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The systematic admixture of high angular momentum into the low-lying states of atoms constitutes a class of correlated electron motion resulting from a single physicomathematical mechanism. In the region of configuration space where the mean-square distance of electrons from the nucleus (R²=Σi=1Nrᵢ²N) is less than its expectation value, the atomic shell structure is strongly perturbed. In the limit R→0 high angular momentum becomes more favorable energetically and the shell structure approaches that of a Fermi gas. Results include a list of configurations which mix strongly with ground states of atoms from beryllium to argon.
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M. J. Cavagnero (1984) studied this question.
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