15min:
STIMULATED EMISSION PUMPING (SEP) SPECTROSCOPY APPLIED TO THE METHOXY RADICAL.

JINJUN LIU, Laser Spectroscopy Facility, Department of Chemistry, The Ohio State University, 120 W. 18th Avenue, Columbus, Ohio 43210 (present address: Laboratory of Physical Chemistry, ETH Zurich, Building HCI, Wolfgang-Pauli-Str. 10, 8093 Zurich, Switzerland); MING-WEI CHEN, Laser Spectroscopy Facility, Department of Chemistry, The Ohio State University, 120 W. 18th Avenue, Columbus, Ohio 43210; JOHN T. YI, Laser Spectroscopy Facility, Department of Chemistry, The Ohio State University, 120 W. 18th Avenue, Columbus, Ohio 43210 (present address: Department of Chemistry, Winston-Salem State University, Wilveria B. Atkinson Science Bldg, Room 311, Winston-Salem NC 27110); TERRY A. MILLER, Laser Spectroscopy Facility, Department of Chemistry, The Ohio State University, 120 W. 18th Avenue, Columbus, Ohio 43210.

Methoxy radical, CH3O is a widely studied and benchmark molecule, both for its spectroscopy and its role in chemical reactions. It possesses a ground 2E state which is distorted by the Jahn-Teller interaction and split into 2E1/2 and 2E3/2 components by the spin-orbit interaction. The LIF spectra of the A2A1--X2E transitions is well-known, but under jet expansion conditions the E1/2 component is not observed because it is sim60cm-1 higher than E3/2 and not populated. A feasible way to study the features of the X2E1/2 level is to use the Stimulated Emission Pumping (SEP) technique. We have combined our high-resolution laser-induced fluorescence (LIF) spectroscopic ( Delta nu sim200MHz) with a moderate-resolution laser ( Delta nu sim0.2cm-1). These lasers are controlled by a computer program, which permits both the pump and dump lasers to be fired at specified delays after the photolysis laser producing CH3O. SEP spectra of CH3O were recorded with a resolution of ~300MHz linewidth and measured with a precision <100MHz and these data were included in a global data (LIF, SEP, microwave) fitting to determine the parameters of the X2E1/2 state. The previous assignment of parity for the 2E1/2 state is modified and the value of the spin-orbit splitting revised.