Non-dissociative collision processes are classified and the accepted notation is given. The basic kinematics of binary collisions are derived and practical considerations based on Massey's adiabatic criterion together with the effects of pressure and temperature are discussed. A general description of instrumental developments and the performance achieved are given and the predictions of the Wigner spin conservation rule as regards the spectroscopic states of the products are summarized.Translational energy spectroscopy enables details of collisional processes to be investigated. This first part of the paper devoted to this technique attempts to set out the background necessary to understand binary elastic and inelastic non-dissociative collisions and how information concerning transfer of kinetic and internal energy can be gleaned using recently developed techniques. The resolution achieved by modern instruments is discussed and the Wigner spin-conservation rule is detailed. The second part of the paper will give detailed experimental results from the authors' laboratory and discuss tests of Wigner's hypothesis.
CLASSIFICATION OF NON-DISSOCIATIVE COLLISIONAL PROCESSESA collision between two independent bodies will produce physical changes which can include changes in deflection angle, changes in kinetic or internal potential energies, chemical changes and the gain or loss of electrons. Reactive collisions which result in chemical changes and which are only of significance at low impact energies are not dealt with. All non-reactive collisions are either classed as being elastic or inelastic. Elastic collisions only involve the exchange of kinetic energy and hence there is no change in the internal energy states of either collision partner. In contrast, inelastic collisions involve the interconversion of kinetic and internal energy, resulting in overall changes to the internal energy states of the collision partners. Inelastic collisions, during which internal energy is converted into kinetic energy are more commonly referred to as superelastic collisions.
NotationHasted' devised a useful notation method for the description of two-body inelastic collisional processes. The symbols used by Hasted to represent the collidants are listed in Table 1. In this notation, the charge and state of excitation of both collidants before and after the binary collision are specified explicitly. For example, a process in which a projectile of charge A collides with a target of charge B resulting in the production of species of charges P and Q is abbreviated using this