Nascent rotational and vibrational distributions in 16OH and 18OH produced in the reaction of O(1D) with H2 18O
โ Scribed by Nobuaki Tanaka; Masao Takayanagi; Ichiro Hanazaki
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 445 KB
- Volume
- 254
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
Rotational and vibrational state distributions of the OH radicals produced in the reaction 160( I D) "at" H21So ~ x6OH + IsOH have been determined using a laser-induced fluorescence technique. 160(ID) was prepared by the 193 nm photodissociation of N20. The rotational distributions for 16OH and 1sOH in the v = 0 level are characterized by the Boltzmann temperatures of 6000 and 2600 K, respectively. A considerable amount of 16OH exists in the v = 1 state while ~8OH was produced predominantly in the v = 0 state.
๐ SIMILAR VOLUMES
A lower limit to t?re OH(X a 11) vibrational escitation produced by the reaction O(r D) + Ha has been obsewed using a low-pressure infrared chemilumiuescence anoaratus. The O(' D) was generated by laser photolysis of OS\_ The measured \_\* OH(v') vibrational distribution is inverted; it peaks at U'
The cherniluminescence in the H+ 0, -OH(X \*lIIW,& +O, reaction was observed uvng a crossed beam tcebnlqu& l%e tnilial population of the OH radicals tn the vibratIonal slate v (4 < u UG 9) were found to be N( 9) -1.0, N(B) -0.95&O 1, N(7) -0.9kO.2, N(6) -0 2\*0 1 and N(5) -N(4) -0 2&O 2 The IOEII cr
## AbStlWt The nascent OH rovibrational distribution for the reaction CH4\*03+h~266,,,,, + CH3 + OH + Oz are reported. The population ratio betweenthevibrationallevelswasfound tobe u(O)/v( 1) = l.Of0.2 (2a), v( 1)/u(2) =0.67?0.26, and u(2)/u(3) = l.SkO.2; and significant rotational excitation was