TY - JOUR
T1 - Photofragment excitation spectroscopy of the formyl (HCO/DCO) radical
T2 - Linewidths and predissociation rates of the Ã(A″) state
AU - Loison, Jean Christophe
AU - Kable, Scott H.
AU - Houston, Paul L.
AU - Burak, Itamar
PY - 1991
Y1 - 1991
N2 - Photofragment excitation (PHOFEX) spectra of the jet-cooled formyl (HCO and DCO) radical have been measured by monitoring laser-induced fluorescence of the CO fragment. The following Ã(A″)←X̃(A′) vibronic transitions were measured: (ν1,ν2,ν3) ←(0,0,0) where for HCO ν2 = 6-16 with ν1, ν3 = 0; ν2 = 7-12 with ν1 = 1, ν3 = 0; ν2 = 9-12 with ν1 = 0, ν3 = 1 and for DCO ν2 = 14-18 with ν1,ν3 = 0. The PHOFEX technique provides a powerful method for discriminating against strong transitions so as to allow assignment and measurement of many weaker Franck-Condon bands. The linewidths of the diffuse transitions lie in the 16-150 cm-1 (FWHM) range; they increase strongly with K′ (the projection of the total angular momentum onto the a axis) and decrease slightly with ν′2 (the number of HCO/DCO bending quanta). The linewidths are interpreted as radiationless transition rates and yield upper Ã-state lifetimes ranging from 70 to 700 fs. These data are in excellent agreement with a dynamical model of HCO/DCO curve crossing developed by R. N. Dixon [Mol. Phys. 54, 333 (1985)].
AB - Photofragment excitation (PHOFEX) spectra of the jet-cooled formyl (HCO and DCO) radical have been measured by monitoring laser-induced fluorescence of the CO fragment. The following Ã(A″)←X̃(A′) vibronic transitions were measured: (ν1,ν2,ν3) ←(0,0,0) where for HCO ν2 = 6-16 with ν1, ν3 = 0; ν2 = 7-12 with ν1 = 1, ν3 = 0; ν2 = 9-12 with ν1 = 0, ν3 = 1 and for DCO ν2 = 14-18 with ν1,ν3 = 0. The PHOFEX technique provides a powerful method for discriminating against strong transitions so as to allow assignment and measurement of many weaker Franck-Condon bands. The linewidths of the diffuse transitions lie in the 16-150 cm-1 (FWHM) range; they increase strongly with K′ (the projection of the total angular momentum onto the a axis) and decrease slightly with ν′2 (the number of HCO/DCO bending quanta). The linewidths are interpreted as radiationless transition rates and yield upper Ã-state lifetimes ranging from 70 to 700 fs. These data are in excellent agreement with a dynamical model of HCO/DCO curve crossing developed by R. N. Dixon [Mol. Phys. 54, 333 (1985)].
UR - http://www.scopus.com/inward/record.url?scp=0001364980&partnerID=8YFLogxK
U2 - 10.1063/1.459953
DO - 10.1063/1.459953
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AN - SCOPUS:0001364980
SN - 0021-9606
VL - 94
SP - 1796
EP - 1802
JO - The Journal of Chemical Physics
JF - The Journal of Chemical Physics
IS - 3
ER -