Scattering
Abstract
Abstract Besides the bounded, periodic classical motion of particles in potentials as shown in Fig. 5.2 (for energy E1 ), there is also the possibility of unbound states which are not localized in space and not repetitive in time; these correspond to particles incident on the potential and which subsequently “bounce “ off (energy E2 in Fig. 5.2) or temporarily change their speeds as they go over the potential (energy E3 ). Classical mechanics, which solves for the exact trajectories in either case, makes little distinction between the two types of motion aside from some tech- nical details,