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The frequency dependence of the hyperpolarizability ({γ}) of the nonrelativistic hydrogen atom is calculated for a range of third-order nonlinear optical processes using an expansion in Sturmian functions. It is shown that the quantitative relations between the various nonlinear optical processes are made much clearer when {γ} is treated as a function of an effective frequency ωL. The detailed, systematic exploration of the dispersion of {γ} of the hydrogen atom presented here should serve as a guide in the analysis and interpretation of experimental or theoretical results for less accessible systems.
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David P. Shelton (1987) studied this question.
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