Collisional energy transfer probabilities of highly excited molecules from kinetically controlled selective ionization (KCSI). II. The collisional relaxation of toluene: P(E ',E) and moments of energy transfer for energies up to 50 000 cm(-1)

2000 | journal article. A publication of Göttingen

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​Collisional energy transfer probabilities of highly excited molecules from kinetically controlled selective ionization (KCSI). II. The collisional relaxation of toluene: P(E ',E) and moments of energy transfer for energies up to 50 000 cm(-1)​
Lenzer, T.; Luther, K.; Reihs, K. & Symonds, A. C.​ (2000) 
The Journal of Chemical Physics112(9) pp. 4090​-4110​.​ DOI: https://doi.org/10.1063/1.480958 

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Authors
Lenzer, T.; Luther, Klaus; Reihs, K.; Symonds, A. C.
Abstract
Complete and detailed experimental transition probability density functions P(E',E) have been determined for the first time for collisions between a large, highly vibrationally excited molecule, toluene, and several bath gases. This was achieved by applying the method of kinetically controlled selective ionization (KCSI) (Paper I [J. Chem. Phys. 112, 4076 (2000), preceding article]). An optimum P(E-',E) representation is recommended (monoexponential with a parametric exponent in the argument) which uses only three parameters and features a smooth behavior of all parameters for the entire set of bath gases. In helium, argon, and CO2 the P(E-',E) show relatively increased amplitudes in the wings-large energy gaps \E'-E\-which can also be represented by a biexponential form. The fractional contribution of the second exponent in these biexponentials, which is directly related to the fraction of the so-called "supercollisions," is found to be very small (< 0.1%). For larger colliders the second term disappears completely and the wings of P(E-',E) have an even smaller amplitude than that provided by a monoexponential form. At such low levels, the second exponent is therefore of practically no relevance for the overall energy relaxation rate. All optimized P(E-',E) representations show a marked linear energetic dependence of the (weak) collision parameter alpha(1)(E), which also results in an (approximately) linear dependence of <Delta E > and of the square root of <Delta E-2>. The energy transfer parameters presented in this study form a new benchmark class in certainty and accuracy, e.g., with only 2%-7% uncertainty for our <Delta E > data below 25 000 cm(-1). They should also form a reliable testground for future trajectory calculations and theories describing collisional energy transfer of polyatomic molecules. (C) 2000 American Institute of Physics. [S0021-9606(00)01604-4].
Issue Date
2000
Status
published
Publisher
Amer Inst Physics
Journal
The Journal of Chemical Physics 
ISSN
0021-9606

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