15min:
MECHANISM OF THE MULTIPHOTON DISSOCIATION OF SO2 VIA THE H RYDBERG STATE.

YUXIU LEI, Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104; EDWIN QUI NONES, Department of Chemistry, University of Puerto Rico, San Juan, PR 00931; AMITAVIKRAM A. DIXIT, KEON WOO LEE, PAUL L. HOUSTON, Department of Chemistry and Chemical Biology, Cornell University, Ithaca, NY 14853.

We will present a study on the mechanism of multiphoton dissociation of the SO2 molecule through the H Rydberg state. For this study, a homemade Wiley-McLaren linear time-of-flight (TOF) spectrometer was constructed to characterize the fragments produced during irradiation of SO2 with a laser beam in the 222 - 234 nm region. Both SO+ and S+ fragment ions were detected but no parent SO2+ appeared. The mass resolved excitation spectra (MRES) of both SO+ and S+ display the \mathrmSO2 C 1\mathrmB2 leftarrow X 1\mathrmA1 vibrational progressions. The first photon in the studied region pumps SO2 to the C 1\mathrmB2 electronic state. The second photon further excites the molecule to the H Rydberg state, where it dissociates into SO + O and S + O2 fragments. The third photon then ionizes the SO fragment. From the power dependence of the ion intensity and a kinetic model we developed, we conclude that S+ is produced by a one-photon dissociation, \mathrmSO+ + h nu rightarrow \mathrmS+ + \mathrmO. The internal energy distributions of the fragmentation products from dissociation of SO2 via the H Rydberg state were also obtained using an ion-imaging spectrometer. The following five dissociation channels are observed: SO(B 3 Sigma-) + O(3\mathrmP2), SO(A3 Pi) + O(3\mathrmP2) , S(1D) + O2(b1 Sigma_\mathrmg), S(1D) + O2(a1 Delta_\mathrmg), and S(1D) + O2(X3 Sigma-).