Collisional energy transfer probabilities of highly excited molecules fromkinetically controlled selective ionization (KCSI). I. The KCSI technique:Experimental approach for the determination of P(E-',E) in the quasicontinuous energy range
U. Hold et al., Collisional energy transfer probabilities of highly excited molecules fromkinetically controlled selective ionization (KCSI). I. The KCSI technique:Experimental approach for the determination of P(E-',E) in the quasicontinuous energy range, J CHEM PHYS, 112(9), 2000, pp. 4076-4089
The method of kinetically controlled selective ionization (KCSI) for invest
igating collisional energy transfer in highly vibrationally excited molecul
es is presented in detail. In this first paper of a series the focus is on
the key concepts and the technical realization of KCSI experiments to provi
de a common basis for following reports on our available results of KCSI st
udies on the vibrational relaxation of a variety of larger molecules. The K
CSI technique directly monitors the energetic position and shape of the pop
ulation distributions g(E,t) during the relaxation process by means of an e
nergy selective two photon ionization process via an electronic intermediat
e state. Such measurements allow-for the first time-to extract complete and
accurate experimental sets of transition probability distributions P(E',E)
even at quasicontinuous densities of states. Basic energy transfer quantit
ies are already obtained from a straightforward analysis of the arrival tim
e and width of the KCSI curves. A master equation formalism is outlined whi
ch is the basis of a data inversion providing a complete evaluation of the
experimental information content. Various examples of characteristic KCSI d
ata on collisional deactivation of highly vibrationally excited molecular p
opulations are used to discuss important aspects of the quality and the gen
eral character of P(E-',E) parameters deduced from such measurements. The c
onditions for a successful modeling of these data are very tightly bound, a
nd the resulting energy transfer parameters <Delta E(E)(n)> are therefore o
f high precision. In Paper II [J. Chem. Phys. 112, 4090 (2000), following a
rticle] we give a full account of the toluene KCSI experiments. We will dea
l with our completed studies on azulene, azulene-d(8), pyrazine and pyridin
e in follow-up publications of this series. (C) 2000 American Institute of
Physics. [S0021-9606(00)01504-X].