LASER-INDUCED PREDISSOCIATIVE FLUORESCENCE - DYNAMICS AND POLARIZATION AND THE EFFECT OF LOWER-STATE ROTATIONAL ENERGY-TRANSFER ON QUANTITATIVE DIAGNOSTICS
Ew. Rothe et al., LASER-INDUCED PREDISSOCIATIVE FLUORESCENCE - DYNAMICS AND POLARIZATION AND THE EFFECT OF LOWER-STATE ROTATIONAL ENERGY-TRANSFER ON QUANTITATIVE DIAGNOSTICS, Applied optics, 35(6), 1996, pp. 934-947
Laser-induced predissociative fluorescence is often used for diagnosti
cs because its short-lived upper states are minimally disturbed by col
lisions. We discuss the effects of lower-state collisions with paramet
ers relevant to our atmospheric H-2-O-2 flame. A pulse of tunable KrF
excimer-laser light induces the A <-- X, Q(1)(11), 3 <-- 0 transition
in OH. We measure the intensity and the polarization of the resulting
A --> X, Q(1)(11), 3 --> 2 fluorescence as a function of laser brightn
ess. A simple model that uses no adjustable parameters produces a reas
onable fit to the data. It predicts that, even at very modest laser en
ergies, the fluorescence intensity is almost directly proportional to
the rate constant for rotational energy transfer (RET) within the lowe
r vibrational state. That rate constant can be a strong function of lo
cal conditions. Furthermore, under typical operating conditions the ex
cimer will pump an amount of OH out of the lower state that is many ti
mes as large as that originally present. This occurs because RET withi
n the X-state continuously replenishes the lower state during the lase
r pulse. Even when this occurs, the signal may still vary linearly wit
h laser intensity, and the polarization may be nearly that expected fo
r weak pumping. At the higher laser intensities, a significant fractio
n of the measured OH arises from two-photon photodissociation of the w
ater from the flame reaction. (C) 1996 Optical Society of America