Wy. Lee et al., Ionization and dissociation mechanisms of ketene using resonance-enhanced multiphoton ionization mass spectrometer: (2+2) versus (2+1) schemes, J CHEM PHYS, 115(16), 2001, pp. 7429-7435
By using a resonance-enhanced multiphoton ionization (REMPI) technique, we
have studied ionization and photodissociation mechanisms of ketene. Prior t
o ionization, the jet-cooled ketene is first excited at a wavelength 355 nm
to a 3p(y),0(0) Rydberg state through a two-photon absorption. The (2+2) a
nd (2+1) REMPI schemes may be distinguished depending on the impinging lase
r energy. If the (2+2) REMPI process dominates, the ketene ion is produced
by the autoionization of a superexcited state, which lies in a rovibrationa
lly excited Rydberg state. The autoionization then occurs due to energy tra
nsfer from nuclear to electronic degrees of freedom. The CH2+ is fragmented
following two schemes. One is a consecutive process, i.e., the fragment io
n is produced from the autoionized ketene. This conclusion is supported by
a series of measurements of pulse field and pressure effects in this work.
The factors of pulse field and collisions may enhance the autoionization ra
te significantly, imposing the same influence on the ketene ion and CH2+. T
he second is a dissociative ionization, i.e., the CH2+ ion is fragmented fr
om the superexcited state in competition with the autoionization, as report
ed previously. These two schemes exclude the probability of ionic ladder or
neutral ladder dissociation mechanisms. On the other hand, if the (2+1) RE
MPI scheme dominates under a low ionizing laser energy, the ketene ions are
led by a direct photoionization. The increase of either pulse field intens
ity or interacting duration simply shortens the arrival time of the ketene
ion on the detector. Finally, a time-resolved ketene ion spectrum is measur
ed to characterize temporal behaviors for the autoionization and direct pho
todissociation. The relaxation lifetime for the autoionized ketene is found
to be much faster than that for the directly photoionized source. (C) 2001
American Institute of Physics.