in the energy dependence in the differential cross section {sigma}({theta},E), as a peak along a line in the E-{theta} plane. The equation of this resonance line is E = E{sub r}(J({theta})), where E{sub r}(J) is the resonance energy as a function of total angular momentum J (i.e., the rotational quantum number of the complex) and J({theta}) is the inverse function of {Theta}(J), the effective classical deflection function for the transition. Observation of this resonance structure requires cross section to individual final ({nu}{prime}, j{prime}) states; it is quenched by summing over j{prime}. The results reported are all from rigorous three-dimensional quantum mechanical reactive scattering calculations for these cross sections.
DOE Contract Number:
AC03-76SF00098
OSTI ID:
5926152
Journal Information:
Journal of Physical Chemistry; (USA), Journal Name: Journal of Physical Chemistry; (USA) Vol. 95:1; ISSN 0022-3654; ISSN JPCHA
Country of Publication:
United States
Language:
English