Exact second-order Born calculations for relativistic electron capture

Abstract
Second-order Born cross sections for electron capture in relativistic collisions have been calculated without further approximations for a large number of projectile-target combinations and energies. Within the regime of high-Z target atoms and energies of a few GeV/u, the exactly evaluated cross sections are considerably larger than first-order cross sections, which already overestimate the experimental results. This shows that the Born expansion is not a suitable perturbation series in the charge and energy regime considered. At the same time it is demonstrated that previous evaluations using peaking approximations and αZ expansions are in error by more than an order of magnitude. For p+H collisions the differential cross section exhibits a peak at the classical relativistic Thomas angle.

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