2007
DOI: 10.1007/s12039-007-0036-2
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Lyman-α photodissociation of CH3CFCl2 (HCFC-141b): Quantum yield and translational energy of hydrogen atoms

Abstract: The collision-free, room temperature gas-phase photodissociation dynamics of CH 3 CFCl 2 (HCFC-141b) was studied using Lyman-α laser radiation (121⋅6 nm) by the laser photolysis/laserinduced fluorescence 'pump/probe' technique. Lyman-α radiation was used both to photodissociate the parent molecule and to detect the nascent H atom products via (2p 2 P → 1s 2 S) laser-induced fluorescence. Absolute H atom quantum yield, φ H = (0⋅39 ± 0⋅09) was determined by calibration method in which CH 4 photolysis at 121⋅6 nm… Show more

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“…The laser pulse shape is shown in Fig. ( 6). Many parameters are varied in order to get the optimum conditions for the laser pulse.…”
Section: Resultsmentioning
confidence: 99%
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“…The laser pulse shape is shown in Fig. ( 6). Many parameters are varied in order to get the optimum conditions for the laser pulse.…”
Section: Resultsmentioning
confidence: 99%
“…Hirokozn, 1984. The chain reaction, which is initiated by UV flash using F 2 -H 2 mixture, to achieve (14.6) J/Pluse laser output energy at (0.7 atm) [6].In 1986 A.S.Bashkin, utilized the chain reaction for (D 2 -F 2 ) mixture, using flash lamp.In 1996 B.G.Bravy, utilized the chain reaction for F 2 -H 2 mixture, initiated by flash lamp to get 1KJ output laser energy at total pressure of 0.7 atm, with 50 litter. The beam divergence was 10 -4 rad [10].A ClF and H 2 mixture chain reaction, initiated by using XeCl laser (308 nm), 50 J/  laser energy pulse, was utilized by E.B.…”
Section: Duringmentioning
confidence: 99%
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