Abstract
Differential and total cross sections for electron-transfer rearrangement collisions are calculated in the first-order Faddeev-Watson multiple-scattering approximation for a number of three-body atomic systems. For the (p+, H) system, it is shown that the inclusion of the pure p+p+ interaction to all orders (including the contributions coming from the on-shell Coulomb cuts) cancels only part of the effect given by the bare p+p+ interaction so that the present electron-transfer cross section lies in between the Brinkman-Kramers and Jackson-Schiff cross sections and asymptotically approaches the Jackson-Schiff cross section from above in the high-energy limit (where the nonrelativistic approximation is no longer expected to be valid). The knock-out contributions to the electron-transfer amplitude at large angles are particularly important for the equal-mass resonant (e+, ee+) electron-transfer collision. Owing to the e+e+ knock-out contribution, the total (e+, ee+) electron-transfer cross section exhibits an E3 energy dependence in the high-energy limit.