Abstract

We report on the measurements of double differential cross sections, at zero degree, for the production of secondary electrons from the collision of 0.6 MeV amu-1 Cu5+, I7+, Au11+, U13+, Cu19+ I23+ and Au29+ projectiles with H2 and He. The shapes and positions of the observed binary encounter electron peaks are compared with continuum distorted wave-eikonal initial state (CDW-EIS), impulse approximation and classical trajectory Monte Carlo calculations, as well as with predictions from an adiabatic resonant tunnelling model proposed by Fainstein and co-workers (1992). The experimentally observed binary peak positions were essentially determined by the projectile's ionic charge q and were independent of the projectile's nuclear charge Zp. Although the experimental conditions correspond to the strong perturbation regime. i.e. 1.0<or=q/VP<or=5.9 (VP being the projectile velocity), the CDW-EIS approach accounts well for the position and shape of the binary peak.

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