Abstract
The inelastic energy-loss distribution Q has been measured for single large-angle collisions between argon atoms and incident projectile ions with atomic numbers Z1 ranging from 13 to 25. The data are obtained by measuring the energy and scattering angle of the scattered incident particle. This method provides well-resolved Q spectra, being almost undisturbed by thermal target motion. In all cases studied, the Q value exhibits a sudden change and a triple-peaked structure in a narrow range of distance of closest approach r0. The location of the three peaks QI, QII, and QIII varies with r0, but their energy separations remain independent of r0. For the heteronuclear collisions reported here, the values of the Q-peak separations suggest that QII and QIII correspond to the production of one and two L2,3 vacancies, respectively, in one of the colliding particles, viz., the one with the lower atomic number. This is further supported by studies of Auger electrons emitted in the collisions.