Abstract
Z2 (target atomic number) dependence of the electronic stopping powers for MeV helium-ion beams is investigated where the charge-state fractions before emerging from matter play a significant role. The electronic stopping powers for a single helium ion in various charge states and a proton (SHeq+, q=1 and 2, SH+) are calculated on the basis of Lindhard-Winther theory with the local-electron-density model. The ratio SHe+SH+ shows the Z2 oscillation as well as SHe+ and SH+. The relation between the effective charge qeff and the mean charge q¯ is elucidated in some cases of the incident energy where qeff>q¯ is valid regardless of Z2 and the qeff values show the oscillatory Z2 dependence with a small amplitude in contrast with a strong Z2 oscillation of q¯.