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The single-electron capture process in the collision of fast protons with ground-state helium atoms is studied assuming an independent-particle model. The three-body first-order Coulomb–Born distorted wave formalism, including nuclear–electronic and internuclear interactions, with correct boundary conditions is applied to the considered rearrangement process. A single-zeta Roothaan–Hartree–Fock wave function describing helium in its ground state is used to carry out the calculations. Differential and integrated cross sections are calculated for a range of the incident energy for which the present formalism is valid. The comparison of the obtained results with the corresponding experimental measurements and other three- and four-body theoretical calculations shows reasonable agreement.
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Ebrahim Ghanbari-Adivi (2011) studied this question.
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