✍ Scribed by Husain, D.; Kirsch, L. J.
No coin nor oath required. For personal study only.
📜 SIMILAR VOLUMES
Eiectronicalfy excited carbon atoms in the lowest lying singtet state, C(Zf13.$ ~ have been monitored directly by photoelectric measurement of the attenuation of the resonance transition C(VYI~P\* -2lD2) at 193.1 nm. The rate of decay of Lhe atom has been measured in the presence of hydrogen an fd n
EIectronicalJy excited oxygen atoms, O(2lD23, generated by the pulsed irradiatkn of ozone in the Hartley continuum, have been observed by bsorption spectroscopy using time-resolved attenuation of resonance radiation in the vacuum ultra-violet (O(31D2$41(21D ) 2 , h 115.2 nm). The concentration profi
## Abstract Electronically excited oxygen atoms O(2^1^__D__~2~) have been generated by the pulsed irradiation of ozone in the Hartley‐band continuum and monitored photoelectrically in absorption by time‐resolved attenuation of atomic resonance radiation at λ = 115.2 nm [O(3^1^__D__~2~°) → O(2^1^__D
Time-resolved atomic absorption spectroscopy in the vacuum ultraviolet has been employed to monitor electronically excited oxygen atoms, 0(2\*D2), following their generation by the flash photolysis of ozone in the Hartley band region. We report the first values for the absolute second-order rate con