Electronically excited CH radicals have been prepared in chosen vibrational
levels of the A (2)Delta and B (2)Sigma(-) states by selective laser excit
ation. The evolution of the populations in the initial and collisionally pr
oduced vibronic levels has been followed by time- and wavelength-resolved f
luorescence spectroscopy. It is found that CO2, as a model collision partne
r, efficiently promotes the coupling of the A (2)Delta and B (2)Sigma(-) st
ates at room temperature (similar to 295 K). CH A (2)Delta, upsilon = 1 is
reversibly transferred to the near-degenerate B (2)Sigma(-), upsilon = 0 le
vel, and irreversibly vibrationally relaxed to A (2)Delta, upsilon = 0, wit
h comparable probabilities for these competing processes. CH B(2)Sigma(-),
upsilon = 0 is correspondingly reversibly transferred to A (2)Delta, upsilo
n = 1 and irreversibly transferred to A (2)Delta, upsilon = 0. The branchin
g ratio for these two product vibrational states is ca. 2:1, which contrast
s markedly with the predictions of energy-gap scaling laws. The A (2)Delta,
upsilon = 0 level is found to be only weakly quenched by CO2, in agreement
with previous measurements. These observations have important consequences
for the use of laser-induced fluorescence spectroscopy as a tool for monit
oring the density of CH in collisional environments, and in the interpretat
ion of previously measured quenching rate constants for electronically exci
ted CH.