The Goverment reserves for itself and others acting on its behalf a rayalty free, nonexclusive, irrevocable, world-wide license for goverrxnental purposes t o publish, distribute, translate, &plicate, exhibit, and perform ary such data aopyri*ted ky the antractor. Chapter 2 describes the photofragment ion imaging technique, which we have used to study the atomic v-J correlation in chlorine and ozone dissociation. With this technique, a three-dimensional velocity vector distribution of stat e-selectively ionized photofragments is mapped into a two-dimensional spatial distribution. Photofragments are ionized with a resonant multiphoton technique, which also provides sensitivity to angular momentum polarization. This polarization is observed as small modulations in the ion images, which depend on the probe laser polarization and on the symmetry of the chosen spectroscopic probe transition.
2Chapter 3 outlines a method for isolating and describing the contribution to the image signal which is due exclusively to angular momentum alignment. This method is based on recently-developed theoretical tools in combination with wellknown two-photon linestrength expressions. We show that four molecular excitation processes-parallel and perpendicular incoherent excitation and two types of coherent excitation-each contribute a unique spatial structure to the ion images. These mechanisms are represented by a set of alignment anisotropy parameters, which are analogous to the familiar velocity anisotropy parameter ,f3.Ion imaging results are presented and discussed in Chapter 4. We show that the alignment contribution to images of ground state chlorine atom photofragments results primarily from a perpendicular optical excitation in the parent Cl2 molecule.In order to adequately simulate the data, it was necessary to include contributions from both incoherent and coherent excitation. We also argue that nonadiabatic transitions must have occurred in the asymptotic region of the molecular potential energy curves. Preliminary measurements of polarized O( 'D2) from ozone dissociation show a strong polarization effect, which depends on the vibrational state of the 0 2 partner fragment.Chapter 5 discusses a different set of experiments on the three-fragment dissociation of azomethane. We measured appearance times and kinetic energy release for two vibrational quantum states of the methyl radical photofragments and have characterized multiphoton processes which would otherwise complicate the analysis of these data. The results are consistent with a previously proposed mechanism of a concerted dissociation following randomization of internal energy.