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Molecular angular momentum reorientation of electronically excited hydrogen ( B sup 1. Sigma. sup + sub u )

Journal Article · · Journal of Chemical Physics; (USA)
DOI:https://doi.org/10.1063/1.458671· OSTI ID:6424782
;  [1]
  1. Department of Chemistry, University of California, Berkeley, CA (USA)
The room temperature rate constants for molecular angular momentum reorientation of H{sub 2}, HD, and D{sub 2} ({ital B} {sup 1}{Sigma}{sup +}{sub {ital u}}, {ital v}{prime}=0, {ital J}{prime}=1, {ital M}{sub {ital J}{prime}}=0) in collisions with He, Ne, Ar and H{sub 2} ({ital X} {sup 1}{Sigma}{sup +}{sub {ital g}}) have been measured. The effective cross sections for changing {ital M}{sub {ital J}{prime}} in collisions of H{sub 2}, HD, D{sub 2} with He and Ne were found to be about 30 A{sup 2} and were nearly the same for each isotope and with He and Ne as collision partners. The measured He--H{sub 2}({ital B}) reorientation cross section is about 50% larger than the cross section calculated with a simple semiclassical model using a potential that approximates the {ital ab} {ital initio} data for the H{sub 2}({ital B})--He potential energy surface. The cross sections for reorientation of HD and D{sub 2} in collisions with Ar were found to be 10.6{plus minus}2.0 and 13.9{plus minus}3.0 A{sup 2}, respectively. The smaller cross section is due to the dominant role played by quenching of the electronic energy of molecular hydrogen in collisions with Ar. The reorientation of D{sub 2}({ital B}) in collisions with room temperature H{sub 2}({ital X}) occurs with a 7.6{plus minus}3.4 A{sup 2} cross section. The small cross section for reorientation of the angular momentum is again due to the dominance of quenching in the collision dynamics.
OSTI ID:
6424782
Journal Information:
Journal of Chemical Physics; (USA), Journal Name: Journal of Chemical Physics; (USA) Vol. 93:7; ISSN JCPSA; ISSN 0021-9606
Country of Publication:
United States
Language:
English