“…With heavy ions, such charging phenomena should become even more important, since electron emission yields are much higher than in the case of electron or proton impact. For a carbon foil, with protons as projectiles, less than 10 electrons per incoming projectile are emitted even around the maximum of the electronic stopping power, the yield dropping below one electron per projectile for 10 MeV protons [5]. In contrast, for a heavy Kr ion at 64 MeV u −1 , it can be estimated from known scaling relations [6,7] that about 130 electrons are emitted per incoming projectile: about 100 in the forward direction (beam exit side) and about 30 in the backward direction (beam entrance side) with a carbon foil of ≈130 μg cm −2 thickness.…”