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The formal development of the problem of electron-atom scattering in the presence of a laser field is considered. A time-dependent close-coupling method and a time-dependent optical-potential method are presented. With hydrogen as an example, and a weak laser tuned near the 1S-2P resonance, the effective long-range potentials are explicitly obtained. These potentials are time dependent, noncentral, and fall off as r^-n, where we limit ourselves to terms with n=2, 3, and 4. They are then used to find the elastic, inelastic, and superelastic cross sections for small momentum transfer.
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Gersten et al. (1976) studied this question.
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