Abstract
A continuum-distorted-wave (CDW) theory of charge transfer is developed to second order. Closed analytical results are obtained for the second-order CDW (CDW2) non-relativistic double-scattering Thomas total cross sections for 1sZA to nBlmZB, nBlZB and nBZB charge transfer transitions, where the omission of a quantum number implies summation. It is proven that these cross sections agree exactly with the corresponding second-order Oppenheimer-Brinkman-Kramers (OBK2) non-relativistic double-scattering Thomas cross sections. The first-order CDW (CDW1) Thomas theory is shown to be correct fortuitously for only 1sZA to 1sZB transitions. It is shown that the CDW2-OBK2 cross section for the 1sZA to nBZB transition is simply the corresponding CDW1 cross section multiplied by the Jacobi polynomial 2F1(1-nB, 1/2; 2; (4ZAZB/nB)/(ZA+ZB/nB)2). Specimen l and nB distributions are presented. It is concluded that existing criticisms of CDW theory are now well founded.

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