It is shown that at a high impact velocity →v the second-order Born term can provide a significant asymmetric (skew) contribution to the cusp at |→vₑ|=|→v| in the differential cross section for "electron capture to the continuum" from a hydrogenlike atom in its $1s$ state by a bare ion, where →vₑ≈→v is the velocity of the emergent electron. The asymmetry in the cusp, heretofore unexplained, has been observed in several recent experiments.
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Shakeshaft et al. (1978) studied this question.
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