Abstract
The authors extend the quantum theory of charge exchange in a static magnetic field to the asymmetric case and apply this theory to He2++H(1s) to He+(n=2)+H+ at velocities 0.5<or= upsilon <or=4 au and fields 0<or=B<or=4.7*104T. The principal effect occurs for upsilon <or=1.0, and is a redistribution of flux among final sublevels, so that at high fields the lowest lying level of the final manifold dominates.
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