ArF EXCIMER LASER PHOTODISSOCIATION OF $NH_{3}$: INTERNAL ENERGY DISTRIBUTION IN $NH_{2}$ $A_{2}A$, AND $X_{2}B_{1}$

Loading...
Thumbnail Image

Date

1978

Journal Title

Journal ISSN

Volume Title

Publisher

Ohio State University

Research Projects

Organizational Units

Journal Issue

Abstract

Low pressure (P<35 mtorr) samples of NH3 are photolyzed with a Tachisto Model XR 150 pulsed excimer laser operating on the 193 nm line of ArF (20 nsec pulse duration, 35 mJ per pulse, ∼3 Hz repetition rate). Contrary to previous findings1,2 (for NH3 dissociation) in this excitation region, we find that NH2(A2A1) is a major product formed by single photon, primary photolysis. Strong NH2(A2A1X2B1) banded emission is observed between 620 and 1100 nm. Most of the lines are assignable to transitions catalogued in absorption by Dressier and Ramsay3 and Johns, Ramsay, and Ross4 The relative intensities in our emission experiments are much different than those in absorption, indicating that much of the 0.74 eV excess dissociation energy appears as bending vibrational energy and rotational excitation about the a-axis. These observations are expected, an the basis of changes in geometry in the primary photolysis process. Experiments are also under way to probe energy distributions with the NH2(X2B1) primary photofragment, Using dye laser-induced fluorescence excitation spectroscopy on the A2A1X2B1 transition. In addition, NH(A3Π) is formed in a two photon NH3 dissociation process, giving rise to a A3ΠX3Σ emission at 336 nm.

Description

1 H. Okabe and M. Lenzi, J. Chem. Phys. 47, 5241 (1967). 2 J. Masamet, A. Gilles, and C. Vermeil, J. Photochem., 3, 417 (1974/1975). 3 K. Dressler and D. A. Ramsay, Phil. Trans. Roy. Soc. London 251, 553 (1959). 4 J.W.C. Johns, D. A. Ramsay, Can. J. phys. 54, 1804 (1976). V. M. Donnelly has been a NRC/NRL Resident Research Associate.""


Author Institution: Naval Research Laboratory

Keywords

Citation