Abstract
Angular distributions of the fast H and dissociation fragments produced in single collisions of with have been measured in the energy range 5-80 keV. The observed distributions are discussed in terms of three dissociation reactions, → +H, , and , whose relative proportions vary strongly over the energy range of the investigation. Distributions of the component of velocity of the dissociation fragments transverse to the beam direction are deduced from the measurements. The H-atom transverse velocity distributions are approximately independent of projectile energy and are dominated by H atoms from the H+H dissociation reaction. The transverse velocity distributions vary in width as the ion energy is varied. At low energies, where the production is dominated by the +H reaction, the transverse velocity spread is narrower than at high energies where the reaction dominates the production. A theory of the dissociation mechanism which predicts the angular distribution of dissociation fragments is developed. The theory is based upon Born-approximation calculations of the dissociation cross section versus internuclear axis orientation and internuclear spacing of the ions prior to the collision. These calculations, presently available only for the case of an H-atom target and for the dissociative transition of the incident ion, were used to deduce the angular distribution of dissociation fragments in the laboratory coordinate system. Fairly comprehensive agreement is found between the calculated distribution and the observed distribution for an target at 10 keV where the H+ dissociation mode dominates the production. The theoretical model is used to discuss qualitatively the observed shapes and widths of the and H transverse velocity distributions and to relate qualitatively the shapes of these distributions to the distribution of ion internuclear spacings prior to the collision.
- Received 19 April 1965
DOI:https://doi.org/10.1103/PhysRev.140.A769
©1965 American Physical Society