Cross sections for collisional quenching of CH A 2A, u' =O were measured at 1300 K for a variety of collision partners. A laser pyrolysis/laser fluorescence technique was used, involving rapid heating by a pulsed CO2 laser and direct time decay of fluorescence excited by a pulsed dye laser. Where co
Collisional quenching of NO(A, v' =0) by various gases
β Scribed by Gary D. Greenblatt; A.R. Ravishankara
- Publisher
- Elsevier Science
- Year
- 1987
- Tongue
- English
- Weight
- 432 KB
- Volume
- 136
- Category
- Article
- ISSN
- 0009-2614
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β¦ Synopsis
The rate coefficients for the quenching of NO(A ?Z, u' =0) by NO, N20, H20, 02, SF6, and CO* were measured to be (in units of lo-"' cm3 molecule-' s-l): 2.67k0.41, 3.79f.0.49, 7.8? 1.0, 1.46f0.25, 3.82f0.49, and 4.3OkO.26, respectively. Upper limits for the quenching rate constants by Nz. Ar, Ne, Hz, and CF., were also measured. All experiments were carried out by monitoring the temporal profiles of A 'E, u' = O-+X %, u" = 3 fluorescence after 226 nm pulsed laser excitation of NO( X % ) to NO(A%, u'=O).
π SIMILAR VOLUMES
Rate cocfticicnts for the collisiona! quenching of Of (' a,) by NO and CO, at 2-8 torr and 300 K have been determined. X-NO = (2.48 t 0.23) X lo-" cm3 moleculc~' s-' anzkCOz = (2.56 5 0.12) X IO-" cm3 moleculc~ s-l.
The rate constant for N,(A, v=O) deactivation by H has been measured by monitoring the decrease in the N,(A, v=O) -+N,(X, v=6) emission when H is added to a flow stream containing N\*(A). The value is found to be 5 x lo-" cm3 s-l, with an uncertainty of z 50%.
## Abstract CCl~2~ free radicals were produced by a pulsed dc discharge of CCl~4~ in Ar. Ground electronic state CCl~2~(X) radicals were electronically excited to the A^1^B~1~ (0,4,0) vibronic state with an Nd:YAG laser pumped dye laser at 541.52 nm. Experimental quenching data of excited CCl~2~(A^
## Abstract Electronically excited oxygen atoms O(2^1^__D__~2~) have been generated by the pulsed irradiation of ozone in the Hartleyβband continuum and monitored photoelectrically in absorption by timeβresolved attenuation of atomic resonance radiation at Ξ» = 115.2 nm [O(3^1^__D__~2~Β°) β O(2^1^__D