The static electric dipole polarizabilities of neutral inert gas atoms are obtained with the Thomas–Fermi (TF) and the Thomas–Fermi–Dirac (TFD) statistical models. The TF model yields an infinite polarizability; the TFD model yields polarizabilities which are much larger than experiment, though the percent error decreases with increasing atomic number.
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Bruch et al. (1976) studied this question.
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