One consequence of the Wannier theory of correlations between electrons is that states of high orbital angular momentum can be populated efficiently by electron impact on the ground (or a low-lying excited) state of an atom, provided the incident energy is close to the ionisation threshold of the atom. This feature was first pointed out by Fano (1974), who gave a qualitative estimate that l values up to O(n 1 2/) would be populated. A recent note by Drukarev (1982), based on an assumption of the nature of the wavefunction involved, provides a quantitative distribution which peaks at l max approximately=( 1 / 2 n) 1 2/. An alternative argument, which follows from the description of angular correlation between the electrons in O 4 group symmetry is presented and supported by numerical evidence. The peak of the distribution lies at l max approximately= 1 / 2 n 1 2/.
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A. Rau (1984) studied this question.
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