TY - JOUR
T1 - Chemical lasers produced from O(3P) atom reactions. III. 5‐μm CO laser emission from the O + CH reaction
AU - Lin, Ming-Chang
PY - 1974/1
Y1 - 1974/1
N2 - Very strong laser emission at 5 μm was detected when SO2 and CHBr3 were flash photolyzed in the vacuum ultraviolet (λ ≥ 165 nm) in the presence of a large amount of diluent (SF6, He, or Ar). About 110 vibration–rotation transitions ranging from Δv = 18 → 17 to 3 → 2, except 16 → 15, were identified. The primary reactions leading to the CO stimulated emission are as follows: (Formula Presented.) The product analysis results and the variation of laser intensity with flash energy and SO concentration indicate that the following side reactions (Formula Presented.) are also occurring. Addition of a small amount of O2 enhances the laser output by both eliminating these side reactions and simultaneously producing vibrationally excited CO via reaction (8), (Formula Presented.) which has been previously shown to generate CO stimulated emission. The effects of various reactive (NO and H2) and inert (He, Ar, SF6, CO, N2, N2O, and CO2) gases have been examined. All additives (P ≤ 20 torr), except NO and H2, increase the total laser output. N2O enhances the power most efficiently, whereas CO, N2, and CO2 are less effective and have similar efficiencies. The enhancement of the laser intensity by these near‐resonant gases is ascribed to the depletion of CO population at lower levels which thus increases the rates cascading from higher levels. NO and H2 quench the laser output by chemically reducing the concentration of the CH radical.
AB - Very strong laser emission at 5 μm was detected when SO2 and CHBr3 were flash photolyzed in the vacuum ultraviolet (λ ≥ 165 nm) in the presence of a large amount of diluent (SF6, He, or Ar). About 110 vibration–rotation transitions ranging from Δv = 18 → 17 to 3 → 2, except 16 → 15, were identified. The primary reactions leading to the CO stimulated emission are as follows: (Formula Presented.) The product analysis results and the variation of laser intensity with flash energy and SO concentration indicate that the following side reactions (Formula Presented.) are also occurring. Addition of a small amount of O2 enhances the laser output by both eliminating these side reactions and simultaneously producing vibrationally excited CO via reaction (8), (Formula Presented.) which has been previously shown to generate CO stimulated emission. The effects of various reactive (NO and H2) and inert (He, Ar, SF6, CO, N2, N2O, and CO2) gases have been examined. All additives (P ≤ 20 torr), except NO and H2, increase the total laser output. N2O enhances the power most efficiently, whereas CO, N2, and CO2 are less effective and have similar efficiencies. The enhancement of the laser intensity by these near‐resonant gases is ascribed to the depletion of CO population at lower levels which thus increases the rates cascading from higher levels. NO and H2 quench the laser output by chemically reducing the concentration of the CH radical.
UR - http://www.scopus.com/inward/record.url?scp=84986794824&partnerID=8YFLogxK
U2 - 10.1002/kin.550060102
DO - 10.1002/kin.550060102
M3 - Article
AN - SCOPUS:84986794824
SN - 0538-8066
VL - 6
SP - 1
EP - 14
JO - International Journal of Chemical Kinetics
JF - International Journal of Chemical Kinetics
IS - 1
ER -