We propose an electron density in atoms and ions, which has the Thomas-Ferm
i-Dirac form in the intermediate region of r, satisfies the Kato condition
for small r, and has the correct asymptotic behavior at large values of r,
where r is the distance from the nucleus. We also analyze the perturbation
in the density produced by multipolar fields. We use these densities in the
Poisson equation to deduce average values of r(m), multipolar polarizabili
ties, and dispersion coefficients of atoms and ions. The predictions are in
good agreement with experimental and other theoretical values, generally w
ithin about 20%. We tabulate here the coefficient A in the asymptotic densi
ty; radial expectation values [r(m)] for m = 2, 4, 6; multipolar polarizabi
lities alpha(1), alpha(2), alpha(3); expectation values [r(0)] and [r(2)] o
f the asymptotic electron density; and the van der Waals coefficient C-6 fo
r atoms and ions with 2 greater than or equal to Z greater than or equal to
92. Many of our results, particularly the multipolar polarizabilities and
the higher order dispersion coefficients, are the only ones available in th
e literature. The variation of these properties also provides interesting i
nsight into the shell structure of atoms and ions. Overall, the Thomas-Ferr
ni-Dirac model with the correct boundary conditions provides a good global
description of atoms and ions. (C) 1999 Academic Press.