Abstract
Charge exchange in ${\mathrm{He}}^{+}$ and ${\mathrm{Ar}}^{+}$ collisions with ${\mathrm{H}}_{2}$ (${\mathrm{D}}_{2}$) and ${\mathrm{N}}_{2}$ is studied at small angles. This work extends our earlier studies which primarily emphasized the direct inelastic scattering at low keV energies. Using time-of-flight techniques for energy analysis of the scattered atoms, it is directly shown, for the first time, that in ${\mathrm{Ar}}^{+}$ + ${\mathrm{H}}_{2}$, ${\mathrm{Ar}}^{+}$ + ${\mathrm{N}}_{2}$, and ${\mathrm{He}}^{+}$ + ${\mathrm{N}}_{2}$ the dominant small-angle charge-exchange process is quasiresonant ($Q\ensuremath{\approx}0$). In ${\mathrm{He}}^{+}$ + ${\mathrm{H}}_{2}$ there is no available quasiresonant channel, and here the dominant final channels are associated with energy losses from 13 to 18 eV. A simple model is proposed.
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